ICOMEA International Conference on Materials for Energy Applications 3 - 6 January 2017 COSDAF 超金剛石及 先進薄膜研究中心 Center Of Super-Diamond and Advanced Films TABLE OF CONTENTS: Organizing Committee …………………………………………………….. Sponsors ………………………………………………………………..….... Plenary & Invited Speakers .……………………………………….……… Conference Information ……..……………………………………….…..... Conference Venue Direction ...………………………………………….…. Program Summary ..………………………………………….…………….. Details of Technical Program ……………………………………………… January 3, 2017 (Tuesday) ……………………………………………………... 8 Registration and Welcoming Reception January 4, 2017 (Wednesday)….……………………………………………… 8 Plenary Talks I By CUI Yi and HYEON Taeghwan [LT-17] Session I-A: Organic Photovoltaics I [LT-17] Session I-B: Advanced Functional Materials and Devices I [LT-13] Session I-C Nanomaterial for Energy Applications I [LT-15] Plenary Talks II By TUNG Chen-Ho [LT-17] Session II-A: Organic Electronics [LT-17] Session II-B: Catalysis Generation and Storage I [LT-13] Session II-C Nanomaterial for Energy Applications II [LT-15] Session III-A: Organic Photovoltaics II [LT-17] Session III-B: Catalysis Generation and Storage II [LT-13] Session IIII-C Perovskite Solar Cells I [LT-15] January 5, 2017 (Thursday) ……………………………….................................. 13 Plenary Talks III By ADACHI Chihaya and ZHU Daoben [LT-17] Session IV-A: Organic Light-Emitting Diode I [LT-17] Session IV-B: Battery I [LT-13] Session IV-C Perovskite Solar Cells II [LT-15] Plenary Talks IV By WAN Li-Jun [LT-17] Session V-A: Organic Light-Emitting Diode II [LT-17] Session V-B: Battery II [LT-13] Session V-C Electrochemical Energy Storage I [LT-15] Session VI-A: Organic Light-Emitting Diode III [LT-17] Session VI-B: Battery III [LT-13] Session VI-C Electrochemical Energy Storage II [LT-15] January 6, 2017 (Friday) ……………………………………………………..…18 Session VII-A: Organic Photovoltaics III [LT-13] Session VII-B Advanced Functional Materials and Devices II [LT-15] Session VIII-A: Organic Photovoltaics IV [LT-13] Session VIII-B: Perovskite Solar Cells IV [LT-15] 1 2 3 4 5 6 8 January 5, 2017 (Thursday) ……………………………………..…………… 20 Poster Session Abstracts of Talks …………………………………………………………...23 Wednesday (Plenary Talks I, II & Session I-III) ……………………..………… 24 Thursday (Plenary Talks III, IV & Session IV-VI) …………………….............. 58 Friday (Session VII-VIII) ………………………..……………………………. 91 Abstracts of Posters …………………………………………………….…. 105 List of Participants …..……………………………………………………..139 ORGANIZING COMMITTEE: ICOMEA2017 Chair: LEE Chun-Sing Center of Super-Diamond and Advanced Films City University of Hong Kong, Hong Kong Tel: +852 3442 7826 Email: [email protected] Co-Chair: MENG Xiangmin Technical Institute of Physics and Chemistry, CAS, China Co-Chair: ZHANG Wen-Jun City University of Hong Kong, Hong Kong International Advisory Committee Members: ADACHI Chihaya, Kyushu University, Japan FORREST Stephen, University of Michigan, USA HYEON (Tag) Taeghwan, Seoul National University, Korea IMAHORI Hiroshi, Kyoto University, Japan KOCH Norbert, Humboldt-Universität zu Berlin, Germany LI Yongfang, Institute of Chemistry, CAS, China LIFSHITZ Yeshayahu, Technion – Israel Institute of Technology, Israel LOU David Xiong-Wen, Nanyang Technological University, Singapore PARK Nam-Gyu, Sungkyunkwan University, Korea WAN Li-Jun, University of Science and Technology of China, China WANG Pengfei, Technical Institute of Physics and Chemistry, China WU Chung-Chih, National Taiwan University, Taiwan YAM Vivian Wing-Wah, The University of Hong Kong, HKSAR ZHANG Hua, Nanyang Technological University, Singapore Local Organizing Committee Members: CHAN Paddy K.L., The University of Hong Kong CHOY Wallace C.H., The University of Hong Kong KIM Jang-Kyo, The Hong Kong University of Science and Technology LI Quan, The Chinese University of Hong Kong LI Yangyang, City University of Hong Kong WONG Raymond Wai Yeung, The Hong Kong Polytechnic University YAM Vivian Wing-Wah, The University of Hong Kong YAN Feng, The Hong Kong Polytechnic University YANG Shihe, The Hong Kong University of Science and Technology YU Y.W. Denis, City University of Hong Kong ZAPIEN Juan Antonio, City University of Hong Kong ZHANG Xuming, Hong Kong Polytechnic University ZHU Furong, Hong Kong Baptist University 1 SPONSORS: The organizers gratefully acknowledge financial support from:- 2 PLENARY* & INVITED SPEAKERS: (IN ALPHABETICAL ORDER) * ADACHI Chihaya, Kyushu University, Japan CHEN Chin-Ti, Institute of Chemistry, Academia Sinica, Taiwan CHEN Hongzheng, Zhejiang University, China CHEN Xiaodong, Nanyang Technological University, Singapore CHENG Huiming, Institute of Metal Research, China CHO Kilwon, Pohang University of Science and Technoloy (POSTECH), Korea * CUI Yi, Stanford University, USA DUAN Lian, Tsinghua University, China GAO Feng, Linköping University, Sweden GONG Xiong, University of Akron, USA HE Jr-Hau, King Abdullah University of Science & Technology, Kingdom of Saudi Arabia HE Le, Soochow University, China HU Bin, The University of Tennessee, Knoxville, USA & Beijing Jiaotong University, China HU Junqing, * HYEON Taeghwan, Seoul National University & Institute for Basic Science, Korea IMAHORI Hiroshi, Kyoto University, Japan JEN Alex K-Y, City University of Hong Kong, Hong Kong JIANG Yang, Hefei University of Technology, China KIM Jang-Kyo, The Hong Kong University of Science and Technology, Hong Kong KOCH Norbert, Helmholtz-Zentrum Berlin, Germany LEE Tae-Woo, Seoul National University, Korea LI Lain-Jong (Lance), King Abdullah Univ of Sci and Tech, Kingdom of Saudi Arabia LI Quan, The Chinese University of Hong Kong, Hong Kong LI Yangyang, City University of Hong Kong, Hong Kong LI Yongfang, Institute of Chemistry, CAS, China LIN Zhiqun, Georgia Institute of Technology, USA LIU Bin, Nanyang Technological University, Singapore LIU Yunqi, Institute of Chemistry, CAS, China LU Jian, City University of Hong Kong, Hong Kong PAN Xiao-Qing, University of California, Irvine, USA QIN Chuanjiang, Kyushu University, Japan SHRESTHA Lok Kumar, National Institute for Materials Science (NIMS), Japan SO Franky, North Carolina State University, USA SONG Li, University of Science and Technology of China, China SONG Weiguo, Institute of Chemistry, CAS, China TANG Jianxin, Soochow University, China TANG Yongbing, Shenzhen Institute of Advanced Technology, CAS, China TANG Zhiyong, National Center for Nanoscience and Technology (NCNST), China * TUNG Chen-Ho, Technical Institute of Physics and Chemistry, CAS, China * WAN Lijun, Institute of Chemistry, CAS, China WANG Chunru, Institute of Chemistry, CAS, China WANG Dan, Griffith University, Australia & Institute of Process Engineering, CAS, China WANG Xun, Tsinghua University, China 3 WANG Ying, Technical Institute of Physics and Chemistry, China WEI Zhixiang, National Center for Nanoscience and Technology, China WONG Ken-Tsung, National Taiwan University, Taiwan WONG Wai-Yeung Raymond, The Hong Kong Polytechnic University, Hong Kong WU Chung-Chih, National Taiwan University, Taiwan XIE Zengqi, South China University of Technology, China YAN Feng, Hong Kong Polytechnic University, Hong Kong YAN He, The Hong Kong University of Science and Technology, Hong Kong YANG Shihe, The University of Hong Kong, Hong Kong YIN Longwei, Shandong University, China YIP Hin-Lap Angus, South China University of Technology, China YONG Kijung, Pohang University of Science and Technology, Korea YOO Seunghyup, Korea Advanced Institute of Science and Technology (KAIST), Korea YU Y.W. Denis, City University of Hong Kong, Hong Kong ZHANG Hua, Nanyang Technological University, Singapore ZHANG Qichun, Nanyang Technological University, Singapore ZHAO Huijun, Griffith University, Australia ZHENG Zijian, The Hong Kong Polytechnic University, Hong Kong ZHONG Xinhua, East China University of Science and Technology, China * ZHU Daoben, Institute of Chemistry, CAS, China ZHU Furong, Hong Kong Baptist University, Hong Kong CONFERENCE INFORMATION 4 Venue Lecture Theatre 13, 15, 17 4/F. Podium, Academic Building 1, City University of Hong Kong Phone No. +852 3442 4204 Fax. No. +852 3442 0541 Mailing Address Center Of Super-Diamond and Advanced Films (COSDAF) City University of Hong Kong Tat Chee Avenue, Kowloon Tong Hong Kong SAR E-mail [email protected] / [email protected] Website http://www.cityu.edu.hk/cosdaf/ICOMEA2017/Index.html CONFERENCE VENUE DIRECTION: Venue: Lecture Theatre 13, 15, 17 4/F. Podium, Academic Building 1, City University of Hong Kong Conference Venue: LT-13, 15, 17 4/F. Podium, Academic Building 1 (AC1) City University is located near the Kowloon-Tong Mass Transit Railway (MTR) station and can be easily accessed via the #3M entrance of the Academic Building by the following transportation means: MTR Taxis Arrived at Pedestrian Subway 1. Take MTR East Rail Line or MTR Kwun Tong Line to “Kowloon Tong” station. 2. Exit at “Festival Walk” Exit C2 3. Find Shop LG1-10, take the escalator next to it, which bring you to a pedestrian subway leading to CityU. 4. Pass through the pedestrian subway, go straight, and enter Academic 1. 5. Turn right and take the escalator to level 4 to the Podium 6. You will find the Signage to Lecture Theatre 13, 15 & 17. Arrived at University Circle (U-Circle) 1. When you drop off at the University Circle, go along the covered walkway which will lead you to the Academic Building 1. 2. Walk through the red doors, you will be on the 4th floor of Academic Building 1. 5 6 PROGRAM SUMMARY Session VII-B: Advanced Functional Materials and Devices III [LT-15] (09:00-10:15) Session VIII-A: Organic Photovoltaics IV [LT-13] (10:30-12:10) Session VIII-B: Perovskite Solar Cells III [LT-15] (10:30-12:10) Session IV-C: Perovskite Solar Cells II [LT-15] (10:35-12:15) Session IV-B: Battery I [LT-13] (10:35-12:15) Session IV-A: Organic Light-Emitting Diode I [LT-17] (10:35-12:15) Session I-C: Nanomaterial for Energy Applications I [LT-15] (10:35-11:50) Session I-B: Advanced Functional Materials and Devices I [LT-13] (10:35-11:50) Session I-A: Organic Photovoltaics I [LT-17] (10:35-11:50) AM Session Lunch (City Top Restaurant, 9/F, Amenities Building) Session VII-A: Organic Photovoltaics III [LT-13] (09:00-10:15) Welcome & Opening [LT-17] (08:45-09:00) Closing Remarks & Poster Award Presentation (12:10-12:25) Group Photo Taking (11:50) Plenary Talk II [LT-17] (09:00-10:20) Plenary Talk by Prof. ADACHI Chiyaha & Prof. ZHU Daoben Plenary Talk I [LT-17] (09:00-10:20) Plenary Talk by Prof. CUI Yi & Prof. HYEON Taeghwan Jan 6, 2017 Fri Jan 5, 2017 Thu Jan 4, 2017 Wed Jan 3, 2017 Tue Tea Break (10:20-10:35) Plenary Talk III (13:30-14:10) Plenary Talk by Prof. TUNG Chen-Ho Plenary Talk IV (13:30-14:10) Plenary Talk by Prof. WAN Li-Jun Session V-C: Electrochemical Energy Storage I [LT-15] (14:15-15:10) Session V-B: Battery II [LT-13] (14:15-15:10) Session VI-C: Electrochemical Energy Storage II [LT-15] (16:35-17:30) Session VI-B: Battery III [LT-13] (16:35-17:30) Session VI-A: Organic Light-Emitting Diode III [LT-17] (16:35-17:30) Session III-C: Perovskite Solar Cells I [LT-15] (15:50-17:20) Session III-B: Catalytic-Splitting for Energy Applications II [LT-13] (15:50-17:20) Session III-A: Organic Photovoltaics II [LT-17] (15:50-17:20) Conference Banquet Session V-A: Organic LightEmitting Diode II [LT-17] (14:15-15:20) Session II-C: Nanomaterial for Energy Applications II [LT-15] (14:15-15:30) Session II-B: Catalytic-Splitting for Energy Applications I [LT-13] (14:15-15:30) Session II-A: Organic Electronics [LT-17] (14:15-15:30) PM Session (16:00-18:00) Tea Break Outside LT-15 Poster Session [Outside LT-15] (15:10-16:35) Registration & Welcoming Reception Jan 5, 2017 Thu Jan 6, 2017 Fri Jan 4, 2017 Wed Jan 3, 2017 Tue 7 DETAILS OF TECHNICAL PROGRAM TUESDAY January 3, 2017 16:00 – 18:00 Registration with Welcoming Reception [Venue: Outside LT-15, Academic Building 1] WEDNESDAY January 4, 2017 07:45 Registration [Venue: Outside LT-15, Academic Building 1] 08:45 Welcome & Opening [Venue: LT-17, Academic Building 1] LU Jian Vice President of Research and Technology City University of Hong Kong, Hong Kong Plenary Talks I Venue: LT-17, Academic Building 1 Chairman: TANG Zhiyong (National Center for Nanoscience and Technology (NCNST), China) 09:00 Plenary 1.1 Nanomaterials Design for Energy CUI Yi Stanford University, USA [Plenary] 09:40 Plenary 1.2 Engineering Archtecture Of Oxide And Chalcogenide Nanomaterials For Energy Applications HYEON Taeghwan [Plenary] 10:20 8 BREAK & POSTER VIEWING Session I-A: Organic Photovoltaics I Venue: LT-17, Academic Building 1 Chairman: SO Franky (North Carolina State University, USA) 10:35 1.1.1 Metalloporphyrin-Based Small Molecules for Photovoltaic Applications ZHU Xunjin, WONG Wai-Kwok, WONG Wai-Yeung (Raymond) The Hong Kong Polytechnic University, Hong Kong [Invited] 11:00 1.1.2 Interface and Tandem Design for Polymer and Perovskite Solar Cells YIP Hin-Lap South China University of Technology, Guangzhou, China [Invited] 11:25 1.1.3 Molecular Approach for Donor-Acceptor Linked Systems and Organic Photovoltaics IMAHORI Hiroshi Kyoto University, Japan [Invited] Session I-B: Advanced Functional Materials and Devices I Venue: LT-13, Academic Building 1 Chairman: HE Le (Soochow University, China) 10:35 1.2.1 11:00 1.2.2 11:25 1.2.3 2D Transition Metal Dichalcogenide Monolayer: A Promising Candidate for Next Generation Electronics LI Lain-Jong (Lance) King Abdullah University of Science and Technology, Kingdom of Saudi Arabia [Invited] Synthesis and Applications of Novel Two-Dimensional Nanomaterials ZHANG Hua Nanyang Technological University, Singapore [Invited] Fullerene Nanoarchitectonics from Zero to Higher Dimensions SHRESTHA Lok Kumar National Institute for Materials Science (NIMS), Japan [Invited] Session I-C: Nanomaterial for Energy Applications I Venue: LT-15, Academic Building 1 Chairman: KIM Jang Kyo (The Hong Kong University of Science and Technology, Hong Kong) 10:35 1.3.1 Nanocarbons for Electrochemical Energy Storage CHENG Hui-Ming Institute of Metal Research, Chinese Academy of Sciences, China [Invited] 11:00 1.3.2 Structural Nanomaterials For Advanced Energy Systems (Nuclear, Solar, Ocean Thermal Energy Conversion) LU Jian City University of Hong Kong, Hong Kong [Invited] 11:25 1.3.3 Compromising Nanocarbons and Layered Materials for Energy Applications SONG Li University of Science and Technology of China, China [Invited] 11:50 GROUP PHOTO TAKING 12:10 LUNCH (City Top Restaurant, 9/F, Amenities Building) 9 Plenary Talks II Venue: LT-17, Academic Building 1 Chairman: TANG Jianxin (Soochow University, China) 13:30 Plenary 2.1 Photocatalytic Splitting of Water into Molecular Hydrogen and Oxygen TUNG Chen-Ho, WU Li-Zhu, LI Zhi-Jun Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, China [Plenary] Session II-A: Organic Electronics Venue: LT-17, Academic Building 1 Chairman: TANG Jianxin (Soochow University, China) 14:15 2.1.1 Design and Synthesis of Semiconducting Polymers for High-Performance Field-Effect Transistors LIU Yunqi Institute of Chemistry, Chinese Academy of Sciences, China [Invited] 14:40 2.1.2 Advanced Nanotechnology For High-Performance Photovoltaic Devices YAN Feng The Hong Kong Polytechnic University, Hong Kong [Invited] 15:05 2.1.3 Flexible, Foldable and Multi-Functional Paper-Based Electronics HE Jr-Hau King Abdullah University of Science and Technology, Kingdom of Saudi Arabia [Invited] Session II-B: Catalysis Generation and Storage I Venue: LT-13, Academic Building 1 Chairman: SONG Weiguo (Institute of Chemistry, Chinese Academy of Sciences, China) 10 14:15 2.2.1 Combination of Biomimicking Methods of Natural Leaf: Regeneration of Nonwetting Surface using Solar water Splitting YONG Kijung, LEE Junghan, BAEK Seunghyun POSTECH, Korea [Invited] 14:40 2.2.2 Promoting Catalytic Properties of Nanocrystals by Tuning Their Chemical Environments WANG Xun Tsinghua University, China [Invited] 15:05 2.2.3 Unlocking Catalytic Potentials of Earth Abundant Materials for Energy Conversion and Device Fabrication ZHAO Huijun Griffith University, Australia [Invited] Session II-C: Nanomaterial for Energy Applications II Venue: LT-15, Academic Building 1 Chairman: SONG Li (University of Science and Technology of China, China) 14:15 2.3.1 14:40 2.3.2 15:05 2.3.3 15:30 Multi-Shelled Metal Oxides Hollow Microspheres: Synthesis, property & Application WANG Dan Griffith University, Australia & Institute of Process Engineering, CAS, China [Invited] Unlocking Catalytic Potentials of Earth Abundant Materials for Energy Conversion and Device Fabrication XU Zheng-Long, KIM Jang-Kyo The Hong Kong University of Science and Technology, Hong Kong [Invited] Hierarchical composite structure of few-layers MoS2 nanosheets supported by vertical graphene on carbon cloth for lithium ion battery and hydrogen evolution reaction electrodes ZHANG Zhenyu, ZHANG Wen-Jun City University of Hong Kong, Hong Kong BREAK & POSTER VIEWING Session III-A: Organic Photovoltaics II Venue: LT-17, Academic Building 1 Chairman: YAN Feng (The Hong Kong Polytechnic University, Hong Kong) 15:50 3.1.1 Dielectric Properties of Polymer-Fullerene Blends for High Performance Solar Cells SO Franky North Carolina State University, USA [Invited] 16:15 3.1.2 Planar Organic Heterojunctions: From Photovoltaic Cell To Charge Generation Layer OPITZ Andreas, KOCH Norbert, BRÜTTING Wolfgang,MOONS Ellen Humboldt-Universität zu Berlin, Germany 16:30 3.1.3 Vacuum-Processed High Efficiency Organic Solar Cells Based on Small Molecule WONG Ken-Tsung National Taiwan University, Taiwan [Invited] 16:55 3.1.4 Design Fullerene Acceptor Materials for High-performance Polymer Solar Cells WANG Chunru, ZHAO Fuwen, JIANG Li, MENG Xiangyue Institute of Chemistry, Chinese Academy of Sciences, China [Invited] 17:20 3.1.5 An Insight on Oxide Interlayer in Organic Photovoltaics: From Light Harvesting, Charge Recombination and Collection Perspectives WU Bo, LAN Weixia, ZHU Furong Hong Kong Baptist University, Hong Kong [Invited] 11 Session III-B: Catalysis Generation and Storage I Venue: LT-13, Academic Building 1 Chairman: ZHAO Huijun (Griffith University, Australia) 15:50 3.2.1 Nanoscale Metal-Organic Frameworks: Emerging Materials for Catalysis TANG Zhiyong National Center for Nanoscience and Technology, China [Invited] 16:15 3.2.2 Theoretical Calculations of Electrochemical Activities of Cu-BHT Nanostructures on Catalyzing Hydrogen Evolution Reaction YAO Huiying, HUANG Xing, HAO Wei, ZHU Jia, LI Shuzhou, XU Wei Beijing Normal University, China 16:30 3.2.3 Carbon based Nanostructures for High Performance Catalysis SONG Weiguo Institute of Chemistry, Chinese Academy of Sciences, China [Invited] 16:55 3.2.4 Improving Electron Transport in Nanostructured TiO2 Electrode LIU Bin Nanyang Technological University, Singapore [Invited] Session III-C: Perovskite Solar Cells I Venue: LT-15, Academic Building 1 Chairman: CHEN Chin-Ti (Institute of Chemistry, Academia Sinica, Taiwan) 15:50 3.3.1 16:15 3.3.2 16:30 3.3.3 Rational Material Design, Interface, and Device Engineering for High-Performance Polymer and Perovskite Solar Cells JEN K-Y (Alex) City University of Hong Kong, Hong Kong [Invited] 16:55 3.3.4 Energy Levels In Organic- And Perovskite-Based Photovoltaic Cells KOCH Norbert Humboldt-Universität zu Berlin, Germany [Invited] 18:00 12 High Efficiency Organic-Inorganic Hybrid Perovskite Solar Cells and Light-Emitting Diodes CHO Himchan, KIM Young-Hoon, AHN Soyeong, JEONG Su-Hun, PARK Min-Ho, LEE Tae-Woo Seoul National University, Korea [Invited] Robust Interface Engineering For Planar Perovskite Solar Cells Via A Low Temperature, Stable And Solution Process HE Zhubing South University of Science and Technology of China, China BANQUET THURSDAY January 5, 2017 Plenary Talks III Venue: LT-17, Academic Building 1 Chairman: WU Chung-Chih (National Taiwan University, Taiwan) 09:00 Plenary 3.1 Control Of Excitonic Processes In Organic Semiconductors Aimed For High Performance Oleds And Organic Lasers TSANG Daniel Ping-Kuen, NAKANOTANI Hajime, SANDANAYAKA Atula S. D., MATSUSHIMA Toshinori, ADACHI Chihaya Kyushu University, Japan [Plenary] 09:40 Plenary 3.2 Thermoelectric Conversion: New Opportunities and Challenges of Organic Materials ZHU Daoben Institute of Chemistry,Chinese Academy of Sciences, China [Plenary] 10:20 BREAK & POSTER VIEWING Session IV-A: Organic Light-Emitting Diode I Venue: LT-17, Academic Building 1 Chairman: YOO Seunghyup (Korea Advanced Institute of Science and Technology (KAIST), Korea) 10:35 4.1.1 11:00 4.1.2 11:25 4.1.3 11:50 4.1.4 Highly Efficient And Color-Stable Hybrid White Organic LightEmitting Diodes Using A Blue Emitter With Thermally Activated Delayed Fluorescence DUAN Lian Tsinghua University, China [Invited] Controllable Synthesis of Highly-Fluorescent Cesium Lead Halide Perovskite Quantum Dots and Their Use in White Light Emitting Diodes JIANG Yang, LI Guopeng, CHANG Yajing, ZHU Zhifeng, WANG Hui Hefei University of Technology (HFUT), China [Invited] Enhanced Extraction in Flexible OLEDs with Nanostructured Substrates TANG Jianxin Soochow University, China [Invited] Development of High EQE OLEDs: from Efficient Internal Generation to External Extraction WU Chung-Chih, WONG Ken-Tsung, CHI Yun National Taiwan University, Taiwan [Invited] 13 Session IV-B: Battery I Venue: LT-13, Academic Building 1 Chairman: YU Y.W. (Denis) (City University of Hong Kong, Hong Kong) 10:35 4.2.1 Rational Materials Design for Ultrafast Rechargeable Lithium-ion Batteries CHEN Xiaodong Nanyang Technological University, Singapore [Invited] 11:00 4.2.2 Hierarchically Porous Materials as Electrodes for Energy Storage Batteries YIN Longwei, LI Zhaoqiang, GE Xiaoli, ZHANG Zhiwei, LI Qun Hefei University of Technology (HFUT), China [Invited] 11:25 4.2.3 Developing Sn Based Alloy Materials For Anode Applications In NaIon Batteries WANG Wenhui, LAN Danni, LI Quan The Chinese University of Hong Kong, Hong Kong [Invited] 11:50 4.2.4 Recent Progress of the Novel Aluminum-Graphite Dual-Ion Battery ZHANG Xiaolong, ZHANG Fan, TONG Xuefeng, JI Bifa, SHENG Maofa, LEE Chun-Sing, TANG Yongbing Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, China [Invited] Session IV-C: Perovskite Solar Cells II Venue: LT-15, Academic Building 1 Chairman: KOCH Norbert (Humboldt-Universität zu Berlin, Germany) 10:35 4.3.1 High Performance Solution-Processed Perovskite Hybrid Solar Cells via Device Engineering and Novel Materials GONG Xiong The University of Akron, USA [Invited] 11:00 4.3.2 Stable Planar Perovskite Solar Cells under Continuous Light Irradiation QIN Chuanjiang, MATSUSHIMA Toshinori, ADACHI Chihaya Kyushu University, Japan [Invited] 11:25 4.3.3 11:50 4.3.4 Surfactant n-Dopant in Cathode Interlayer or Electron Transport Layer for Polymer or Perovskite Solar Cells with Improving Performance CHANG Chih-Yu, HUANG Wen-Kuan, LEE Kuan-Ting, WU Jhao-Lin, CHEN Chao-Tsen, CHEN Chin-Ti 3Institute of Chemistry, Academia Sinica, Taiwan [Invited] Interface and Crystallization Engineering of Organic/Inorganic Hybrid Materials for High-Performance Perovskite Solar Cells YANG Shihe The Hong Kong University of Science and Technology, Hong Kong [Invited] 12:15 14 LUNCH (City Top Restaurant, 9/F, Amenities Building) Plenary Talks IV Venue: LT-17, Academic Building 1 Chairman: JIANG Yang (Hefei University of Technology, China) 13:30 Plenary 4.1 Electrochemical Process and Interfacial Structure in Lithium-Sulfur Battery: Materials and in Situ AFM Study WAN Li-Jun Institute of Chemistry, Chinese Academy of Sciences, and University of Science and Technology of China, China [Plenary] Session V-A: Organic Light-Emitting Diode II Venue: LT-17, Academic Building 1 Chairman: : JIANG Yang (Hefei University of Technology, China) 14:15 5.1.1 14:40 5.1.2 14:55 5.1.3 Multilayer Transparent Electrodes: from Flexible OLEDs to Seethrough Solar Cells YOO Seunghyup, LEE Jaeho, KIM Hoyeon Korea Advanced Institute of Science and Technology (KAIST), Korea [Invited] Triplet Harvesting in Fluorescence and Phosphorescence Hybrid White OLEDs LIU Xiaoke, LEE Chun-Sing, ZHANG Xiao-Hong Linköping University, Sweden Novel Thermally Activated Delayed Fluorescence MaterialsThioxanthone Derivatives and Their Application for OLEDs WANG Ying, WANG Hui, MENG Lingqiang, XIE Lisha, LV Xiaopeng, WANG Pengfei Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, China [Invited] Session V-B: Battery II Venue: LT-13, Academic Building 1 Chairman: : LI Quan (The Chinese University of Hong Kong, Hong Kong) 14:15 5.2.1 14:40 5.2.2 14:55 5.2.3 15:10 5.2.4 In-Situ Measurement Of The Thickness Change Of Dense Si Electrodes In Lithium-Ion Batteries Using Electrochemical Dilatometry LEE Pui-Kit, LI Yingshun, YU Y.W. (Denis) City University of Hong Kong, Hong Kong [Invited] Improved Electrochemical Performance Of Sno2/CNT Anodes For Na-Ion Batteries With Controlled Crystallinity And Reaction Kinetics CUI Jiang, YAO Shanshan, KIM Jang-Kyo The Hong Kong University of Science and Technology, Hong Kong Nanorod to Porous Nanofibers: a Novel Strategy to Improve Lithium-Ion Storage LI Huan-Huan, ZHANG Jing-Ping Northeast Normal University, China Functional Polymer Electrolytes For Flexible Energy Storage Devices ZHI Chunyi City University of Hong Kong, Hong Kong 15 Session V-C: Electrochemical Energy Storage I Venue: LT-15, Academic Building 1 Chairman: : PAN Xiao-Qing (University of California, Irvine, USA) 14:15 5.3.1 14:40 5.3.2 14:55 5.3.3 15:10 Functional Porous Nanomaterials Enabled By Convenient Electrochemical Methods For Energy Applications BIAN Haidong, XIAO Xufen, WANG Aiwu, ZENG Shanshan, ZHAN Yawen, LI Yang Yang City University of Hong Kong, Hong Kong [Invited] Nanorod to Porous Nanofibers: a Novel Strategy to Improve Lithium-Ion Storage NAZARIAN-SAMANI Masoud, HAGHIGHAT-SHISHAVAN Safa, KIM Myeong-Seong, LEE Suk-Woo, KASHANI-BOZORG Seyed Farshid, KIM Kwang-Bum Yonsei University, Korea Nanowire Devices for Electrochemical Energy Storage MAI Liqiang, ZHAO Yunlong, NIU Chaojiang Wuhan University of Technology, China POSTER SESSION Session VI-A: Organic Light-Emitting Diode III Venue: LT-17, Academic Building 1 Chairman: DUAN Lian (Tsinghua University, China) 16 16:35 6.1.1 17:00 6.1.2 17:15 6.1.3 Effects of Spin States in Perovskite Solar Cells and Light-emitting Devices HU Bin The University of Tennessee, Knoxville, USA and Beijing Jiaotong University, China [Invited] High-efficiency Nondoped Deep Blue Light-emitting Materials Based on Bisphenanthroimidazole Derivatives TONG Qing-Xiao, LEE Chun-Sing, CHEN Wen-Cheng Shantou University, China Highly Efficient Blue-Green-Emitting Diodes With Cationic Iridium(III) Complexes MA Dongxin, QIU Yong, DUAN Lian Tsinghua University, China Session VI-B: Battery III Venue: LT-13, Academic Building 1 Chairman: YIN Longwei (Shandong University, China) 16:35 6.2.1 Conjugated Polymers as promising electrode materials for Li-ion Batteries ZHANG Qichun Nanyang Technological University, Singapore [Invited] 17:00 6.2.2 Sub-2nm Thick Fluoroalkylsilane Self-Assembled Monolayer-Coated High Voltage Spinel Crystals as Promising Cathode Materials for Lithium Ion Batteries ZETTSUA Nobuyuki, TESHIMA Katsuya Shinshu University, Japan 17:15 6.2.3 Charge-driven Synthesis of Straw-sheaf-like Cobalt Oxides with Excellent Cyclability and Rate Capability for Advanced Lithium-ion Batteries LU Xiao-Ying, WANG Bin, AU Wai Kuen, GUO Hongfan Technological and Higher Education Institute of Hong Kong, Hong Kong Session VI-C: Electrochemical Energy Storage II Venue: LT-15, Academic Building 1 Chairman: LI Yangyang (City University of Hong Kong, Hong Kong) 16:35 6.3.1 Epitaxial CaTi5O11 and TiO2-B Thin Films for High Rate LithiumIon Batteries PAN Xiao-Qing University of California – Irvine, USA [Invited] 17:00 6.3.2 Enhancing The Anode Performance Of Antimony Through NitrogenDoped Carbon And Carbon Nanotubes LIU Xia, DAI Zhihui Nanjing Normal University, China 17:15 6.3.3 Composition and Interface Engineering of MoS2xSe2-2x Nanosheets for Superior Electrochemical Performance XU Jun Hefei University of Technology, China 17 FRIDAY January 6, 2017 Session VII-A: Organic Photovoltaics III Venue: LT-13, Academic Building 1 Chairman: GAO Feng (Linköping University, Sweden) 09:00 7.1.1 Non-fullerene acceptor-based polymer solar cells with high opencircuit voltage CHEN Hongzheng Zhejiang University, China [Invited] 09:25 7.1.2 09:50 7.1.3 Ternary Blends For Large Area Flexible Organic Solar Cells ZHANG Yajie, ZHANG Jianqi, LU Kun, WEI Zhixiang National center for Nanoscience and Technology, Chinese Academy of Sciences, China [Invited] Photoconductive Cathode Interlayers for High Performance Organic Solar Cells XIE Zengqi South China University of Technology, China [Invited] Session VII-B: Advanced Functional Materials and Devices II Venue: LT-15, Academic Building 1 Chairman: SHRESTHA Lok Kumar (National Institute for Materials Science (NIMS). Japan) 09:00 7.2.1 Functional Optical Nanostructures: Assembly, Properties and Applications HE Le, ZHANG Xiao-Hong Soochow University, China [Invited] 09:25 7.2.2 Interesting Flowing Of Molten Metal/Alloy In A Nanotube/Nanowire ZOU Rujia, LIU Qian, ZHANG Zhenyu, HU Junqing Donghua University, China [Invited] 09:50 7.2.3 High-performance Wearable Supercapacitor Textiles ZHENG Zijian The Hong Kong Polytechnic University [Invited] 10:15 18 BREAK & POSTER VIEWING Session VIII-A: Organic Photovoltaics IV Venue: LT-13, Academic Building 1 Chairman: WEI Zhixiang (National center for Nanoscience and Technology, Chinese Academy of Sciences, China) 10:30 8.1.1 10:55 8.1.2 11:20 8.1.3 Metal Nanoparticle-assisted Crystallization of Perovskite Active Layer for High Performance Solar Cells ALI Asgher Syed, ZHU Furong The Hong Kong Baptist University, Hong Kong 11:35 8.1.4 Two-Dimension-Conjugated Polymer Donor Materials for Polymer Solar Cells LI Yongfang Institute of Chemistry, Chinese Academy of Sciences, China [Invited] Molecular Orientation-Dependent Photovoltaic Performance in Organic Solar Cells CHO Kilwon Pohang University of Science and Technology, Korea [Invited] Non-Radiative Recombination In Organic Solar Cells GAO Feng Linköping University, Sweden [Invited] Session VIII-B: Perovskite Solar Cells III Venue: LT-15, Academic Building 1 Chairman: GONG Xiong (The University of Akron, USA) 10:30 8.2.1 High Efficiency Quantum Dot Sensitized Solar Cells ZHONG Xinhua East China University of Science and Technology, China [Invited] 10:55 8.2.2 11:20 8.2.3 Engineering Light Absorption and Film Crystallization for HighEfficiency Perovskite Solar Cells HE Ming, LIN Zhiqun Georgia Institute of Technology, USA [Invited] Efficient Non-fullerene Organic Solar Cells with a Negligible Charge Separation Driving Force YAN, He The Hong Kong University of Science and Technology, Hong Kong [Invited] 12:00 CLOSING REMARKS & POSTER AWARD PRESENTATION (LT-13) 12:20 LUNCH (City Top Restaurant, 9/F, Amenities Building) ----- End ----- 19 THURSDAY January 5, 2017 Poster Session Venue: Outside LT-15, Academic Building 1 Time: 15:10-16:35 P-01 P-02 P-03 P-04 P-05 Boosting the Performances of Perovskite Photodetectors by Periodic NanoGrating Hole Transporting Layer LI Ning, ALI Asgher Syed, , ZHU Furong Hong Kong Baptist University, Hong Kong Improved efficiency and stability of organic photovoltaic device using UVozone treated ZnO anode buffer CHAN Chiu-Yee, WEI Yu-Fang, THACHOTH CHANDRAN Hrisheekesh, LEE Chun-Sing, LO Ming-Fai, NG Tsz-Wai City University of Hong Kong, Hong Kong Low-Temperature-Processed Flexible Organic-Inorganic Hybrid Heterojunction Rectified Diodes CHANG Ching-Hsiang, HSU Chao-Jui, WU Chung-Chih National Taiwan University, Taiwan Anodic nanoporous SnO2 grown on Cu foils as superior binder-free Na-ion battery anodes BIAN Haidong, ZHANG Jie, YUEN Muk-Fung, KANG Wenpei, ZHANG Yawen, YU Denis Y.W., XU Zhengtao, LI Yang City University of Hong Kong, Hong Kong First-Principles Design of Iron-Based Active Catalysts for Adsorption and Dehydrogenation of H2O Molecule on Fe(111), W@Fe(111), and W2@Fe(111) Surfaces HSIAO Ming-Kai, YAO Bo-Ting, JU Shin-Pon, CHEN Hui-Lung P-06 P-07 P-08 P-09 P-10 20 Chinese Culture University, Taiwan Highly Efficient Deep-Blue Electroluminescence from a Charge-Transfer Emitter with Stable Donor Skeleton CHEN Wen-Cheng, LEE Chun-Sing City University of Hong Kong, Hong Kong High-Performance Color-Tunable Perovskite Light Emitting Devices through Structural Modulation from Bulk to Layered Film CHEN Ziming, ZHANG Chongyang, JIANG Xiao-Fang, LIU Meiyue, XIA Ruoxi, SHI Tingting, CHEN Dongcheng, XUE Qifan, ZHAO Yu-Jun, SU Shijian, YIP Hin-Lap, CAO Yong South China University of Technology, China The Detrimental Effect of Excess Mobile Ions in Planar CH3NH3PbI3 Perovskite Solar Cells CHENG Yuanhang, LI Ho-Wa, XIE Yuemin, XU Xiuwen, TSANG Sai Wing City University of Hong Kong, Hong Kong Edge-exposed Graphene Flexible Supercapacitor with Polymer Electrolyte CHOI Yeon Jun, LEE Suk Woo, LEE Geon-Woo, PARK Byung-Hoon, KIM Tae-Ho, JUNG Dae Soo, KIM Kwang-Bum Yonsei University, Korea Flexible Fiber-Shaped Supercapacitor Based On Nickel-Cobalt Double Hydroxide And Pen Ink Electrodes On Metallized Carbon Fiber GAO Libo, LU Yang City University of Hong Kong, Hong Kong P-11 Low-Light Photodetectors and Photovoltaics Based on Si/PEDOT:PSS Hybrid Devices TSAI Meng-Lin, TANG Libin, CHEN Lih-Juann, LAU Shu-Ping, HE Jr-Hau King Abdullah University of Science and Technology, P-12 High-Rate Li4Ti5O12/N-doped Reduced Graphene Oxide Composite for High Power Energy Storage Devices JEONG Jun Hui, KIM Myeong-Seong, KIM Young-Hwan, KIM Kwang-Bum Yonsei University, Korea Enhanced Light Harvesting in Perovskite Solar Cells via Nanostructures Patterned Fullerene Passivation Layers WEI Jian, XU Rui-Peng, TANG Jian-Xin Soochow University, China Activated Graphene Microspheres for Supercapacitor Application KIM Young-Hwan, KIM Kwang-Bum Yonsei University, Korea Sn4P3 Nanotops Based Anodes for Sodium Ion Batteries LAN Danni, WANG Wenhui, LI Quan The Chinese University of Hong Kong, Hong Kong On the Study of Exciton Binding Energy with Direct Charge Generation in Photovoltaic Polymers LI Ho-Wa, GUAN Zhiqiang, CHENG Yuanhang, LUI Taili, YANG Qingdan, LEE Chun-Sing, CHEN Song, TSANG Sai-Wing City University of Hong Kong, Hong Kong Rational Design of Hollow Carbon Nanofibers Inserted MnO Micro-Nano Spheres with Enhanced Electrochemical Performance for Li-Ion Batteries LI Huan-Huan, ZHANG Jing-Ping Northeast Normal University, China. Solution-Processed, Mercaptoacetic Acid-Engineered Quantum Dots Photocathode for Efficient Hydrogen Generation under Visible Light Irradiation LIU Bin, LI Xu-Bing, WU LI-Zhu, TUNG Chen-Ho, ZHANG Wen-Jun City University of Hong Kong, Hong Kong Low Temperature Processed Photoconductive Cathode Interlayer For Inverted Polymer Solar Cells LUO Yinqi, XIE Zengqi South China University of Technology, China Various Morphologies Of WO3 Nanostructures Fabricated By Hydrothermal Methods And Its Effects On Photo-Catalytic Properties PARK Soo-Min, RYU Sung-Myung, NAM Chunghee Hannam University, Korea Efficient Thermally Activated Delayed Fluorescence OLEDs Based on Functional Phenylpyridinato Boron Complexes SHIU Yi-Jiun, CHEN Yi-Ting, LEE Wei-Kai, WU Chung-Chih, LIN Tzu-Chieh, LIU Shih-Hung, CHOU Pi-Tai, LU Chin-Wei, CHENG I-Chen, LIEN Yi-Jyun, CHI Yun National Taiwan University, Taiwan Metal-Oxide-Semiconductor (MOS) Photoanodes For Photoelectrochemical Water Splitting Devices SHI Yuanyuan, HAN Tingting, SONG Xiaoxue, MIO Antonio, VALENTI Luca, PRIVITERA Stefania, LOMBARDO Salvatore, LANZA Mario Soochow University, China User Infrastructures for Energy Material Science at the Helmholtz Zentrum Berlin für Materialien und Energie HZB VOLLMER Antje Helmholtz Zentrum Berlin für Materialien und Energie, Germany Kingdom of Saudi Arabia P-13 P-14 P-15 P-16 P-17 P-18 P-19 P-20 P-21 P-22 P-23 21 P-24 P-25 P-26 P-27 P-28 P-29 P-30 P-31 P-32 P-33 Enhanced Cycle Performance Of Sn4P3 Anode in Na-Ion Batteries Using TiC WANG Wenhui, LI Quan The Chinese University of Hong Kong, Hong Kong Studies of Charge Recombination and Collection Behaviors in Non-fullerene Based Organic Solar Cell WANG Yiwen, ZHU Furong Hong Kong Baptist University, Hong Kong Theoretical Calculations of Electrochemical Activities of Cu-BHT Nanostructures on Catalyzing Hydrogen Evolution Reaction YAO Huiying, HUANG Xing, HAO Wei, ZHU Jia, LI Shuzhou, XU Wei Beijing Normal University, China Amorphous Red P Encapsulated In Hollow Porous Carbon Nanoshpere For Sodium Storage With Exceptional Long-Term Cyclic Stability YAO Shanshan, CUI Jiang, KIM Jang-Kyo The Hong Kong University of Science and Technology, Hong Kong High Efficiency Hysteresis-Free Perovskite Solar Cells With A Solution Processed Vanadium Oxide (VOx) Hole Extraction Layer YAO Xiang, GONG Xiong South China University of Technology, China Color-Tunable Microwave Synthesis of Cadimum-Free ZnS:Cu Nanocrystals and Potential Application for LEDs ZHANG Kui, CHEN Shengmei, ZAPIEN Juan Antonio City University of Hong Kong, Hong Kong Increase the Stability of TADF based OLED by Using Modified Carbazole with Tert-Butyl and Phenyl DUAN Lian, ZHANG Yunge Tsinghua University, China Hierarchical Composite Structure of Few-Layers MoS2 Nanosheets Supported by Vertical Graphene on Carbon Cloth for Lithium Ion Battery and Hydrogen Evolution Reaction Electrodes ZHANG Zhenyu, ZHANG Wen-Jun City University of Hong Kong, Hong Kong A Dual-Ion Battery Constructed with Aluminum Foil Anode and Mesocarbon Microbead Cathode in an Ionic Liquid Electrolyte ZHANG Fan, JI Bifa, TONG Xuefeng, SHENG Maohua, TANG Yongbing, LEE Chun-Sing City University of Hong Kong, Hong Kong Epitaxy of Layered Orthorhombic SnS-SnSxSe(1-x) Core-Shell Heterostructures with Anisotropic Photoresponse XIA Jing, MENG Xiang-Min Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, China ----- End ----- 22 Abstract of Talks 23 Plenary1.1 Nanomaterials Design for Energy 1 Yi Cui1,2*# Department of Materials Science and Engineering, Stanford University, USA; 2 Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, USA Keywords: Nanomaterials, Energy, Battery, Catalysis, textile. Materials design at nanoscale has enabled novel technologies which can address critical energy problems. My group’s research in the past decade has been focused on innovative ideas in this area. Here I will show multiple examples how nanomaterials design can allow us to control photons, electrons, ions and heat. Examples include: 1) high energy batteries; 2) electrochemical tuning of catalysts 3) cooling and heating textile for personal thermal management. # * Presenting Author Corresponding Author 24 Plenary1.2 Engineering Architecture of Oxide and Chalcogenide Nanomaterials For Energy Applications Taeghwan Hyeon1,2 1 Center for Nanoparticle Research, Institute for Basic Science (IBS), Seoul 151-742, Korea; 2School of Chemical and Biological Engineering, Seoul National University, Seoul 151-742, Republic of Korea. Engineering of dimension, shape, and topology of nanomaterials is critical for their energy device applications. Over the last 17 years, our laboratory has focused on the designed chemical synthesis, assembly and applications of uniform-sized nanocrystals. More recently we have been focused on the architecture engineering of nanomaterials for their applications to lithium ion battery, fuel cell electrocatalysts, solar cells, and thermoelectrics. For example, we demonstrated galvanic replacement reactions in metal oxide nanocrystals for the first time. When Mn3O4 nanocrystals were reacted with iron(II) perchlorate, hollow box-shaped nanocrystals of Mn3O4/γ-Fe2O3 were produced. These oxide-based nanomaterials exhibit very high specific capacity and good cyclability for lithium ion battery anodes. We report a simple synthetic method of carbon-based hybrid cellular nanosheets loaded with SnO2 nanoparticles. The resulting SnO2-carbon nanosheets exhibit specific capacity of 914 mAh g-1 with the retention of 97.0% during 300 cycles, and the reversible capacity is decreased by only 20% as the current density is increased from 200 mA g-1 to 3000 mA g-1. We present a synthesis of highly durable and active intermetallic ordered face-centered tetragonal (fct)-PtFe nanoparticles (NPs) coated with “dual purpose” N-doped carbon shell. Our ordered fctPtFe/C nanocatalyst coated with N-doped carbon shell shows 11.4 times-higher mass activity and 10.5 times-higher specific activity than commercial Pt/C catalyst. Moreover, we accomplished the long-term stability in membrane electrode assembly (MEA) for 100 hr without significant activity loss. We demonstrate that the photovoltaic performance of copper-indium-selenide (CISe) quantum dot (QD)-sensitized solar cells (QDSCs) can be greatly enhanced simply by optimizing the thickness of ZnS overlayers on the QD-sensitized TiO2 electrodes. Our best cell yields a conversion efficiency of 8.10% under standard solar illumination, a record high for heavy metal-free QD solar cells to date. Thermoelectrics directly converts waste heat into electricity and is considered a promising means of sustainable energy generation. While most of the recent advances in the enhancement of the thermoelectric figure of merit (ZT) resulted from a decrease in lattice thermal conductivity by nanostructuring, there have been very few attempts to enhance electrical transport properties, i.e., power factor. We use nanochemistry to stabilize bulk bismuth telluride (Bi2Te3) that violates phase equilibrium, namely, phase-pure n-type K0.06Bi2Te3.18. Incorporated potassium and tellurium in Bi2Te3 far exceeds their solubility limit, inducing simultaneous increase in the electrical conductivity and the Seebeck coefficient along with decrease in the thermal conductivity. Consequently, a high power factor of ~43 W cm–1 K–2 and a high ZT > 1.1 at 323 K are achieved. 25 1.1.1 Metalloporphyrin-Based Small Molecules for Photovoltaic Applications Xunjin Zhu1*, Wai-Kwok Wong1, Wai-Yeung Wong1,2*# Institute of Molecular Functional Materials and Department of Chemistry, Hong Kong Baptist University, Waterloo Road, Kowloon Tong, Hong Kong. 2 Department of Applied Biology and Chemical Technology, The Hong Kong Polytechnic University, Hung Hom, Hong Kong. E-mail: [email protected], [email protected] 1 Keywords: energy, organic solar cell, photovoltaics, porphyrin, transition metal With the development of accessible and renewable energy sources, solution-processed bulk heterojunction organic solar cells (BHJ OSCs) have been well developed and recognized as one of the most promising next-generation green technology alternatives to inorganic solar cells because of their solution processability, low cost, light weight, and flexibility. Specifically, small-molecule BHJ OSCs have attracted much attention recently, in which small molecules as donor materials show defined molecular structure and molecular weight, high purity, and less batch-to-batch variations in comparison with their polymer counterparts. In dye-sensitized solar cells, porphyrin-based push–pull photosensitizers have demonstrated their success for their large and rigid planar conjugated structures, which can enhance π-electron delocalization and promote intermolecular π–π interaction, as well as charge transport in devices. However, either polymers or small molecules that are porphyrin based show less contribution in BHJ OSCs, and the main impediments to performance are unfavorable aggregation, short exciton diffusion length and low charge mobility. In this talk, a series of new A-D-A metalloporphyrin-based molecules were designed, synthesized and characterized. These molecules can be used as efficient electron donors in high-performance solution-processed BHJ OSCs. Acknowledgement We thank the financial support from the Areas of Excellence Scheme, University Grants Committee, Hong Kong SAR (AoE/P-03/08). We also thank Prof. X.B. Peng for the device measurements. References [1] Chen, S.; Xiao, L.; Zhu, X.; Peng, X.; Wong, W.-K.; Wong, W.-Y. Chem. Commun., 2015, 51, 14439. [2] Wang, H.; Xiao, L.; Yan, L.; Chen, S.; Zhu, X.; Peng, X.; Wang, X.; Wong, W.-K.; Wong, W.-Y. Chem. Sci., 2016, 7, 4301. [3] Xiao, L.; Chen, S.; Gao, K.; Peng, X.; Liu, F.; Cao, Y.; Wong, W.-Y.; Wong, W.-K.; Zhu, X. ACS Appl. Mater. Interfaces, 2016, 8, 30176. 26 1.1.2 Interface and Tandem Design for Polymer and Perovskite Solar Cells Hin-Lap Yip*,# State Key Laboratory of Luminescent Materials and Devices, South China University of Technology, Guangzhou, China Keywords: Interface engineering, tandem cell design, polymer solar cells, perovskite solar cells Interface engineering is a critical strategy for improving the performance of both polymer and organometal trihalide perovskite (eg. CH3NH3PbI3) solar cells. A good interfacial material should fulfil several requirements including 1) good charge selectivity to improve the charge collection efficiency at the corresponding electrodes, 2) matched energy levels with the conduction band and valence band of the light harvesting film to maximize the photovoltage of the solar cells, 3) high conductivity to minimize the interfacial resistance loss and forming Ohmic contact with the electrodes.1 In the first part of my talk I will discuss several strategies to design new conjugated polymer-based interfacial materials with desired electrical conductivity, energy levels and processibility to improve the charge collection efficiency of polymer solar cells.2 The application of these interfacial materials as interconnection layer for highly efficient tandem polymer solar cells will also be discussed.3 In the second part of my talk, I will discuss how we can apply the knowledge we learned from the interface engineering of polymer solar cells to design new class of electron4,5 and hole transport materials6,7 as efficient charge selective layers to improve the performance of perovskite solar cells. Polymer Solar Cell Perovskite Solar Cell Metal Electron selec ve layer Bulk‐heterojunc on Hole selec ve layer ITO Glass or Plas c Metal Electron selec ve layer Perovskite Hole selec ve layer ITO Glass or Plas c Donor LUMO e"# X# HSL h+# Acceptor LUMO e"# EF,e Metal - BHJ EF,h Voc ESL + X# Donor HOMO Acceptor HOMO X# HSL h+# Transparent electrode Transparent electrode h+# e"# Conduction band e"# Metal Perovskite Voc ESL X# Valence band h+# References [1] [2] [3] [4] [5] [6] [7] # * H.-L. Yip, A. K.-Y. Jen, Energy Environ. Sci. 2012, 5, 5994-6011. Z. Wu, H.-L. Yip, F. Huang, Y. Cao, et al. J. Am. Chem. Soc., 2016, 138, 2004–2013 K. Zhang, F. Huang, X. Peng, L. Ding, H.-L. Yip, et al, Adv. Mater., 2016, 28, 4817-4823. S. Chen, H.-L. Yip, M. Wang, F. Huang, et al, Adv. Energy Mater., 2016, 6, 1501534. Y. Xing, H.-L. Yip, G. C. Bazan, F. Huang, Y. Cao, et al, Nano Energy, 2016, 26, 7-15. Q. Xue, B. Zhang, H.-L. Yip, Y. Cao, et al, Adv. Energy Mater., 2016, 6, 1502021. Y. Bai, H.-L. Yip, S. Yang, et al, Adv. Funct. Mater., 2016, 26, 2950–2958. Presenting Author Corresponding Author 27 1.1.3 G Molecular Approach for Donor-Acceptor Linked Systems and Organic Photovoltaics Hiroshi Imahori1,2*,# Institute for Integrated Cell-Material Sciences (WPI-iCeMS), Kyoto University, Nishikyo-ku, Kyoto 6158510, Japan 2 Department of Molecular Engineering, Graduate School of Engineering, Kyoto University, Nishikyo-ku, Kyoto 615-8510, Japan 1 Keywords: photoinduced electron transfer, donor-acceptor interaction, porphyrin, nanocarbons, organic photovoltaics Photoinduced electron transfer (ET) is one of the most fundamental processes in physics, chemistry, and biology. Photoinduced charge separation (CS) at the interfaces of polymer solar cells (PSCs) and dyesensitized solar cells (DSSCs) generates an electron-hole pair, eventually achieving light-to-electricity conversion. However, the interfaces of semiconductor/dye and donor/acceptor (D/A) in artificial photosynthesis and organic photovoltaic cells often suffer from the partial or even large loss of the chargeseparated state at the early stage, which has still been controversial and not unveiled owing to inevitable inhomogeneous spatial distribution of D-A components. In this talk I will give an overview of our recent results on D-A linked models and organic photovoltaics based on rational molecular design. First, unprecedented dependence of final CS efficiency as a function of D-A interaction in the covalentlylinked molecules with a rectilinear rigid oligo-p-xylene bridge is described. Optimization of the D-A electronic coupling remarkably inhibits the undesirable rapid decay of the singlet charge-separated state to the ground state, yielding the final long-lived, triplet charge-separated state with ~100% efficiency. This finding is extremely useful for rational design of artificial photosynthesis and organic photovoltaics toward efficient solar energy conversion. Second, DSSCs are presented in terms of power conversion efficiency (PCE) and durability. Specifically, tropolone was employed as a new anchoring group for DSSCs. The DSSC based on a porphyrin with the tropolone moiety, YD2-o-C8T exhibited a PCE of 7.7%, which is almost comparable to a reference porphyrin with a conventional carboxylic group, YD2-o-C8. More importantly, YD2-o-C8T was found to display the superior DSSC durability as well as binding ability to TiO2 to YD2-o-C8. These results unambiguously demonstrate that tropolone is the highly promising anchoring group of any dyes for DSSCs in terms of device durability as well as photovoltaic performance. Finally, I will focus on PSCs. C60 and C70 derivatives are predominantly used as electron acceptors in efficient PSCs. However, as-prepared C60 bis-adducts as well as C70 mono-adducts intrinsically comprise regioisomers that would mask individual device performances depending on the substituent position on the fullerenes. We separated the regioisomers of C60 bis-adducts and C70 mono-adducts for the PSC applications for the first time. In particular, systematic investigations of the substituent position effect using a novel symmetric C70 mono-adduct ([70]NCMA) and a prevalent, high-performance one ([70]PCBM) reveals that we can control the structures of the blend films with conjugated polymers and thereby improve the PSC performances by the regioisomer separation. Our approach demonstrates the significance of exploring the best-matching regioisomer of C60 bis-adducts and C70 mono-adducts with high-performance conjugated polymers, which would achieve a remarkable progress in PSC devices. 1) T. Higashino, T. Yamada, M. Yamamoto, A. Furube, N. V. Tkachenko, T. Miura, Y. Kobori, R. Jono, K. Yamashita, and H. Imahori, Angew. Chem. Int. Ed., 55, 629-633 (2016). 2) T. Miura, R. Tao, S. Shibata, T. Umeyama, T. Tachikawa, H. Imahori, and Y. Kobori, J. Am. Chem. Soc., 138, 5879-5885 (2016). 3) T. Higashino, Y. Fujimori, K. Sugiura, Y. Tsuji, S. Ito, and H. Imahori, Angew. Chem. Int. Ed., 54, 90529056 (2015). 4) T. Umeyama, T. Miyata, A. C. Jakowetz, S. Shibata, K. Kurotobi, T. Higashino, T. Koganezawa, M. Tsujimoto,, S. Gélinas, W. Matsuda, S. Seki, R. H. Friend, and H. Imahori, Chem. Sci., in press. 28 1.2.1 2D Transition Metal Dichalcogenide Monolayer: A Promising Candidate for Next Generation Electronics Lain-Jong (Lance) Li Physical Science and Engineering Division, King Abdullah University of Science and Technology, Thuwal, 23955-6900, Keywords: 2D materials, Transition metal dichalcogenides Atomically thin 2D Transition metal dichalcogenide (TMD) materials provide a wide range of basic building blocks with unique electrical properties which do not exist in their bulk counterparts. Our recent demonstration in vapor phase growth of TMD monolayer such as MoS2 and WSe2 [1] has stimulated the research in growth and applications [2]. The growth of TMD layers is scalable and these layer materials can be transferred to desired substrates, making them suitable building blocks for constructing multilayer stacks for various applications [3].These 2D monolayer building blocks can be used to form p-n junctions. For example, the heterostructures of 2D materials formed by vertical stacking have been realized recently via transfer of their exfoliated flakes, where their properties are dominated by the stacking orientation and strength of interlayer coupling. The method to determine valence band and conduction band alignment for various TMD materials is proposed [4]. Another very attractive structure is the lateral heterostructure, where the atomically sharp p-n junction exhibits diode properties and a large strain exhibits at the junction region which offers tunability in electronic structures. The direct growth of such lateral heterostructures is shown below [5]. These unique 2D heterostructures have abundant implications for many potential applications. It is known that Moore’s law may not be valid in 7 nm technology nodes if we consider only Si or IIIV semiconductors. 2D TMD materials are also promising materials for post-Si electronics, where their ultra-thin body structure may be able to serve for 5 nm and 3 nm technology nodes,[6] meaning that Moore’s law could be further extended with these materials. We have demonstrated a 10 nm channel length of transistor based on MoS2 few layers using microelectronic compatible processes [7]. References [1] Y.-H. Lee et al. Adv. Mater. 24, 2320 (2012) [2] M. Chhowalla et al. Nature Chem. 5, 263-275 (2013) [3] C.-H. Chen et al. Adv. Mater. 26, 4838 (2014) [4] M.-H. Chiu et al. Nature Comm. 6, 7666 (2015) [5] M.-Y. Li et al. Science 349, 524 (2015) [6] M.C. Chen et al. IEDM (2015) [7] K.H. Li et al VLSI (2016) Figure (a) Lateral heterostructure of MoS2 and WSe2 monolayers (b) The structure of 10 nm transistor based on few-layered MoS2 channel. . 29 1.2.2 Synthesis and Applications of Novel Two-Dimensional Nanomaterials Hua Zhang#,a)* Center for Programmable Materials, School of Materials Science and Engineering, Nanyang Technological University, 50 Nanyang Avenue, Singapore 639798, Singapore Keywords: Two-dimensional nanomaterials; Transition metal dichalcogenides; Nanodevices; Fieldeffect transistors; Clean energy. In this talk, I will summarize the recent research on synthesis, characterization and applications of two-dimensional nanomaterials in my group. I will introduce the synthesis and characterization of novel low-dimensional nanomaterials, such as graphene-based composites including the first-time synthesized hexagonal-close packed (hcp) Au nanosheets (AuSSs) on graphene oxide, surfaceinduced phase transformation of AuSSs from hcp to face-centered cubic (fcc) structures, the synthesis of ultrathin fcc Au@Pt and Au@Pd rhombic nanoplates through the epitaxial growth of Pt and Pd on the hcp AuSSs, respectively, the first-time synthesis of 4H hexagonal phase Au nanoribbons (NRBs) and their phase transformation to fcc Au RNBs as well as the epitaxial growth of Ag, Pt and Pd on 4H Au NRBs to form the 4H/fcc Au@Ag, Au@Pt and Au@Pd core–shell NRBs, and the epitaxial growth of metal and semiconductor nanostructures on solution-processable transition metal dichalcogenide (TMD) nanoshees at ambient conditions, single- or few-layer metal dichalcogenide nanosheets and hybrid nanomaterials, the large-amount, uniform, ultrathin metal sulfide and selenide nanocrystals, other 2D nanomaterials, nanodots prepared from 2D nanomaterials, and self-assembled 2D nanosheets and chiral nanofibers from ultrathin lowdimensional nanomaterials. Then I will demonstrate the applications of these novel nanomaterials in chemical and bio-sensors, solar cells, water splitting, hydrogen evolution reaction, electric devices, memory devices, conductive electrodes, other clean energy, etc. # * * Presenting Author Corresponding Author Corresponding Author (Email: [email protected]) 30 1.2.3 Fullerene Nanoarchitectonics from Zero to Higher Dimensions Lok Kumar Shrestha1)* #, Rekha Goswami Shrestha1), Partha Bairi1) Jonathan P. Hill1) Katsuhiko Ariga1) 1International Center for Materials Nanoarchitectonics (WPI-MANA), National Institute for Materials Science (NIMS), 1-1 Namiki, Ibaraki Tsukuba 305-0044, Japan. Keywords: fullerene crystals, liquid-liquid interface, nanoporous graphitic carbon, supercapacitance, VOC sensing. Self-assembled single crystalline fullerenes (C60 or C70) nanostructures exhibit excellent physicochemical and optoelectronic properties including high electron mobility, high photosensitivity [1,2]. Owing to these appealing features together with excellent electron accepting properties, dimensionally-integrated fullerene crystals have received considerable interest for the possible applications in diverse fields such as material engineering and device fabrications including flexible optoelectronics device, field effect transistors, light emitting diodes, photovoltaic cells, sensors, and photodetectors [3,4]. Insertion of porous structures in the fullerene crystals is expected to increase the effective surface area drastically, which is expected to offer a great utility in many applications such as supercapacitors, large hydrogen storages, chemical and physical sensors) [5]. In this contribution, we present a simple recipe of producing selfassembled fullerene C60 and C70 microcrystals from zero to higher dimensions using solution based strategy called liquid-liquid interfacial precipitation (LLIP) method under mild conditions of temperature and pressure [6]. We also discuss the recently developed novel technique for the expansion of fullerene nanomaterials into hierarchic macro- and mesopores architectures with crystallized frameworks [7]. These novel materials offered enhanced surface textural properties compared to pristine fullerenes and it could be flexibly controlled by adjusting the synthetic conditions. We also discuss our recent results on the thermal conversion of single crystalline fullerene crystals (tubes to cubes) into high surface area nanoporous graphitic carbons [8]. The fullerene crystals derived graphitic carbon materials displayed enhanced electrochemical supercapacitive performance followed by excellent sensing performance sensitive towards aromatic solvents [8,9]. Note that the C60 molecule can be regarded as an ideal zero dimensional building blocks with striking functions. Therefore, construction of zero to higher-dimensional objects, such as 1D, 2D or 3D including porous nanomaterials may realize important aspects of fullerene nanoarchitectonics [10]. References [1] K. Komatsu, M. Murata and Y. Murata, Science, 307 (2005) 238 [2] E. Nakamura and H. Isobe, Acc. Chem. Res., 36 (2003) 807 [3] N. S. Sariciftci, L. Smilowitz, A. J. Heeger and F. Wudl, Science, 258 (1992), 1474 [4] Y. Matsuo, Y. Sato, T. Niinomi, I. Soga, H. Tanaka, E. Nakamura, J. Am. Chem. Soc., 131 (2009), 16048 [5] K. Ariga, A. Vinu, Y. Yamauchi, J. Qingmin and J. P. Hill, Bull. Chem. Soc. Jpn., 85 (2012), 1 [6] L. K. Shrestha, Q. Ji, T. Mori, K. Miyazawa, Y. Yamauchi, J. P. Hill and K. Ariga, Chem. –Asian J. 8 (2013), 1662 [7] L. K. Shrestha, Y. Yamauchi, J. P. Hill, K. Miyazawa and K. Ariga, J. Am. Chem. Soc., 135 (2013), 586 [8] L. K. Shrestha, R. G. Shrestha, Y. Yamauchi, J. P. Hill, T. Nishimura et al. Angew. Chem. Int. Ed., 54 (2015), 951 [9] P. Bairi, R. G. Shrestha, J. P. Hill, T. Nishimura, K. Ariga and L. K. Shrestha, J. Mater. Chem. A, 4 (2016), 13899. [10] P. Bairi, K. Minami, W. Nakanishi, J. P. Hill, K. Ariga and L. K. Shrestha, ACS Nano, 10 (2016), 6631 # Presenting Author *Corresponding Author 31 1.3.1 Nanocarbons for electrochemical energy storage Hui-Ming Cheng1,2 1 Shenyang National Laboratory for Materials Science Institute of Metal Research, Chinese Academy of Sciences 72 Wenhua Road, Shenyang 110016, China 2 Laboratory for Low-Dimensional Materials and Devices Tsinghua-Berkeley Shenzhen Institute (TBSI), Tsinghua University 1001 Xueyuan Road, Shenzhen 518055, China Email: [email protected] Keywords: Nanocarbons, Battery, Supercapacitor, Carbon nanotubes, Graphene In recent years, electrochemical energy storage devices, such as supercapacitors, lithium-ion batteries and lithium-sulfur batteries, have been extensively explored in response to the everincreasing demand for clean energy and climate change mitigation technologies. Carbon materials with different structures and functionalities play a key role in various energy storage devices for use as electrodes, conductive fillers, coating layers, etc. Nanocarbons, including carbon nanotubes (CNTs) and graphene have unique low-dimensional structures, good electrical conductivity, high strength, and desirable chemical stability. Therefore, nanocarbons are expected to find extensive and important applications in the field of electrochemical energy storage. We have fabricated a serious of nanocarbon-based hybrid electrode materials by mechanical mixing, hydrothermal deposition, in-situ growth, or selective filling. These hybrid electrode materials showed desirable electrochemical properties in terms of long cycling life, good high rate capability, and high reversible capacity. The working mechanism of nanocarbons in hybrid electrodes was investigated by an in situ TEM approach. It was found that nanocarbons take a significant role in forming electrical conductive network and preventing the volume expansion of active materials. And we also designed and developed nanocarbon-based sandwich structure, integrated structure and flexible structure for high-capacity, high-power, long-life and high energy lithium-sulfur batteries. Using graphene and CNTs in flexible energy storage devices is another emerging field, and we have also explored several kinds of nanocarbon-based flexible electrodes. Based on the understanding of electric double layer and tuning electrochemical potential windows, a smart lithium ion capacitor with an extra Li electrode to monitor the operation state and to regenerate its capacity was developed, which can allow a real-time diagnosis of capacity decay, safety control, and self-healing of a degraded capacitor through a feedback system. The smart electrochemical energy storage devices can work as a bridge that connects users and R&D engineers to create a safer and more intelligent electrochemical energy storage future. 32 1.3.2 Structural Nanomaterials For Advanced Energy Systems (Nuclear, Solar, Ocean Thermal Energy Conversion) Prof. Jian LU Centre for Advanced Structural Materials (CASM), City University of Hong Kong To develop efficient and advanced energy system, new energy saving and storage system is one of the key directions to safeguard the sustainable development of mankind. This presentation will feature recent development of structural nanomaterials and high mechanical properties of functional nanomaterials. The mechanisms of materials formation with different nano-structures by high efficient physical method will firstly be reported by illustrating our latest findings / research progress on the nanomaterials with high strength and high ductility, nanostructure materials with gradient structure, nanostructure materials with multilayers, hierarchical nano-twinned materials, materials with nano-precipitation, nanomaterials with multiphase embedded structure, etc. The feasibility of applying new nanomaterials on various advanced energy systems, such as wind power plant, next generation of nuclear plant and concentrated solar energy, and ocean thermal energy conversion will be discussed. The application of new nanomaterials on the newly designed light-weight automotive parts will be introduced. The latest findings on the nano-porous materials with high mechanical properties for energy storage devices such as supercapacitor will be revealed. By enhancing the mechanical properties of the nano-porous materials, the collapse problems caused by dealloying has been solved and the large-scale fabrication process for super nanostructured porous materials with pore size smaller than 10 nm has been developed. Lastly, the development and research direction of the biomimetic nanostructured materials on advanced energy systems will be discussed. Reference [1] J.C.Ye, J.Lu, C.T.Liu, Q.Wang, Y.Yang, Atomistic Free-Volume Zones and Inelastic Deformation of Metallic-Glasses Characterized by High-Frequency Dynamic Micropillar Tests, Nature Materials, Volume 9, Issue 8, pages 619-623, August 2010 [2] Q.Wang, C.T.Liu, Y.Yang, Y.D.Dong, J.Lu, Atomic-Scale Structural Evolution and Stability of Supercooled Liquid of a Zr-Based Bulk Metallic Glass, Physical Review Letters, May 2011, Volume 106, Issue 21, N. 215505 [3] H.N.Kou, J.Lu, Y.Li, High-Strength and High-Ductility Nanostructured and Amorphous Metallic Materials, Advanced Materials, 2014, 26, p5518–5524 [4] Q. Wang, S.T.Zhang, Y.Yang, Y.D.Dong, C.T.Liu, J.Lu, Unusual fast secondary relaxation in metallic glass, Nature Communications, 24 Jul 2015, DOI: 10.1038/ncomms8876 [5] L.L.Zhu, S.Q.Qu, X.Guo, J.Lu, Analysis of the twin spacing and grain size effects on mechanical properties in hierarchically nanotwinned face-centered cubic metals based on a mechanism-based plasticity model, Journal of the Mechanics and Physics of Solids, Vol.76, Pages:162-179, Mar. 2015 [6] Y.F.Ye, Q.Wang, J.Lu, C.T.Liu, Y.Yang, High-entropy alloy: challenges and prospects, Materials Today, Volume: 19, Issue: 6, Pages: 349-362, July-August 2016 [7] Y.W.Zhan, S.S.Zeng, H.D.Bian, Z.Li, Z.T.Xu, J.Lu, Y.Y.Li, Bestow metal foams with nanostructured surfaces via a convenient electrochemical method for improved device performance, Nano Research, Volume: 9, Issue: 8, Pages: 2364-2371, Aug. 2016 [8] J.Zhang, L.C.Chan, T.Gao, Q.Wang, S.Zeng, H.Bian, C.Lee, Z.T.Xu, Y.Y.Li, J.Lu, Bulk monolithic electrodes enabled by surface mechanical attrition treatment-facilitated dealloying, Journal of Materials Chemistry A, Vol. 4, Issue: 39, Pages: 15057-15063, Oct. 2016 33 1.3.3 Compromising nanocarbons and layered materials for energy applications Li Song a)*# National Synchrotron Radiation Laboratory, CAS Center for Excellence in Nanoscience, University of Science and Technology of China, Hefei, Anhui 230029, P. R. China [email protected] Keywords: carbon nanomaterials, layered-materials, synergistic effect, energy applications The carbon materials, presenting various forms ranging from well-developed crystalline structures to other less ordered varieties, have been involved in many industrial applications for our life. Thank to these unique novelties, various nano-scale carbon materials with different dimensions have been proposed for a number of applications, such as gas storage, catalyst support, electrochemical energy storage. Interestingly, 2D-graphene, 1D-CNT and 0D-fullerene have the same sp2 bonding structure, resulting in extremely stable covalent bonds between carbon atoms and nearest neighbors. However, the microstructure and properties of various nanocarbons are distinctly different. On the other side, layered materials recently attracted a lot of attention as a promising candidate for energy applications, because it is earth-abundant and inexpensive. Therefore, it is highly desirable to develop a suitable route to compromise the merit of nanocarbons layered materials or others. Herein, we will present our recently studies on the design and relazation of new promising energy materials via integrating various nanocarbons and layered materials. Combining with theorical calculations, synchrotron radiation based techniques and atomic miscrscopes were employed to identify the microstructure and electrical structures in the new hybrids. The relationship between the structures and properties were further buildt up for better understanding in energy devices. # * Presenting Author Corresponding Author 34 Plenary2.1 Photocatalytic Splitting of Water into Molecular Hydrogen and Oxygen Chen-Ho Tung*#, Li-Zhu Wu, Bin Chen, Zhi-Jun Li Key Laboratory of Photochemical Conversion and Optoelectronic Materials, Technical Institute of Physics and Chemistry, the Chinese Academy of Sciences, Beijing 100190, P. R. China Keywords: Photocatalytic splitting of water, Quantum dot, [FeFe] hydrogenase, Transition metal cluster, Oxidation of Water. One of the best solutions for meeting future energy demands is the conversion of water into hydrogen fuel using solar energy. The splitting of water into molecular hydrogen (H2) and oxygen (O2) using light involves two half-reactions: the oxidation of water to O2 and the reduction of protons to H2. To take advantage of the full range of the solar spectrum, researchers have extensively investigated artificial photosynthesis systems consisting of two photosensitizers and two catalysts with a Z-configuration: one photosensitizercatalyst pair for H2 evolution and the other for O2 evolution. This report reviews advances our laboratory has made in the development of new systems for photocatalytic splitting of water that use earth-abundant materials and is both efficient and durable. We constructed several assemblies of CdTe and CdSe QDs as photosensitizers with [FeFe]-H2ase mimics as catalysts. These assemblies produced H2 in aqueous solutions photocatalytically and efficiently, with turnover numbers (TONs) up to hundreds of thousands. Assemblies of 3-mercaptopropionic acid (MPA)-capped CdTe Qds with Co2+ ions formed Coh-CdTe hollow nanospheres, and (MPA)-capped-CdSe Qds with Ni+ ions produced Nih-CdSe/CdS core/shell hybrid in situ in aqueous solutions upon irradiation. The resulting photocatalytic systems proved robust for H2 evolution. These systems showed excellent activity and impressive durability in the photocatalytic reaction, suggesting that they can serve as a valuable part of an overall water splitting system. We also constructed several systems for photocatalytic oxidation of water to O2. Overall water splitting was achieved in our laboratory. References [1]. Wu, L.-Z.; Chen, B.; Li, Z.-J.; Tung, C.-H. Acc. Chem. Res. 2014, 47, 2177-2185. [2]. Wang, F.; Wang, W.-G.; Wang, X.-J.; Wang, H.-Y.; Tung, C.-H.; Wu, L.-Z. Angew. Chem. Int. Ed. 2011, 50, 3193-3197. [3]. Wang, F.; Liang, W.-J.; Jian, J.-X.; Li, C.-B.; Chen, B.; Tung, C.-H.; Wu, L.-Z. Angew. Chem. Int. Ed. 2013, 52, 8134-8138. [4]. Jian, J.-X.; Liu, Q.; Li, Z.-J.; Wang, F.; Li, X.-B.; Li, C.-B.; Liu, B.; Meng, Q.-Y.; Chen, B.; Feng, K.; Tung, C.-H.; Wu, L.-Z. Nature Commun 2013, 4, 2695. [5]. Li, Z.-J.; Wang, J.-J.; Li, X.-B.; Fan, X.-B.; Meng, Q.-Y.; Feng, K.; Chen, B.; Tung, C.-H.; Wu, L.-Z. Adv. Mater. 2013, 25, 6613-6618. [6]. Li, Z.-J.; Fan, X.-B.; Li, X.-B.; Li, J.-X.; Ye C.; Wang, J.-J.; Yu S.; Li, C.-B.; Gao, Y.-J.; Meng, Q.-Y.; Tung, C.-H.; Wu, L.-Z. J. Am. Chem. Soc. 2014, 136, 8261-8268. [7]. Yang, B.; Jiang, X.; Guo, Q.; Lei, T.; Zhang, L.-P.; Chen, B.; Tung, C.-H.; Wu, L.-Z. Angew. Chem. Int. Ed., 2016, 55, 6229-6234. [8]. Liu, B.; Li, X.-B.; Gao, Y.-J.; Li, Z.-J.; Meng, Q.-Y.; Tung, C.-H.; Wu, L.-Z. Energy Environ. Sci., 2015, 8, 1443-1449. [9]. Li, J.; Gao, X.; Liu, B.; Feng, Q.; Li, X.-B.; Huang, M.-Y.; Liu, Z.; Zhang, J.; Tung, C.-H.; Wu, L.-Z. J. Am. Chem. Soc., 2016, 138, 3954-3957. # Presenting Author Corresponding Author * 35 2.1.1 Design and Synthesis of Semiconducting Polymers for High-Performance Field-Effect Transistors Yunqi Liu Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190, China Email: [email protected] Keywords: synthesis, semiconducting polymers, field-effect transistors Polymeric field-effect transistors (PFETs) are of great interest for practical applications in active-matrix displays, radiofrequency identification tags, biosensors, and integrated circuits owing to their advantages of low cost, light weight, and mechanical flexibility. In terms of chemical structure, donor-acceptor (D–A) type conjugated polymers have been investigated extensively. The results indicate that this kind of polymers can provide enhanced intermolecular interactions between D and A moieties around neighbouring chains, therefore facilitating efficient intermolecular carrier hopping. Recently, D–A type polymer semiconductors based on thienoisoindigo (TIIG) and diketopyrrolopyrrole (DPP) moieties exhibit ultrahigh hole mobilities up to 14.4 and 17.8 cm2 V–1 s–1, respectively. Moreover, a state-of-the-art hole mobility of 36.3 cm2 V–1 s–1 has been achieved for the macroscopic alignment of D–A type polymer (PCDTPT) films prepared from an onedimensional nano-template technique, which are far superior to that of amorphous silicon FETs and even comparable to vacuum-deposited small molecule FETs and organic single-crystal FETs. In this presentation, I will report design and synthesis of a series of semiconducting polymers, fabrications of their PFETs, and investigation of corresponding electronic performances.[1–7] References [1] Hanlin Wang, Hongtao Liu, Qiang Zhao, Cheng, Wenping Hu and Yunqi Liu, Adv. Mater., 2016, 28(4), 624630. [2] Zhengran Yi, Shuai Wang and Yunqi Liu, Adv. Mater., 2015, 27(24), 35893606. [3] Hanlin Wang, Cheng, Lei Zhang, Hongtao Liu, Yan Zhao, Yunlong Guo, Wenping Hu, Gui Yu and Yunqi Liu, Adv. Mater., 2014, 26(27), 46834689. [4] Weifeng Zhang, Yunqi Liu and Gui Yu, Adv. Mater., 2014, 26(40), 68986904. [5] Yan Zhao, Yunlong Guo and Yunqi Liu, Adv. Mater., 2013, 25(38), 5372–5391. [6] Lei Zhang, Hanlin Wang, Yan Zhao, Yunlong Guo, Wenping Hu, Gui Yu and Yunqi Liu, Adv. Mater., 2013, 25(38), 5455–5460. [7] Zhiyuan Zhao, Zhihong Yin, Huajie Chen, Liping Zheng, Chunguang Zhu, Long Zhang, Songting Tan, Hanlin Wang, Yunlong Guo, Qingxin Tang and Yunqi Liu, Adv. Mater., in press. 36 2.1.2 Advanced nanotechnology for high-performance photovoltaic devices Feng Yan*# Department of Applied Physics, The Hong Kong Polytechnic University Keywords: solar cell, graphene, perovskite, plasmonic High-performance organic solar cells have been developed by our group based on various nanotechnology in recent years.[1] First, the efficiency of organic solar cells have been improved by introducing plasmonic nanoparticles, high mobility conjugated polymers or 2-D materials. Pronounced effects have been observed in the devices due to the improvement of the carrier mobility or light absorption in the active layer. Graphene has shown promising applications in photovoltaic devices for its high carrier mobility and conductivity, high transparency, excellent mechanical flexibility and ultrathin thickness, and can be used in solar cells as transparent electrodes or interfacial layers. Package-free flexible organic solar cells are fabricated with multilayer graphene as top transparent electrodes, which show high power conversion efficiency, excellent flexibility and bending stability.[2] Semi-transparent organic solar cells and perovskite solar cells were prepared by using graphene transparent electrodes.[3] For the perovskite solar cells, the devices show high power conversion efficiencies (~12%) when they are illuminated from both sides. Considering the poor stability of perovskite solar cells in ambient air especially with high humidity, we have recently developed a novel technique to improve the device stability by introducing SCN- to partially replace I- in the perovskite material,[4] which can dramatically improve the lifetime of package-free device in air. All of the techniques will be very useful for the practical applications of the novel photovoltaic devices. Acknowledgement This work is financially supported by the Research Grants Council (RGC) of Hong Kong, China (project number: C4030-14G). References [1] Energy Environ. Sci. 8, 1463-1470 (2015); Energy Environ. Sci. 9, 898-905 (2016); Adv. Funct. Mater. 26, 864-871 (2016) [2] Adv. Mater. 25, 4296-4301 (2013); Chem Soc. Rev. 44, 5638-5679 (2015); Nano Energy, 28, 151-157 (2016). [3] ACS Nano 6, 810-818 (2012); Adv. Mater. 27, 3632-3638 (2015); ACS Nano 9, 12026–12034 (2015). [4] Nature Comm. 7:11105 (2016). # * Presenting Author Corresponding Author 37 2.1.3 Flexible, Foldable and Multi-Functional Paper-Based Electronics Jr-Hau He King Abdullah University of Science and Technology [email protected] Great advances have been made in developing cheap, simple, multi-functional and energy-saving fabrication processes for flexible electronics. Paper, as a flexible, foldable, cost-efficient and mass productive substrate, has shown diverse applications for flexible electronics to meet such demand. Recently, we have successfully demonstrated the first nonvolatile resistive memory using paper as substrates by means of all-printing techniques. Moreover, we also implemented the algorithm of Origami art into the device design for the flexible electronics, such as photodetectors and nanogenerators, taking advantage of the foldability and adaptability of paper substrates. In particular, paper origami triboelectric nanogenerators using paper as the starting material, with high degree of flexibility, light weight, low cost, and recyclability is presented. We believe that these findings will pave a way for future energy harvesting and sensor design, especially for the development of green flexible electronics. 38 2.2.1 Combination of Biomimicking Methods of Natural Leaf: Regeneration of Nonwetting Surface using Solar water Splitting Kijung Yong,#, * Junghan Lee, Seunghyun Baek Department of Chemical Engineering, POSTECH, Pohang 790-784, Korea Keywords: Photoelectrochemical cell, Non-wetting state, Hydrogen generation, Superhydrophobic surface Biomimetics is imitation of natural unique properties for solving human problems. One of the best examples of this biomimetics is biomimicking natural leaf. Basically there are two approaches of biomimicking natural leaf: physical biomimicking and chemical biomimicking. In physical biomimicking, we can imitate the surface structure of natural leaf, such as lotus leaf and develop non-wetting superhydrophobic surface, which has many interesting eco-friendly energy saving applications like self-cleaning, anti-fouling, and drag reduction. On the other hand, in chemical biomimicking, we can imitate photosynthesis of natural leaf and develop artificial photosynthesis system for hydrogen and solar fuel generation. In this paper, we will present combination of physical and chemical biomimicking of natural leaf and present a unique method for regeneration of air interlayer of non-wetting surface in underwater condition. According to Cassie-Baxter model, the superhydrophobic surface has non-wetting property due to the air interlayer present between water layer and solid surfaces. However the air inter-layer, known as plastron, is thermodynamically instable and thus has limited lifetimes because of dissolution into the water. In the current work we have developed the regeneration of air interlayer by applying solar water splitting reaction. Under solar light illumination, the nanostructure solid surface generates hydrogen/oxygen through solar water splitting and the surface captures the air gas to reform the plastron. This regenerable underwater non-wetting property has important applications in drag reduction and antifouling in underwater conditions. Also we have studied the fabrication of unassisted solar water splitting system by combining PEC and PV cells. Our PV (photovoltaic) cells were prepared by fabrication of CIS thin film solar cells in series, which are connected with electrodes for water oxidation/hydrogen reduction reaction assisted by OER (oxygen evolving reaction) and HER (hydrogen evolving reaction) catalysts. Our unassisted solar water splitting system shows a promising application in solar hydrogen generation. # * Presenting Author Corresponding Author 39 2.2.2 Promoting Catalytic Properties of Nanocrystals by Tuning Their Chemical Environments Xun Wang* Department of Chemistry, Tsinghua University, Beijing 100084, P. R. China * Corresponding author, email: [email protected] Abstract In this presentation, we will show that the proper tuning of chemical environments of inorganic nanocrystals/clusters may greatly enhance their catalytic properties. This talk will involve the controlled assembly of surfactant-encapsulated POM clusters into nanostructures that show enhanced catalytic properties as well as formation of MOF hollow nanocages or hierarchical porous nanostructures embedded with noble metal nanocrystals showing kinetic advantages during catalytic reactions. References [4] Z. ZHANG, B. XU, X. WANG. CHEM. SOC. REV. 2014, 43, 7870-7886. [1] P. HE, B. XU, X. XU, L. SONG, X. WANG. CHEM. SCI. 2016, 7, 1011-1015. [2] X. XU, S. CHEN, Y. CHEN, H. SUN, L. SONG, W. HE, X. WANG. SMALL 2016, 12, 2982-2990. [3] X. XU, Z. ZHANG, X. WANG. ADV. MATER. 2015, 27, 5365-5371. [4] X. XU, Y. LU, Y. YANG, F. NOSHEEN, X. WANG. SCI. CHINA MATER. 2015, 58, 370-377. [5] P. HE, B. XU, P. WANG, H. LIU, X. WANG. ADV. MATER. 2014, 26, 4339-4344. [6] Z. ZHANG, X. XU, J. ZHANG, G. XIANG, B. XU, P. HE, F. NOSHEEN, F. SALEEM, X. WANG. ANGEW. CHEM. INT. ED. 2014, 53, 429-433. [7] Z. ZHANG, Y. CHEN, S. HE, J. ZHANG, X. XU, Y. YANG, F. NOSHEEN, F. SALEEM, W. HE, X. WANG. ANGEW. CHEM. INT. ED. 2014, 53, 12517-12521. [8] A. NISAR, Y. LU, J. ZHUANG, X. WANG. ANGEW. CHEM. INT. ED. 2011, 50, 3187-3192. [9] A. NISAR, J. ZHUANG, X. WANG. ADV. MATER. 2011, 23, 1130-1135. 40 2.2.3 Unlocking Catalytic Potentials of Earth Abundant Materials for Energy Conversion and Device Fabrication Huijun Zhao1.2,*# Centre for Clean Environment and Energy, Griffith University, Queensland, 4222, Australia 2 Centre for Environmental and Energy Nanomaterials, Institute of Solid State Physics, CAS [email protected]; [email protected] 1 Keywords: 5 Electrocatalyst, photocatalyst, hydrogen generation, oxygen reduction, oxygen evolution. The photo- and electrocatalysts play a critical role in clean energy generation and conversion technologies. Although the precious metal-based materials are widely recognized as superior catalysts for energy applications, their large-scale commercial use has been hindered by their expensive and scarcity nature. The development of high performance, plentiful and cheap nonprecious-metal catalysts is therefore vital for the commercial viability of clean energy future. Unfortunately, the most of nonprecious metal materials in their pristine forms possess little or no catalytic activity. As such, the unlocking the catalytic potential of nonprecious and earth abundant materials has become a paramount scientific task of the research field, nevertheless, highly challenging. This presentation intends to report few widely applicable approaches to unlock the catalytic activities of transition metal oxides and graphitic carbon materials for energy conversion and device fabrication.1-8 [1] S. Zhao, Y. Wang 3, J. Dong, C. He, H. Yin, P. An, K. Zhao, X. Zhang, C. Gao, L. Zhang, J. Lv, J. Wang, J. Zhang, A. Khattak, N. Khan, Z. Wei, J. Zhang, S. Liu, H. Zhao and Z. Tang, Nature Energy, 2016, In press, “Coordinative unsaturation engineering on ultrathin bimetal-organic frameworks nanosheets toward high performance electrocatalysts” [2] S. Yang, Y. Wang, P. Liu, Y. B. Cheng, H. Zhao & H. G. Yang, Nature Energy, 1 (2016), 15016, “Functionalization of perovskite thin films with moisture-tolerant molecules” [3] C. W. Wang, S. Yang, W. Q. Fang, P. Liu, H. Zhao & H. G. Yang, Nano Letters, 16 (2016) 427-433, “Engineered hematite mesoporous single crystals drive drastic enhancement in solar water splitting” [4] H. Zhang, Y. Wang, P. Liu, S. L. Chou, J. Z. Wang, H. Liu, G. Wang & H. Zhao, ACS Nano, 10 (2016) 507-514, “Highly ordered single crystalline nanowire array assembled three-dimensional Nb3O7(OH) and Nb2O5 superstructures for energy storage and conversion applications” [5] Y. Li, P. Liu, L. Pan, H. Wang, Z. Yang, L. Zheng, P. Hu, H. Zhao, L. Gu & H. Yang, Nature Communications, 6 (2015) 8064, “Local atomic structure modulations activate metal oxide as electrocatalyst for hydrogen evolution in acidic water” [6] Y. Hou, D. Wang, X. Yang, W. Fang, B. Zhang, H. Wang, G. Lu, P. Hu, H. Zhao & H. Yang, Nature Communications, 4 (2013) 1583, “Rational screening low-cost counter electrodes for dye-sensitized solar cells” [7] Y. Li, J. Xing, Z. Chen, Z. Li, F.Tian, L. Zheng, H. Wang, P. Hu, H. Zhao & H. Yang, Nature Communications, 4 (2013) 2500, “Unidirectional suppression of hydrogen oxidation on oxidized platinum cluster” [8] Y. Li, H. Zhang, Y. Wang, P. Liu, H. Yang, X. Yao, D. Wang, Z. Tang & H. Zhao, Energy & Environmental Science, 7 (2014) 3720-3726, “A self-sponsored doping approach for controllable synthesis of S and N co-doped trimodal-porous structured graphitic carbon electrocatalysts” 41 2.3.1 Multi-Shelled Metal Oxides Hollow Microspheres: Synthesis, property & Application Dan Wang *,# State Key Laboratory of Biochemical Engineering, Institute of Process Engineering, Chinese Academy of Sciences, Beijing, China Centre for Clean Environment and Energy, Gold Coast Campus, Griffith University, Queensland 4222, Australia Keywords: metal oxide, multi shelled hollow spheres, energy application Great progress has been made in the preparation and application of multi-shelled hollow micro/nanostructures during the past decade. However, the synthetic methodologies and potential applications of these novel and interesting materials have not been reviewed comprehensively in the literatures. In this paper we will describe different synthetic methodologies for multi-shelled hollow micro-/nanostructures as well as their compositional and geometric manipulation and then review their applications in energy conversion and storage, sensor, phtotocatalysis, drug delivery. The correlations between the geometric properties of multi-shelled hollow micro-/nanostructures and their specific performance are highlighted in different applications, including dye-sensitized solar cells (DSSCs), lithium ion batteries, supercapacitors, sensors, photocatalysis and drug delivery. These results demonstrate that the geometry has a direct impact on the properties and potential applications of such materials. Finally, the emergent challenges and future developments of multishelled hollow micro-/nanostructures are further discussed. [1] X. Lai, J. Halpert, D. Wang*, Energy Environ. Sci. 2012, 5, 5604. [2] J. Qi, X. Lai, J. Wang, et.al. Chem. Soc. Rev. 2015, 44, 6749-6773 [3] X. Lai, J. Li, B. Korgel, et. al. Angew. Chem. Int. Ed. 2011, 50, 2738. [4] Z. Dong, X. Lai, J. Halpert, et. al. Adv. Mater. 2012, 24, 1046. [5] Z. Dong, H. Ren, C. Hessel, et.al. Adv. Mater. 2014, 26, 905. [6] J. Wang, N. Yang, H. Tang, et. al. Angew. Chem. Int. Ed. 2013, 52, 6417. [7] S. Xu, C. Hessel, H. Ren, et. al. Energy Environ. Sci. 2014, 27, 632. [8] J. Wang, H. Tang, L. Zhang, et. al. Nat. Energy 2016, Accepted. 42 2.3.2 Study of Structural Evolution in Si/Nanocarbon Electrodes by In-situ Characterization Zheng-Long Xu, Jang-Kyo Kim*# Department of Mechanical and Aerospace Engineering, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong Keywords: Silicon/nanocarbon, anodes, Li-ion batteries, in-situ TEM. This talk presents our recent studies of the synthesis of high performance Si/nanocarbon composite anodes for Li-ion batteries and the insightful understanding of their reaction mechanisms via in-situ characterization. Li-ion batteries with graphite as anodes have dominated the market for more than two decades due to its high energy density and low cost. Nevertheless, the capacity delivered by graphite anodes with a theoretical capacity of 372 mAh g-1 is far from sufficient to satisfy today’s demanding applications like electric vehicles, which require much higher energy densities and lower costs than the current LIBs can offer. Thus, developing new electrode materials becomes exigent and imperative. Si has long been considered one of the most promising alternatives to graphite owing to its overwhelming advantages of high specific capacity of ~4200 mAh g-1, moderate working potential of 370 mV and abundance in nature. Despite these intriguing benefits, Si electrodes suffer from significant drawbacks, like fast capacity degradation, potential electrode pulverization and the formation of unstable solid electrolyte interlayers along with a huge volume expansion of ~300 %. High-performance Si/C composites are prepared to take advantage of both the high theoretical capacity of Si and the excellent structural stability and electrical conductivities of carbon materials. First, carbon nanofibers (CNFs) containing Si particles are synthesized via one-pot electrospinning and carbonization as freestanding electrodes. A few ameliorating modifications, including monodipersion of Si particles, addition of graphene sheets or Ni particles and engineered nanocavities around Si particles, have been incorporated into the Si/CNF electrodes to improve their electrochemical performance. Second, carbon-coated Si composites with a high Si content of 81 wt% are synthesized by one-pot carbonization of the mixture of commercial Si particles and polyvinylidene fluoride binder. The Si/C electrodes present discernible improvement in electrochemical performance over pristine Si electrodes, and their energy storage mechanisms are studied by in-situ TEM. Third, mesoporous Si/C microspheres are synthesized by magnesiothermic reduction of porous silica followed by chemical vapor deposition of a thin carbon layer. The structural features of the fine Si nanocrystals, abundant internal pores and highly conductive carbon coating offer a unique synergy giving rise to cyclic stability of the Si/C electrode. The Si/C electrodes deliver exceptional stability of ~90 % capacity retention after 1000 cycles at 1 A g-1 and a high capacity of ~1100 mAh g-1 after 500 cycles at 0.5 A g-1. In-situ TEM technique has been used to probe in real time the reaction mechanisms of Si/C composites. It is revealed that carbon-coated Si particles undergo an isotropic to anisotropic transition during initial lithiation at a lithiation rate 3 to 4.5 times faster than the bare Si. Mesoporous Si/C spheres expand isotropically during lithiation and present a low volume expansion of ~85 % without pulverization at full lithiation stage. The above efforts can not only offer fundamental understanding of the lithiation process and failure mechanisms of Si/C composites, but also provide promising methods to develop high performance Si/C electrodes. Reference [1] Z.L. Xu, B. Zhang, J.K. Kim, Nano Energy 6 (2014) 27-35. [2] Z.L. Xu, K. Cao, S. Abouali, M. Akbari Garakani, J.Huang, J.Q. Huang, E. Kamali Heidari, H. Wang and J.K. Kim, Energy Storage Mater. 3 (2016) 45-54. [3] Z.L. Xu, B. Zhang, S. Abouali, M. Akbari Garakani, J.Huang, J.Q. Huang, J.K. Kim, J. Mater. Chem. A 2 (2014) 17944-17951. [4] Z.L. Xu, Y. Gang, S. Abouali, M. Akbari Garakani, J.Huang, J.Q. Huang, E. Kamali Heidari, J.K. Kim, J. Mater. Chem. A 4 (2016) 6098. 43 2.3.3 Hierarchical composite structure of few-layers MoS2 nanosheets supported by vertical graphene on carbon cloth for lithium ion battery and hydrogen evolution reaction electrodes Zhenyu Zhang, # Wenjun Zhang* Center of Super-Diamond and Advanced Films (COSDAF), and Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, People’s Republic of China. * [email protected] Keywords: Vertical graphene, few-layers MoS2 nanosheets, carbon cloth, hydrogen evolution reaction A hierarchical composite structure composed of few-layers molybdenum disulfide nanosheets supported by vertical graphene on conductive carbon cloth (MDNS/VG/CC) for high-performance lithium ion battery and electrochemical hydrogen evolution reaction (HER) is demonstrated in this work. In the fabrication, 3D vertical graphene is first prepared on carbon cloth by a micro-wave plasma enhanced chemical vapor deposition (MPCVD) and then few-layers MoS2 nanosheets are insitu synthesized on the surface of the vertical graphene through a simple hydrothermal reaction. The vertical graphene can effectively increase conductivity and holding active material on current collector, contributing much better cycling performance than the electrode that without graphene. On the other side, this integrated catalyst exhibits an excellent HER electrocatalytic activity including an onset potential of 50 mV, an overpotential at 10 mA cm-2 (η10) of 78 mV, a Tafel slop of 53 mV dec1 , and an excellent cycling stability in acid solution. The excellent electrochemical performance on both sides can be ascribed to the abundant active edges provided by the vertical MoS2 nanosheets, the effective electron transport route provided by the graphene arrays on the conductive substrate and it offers robust anchor sites for MoS2 nanosheets and appropriate intervals for electrolyte infiltration. # * Presenting Author Corresponding Author 44 3.1.1 Dielectric Properties of Polymer-Fullerene Blends for High Performance Solar Cells Franky So Department of Materials Science and Engineering, North Carolina State University, Raleigh, NC 27695, USA It is commonly believed that the reason for lower efficiencies in polymer solar cells compared to silicon solar cells is the low dielectric constant in photoactive polymers. To alleviate this problem, many researchers have attempted to find ways to increase the dielectric constant of photoactive polymers. However, it is difficult to control the polymer-fullerene blend morphology while tuning the polymer chemistry, and this strategy to enhance the solar cell performance has not been successful. Therefore, we have taken a different approach to this problem. Using several high performance polymer systems, we systematically studied how blending photoactive polymers with fullerene affects the photophysical and dielectric properties of the blends. We found several interesting results. First, most high performance polymers have a dielectric constant value smaller than 3, and there are no correlations between dielectric constant and device performance. Second, in all polymer systems we studied, we found that there is a significant increase in the value of the blend dielectric constant upon mixing a polymer with fullerene. We interpret that as an indication of the strong electronic coupling between the polymer and fullerene. Third, while the blend dielectric constant value has a weak correlation with the device performance, we found that the excited state polarizability of the blend is a strong indicator predicting the device performance. Our results indicate that while the dielectric properties of the pristine polymer might not be the critical factor, the control of the electronic coupling between the acceptor moiety and the fullerene molecule is a key factor determining the device performance. 45 3.1.2 Planar organic heterojunctions: from photovoltaic cell to charge generation layer Andreas Opitz1*#, Norbert Koch1,2, Wolfgang Brütting3, Ellen Moons4 Department of Physics, Humboldt-Universität zu Berlin, Berlin, Germany, 2 Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Berlin, Germany, 3 Institute of Physics, University of Augsburg, Augsburg, Germany, 4 Department of Engineering and Physics, Karlstad University, Karlstad, Sweden 1 Keywords: molecular materials, organic heterojunctions, photovoltaic cells, charge generation layer, energy level alignment. The interface of organic heterojunctions plays a crucial role for charge separation in photovoltaic cells or for the charge carrier density in bilayer field-effect transistors. Foremost, the structural and electronic properties are of paramount importance. Here two prototypical interfaces for planar organic heterojunctions will be discussed: the combination of diindenoperylene (DIP) with fullerene (C60) and the combination of copper-phthalocyanine (H16CuPc) with its perfluorinated analog (F16CuPc). Ultraviolet photoelectron spectroscopy (UPS) was performed to determine the energy level alignment together with angle resolved near edge X-ray absorption fine structure (NEXFAS) measurements to determine the molecular orientation at the interface. The highest occupied molecular orbital (HOMO) energy levels do not shift upon deposition of the spherical C60 on top, and the orientation of the rod-like DIP is unaffected. In contrast, co-facial “lying” interface layers with π-orbital stacking of the two phthalocyanines were observed by UPS and NEXAFS. Here energy level pinning for both materials is found. These results can be related to the device performance of these two material combinations. Whereas DIP/C60 solar cells have an open circuit voltage of up to 0.9 V [1], the energy level pinning in planar structures of H16CuPc/F16CuPc leads to a charge generation layer [2,3]. The absence of a photovoltaic effect at the planar heterojunction of the phthalocyanines is thus explained by these findings. The combined experimental approach results in a comprehensive model for the electronic and morphological characteristics of the interface between the two investigated organic semiconductors. The presence of a π-orbital stacking between different molecules at a heterojunction is also of interest for photovoltaic active interfaces or for ground-state charge-transfer. In all cases, the performance of the interface strongly depends on the relative orientation of the π-orbitals of the involved materials. [1] J. Wagner et al., Adv. Funct. Mater. 20 (2010) 4295. [2] A. Opitz et al., Org. Electron. 10 (2009) 1259. [3] A. Opitz et al., Sci. Rep. 6 (2016) 21291. # * Presenting Author Corresponding Author ([email protected]) 46 3.1.3 Vacuum-Processed High Efficiency Organic Solar Cells Based on Small Molecule Donors Ken-Tsung Wong# * Department of Chemistry, National Taiwan University, Institute of Atomic and Molecular Science, Academia Sinica, Taipei 10617, Taiwan Keywords: Organic photovoltaic, small-molecule donor, donor-acceptor-acceptor, vacuum process. Organic photovoltaics (OPVs) have attracted considerable research interest due to their low cost and low energy consumption in fabrication and mechanical flexibility. While intensive interdisciplinary efforts have been dedicated to improving the power conversion efficiencies (PCEs) of solution-processed polymer bulk heterojunction (BHJ) solar cells, organic solar cells employing small molecules as electron donors have also received considerable attentions. To date, small molecule-based organic solar cells (SMOSCs) using p-type small molecules and n-type fullerenes have achieved remarkable PCEs by using either solution-processed or vacuum-deposited fabrication techniques. The search for new donor materials with promising physical properties such as low band gaps, suitable energy levels, high crystallinity, and decent solubility, etc., has taken the center stage. Along this line, a large number of donor molecules with interesting molecular architectures have been extensively investigated to perform varying degrees of success. We recently reported new organic molecules adopting a donor-acceptor-acceptor (D-A-A) configuration, in which an electrondonating moiety is connected to an electron-withdrawing dicyanovinylene moiety through another electron-accepting arene, exhibited narrow optical band gaps and lower HOMO levels, showing potential to concurrently enhance the short circuit current density (Jsc) and open circuit voltage (Voc) as employed in organic photovoltaics. In this symposium, vacuum-processed heterojunction devices incorporating D-A-A type donors and fullerene (C70) acceptor achieved power conversion efficiencies exceeding 7% will be reported. & % ! " #$%&' ( $! $ )*#$+, &‐ . $/ 01#/ 33$%&4%$ 567$4&. +8 $$ % 2$ >&10&%& (1) Y.-H. Chen, L.-Y. Lin, C.-W. Lu, F. Lin, Z.-Y. Huang, H.-W. Lin, P.-H. Wang, Y.-H. Liu, K.-T. Wong, J. Wen, D. J. Miller, S. B. Darling, J. Am. Chem. Soc. 2012, 134, 13616-13623. (2) Che, X.; Chung, C.-L.; Liu, X.; Chou, S.-H.; Liu, Y.-H.; Wong, K.-T.; Forrest, S. R. Adv. Mater. 2016, DOI:10.1002/adma.201601957 #* Presenting & Corresponding Author: K.-T. Wong ([email protected]) 47 3.1.4 Novel nano-theranostics based on human serum albumin Design Fullerene Acceptor Materials for High-performance Polymer Solar Cells Chunru Wang1,a)**, Fuwen zhao1, Li Jiang1, Xiangyue Meng 1 1 Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190, China Keywords: 5 Fullerene acceptor, NCBA, Polymer solar cell, Morphology, High performance The performance of bulk heterojunction (BHJ) polymer solar cells (PSCs) has been largely improved and the power conversion efficiency(PCE) has readily enhanced up to over 11%, which is mainly benefited from the rapid development of high efficient donor and acceptor materials, as well as the introducing of high performance cathode buffer layers (CBL).First, the efficiency of polymer solar cells (PSCs) was essentially enhanced by improving the performance of electron-acceptor materials, by designing a dihydronaphthyl-based [60] fullerene bisadduct derivative, NC(60)BA, which not only possesses a LUMO energy level 0.16 eV higher than PC(61)BM but also has amorphous nature that can overcome thermal-driven crystallization. Further, a new soluble C70 derivative, dihydronaphthyl-based C70 bisadduct (NC70BA), is synthesized and explored as acceptor in PSCs. It was revealed that the PSC based on the blend of poly(3-hexylthiophene) (P3HT) and NC70BA shows a high open-circuit voltage (Voc = 0.83 V) and a high power conversion efficiency (PCE = 5.95%), which are much better than those of the P3HT:PCBM-based device (Voc = 0.60 V; PCE = 3.74%). The effects of fullerene bisadduct regioisomers on photovoltaic performance were also examined. The trans-2, trans-3, trans-4, and e isomers of dihydronaphthylbased [60]fullerene bisadduct (NCBA) are isolated and used as acceptors for P3HT-based PSCs. The four NCBA isomers exhibit different absorption spectra, electrochemical properties, and electron mobilities, leading to varying PCE values of 5.8, 6.3, 5.6, and 5.5%, respectively, which are higher than that based on an NCBA mixture (5.3%), suggesting the necessity to use the individual fullerene bisadduct isomer for high-performance PSCs. Second, we developed a self-doped polar fulleropyrrolidine (named as PCMI:K+) by combining K+-intercalated crown ethers and AIET doping as a highly effective interfacial layer, which was used to modify the ZnO layer in the inverted PSCs tore-engineer the interface between ZnO and the active layer. Finally, PCMI:K+ successfully elevates the performance of PTB7-Th based inverted devices from 8.41% to 10.30% due to the simultaneous improvements of the open-circuit voltage (Voc), the short current density (Jsc) and the fill factor (FF). [1] Meng XY, et al., Chem. Commun., 2012, 48, 425 [2] Meng XY, et al., Adv. Funct. Mater., 2012, 22, 2187 [3] Meng XY, et al., Adv. Funct. Mater., 2014, 24, 158 [4] Zhao FW, et al., Adv. Energy Mater. 2016, 6, 854 48 3.1.5 An Insight on Oxide Interlayer in Organic Photovoltaics: From Light Harvesting, Charge Recombination and Collection Perspectives Bo Wu, Weixia Lan and Furong Zhu# Department of Physics, Hong Kong Baptist University, Hong Kong Keywords: organic photovoltaic, charge recombination, charge collection, exciton dissociation, metal oxide. This talk discusses the understanding of the organic/electrode interfacial exciton dissociation, charge recombination processes and charge collection, which underpin the optimum cell design and performance. The charge transport and recombination properties in the bulk heterojunction OSCs are investigated using the transient photocurrent and photo-induced charge extraction by linearly increasing voltage techniques. Combined with light intensity-dependent J–V characteristic, it is found that the origin of unfavorable electron collection is mainly due to the trap-limited bimolecular recombination, resulting in the compensation of drifted photo-generated electrons at the organic/cathode interface. The undesired charge collection can be eliminated by inserting a thin metal oxide interlayer between the organic layer and electrode. Suppression of the metal oxide subgap states significantly improves the charge extraction and performance reproducibility. 49 3.2.1 Nanoscale Metal-Organic Frameworks: Emerging Materials for Catalysis 1 Zhiyong Tang1,a)* # National Center for Nanoscience and Technology, Beijing, 100190 Keywords: nanoscale, metal-organic frameworks Distinct from classic inorganic nanoparticles of solid cores, nanoscale metal-organic frameworks (NMOFs) are of ordered crystalline pores with tunable composite, size and volume, which provide an ideal platform not only to manipulate the reaction active sites but also to understand the structurefunctionality relationship. In this presentation, we will introduce two recent works involving catalytic application of NMOFS. # * Presenting Author Corresponding Author 50 3.2.2 Theoretical Calculations of Electrochemical Activities of Cu-BHT Nanostructures on Catalyzing Hydrogen Evolution Reaction Huiying Yao1, Xing Huang2, Wei Hao3, Jia Zhu1#*, Shuzhou Li3*, Wei Xu2* Department of Chemistry, Beijing Normal University, Beijing, 100875 P. R. China 2 Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100190 P. R. China 3 School of Material Science and Engineering, Nanyang Technological University, 639798 Singapore *Email: [email protected], [email protected], [email protected] 1 Keywords: DFT, Hydrogen Evolution Reaction, Cu-BHT Hydrogen has been considered as a promising candidate of clean and sustainable energy for its high energy density, abundant resources and environmental friendly. One of the executable and convenient ways to obtain hydrogen is the electrocatalytic splitting of water through hydrogen evolution reaction (HER). Comparing with the well-known HER catalytic materials, the reported two-dimensional conjugated coordination polymer material Cu-BHT1 (BHT=benzenehexathiol) shows underestimated catalytic performance. Herein, we used density functional theory (DFT) to reveal various catalytic performances of electrodes covering by Cu-BHT nanostructures. Two kinds of crystal planes depending on the structure of Cu-BHT have been modeled: (0 0 1) and (1 0 0) surfaces. On (0 0 1), atomic hydrogen is more reliably adsorbed on atop site of S with Eads = 0.315 eV. While on (1 0 0) surface, it prefers to adsorbed above Cu with Eads = -0.256 eV. So far, it can be concluded that preferred adsorbed sites of atomic hydrogen and the strength of adsorption above same element both vary in different surfaces. Furthermore, we have studied the adsorption energy change along with increasing hydrogen coverage to give a better description of catalytic performance. It is expected to give helpful insights for improving the activity of metal organic material catalysts in experiment through controlling their surface morphologies. 1. Huang, X. et al. A two-dimensional p–d conjugated coordination polymer with extremely high electrical conductivity and ambipolar transport behaviour. Nat. Commun. 6:7408 51 3.2.3 Carbon based Nanostructures for High Performance Catalysis Weiguo Song*#,Shuliang Yang, Changyan Cao Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100190; [email protected] Keywords: Core shell;Carbocatalysts;Hydrogenation; Nano Stirrer Abstract: Dispersion & Stabilization of active sites, facile mass transportation, and efficient mixing of the reactants are three key aspects of catalysis. With well controlled nanostructures, there three goals can be met. During recent years, we developed in situ deduction methods to ensure high dispersion of noble metal nanoparticles on various supports, and used a embedment method to physically stabilize the metal nanoparticles. With core/shell structure, in which the shell is nanoporous while the core are loaded with active nanoparticles as well as void spaces, diffusion of reaction species can be controlled, so that the activity and the selectivity of the catalysts are enhanced. One particular advantage of such core/shell structures is shape selectivity. Another advantage is high active carbocatalysts with suited heteroatom doping. In practical applications, high performance catalysts were produced for fine chemical production. Fig. 1 Scheme of the procedure to produce nano stirring bars References: [1] W. G. Song*, et al. Angew. Chem. Int. Ed. 2016, 55, 4016 [2] W. G. Song*, et al. Angew. Chem. Int. Ed. 2015, 54, 2661 52 3.2.4 Improving Electron Transport in Nanostructured TiO2 Electrode Liu Bin* School of Chemical and Biomedical Engineering Nanyang Technological University 62 Nanyang Drive Singapore 637459 Email: [email protected] Keywords: electron transport, mesoporous electrode, solar cells, core-shell Titanium dioxide (TiO2) is one of the most widely used semiconductors in photovoltaics and photocatalysis because it is nontoxic, abundant, stable and photoactive. However, the wide bandgap, low electron mobility and short minority carrier diffusion length of TiO2 limit its quantum efficiency in these applications. In this work, we present a solution chemical approach for making TiO2 nanostructures for improving the electron transport in nanostructured TiO2 electrodes. 53 3.3.1 High Efficiency Organic-Inorganic Hybrid Perovskite Solar Cells and LightEmitting Diodes Himchan Cho1, Young-Hoon Kim1, Soyeong Ahn2, Su-Hun Jeong2, Min-Ho Park2, Tae-Woo Lee1,#,* 1 Department of Materials Science and Engineering, Seoul National University, 1 Gwanak-ro, Gwanak-gu, Seoul 08826, Republic of Korea 1 Department of Materials Science and Engineering, Pohang University of Science and Technology (POSTECH), 77 Cheongam-ro, Nam-gu, Pohang 37673, Republic of Korea Keywords: Metal halide perovskites, alternative emitter, hole injection, color purity, solution process Organometal halide perovskites have been intensively studied as promising materials for solar cells and light emitting diodes due to their excellent semiconducting properties, broad range of light absorption, and high colour purity emission. Here we present advances in this field, such as the use of a novel self-organized hole transporting layer and its application to solution-processed lead halide perovskite solar cells and bright perovskite light-emitting diodes. Using the new hole transport layer, we demonstrate bright and efficient PeLEDs in a range of colours. We also report a systematic approach to achieve high-efficiency green perovskite LEDs in a simplified bilayer structure with comparable efficiency those of phosphorescent organic light-emitting diodes. Finally, we demonstrate a highly flexible perovskite LED based on a self-organized conducting polymer anode and the first large-area PeLED. These results show the great potential of perovskite LEDs in the display/lighting industries as an alternative for organic LEDs and quantum dot LEDs. # * Presenting Author Corresponding Author 54 3.3.2 Robust interface engineering for planar perovskite solar cells via a low temperature, stable and solution process Zhu-Bing He Department of Materials Science and Engineering, Shenzhen Key Laboratory of Full Spectral Solar Electricity Generation (FSSEG), South University of Science and Technology of China, No. 1088, Xueyuan Rd., Shenzhen, Guangdong, P.R. China Low temperature, stable and facile solution processes are the typical characters in mass production of next generation solar cells. According to the intrinsic characters of perovskite solar cells (PSCs), interface engineering plays a key role in enhancing conversion efficiency and stability of PSCs, as well as its impact on each kind of solar cells. In this report, we will introduce a series of low temperature and facile solution processed materials in interface engineering for planar inverted PSCs. Those cathode and anode interfacial materials played an important role in augment of conversion efficiency through band alignment and dipole effect. Moreover, their stabilities in utilization environments were also enhanced by hydromolecules resisting and locking penetrated ions from bilayer, which leads to the degradation of devices. A series of experiments and characterizations were performed and collected to support our discoveries. Our results provide a scientific basis for the scale-up production of future PSCs. 55 3.3.3 Rational Material Design, Interface, and Device Engineering for High-Performance Polymer and Perovskite Solar Cells Alex K-Y. Jen Department of Materials Science & Engineering, University of Washington Seattle, WA 98195, USA E-mail: [email protected] 2 Department of Physics & Materials Science; 3Department of Biology and Chemistry City University of Hong Kong 1 Advances in controlled synthesis, processing, and tuning of the properties of organic conjugated polymers and peroskites have enabled significantly enhanced performance of organic and hybrid solar cells. The performance of polymer and hybrid solar cells is strongly dependent on their efficiency in harvesting light, exciton dissociation, charge transport, and charge collection at the metal/organic/metal oxide or the metal/perovskite/metal oxide interfaces. In this talk, an integrated approach of combining material design, interface, and device engineering to significantly improve the performance of polymer and hybrid perovskite photovoltaic cells (PCE of ~20%) will be discussed. At the end, several new device architectures and optical engineering strategies to make tandem cells and semitransparent solar cells will be discussed to explore the full promise of polymer and perovskite hybrid solar cells. 56 3.3.4 Energy levels in organic- and perovskite-based photovoltaic cells Norbert Koch1,2,3 Institut für Physik & IRIS Adlershof, Humboldt-Universität zu Berlin, Germany, 2HelmholtzZentrum Berlin für Materialien und Energie GmbH, Germany, 3Institute of Functional Nano & Soft Materials (FUNSOM), Soochow University, Suzhou, China 1 Keywords: 5 keywords maximum related to your abstract. The energy level alignment at interfaces in photovoltaic cells is of paramount importance for device function and efficiency. In excitonic solar cells, proper type-II level alignment at the interface between two semiconductors is required to ensure exciton dissociation without leading to excessive energy loss of the charge carriers. Subsequent to charge generation the mobile carriers must be transported towards the respective electrodes, ideally with high charge carrier selectivity. At present, no reliable a priori models exist that would allow for predicting the level alignment at such complex interfaces from individual material parameters. It turns out that the level alignment at organic semiconductor heterojunctions is significantly impacted by the presence of electrodes, even when several 10 nm away. This is exemplified for several prototypical junctions, along with an electrostatic model that helps rationalizing this effect. Moreover, the importance of energetic disorder in molecular and polymeric layers is discussed. Over the past few years, the fundamental mechanism of level alignment with perovskite-based semiconductors for solar cells has remained elusive. The reason is to be sought in the non-trivial surface science of this material class. Our study of the electronic properties of metal halide perovskites as function of ambient conditions is discussed as starting point for increased reliability in interface studies with this material class. 57 Plenary3.1 Control of excitonic processes in organic semiconductors aimed for high performance OLEDs and organic lasers Daniel Ping-Kuen Tsang1, Hajime Nakanotani 1, 2, Atula S. D. Sandanayaka 1, 2, Toshinori Matsushima 1, 2, 3, and Chihaya Adachi1,2,3 1 Center for Organic Photonics and Electronics Research (OPERA), Kyushu University, Japan 2 Japan Science and Technology Agency (JST), ERATO, Adachi Molecular Exciton Engineering Project, c/o OPERA, Japan 3 International Institute for Carbon Neutral Energy Research (WPI-I2CNER), Kyushu University, Japan Email: [email protected] Keywords: OLED, Organic laser, TADF, CW lasing, Excited state Through almost 30 years’ research and development, organic light emitting diodes (OLEDs) finally realized the ultimate electroluminescence (EL) efficiency, i.e., nearly 100% electron to photon conversion. The strong demands for ideal EL emitters pushed the development of novel light emitting molecules. In fact, firstly room temperature phosphorescence molecules such as Ir(ppy)3 broke up the limitation of spin restriction for harvesting electrically generated triplets to light. Furthermore, in recent years, a novel conceptual emitter of thermally activated delayed fluorescence (TADF) also realized 100% internal EL efficiency. The critical molecular design of TADF emitters originates to the sophisticated molecular design for balancing radiative decay rate (kr) and a small energy gap between singlet and triplet energy levels (EST). The unlimited molecular design allowed a wide variety of aromatic compounds for TADF emitters. In this talk, we mention the history of TADF development, rational molecular design for highly efficient TADF, stability and degradation mechanism and future prospective. Further, we introduce our next attempt of organic semiconductor lasers aiming for electrical excitation. We recently succeeded realizing CW lasing by engineering both singlet and triplet excited states. 58 Plenary3.2 Thermoelectric Conversion: New Opportunities and Challenges of Organic Materials Daoben Zhu Institute of Chemistry,Chinese Academy of Sciences, Zhongguancun North First Street 2,100190 Beijing, PR China Thermoelectric conversion has attracted widely interests in the past decades. Organic thermoelectric materials, a new member of thermoelectric materials, are recently considered as promising candidates owing to their intrinsically low thermal conductivity, excellent flexibility and potential low cost. [1] Benefiting from rapid development of materials sciences and chemical doping engineering, the main figure of merit (ZT) of organic materials has experienced dramatic improvement. Both opportunities and challenges, however, still existed in the further development of organic thermoelectrics to go for realizing its true benefits. In this presentation, we demonstrate our recent studies on organic thermoelectric materials as well as the thermoelectric devices. By taking advantages of systematic investigations, we demonstrate high performance polymer and small molecule based n-type thermoelectric materials with ZT and power factor of 0.3 and > 200 μW m−1 K−2, respectively. [2-6] The device engineering of organic thermoelectrics, which mainly on the construction of thermoelectric sensors, are also involved in this presentation.[7] In addition, we propose several strategies to accelerate the development of organic thermoelectric materials and devices. [1] Zhang, Q.; Sun, Y. M.; Xu, W.; Zhu, D. B. Adv. Mater. 2014, 26, 6829. [2] Sun, Y. M.; Sheng, P.; Di, C. A.; Jiao, F.; Xu, W.; Qiu, D.; Zhu, D. B. Adv. Mater. 2012, 24, 932. [3] Sun, Y. H.; Qiu, L.; Tang, L. P.; Wang, H. F.; Zhang, F. J.; Huang, D. Z.; Xu, W.; Yue, P.; Guang, Y. S.; Jiao, F.; Sun, Y. M.; Tang, D. W.; Di, C. A.; Yi, Y. P.; Zhu, D. B. Adv. Mater. 2016, 28, 3351. [4] Zhang, Q.; Sun, Y. M.; Xu, W.; Zhu, D. B. Energy Environ. Sci. 2012, 5, 9639. [5] Zhang, F. J.; Zang, Y. P.; Huang, D. Z.; Di, C. A.; Gao, X. K.; Zhu, D. B. Adv. Funct. Mater. 2015, 25, 3004. [6] Huang, D. Z.; Wang, C.; Zou, Y.; Shen, X. X.; Zang, Y. P.; Shen, H. G.; Gao, X. K.; Yi, Y. P.; Xu, W.; Di, C. A.; Zhu, D. B. Angew. Chem. Int. Ed. 2016, 55, 10672. [7] Zhang, F. J.; Zang, Y. P.; Huang, D. Z.; Di, C. A.; Zhu, D. B. Nat. Commun. 2015, 6, 8356. 59 4.1.1 Highly efficient and color-stable hybrid white organic light-emitting diodes using a blue emitter with thermally activated delayed fluorescence Lian Duan*# Key Lab of Organic Optoelectronics and Molecular Engineering of Ministry of Education, Department of Chemistry, Tsinghua University, Beijing 100084, P. R. China. E-mail: [email protected]. Keywords: TADF, energy transfer, white OLED, blue emitter, stability. Hybrid white organic light-emitting diodes (WOLEDs) often undergo triplet energy loss through the triplet state of the blue fluorophors. Here, blue fluorophors with thermally activated delayed fluorescence (TADF) are introduced to solve this problem. The triplet excitons formed on blue TADF fluorophors can be harvested by either energy transfer to the low-lying triplet states of the phosphor or thermal upconversion to the emissive singlet states, eliminating the energy loss. For example, an optimized WOLED using a TADF blue emitter achieves the highest forward-viewing external quantum efficiency (EQE) of 20.8% and power efficiency of 51.2 lm/W with CIE coordinates of (0.398, 0.456) at a luminance of 500 cd/m2. The device EQE only slightly drops to 19.6% at a practical luminance of 1000 cd/m2 with a power efficiency of 38.7 lm/W. Furthermore, the spectra of the device are rather stable with the raising voltage. Moreover, we have also developed stable blue TADF emitters for WOLEDs with much improved lifetime. # * Presenting Author Corresponding Author 60 4.1.2 Controllable Synthesis of Highly-Fluorescent Cesium Lead Halide Perovskite Quantum Dots and Their Use in White Light Emitting Diodes Yang Jiang1,*,#, Guopeng Li1, Yajing Chang1 Zhifeng Zhu1, Hui Wang1 1 School of Materials Science and Engineering, Hefei University of Technology (HFUT), Hefei, Anhui, 230009, P. R. China. Keywords: Perovskite, colloidal quantum dots, cesium lead halides, white light emitting diodes, stability Cesium lead halide quantum dots (QDs) have the tunable photoluminescence being capable of covering the entire visible spectrum and high quantum yield, which makes them a new family member of fluorescent materials for various applications. Here, we report the synthesis of CsPbX3 (X=Cl, Br, I, or mixed Cl/Br and Br/I) QDs by direct ion reactions in ether solvents, and demonstrate for the first time the synergetic effects of solvent polarity and reaction temperature on the nucleation and growth of QDs. The use of solvent with a low polarity enables controlled growth of QDs, which facilitates the synthesis of high-quality CsPbX3 QDs with broadly tunable luminescence, narrow emission width, and high quantum yield. We also demonstrate a QDs-white LED (WLED) by coating the highly-fluorescent green-emissive CsPbBr3 QDs together with red phosphors on a blue InGaN chip, which presents excellent warm white light emission with a high rendering index of 93.2 and Tc of 5447 K, suggesting the potential applications of highly fluorescent cesium lead halide perovskite QDs as an alternative color converter in the fabrication of WLEDs. We also illustrate a ligand exchange induced co-precipitation (LEIC) approach to fabricate composites based on CsPbX3 QDs incorporated in stearate (e.g., zinc stearate). This approach can be performed in large scale without harsh reaction condition, which is green, fast and efficient. More importantly, this approach enables the purification of QDs and retains their PLQY at the same time. The tight matrix protects QDs from the surrounding environment thus increasing the stability. Figures:Cesium lead halide quantum dots and their white Light Emitting Diodes(left), and CsPbX3 QDs/zinc stearate composite with high stability is synthesized by ligand exchange induced coprecipitation approach(right). # Presenting Author Corresponding Author : Email: [email protected] ( Prof. Yang Jiang ) * 61 4.1.3 Enhanced Extraction in Flexible OLEDs with Nanostructured Substrates Jianxin Tang*,# Institute of Functional Nano & Soft Materials (FUNSOM), Soochow University, Suzhou 215123, China Tel.: +86-512-6588-0942, E-mail: [email protected] Keywords: Flexible OLEDs, light extraction, flexible transparent electrode, Flexible organic light-emitting diodes (OLEDs) hold great promise for future bendable display and curved lighting applications. One key challenge of high-performance flexible OLEDs is to develop new flexible transparent conductive electrodes with superior mechnical, electrical and optical properties. Herein, we demonstrate a new strategy to achieve a powerful transparent conductive electrode on plastic substrate that combines a quasi-random nanostructured optical coupling layer and an ultrathin metal alloy conduction layer. The optimum electrical conductivity, optical manipulation capability, and high tolerance to mechanical bending are realized in this composite electrode, which is favorable for the fabrication of ITO-free flexible OLEDs with state-of-the-art performance on low-refractive-index plastic substrate. The angularly and spectrally independent boost in light outcoupling of white emission is obtained by minimizing the waveguide mode, metallic electrode-related microcavity effect and surface plasmonic loss due to the integrated quasirandom outcoupling structure in the composite electrode. The resulting white flexible OLED exhibits the high enhancement in efficiency, e.g., external quantum efficiency of 47.2% and power efficiency of 112.4 lm/W. In addition, this composite electrode has a scalable manufacturing potential in large-area flexible electronic systems. 10 60 10 3 30 10 2 10 1 4 5 6 Voltage (V) 7 8 -1 Current efficiency (cd A ) 10 10 10 3 10 2 1 3 10 10 5 3 4 1 10 5 (d) 1.0 0.5 0.0 4 10 10 -2 Luminance (cd m ) ITO MDCE NMDCE 10 10 -2 Luminance (cd m ) 2 ITO MDCE NMDCE 20 0 -1 (c) 30 10 Normalized EL (a.u.) 3 Power efficiency (lm W ) -2 Current density (mA cm ) 0 50 40 EQE (%) 90 4 (b) -2 5 ITO MDCE NMDCE Luminance (cd m ) 10 (a) 120 400 ITO MDCE NMDCE 500 600 Wavelength (nm) 700 Fig. 1. Device structure and performance of flexible white OLEDs. (a) Current density and luminance as a function of driving voltage. (b) EQE as a function of luminance. (c) CE and PE as a function of luminance. (d) Normalized EL spectra at 1000 cd m-2. Inset is the photograph of white-emission flexible OLED. References 1. L. H. Xu, Q. D. Ou, Y. Q. Li, Y. B. Zhang, X. D. Zhao, H. Y. Xiang, J. D. Chen, L. Zhou, S. T. Lee, J. X. Tang, ACS Nano 10, 1625 (2016). 2. H. Y. Xiang, Y. Q. Li, L. Zhou, H. J. Xie, C. Li, Q. D. Ou, L. S. Chen, C. S. Lee, S. T. Lee, J. X. Tang, ACS Nano 9, 7553 (2015). 3. L. Zhou, H. Y. Xiang, S. Shen, Y. Q. Li, J. D. Chen, H. J. Xie, I. A Goldthorpe, L. S. Chen, S. T. Lee, J. X. Tang, ACS Nano 8, 12796 (2014). 62 4.1.4 Development of High EQE OLEDs: from Efficient Internal Generation to External Extraction Chung-Chih Wu1,a)* #, Ken-Tsung Wong2, Yun Chi3 Department of Electrical Engineering, National Taiwan University, Taipei, Taiwan 2 Department of Chemistry, National Taiwan University, Taipei, Taiwan 3 Department of Chemistry, National Tsing Hua University, Taipei, Taiwan a) [email protected] 1 Keywords: OLED, internal quantum efficiency, light out-coupling, phosphorescence, TADF. To achieve ultimately high external quantum efficiencies of OLEDs, OLED materials and device architectures that can achieve high internal quantum efficiencies and high optical out-coupling efficiencies are equally important. In the paper, we will present some of our recent works on OLED materials and devices that can provide ideal internal quantum efficiencies and high optical out-coupling efficiencies. In addition to phosphorescent transition metal complexes, metal-free luminophores showing efficient thermally activated delayed fluorescence (TADF) are also emerging as attractive alternatives for harvesting both singlet and triplet excitons in organic electroluminescence (EL) to achieve ideal 100% internal quantum efficiency. In this presentation, in addition to presentation of some efficient (blue to red emitting) phosprescent emitters, a few series of TADF emitters having highly efficient photophyical properties and EL properties will be discussed. For instance, extremely efficient blue organic EL with external quantum efficiency (EQE) of ~37% is achieved in a conventional planar device structure, using a highly efficient TADF emitter based on the spiroacridine-triazine hybrid that simultaneously possesses nearly unitary (100%) photoluminescence quantum yield, excellent thermal stability, and strongly horizontally oriented emitting dipoles (with a horizontal dipole ratio of 83%). Yet as another example, efficient and tunable blue-green to yellow TADF emitters capable of generating OLED EQEs of >31% are developed adopting the acridine donor unit and CN-substituted benzene, pyridine and pyrimidine acceptor units. These materials permit one to systematically probe the influence of different acceptor strengths and also the influence of tunable conformations (twist angles) within the acceptor moieties through controlling the orientation of asymmetric heteroaromatic ring relative to the donor component. On the other hand, we will also show that judicious use of low-index active organic materials and transparent electrodes in OLEDs, together with OLED emitters with preferentially horizontal emitting dipoles, can effectively enhance optical coupling both into substrate and directly into air. We will discuss a few OLED structures that contain low-index active organic materials and transparent conductors and could significantly enhance light out-coupling of OLEDs, including: (1) an OLED using the low-index hole-injection layer, (2) an OLED using the low-index transparent electrode to replace conventional ITO, and (3) an OLED using the low-index transparent electrode and a high-index underlayer. As a result, OLED EQEs of up to 39% had been achieved with the simple planar device structure, while EQE of 64-65% had been achieved further with further adopting simple external extraction schemes. # Presenting Author Corresponding Author * 63 4.2.1 Rational Materials Design for Ultrafast Rechargeable Lithium-ion Batteries Xiaodong Chen* Innovative Center for Flexible Devices, School of Materials Science and Engineering, Nanyang Technological University, 50 Nanyang Avenue, 639798, Singapore [email protected] Rechargeable lithium-ion batteries (LIBs) are important electrochemical energy storage devices for consumer electronics and emerging electrical/hybrid vehicles. However, one of the formidable challenges is to develop ultrafast charging LIBs with the rate capability at least one order of magnitude higher than that of the currently commercialized LIBs. In this talk, I will present our recent development of ultrafast charging LIBs by the rational design of materials. First of all, I will discuss the protocol to rationally grow elongated titanate nanotubes with length up to tens of micrometers by a stirring hydrothermal method. The mechanical forcedriven stirring process synchronously improving the diffusion and surface reaction rate of titanate nanocrystal growth in solution phase is the reason for lengthening the titanate nanotubes via an oriented attachment mechanism. This protocol to synthesize elongated nanostructures can be extended to other nanostructured systems, opening up new opportunities for manufacturing advanced functional materials for high-performance energy storage devices. Then, we will show how a robust three-dimensional network architecture with antiaggregation property is formed for long-time cycling through the assembly of continuous one-dimensional TiO2 nanotubes, which provides direct and rapid ion/electron transport pathways and adequate electrodeelectrolyte contact and short lithium ion diffusion distance comparing with other nanostructures. Finally, the future trends and perspectives for the ultrafast rechargeable LIBs are discussed. Continued rapid progress in this area is essential and urgent to endow LIBs with ultrafast charging capability to meet huge demands in the near future. 64 4.2.2 Hierarchically Porous Materials as Electrodes for Energy Storage Batteries LongweiYin*, Zhaoqiang Li, Xiaoli Ge, Zhiwei Zhang, Qun Li School of Materials Science and Engineering, Shandong University, 17923 Jing Shi Road, Jinan 250061, Emal:[email protected] The increasing demand for higher energy density storage devices steers scientific researches on high capacity electrode materials. Carbon aerogel (CA) represents a novel and special type of porous carbon material with interconnected structure, and higher electrical conductivity than other materials. The principal features of CA materials are a high surface area (400-900 m2/g) and a high pore volume (1-3 cm3/g). Due to its controllable three-dimensional porous structures, CA is considered to be an ideal electrode material for supercapacitors and rechargeable batteries due to their unique three-dimensional nano-network, high specific surface area, abundant mesopores and high electric conductivity. Metal-organic frameworks (MOFs) or coordination polymers have drawn much attention for their applications as electrodes for energy storage applications. MOFs consisting of organic ligands and metal ions, can transform into carbon materials and metal species with proper methods. Carbon materials derived from MOFs by simply carbonization of organic ligand and removal of metal species have shown good electrochemical performance in lithium-sulfur batteries and lithium-selenium battery applications. MOFs derived tailorable metal oxides or metal oxide/carbon nanomaterials with unique nanostructures exhibit outstanding electrochemical performance when used as LIBs anodes. In the present work, nitrogen-doped carbon sponges (NCS) composed of hierarchically micropores carbon layers, a sandwich-like structure with reduced graphene oxide (RGO) wrapped MOFderived ZnCo2O4-ZnO-C polyhedrons on nickel foam as an anode for high performance lithium ion batteries (LIBs), core@shell structure of Fe2O3@Co3O4 hollow structures from MOFs precursors are synthesized. Three dimensional S/carbon aerogel (CA), spinel ZnMn2O4/CA, Co3O4/CA hybrids with abundant pores and large surface area, are designed and synthesized. The electrochemical energy storage performance and related mechanism, the relation between the microstructure and the electrochemical performance are systematically investaiged. offers a new way and provides guidelines for designing electrode architectures and cell configurations to achieve high-energy-density batteries. Keywords: porous; metal-organic framework; carbon aerogel; electrochemical energy storage; electrode. 65 4.2.3 Developing Sn based alloy materials for anode applications in Na-ion batteries Wenhui Wang, Danni Lan, Quan Li *# Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, HongKong 1 Keywords: Sodium ion battery, Anode, Tin-based alloy Na ion batteries (NIBs) are promising alternatives for Lithium ion batteries (LIBs) mainly due to the Na abundance and low cost. Unlike Li-ion batteries, graphite no longer works as a suitable anode, as the larger size of Na+ makes it impossible for its insertion into the spaces between adjacent layers of the graphite. Consequently, developing anode materials for sodium ion batteries becomes a major task to enable practical application of NIBs for large scale storage. Among various material choices, Sn is a promising candidate due to its high theoretical capacity (847mAh/g or 1210Ah/L). Nevertheless, Sn suffers from problems of significant volume change, stress built-up, and aggregation during charge/discharge processes, leading to quick performance decay over a few cycles. In the present work, we tackle this problem by alloying Sn with other elements, trying to reduce the stress built-up and aggregation of Sn, and thus improving the cycling stability of the anode materials. We will discuss the roles of various material parameters of the Sn-based alloys in determining their electrochemical performance of the anode. We show that by choosing the right alloy and controlling the size and composition of the alloy material via different fabrication techniques, the cycling performance of the anode can be largely enhanced. This work is supported by RGC/GRF under project No. 14316716 # Presenting Author Corresponding Author * 66 4.2.4 Recent Progress of the Novel Aluminum-Graphite Dual-Ion Battery Xiaolong Zhang, Fan Zhang, Xuefeng Tong, Bifa Ji, Maofa Sheng, Chun-Sing Lee, Yongbing Tang,* Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen 518055 * Corresponding author, email: [email protected] Abstract We report a novel aluminum-graphite dual-ion battery (AGDIB) in an conventional electrolyte with high reversibility and high energy density. It is the first report on using an aluminum anode in dualion battery. The battery shows good reversibility, delivering a capacity of ~100 mAh g−1 and capacity retention of 88% after 200 charge-discharge cycles at 2 C (1 C corresponding to 100 mA g−1). A packaged aluminum-graphite battery is estimated to deliver an energy density of ~150 Wh kg-1 at a power density of ~1200 W kg-1, which is ~50% higher than most commercial lithium ion batteries. In this talk, we will present recent progress of this battery. Fig. 1 a) Schematic illustration of the AGDIB in the initial state (up) and the charged state (below). b) Galvanostatic charge-discharge curve of the AGDIB at 0.5 C. Insets are the dQ/dV differential curve and a photograph showing that a single AGDIB cell lighting up two yellow LEDs in series. Keywords: aluminum, graphite, anion intercalation, dual ion battery References 1. X.L. Zhang, Y. B. Tang,* et al. Adv. Energy Mater. 2016, DOI: 10.1002/aenm.201502588 2. X.F. Tong, F. Zhang, Y. B. Tang,* et al. Adv. Mater. 2016, DOI: 10.1002/adma.201603735 3. B.F. Ji, F. Zhang, Y. B. Tang*, et al. Adv. Mater. 2016, DOI: 10.1002/adma.201604219 4. F. Zhang, Y. B. Tang*, et al. Adv. Mater. Interfaces, 2016, DOI: 10.1002/admi.201600605 5. M. H. Sheng, Y. B. Tang*, et al. Adv. Energy Mater. 2016, DOI: 10.1002/aenm. 201601963 67 4.3.1 High Performance Solution-Processed Perovskite Hybrid Solar Cells via Device Engineering and Novel Materials Xiong Gong, Ph. D. College of Polymer Science and polymer Engineering, The University of Akron, Akron OH 44325 E-mail: [email protected] Efficiently and economically harnessing the solar energy via photovoltaic (PV) devices presents as one of promising solutions to the global energy crisis. However, over 80% available PVs are silicon-based solar cells and inorganic thin film solar cells, which are expensive and require critical processing techniques. Solutionprocessed perovskites hybrids solar cells have shown great potential as novel, high-efficient and low-cost PV devices, which are renewable, economic and green energy sources in the future energy market. In this presentation, I would like to share with you how we approach high-performance solution-processed perovskite hybrid solar cells. - In order to facilitate electron extraction efficiency in perovskite solar cells and make it comparable to the hole extraction efficiency, we, for the first time, demonstrate bulk heterojuncion perovskite hybrid solar cells with enhanced efficiency and less photo-hysteresis; - By reengineering the interface of solution-processed perovskite materials with cross-linkable ionomer and polymer doped high electrical conductive hole extraction layer, we are able to demonstrate perovskite hybrid solar cells with boosted efficiency and significantly reduced photo-hysteresis; - In order to balance charge transporting properties and eliminate toxic lead, we have developed novel perovskite materials incorporated with transition metals for substituting lead. Both electron and hole transporting properties of resultant perovskite materials are enhanced. As a result, the power conversation efficiencies of solution-processed perovskite hybrid solar cells fabricated by these novel perovskite materials are significantly boosted. Keywords: Perovskite Hybrid Solar Cells, Interfacial Engineering, Device Structures and Novel Materials 68 4.3.2 Stable Planar Perovskite Solar Cells under Continuous Light Irradiation Chuanjiang Qin*,#, Toshinori Matsushima, Chihaya Adachi* Center for Organic Photonics and Electronics Research (OPERA), Kyushu University, Japan Science and Technology Agency (JST), ERATO, Adachi Molecular Exciton Engineering Project, 744 Motooka, Nishii, Fukuoka, 819-0395, Japan E-mail: [email protected], [email protected] Keywords: stability, degradation mechanism, carrier traps, Frenkel defect, perovskite solar cells Organic-inorganic hybrid halide perovskites have emerged as an interesting class of materials that have excellent photovoltaic properties for application to solar cells. In the last four years, the power conversion efficiency of perovskite solar cells (PSCs) over 20% has recently been realized through systematic optimization of materials and fabrication processes. However, the stability of PSCs is just beginning to be studied, and the actual degradation mechanisms of PSCs are not well understand. Carrier traps (in other words, defect states or gap states) are well known to impede carrier collection by the electrodes and act as carrier recombination centers, which are detrimental to solar cell performance. Here, we investigate the degradation mechanisms of CH3NH3PbI3-based PSCs using a thermally stimulated current technique, which is a versatile technique used to analyze carrier traps in inorganic and organic materials. We show that a large density of hole traps is formed in PSCs degraded by continuous solar illumination and that the formation of hole traps is strongly related to the stability. This is the first report describing the trap-induced degradation of PSC performance.[1] One source of the traps is metallic lead resulting from photodegradation of CH3NH3PbI3 in the presence of water. We greatly extended the lifetime of PSCs under standard laboratory weathering testing (ISOS-L-1 Laboratory) with a light intensity of 100 mW cm-2 without using a UV filter from 150 hours to 4000 hours by suppressing the formation of Frenkel defect-metallic lead, which is longest device lifetime reported so far as shown in Figure 1.[2] Figure 1. Evolution curves of JSC, VOC, FF, and η for the device with the longest lifetime under continuous one sun solar irradiation (100 mW cm−2, AM 1.5G) without a UV cut filter at open-circuit conditions. [1] C. Qin, T. Matsushima, T. Fujihara, W. J. Potscavage, Jr., and C. Adachi, “Degradation mechanisms of solution-processed planar perovskite solar cells: thermally stimulated current measurement for analysis of carrier traps”, Advanced Materials, Vol. 28, No. 3, (2016), pp 466-471. [2] C. Qin, T. Matsushima, T. Fujihara, and C. Adachi, “Multifunctional benzoquinone additive for efficient and stable planar perovskite solar cells”, Advanced Materials, in press. 69 4.3.3 Surfactant n-Dopant in Cathode Interlayer or Electron Transport Layer for Polymer or Perovskite Solar Cells with Improving Performance Chih-Yu Chang,1,* Wen-Kuan Huang,1 Kuan-Ting Lee,1 Jhao-Lin Wu,2,3 Chao-Tsen Chen,2 Chin-Ti Chen3,*,# 1 Department of Materials Science and Engineering, Feng Chia University, Taichung 40724, Taiwan, 2 Department of Chemistry, National Taiwan University, Taipei 10617, Taiwan, 3Institute of Chemistry, Academia Sinica, Taipei 11529, Taiwan Keywords: cathode interlayer, n-dopant, polymer photovoltaic, perovskite solar cell, ZrOx, PC61BM. We present a simple and effective method to improve the performance and stability of organic and perovskite solar cells by the incorporation of room temperature solution-processed cetyltrimethylammonium bromide (CTAB)-doped zirconium oxide (ZrOx) as cathode interlayer. Via anion-induced electron transfer between the bromide anions (Br−) of CTAB and ZrOx in the solid state, electrical conductivity was significantly improved from 4.3 × 10-9 to 2.9 × 10-5 S cm-1. CTAB doping lifts up work function of ZrOxcoated Ag electrode from 4.21 to 3.72 eV, which facilitates a better ohmic contact to a polymer (PTB7 or PDPP-TBT):fullerene (PC61BM or PC71BM) bulk heterojunction or perovskite (CH3NH3PbI3)/PC61BM bilayer and a higher built-in potential of the device. These are the causes for higher short-circuit current (JSC), higher open-circuit voltage (Voc), and hence better power conversion efficiency (PCE), 9.3 vs. 3.2% (PTB7), 2.5 vs. 0.6% (PDPP-TBT), 15.9 vs. 7.1% (perovskite). Surfactant CTAB-doped PC61BM works as well in p-type perovskite solar cells. The combination of the ion pair interaction (from PC61BM radical anion and cetyltrimethylammonium cation) and long floppy cetyl group of CTAB reduces the aggregation of PC61BM and promotes the coverage of the PC61BM thin film onto the perovskite layer. Our fabricated p-type perovskite solar cells deliver PCE as high as 17.11%, which is much better than CH3NH3PbI3/PC61BM devices without CTAB dopant (PCE is only 2.15%). Moreover, CTAB-doped perovskite solar cells showed little hysteresis and retained 80% of the initial PCE after 360 hours of shelf-storage, where devices were under ambient conditions (30 oC, ~60% relative humidity) without extra package or encapsulation. 1. Chang, C.-Y.; Huang, W.-K.; Chang, Y.-C.; Lee, K.-T.; Chen, C.-T. J. Mater. Chem. A 2016, 4, 640-648. A solution-processed n-doped fullerene cathode interfacial layer for efficient and stable large-area perovskite solar cells 2. Chang, C.-Y.; Huang, W.-K.; Wu, J.-L.; Chang, Y.-C.; Lee, K.-T.; Chen, C.-T. Chem. Mater. 2016, 28, 242-251. Room-temperature solution-processed n‑ doped zirconium oxide cathode buffer layer for efficient and stable organic and hybrid perovskite solar cells 70 4.3.4 Interface and Crystallization Engineering of Organic/Inorganic Hybrid Materials for High-Performance Perovskite Solar Cells Shihe Yang Department of Chemistry, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong E_mail: [email protected] ABSTRACT Hybrid organic/inorganic perovskite solar cells continue to attract the interest of a wide community of researchers. One of the outstanding features of the perovskite materials is their solution processibility while forming high-quality films for photovoltaic and optoelectronic devices. In order to improve the perovskite film growth from solutions, it is important to understand the physical and chemical processes involved. In this contribution, we will present our studies on the interplay of nanostructured electrodes, perovskite films and their interfaces. The impact of the interplay on solar cell performance, including power conversion efficiency, stability, etc., will be discussed through a few examples using specially designed nanobowl array electrode of mesoporous TiO2, sol-gel processed NiO and nanostructured carbon.. Acknowledgements. The collaborators who have variously contributed to the work presented here are gratefully acknowledged. This work was supported by the HK-RGC (GRF No. 16300915), NSFC/RGC Joint Research Scheme (N_HKUST610/14) and HK-ITF (ITS/004/14). 71 Plenary4.1 Electrochemical Process and Interfacial Structure in Lithium-Sulfur Battery: Materials and in Situ AFM Study Li-Jun Wan Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190 and University of Science and Technology of China, Anhui 230026 E-mail: [email protected]; [email protected] Abstract Lithium-sulfur (Li-S) batteries are highly appealing for large-scale energy storage owing to its promising theoretical energy density. The main issues of the Li-S battery regarding performance fading are highly related to electrode materials as well as the interfacial properties. Here, we present the electrochemical process of a Li-S battery. Based on the electrochemical mechanism, we prepared several electrode materials and made a direct visualization of interfacial structure and dynamics of Li-S discharge/charge processes at nanoscale. In situ atomic force microscopy (AFM) along with ex situ spectroscopic methods directly distinguish the morphology and growth process of insoluble product Li2S2 and Li2S2. These findings reveal a straightforward structure-reactivity correlation and performance fading mechanism in Li-S batteries. 72 5.1.1 Multilayer Transparent Electrodes: from Flexible OLEDs to See-through Solar Cells Seunghyup Yoo1*#, Jaeho Lee1, and Hoyeon Kim1 School of Electrical Engineering, Korea Advanced Institute of Science and Technology (KAIST), Daejeon, 34141, Republic of Korea 1 Keywords: transparent electrodes, graphene, flexible OLED, semitransparent solar cells, perovskite We explore multilayer transparent electrodes (MTEs) as a versatile alternative to transparent conductive oxides. Based on triple layers consisting of an external dielectric layer, a thin metal layer or emerging conducting layer like graphene, and an interfacial transparent buffer layer, these MTEs can be easily tailored to specific applications such as organic light-emitting diodes (OLEDs) and solar cells yet holds a great promise for optical enhancement of efficiency, realization of flexible form factors, and so on. As a key example, this talk will introduce highly flexible OLEDs and see-through perovskite solar cells based on these MTEs. The flexible OLED adopts bottom MTEs based on TiO2 as a high-index dielectric layer, graphene, and a conducting polymer layer as a low-index layer [1]. Its electrode and overall device structure is optimized to take an advantage of their full optical potential for ultra-efficient devices. In case of see-through solar cells, the non-damaging nature of MTEs is utilized as a top transparent electrode essential in semi-transparent devices with active layers having a relatively low damage threshold. With an MTE based on ZnS-Ag-MoOx, see-through perovskite solar cells with high efficiency is realized [2]. The study further reveals that it can provide an additional benefit of thermal IR reflection, which could be useful for smart energy management. # Presenting Author Corresponding Author * REFERENCES [1] Jaeho Lee, Tae-Hee Han, Min-Ho Park, Dae Yool Jung, Jeongmin Seo, Hong-Kyu Seo, Hyunsu Cho, Eunhye Kim, Jin Chung, Sung-Yool Choi, Taek-Soo Kim, Tae-Woo Lee, Seunghyup Yoo, “Synergetic electrode architecture for efficient graphene-based flexible organic light-emitting diodes,” Nature Communications 7, 11791 (2016) [2] Hoyeon Kim, Hui‐Seon Kim, Jaewon Ha, Nam‐Gyu Park, Seunghyup Yoo, “Empowering Semi‐Transparent Solar Cells with Thermal‐Mirror Functionality,” Advanced Energy Materials, 6, 1502466 (2016) 73 5.1.2 Triplet Harvesting in Fluorescence and Phosphorescence Hybrid White OLEDs Xiao-Ke Liu1,a), Chun-Sing Lee2, Xiao-Hong Zhang3 Department of Physics, Chemistry and Biology (IFM), Linköping University, 581 83 Linköping, Sweden 2 Center of Super-Diamond and Advanced Films (COSDAF) and Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR 3 Functional Nano and Soft Materials Laboratory (FUNSOM) and Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou, Jiangsu 215123, P.R. China 1 Keywords: fluorescence, phosphorescence, TADF, exciplex, charge-transfer states Fluorescence and phosphorescence hybrid white OLEDs (F-P WOLEDs) combining blue fluorescent emitters with green/orange/red phosphors have attracted considerable attention in recent years due to their promising applications in solid-state lighting. To realize high-efficiency F-P WOLEDs, electrically generated singlet and triplet excitons are expected to be effectively separated and then respectively harvested by the blue fluorophore and the green/orange/red phosphors to generate white light.[1] One of the most challenging issues for F-P WOLEDs is to achieve full triplet harvesting from the blue fluorophore to green phosphors. This challenge raises new claims on the blue fluorophores, including high efficiency and high triplet energy level, etc. In this talk, we will represent our rational concepts for designing and developing efficient and high-triplet blue fluorophores for high performance F-P WOLEDs. The first concept is to establish intramolecular chargetransfer (CT) states in the blue fluorophores by using donor-π-acceptor (D-π-A) backbones. In such a D-π-A molecule, HOMO and LUMO would be mainly distributed on the D unit and the A unit, respectively, and suitable overlap between the HOMO and the LUMO would be located on the π bridge. This design ensures that the molecule emits strong blue fluorescence and has high triplet energy level. On the basis of this design, we developed a series of blue fluorophores with triplet energy levels >2.4 eV and high EQEs.[2] High performance and simple-structured F-P WOLEDs were achieved based on these blue fluorophores.[2b, 2c] The second concept for effective triplet harvesting in F-P WOLEDs is to use blue exciplexes with thermally activated delayed fluorescence (TADF). Since pioneering work was reported by Adachi and coworkers[3], TADF exciplexes have been widely studied and used as emitters and hosts.[4] Considering that blue TADF exciplexes have intrinsic high triplet energy levels due to their nearly zero singlet-triplet energy gaps, they would be a promising candidate for F-P WOLEDs. Following this concept, we realized high performance F-P WOLEDs based on TADF blue exciplexes.[5] [1] Y. R. Sun, N. C. Giebink, H. Kanno, B. W. Ma, M. E. Thompson, S. R. Forrest, Nature 2006, 440, 908. [2] a) X.-K Liu, C.-J. Zheng, M.-F. Lo, J. X., C.-S. Lee, M.-K. Fung, X.-H. Zhang, Chem. Commun. 2014, 50, 2027; b) X.-K. Liu, C.-J. Zheng, M.-F. Lo, J. Xiao, Z. Chen, C.-L. Liu, C.-S. Lee, M.-K. Fung, X.-H. Zhang, Chem. Mater. 2013, 25, 4454; c) Z. Chen, X.-K. Liu, C.-J. Zheng, J. Ye, X.-Y. Li, F. Li, X.-M. Ou, X.-H. Zhang, J. Mater. Chem. C 2015, 3, 4283. [3] K. Goushi, K. Yoshida, K. Sato, C. Adachi, Nat. Photonics 2012, 6, 253. [4] a) X.-K. Liu, Z. Chen, C.-J. Zheng, C.-L. Liu, C.-S. Lee, F. Li, X.-M. Ou, X.-H. Zhang, Adv. Mater. 2015, 27, 2378; b) X.-K. Liu, Z. Chen, C.-J. Zheng, M. Chen, W. Liu, X.-H. Zhang, C.-S. Lee, Adv. Mater. 2015, 27, 2025; c) J.-H. Lee, S.-H. Cheng, S.-J. Yoo, H. Shin, J.-H. Chang, C.-I. Wu, K.-T. Wong, J.-J. Kim, Adv. Funct. Mater. 2015, 25, 361. [5] a) X.-K. Liu, Z. Chen, J. Qing, W.-J. Zhang, B. Wu, H. L. Tam, F. Zhu, X.-H. Zhang, C.-S. Lee, Adv. Mater. 2015, 27, 7079; b) Z. Chen, X.-K. Liu, C.-J. Zheng, J. Ye, C.-L. Liu, F. Li, X.-M. Ou, C.-S. Lee, X.-H. Zhang, Chem. Mater. 2015, 27, 5206; c) X.-K. Liu, W. Chen, H. T. Chandran, J. Qing, Z. Chen, X.-H. Zhang, C.-S. Lee, ACS Appl. Mater. Interfaces 2016, 8, 26135. a) [email protected] 74 5.1.3 Novel Thermally Activated Delayed Fluorescence Materials-Thioxanthone Derivatives and Their Application for OLEDs Ying Wang1,2#*, Hui Wang1, Lingqiang Meng1, Lisha Xie3, Xiaopeng Lv4, Pengfei Wang1,2 Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, No. 29 Zhongguancun East Road, Haidian District, Beijing, 100190, P. R. China; 2University of Chinese Academy of Sciences, Beijing, 100049, P. R. China; 3College of Life Science and Technology, Beijing University of Chemical Technology, Beijing, 100029, P. R. China; 4 Institute of Functional Nano & Soft Materials (FUNSOM), Jiangsu Key Laboratory for Carbon-Based Functional Materials & Devices, Soochow University, Suzhou 215123, P. R. China 1 Keywords: Thioxanthone derivatives, Thermally activated delayed fluorescence (TADF), Organic light emitting diodes. Thermally activated delayed fluorescent (TADF) emitters based on pure organic aromatic compounds aroused much attention in that an internal quantum efficiency of 100% can be achieved by taking advantage of the efficient up-conversion of the triplet excitons. Novel TADF emitters based on thioxanthone unit, TXOTPA and TXO-PhCz, were reported. Both emitters exhibited high fluorescent efficiency and small energy gap between the triplet and singlet (EST), affording the high efficient up-conversion process from triplet states to singlet states. Their application in the high performance organic light emitting diodes were investigated in detail. Novel phosphorescent host based on thioxanthone unit with TADF was also reported. The host with TADF can be used to reduce the efficiency roll-off of red and yellow light phosphorescent OLEDs. These results made thioxanthone derivatives promising for the application in the future organic flat panel display and solid-state lighting. 100 (b) (a) EQE(%) 10 TXO-TPA TXO-PHCZ 1 0.1 1 10 100 2 Luminance (cd/m ) 1000 (c) MTXSFCz Figure 1. (a) Chemical structure of TXO-TPA and TXO-PhCz (inset) and device performance of OLEDs based on them; (b) EL spectra of multilayer white OLEDs; (c) Chemical structure of MTXSFCz and their device performance of red and yellow phosphorescent OLEDs. References 1. H. Uoyama, K. Goushi, K. Shizu, H. Nomura, C. Adachi*, Nature 2012, 492, 234-238. 2. S. Ishijima, M. Higashi, H. Yamaguchi*, J. Phys. Chem. 1994, 98, 10432-10435. 3. H. Wang, L. Xie, Q. Peng, L. Meng, Y. Wang*, Y. Yi, P. Wang*, Adv. Mater. 2014, 26, 5198−5204. 4. H. Wang, L. Meng, X. Shen, X. Wei, X. Zheng, X. Yi, Y. Wang*, P. Wang*, Adv. Mater. 2015, 26, 5198−5204. 5. L. Meng, H. Wang, X. Wei, X. Lv, Y. Wang*, P. Wang, RSC Adv. 2015, 5, 59137-59141. 6. L. Meng, H. Wang, X. Wei, J. Liu, Y. Chen, X. Kong, X. Lv, P. Wang, Y. Wang*, ACS Appl. Mater. Interfaces 2016, 8, 20955-20961. 7. L. Xie, G. Ge, Y. Chen, H. Wang, X. Kong, X. Wei, J. Liu, Y. Yi, B. Chen, P. Wang, Y. Wang*, J. Mater. Chem. C 2016, Accepted. # Presenting Author Corresponding Author [email protected] * 75 5.2.1 In-situ measurement of the thickness change of dense Si electrodes in lithium-ion batteries using electrochemical dilatometry Pui-Kit Leea, Yingshun Lia,b, Denis Y.W. Yua,b,#,* School of Energy and Environment and bCenter of Super-Diamond and Advanced Films, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kong SAR. [email protected] a Keywords: Lithium-ion battery, silicon, in-situ dilatometry, mechanical issue, binder Silicon has been the focus of many research studies as the next generation high-capacity anode material for lithium-ion batteries. However, the mechanical stability of the electrode remains a bottleneck to the commercialization of the material. Many studies were devoted to nanostructured silicon composites with voids to accommodate the volume expansion [1]. Yet, full capability of silicon cannot be utilized because of the low volumetric energy density of these nanostructures. To increase the volumetric energy density compared to graphite, dense silicon electrodes are needed. Volume expansion within the electrode becomes an important factor affecting its cycle stability. In reality, how much is the volume expansion? What is the mechanism during the charge and discharge? Few studies have addressed these issues. In this work, we employed electrochemical dilatometry to measure the thickness change of Si electrodes during charge and discharge to understand the behavior with time. Fig. 1 shows the change in thickness with respect to cumulative capacity of a Si electrode with 20% carbon black and 20% carboxymethyl cellulose (CMC) during the first three cycles. As expected, an increase in electrode thickness is observed during lithiation (increase in capacity), and a decrease in thickness during delithiation (decrease in capacity). The increase and decrease in electrode thickness are however not linear. A three-stage expansion model is used to describe the observation. At the beginning of lithiation (stage I), the electrode thickness change is small, as the composite electrode contains space between the particles that can Fig. 1: Change in electrode thickness with lithiation and accommodate the volume expansion. Beyond a certain delithiation (Si:AB:CMC = 6:2:2). point, the particles impinge on each other and the volume expansion of the particles lead to an overall increase in the film thickness (stage II). The amount of increment during stage II is similar to the theoretical increase in volume (dotted line in Fig. 1) for alloying Li with Si, indicating that it is due to structural change within the particle. Further incorporation of lithium into the electrode leads to an accelerated increase in thickness (stage III). The onset of stage III expansion depends on the type of binder used in the electrode, which suggests that it is affected by the ability of the binder to hold the particles together. During delithiation (stage IV), the contraction behavior is different from that during expansion. This is partly because the particle can contract in all three directions, as opposed to one direction during lithiation. The Si electrode with CMC shows poor cycle performance, and binder breakdown is one of the main causes of the electrode degradation. Better reversibility in thickness change is achieved by using a high-modulus binder such as polyimide, resulting in better cycle stability. This is attributed to the ability of the PI binder to hold the particles together after expansion. More experimental details and results will be shown during the presentation. References 1) Wu, H. & Cui, Y. Nano Today 7, 414-420 (2012). # Presenting Author Corresponding Author * 76 5.2.2 Improved electrochemical performance of SnO2/CNT anodes for Na-ion batteries with controlled crystallinity and reaction kinetics Jiang Cui,* # Shanshan Yao, Jang-Kyo Kim Department of Mechanical and Aerospace Engineering, The Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong, P. R. China. *Corresponding author: [email protected] (J. Cui) Keywords: Na-ion batteries; SnO2; anode; sodiation kinetics; in situ TEM Li-ion batteries (LIBs) presently dominate the rechargeable battery markets, especially for portable electronics and electric vehicles, and there have been increasing calls for developing batteries with reduced materials and manufacturing costs for large-scale energy storage applications [1,2]. As an alternative to LIBs, cost-effective Na-ion batteries (NIBs) have drawn much attention thanks to the lower cost of sodium and the working principles similar to LIBs. As one of the most promising anode materials for NIBs, SnO2 is non-toxic and abundant together with a high theoretical capacity up to 1378 mAh g-1 [3]. However, the practical capacity is far below the expected value from theory, which has been the major obstacle hindering its further development and commercialization. To resolve the abovementioned issue, this work is devoted to specifically studying the Na storage mechanisms of SnO2 by combining electrochemical characterization tools, including ex situ X-ray diffraction (XRD) analysis and in situ transmission electron microscopy (TEM) examination. On the contrary to previous understanding of the “alloying reaction” as the major sodiation process, we discover [4] that the kinetically-controlled reversible “conversion reaction” between Na and SnO2 is responsible for Na storage in SnO2. To enhance the kinetics of conversion reaction, carbon nanotubes (CNTs) are incorporated into the electrode as the conductive substrate and the SnO2 particle sizes are reduced by controlling their degree of crystallinity. As a result, the SnO2/CNT composite anode delivers a specific capacity of 630.4 mAh g-1 at a current density of 0.1 A g-1, and 324.1 mAh g-1 at a high rate of 1.6 A g-1. Furthermore, the in situ TEM reveals much reduced volume expansion of the composite anode compared to the pristine SnO2, which in turn gives rise to an excellent capacity retention of 69 % after 300 cycles. These findings may provide new insights into fundamental understanding of Na storage mechanisms of SnO2 anodes and offer a potential solution to the conversion reaction-based anode materials with generally low capacities. [1] H. Pan, Y.-S. Hu, L. Chen, Energy Environ. Sci. 2013, 6, 2338. [2] S.-W. Kim, D.-H. Seo, X. Ma, G. Ceder, K. Kang, Adv. Energy Mater. 2012, 2, 710. [3] B. Zhang, J. Huang, J.-K. Kim, Adv. Funct. Mater. 2015, 25, 5222. [4] J. Cui, Z.-L. Xu, S. Yao, J. Huang, J. Huang, S. Abouali, M. A. Garakani, X. Ning, J.-K. Kim, J. Mater. Chem. A 2016, 4, 10964. 77 5.2.3 Nanorod to Porous Nanofibers: a Novel Strategy to Improve Lithium-Ion Storage Performance of Zn2GeO4 Huan-Huan Li, Jing-Ping Zhang* Faculty of Chemistry, National & Local United Engineering Laboratory for Power Batteries, Northeast Normal University, Changchun 130024, China. Keywords: lithium-ion batteries, Zn2GeO4, anode materials, electrospinning, carbon-free. Among various anode materials for lithium ion batteries (LIBs), Zn2GeO4 is proposed as a promising one for LIBs because of its high theoretical capacity up to 1443 mA h g-1 (originated from the dual Li-alloying reactions of Zn and Ge atoms in addition to the conversion reaction) in comparison to other ordinary transition metal oxides (TMOs).1-2 In this work, carbon-free, porous and micro/nanostructural Zn2GeO4 nanofibers (pZGONFs) have been prepared via a dissolution-recrystallization-assisted electrospinning technology. The successful electrospinning to fabricate the uniform p-ZGONFs mainly benefits from the preparation of completely dissolved solution, which avoids the sedimentation of common Ge-containing solid-state precursors. Electrochemical tests demonstrate that the as-prepared p-ZGONFs exhibit superior Li-storage properties in terms of high initial reversible capacity of 1075.6 mA h g-1, outstanding cycling stability (no capacity decay after 130 cycles at 0.2 A g-1) and excellent high-rate capabilities (e.g., still delivering a capacity of 384.7 mA h g-1 at a very high current density of 10 A g-1) when used as anode materials for LIBs. All these Li-storage properties are much better than those of Zn2GeO4 nanorods prepared by a hydrothermal process. The much enhanced Li-storage properties should be attributed to its distinctive structural characteristics including the carbon-free composition, plentiful pores and macro/nanostructures. Carbon-free composition promises its high theoretical Li-storage capacity, plentiful pores can not only accommodate the volumetric variations during the successive lithiation/delithiation but also serve as the electrolyte reservoirs to facilitate Li interaction with electrode materials. Scheme. Schematic illustration for the preparation processes of p-ZGONFs. References 1. Feng, J. K.; Lai, M. O.; Lu, L. Electrochem. Commun. 2011, 13, 287-289. 2. Li, H.-H.; Zhang, L.-L.; Fan, C.-Y.; Wu, X.-L.; Wang, H.-F.; Li, X.-Y.; Wang, K.; Sun, H.-Z.; Zhang, J.-P. J. Mater. Chem. A 2016, 4, 2055-2059. * Corresponding Author: Jing-Ping Zhang; Email: [email protected]; Fax: 86-431-85099668. 78 5.2.4 Functional polymer electrolytes for flexible energy storage devices Chunyi Zhi* Department of Physics and Materials Science, City University of Hong Kong *E-mail: [email protected] Wearable electronic textiles that store capacitive energy are a next frontier in personalized electronics [1-6]. However, the lack of industrially weavable and knittable conductive yarns in conjunction with high capacitance, limits the wide-scale application of such textiles. Here pristine soft conductive yarns are continuously produced by a scalable method with the use of twist-bundledrawing technique, and are mechanically robust enough to be knitted to a cloth by a commercial cloth knitting machine. Subsequently, we demonstrate a combination of textile industry available conductive yarn and conducting polymers can form a great basement for wearable energy storage devices. For example, a combination of metal oxide and conductive polymer can great enhanced tolerance of stretch-induced performance degradation of stretchable supercapacitors [2-3]. In case of self-healable PU sheel applied, a yarn supercapacitor can be self-healable [5]. In addition, we demonstrate a new electrolyte comprising polyacrylic acid dual cross-linked by hydrogen bonding and vinyl hybrid silica nanoparticles (VSNPs-PAA) that addresses all the superior functions and provide an ultimate solution to the intrinsic self-healability and high stretchability of a supercapacitor. Supercapacitors with VSNPs-PAA as the electrolyte are self-healed, achieving an excellent healing efficiency of ~100% even after 20 cycles of breaking/healing. By a designed facile electrode fabrication procedure, they are stretched up to 600% strain with performance enhanced. Our research represents a solid progress in portable and wearable multifunctional devices with extreme selfhealability and stretchability [1]. References (1) Y. Huang, M. Zhong, C. Y. Zhi et al., "A self-healable and highly stretchable supercapacitor based on a dual crosslinked polyelectrolyte”,Nature Communications, vol. 6, 10310, 2015. (2) Y. Huang, H. Hu, M. Zhu, C. Y. Zhi et al., "From Industrially Weavable and Knittable Highly Conductive Yarns to Large Wearable Energy Storage Textiles,"ACS Nano, vol. 9, pp. 4766-4775. (3) Y. Huang, J. Y. Tao, W. J. Meng, M. S. Zhu, Y. Huang, Y. Q. Fu, Y. H. Gao, and C. Y. Zhi, "Superhigh rate stretchable polypyrrole-based supercapacitors with excellent cycling stability," Nano Energy, vol. 11, pp. 518-525, 2015. (4) M. S. Zhu, W. J. Meng, Y. Huang, Y. Huang, and C. Y. Zhi, "Proton-Insertion-Enhanced Pseudocapacitance Based on the Assembly Structure of Tungsten Oxide," Acs Applied Materials & Interfaces, vol. 6, pp. 18901-18910, 2014. (5) Y. Huang, Y. Huang, M. Zhu, W. Meng, Z. Pei, C. Liu, H. Hu, C. Y. Zhi,"A Magnetic-Assisted Self-Healable Yarn-Based Supercapacitor," ACS Nano vol. 9, pp. 6242-6251, 2015. (6) W. J. Meng, W. Chen, L. Zhao, Y. Huang, M. S. Zhu, Y. Huang, Y. Q. Fu, F. X. Geng, J. Yu, X. F. Chen, and C. Y. Zhi, "Porous Fe3O4/carbon composite electrode material prepared from metalorganic framework template and effect of temperature on its capacitance," Nano Energy, vol. 8, pp. 133-140, 2014. 79 5.3.1 Functional porous nanomaterials enabled by convenient electrochemical methods for energy applications Haidong Bian, Xufen Xiao, Aiwu Wang, Shanshan Zeng, Yawen Zhan, Yang Yang Li #,* Center Of Super-Diamond and Advanced Films (COSDAF), Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, China Keywords: anodization; etching; porous materials; oxygen reduction reaction catalysts; batteries Economical bottom-up approaches are presented to achieve structural precision, good scalability and novel properties of nanomaterials for energy applications such as oxygen reduction reaction catalysts and battery electrodes. For example, a facile anodization method is developed for fabricating a novel type of hierarchical mesoporous SnO2 nanostructures that feature highly porous nanosheets with mesoporous pores well below 10 nm and a remarkably high surface area of 203 m2/g which represents one of the highest values reported to date on SnO2 nanostructures. The formation of this novel type of SnO2 nanostructures is ascribed to an interesting self-assembly mechanism of the anodic tin oxalate. The electrochemical measurements of the mesoporous SnO2 nanostructures indicate their promising applications as battery and supercapacitor electrode materials. # Presenting Author Corresponding Author: [email protected] * 80 5.3.2 Robust design of Ru quantum dot/N-doped holey graphene for electrochemical energy storage devices Masoud Nazarian-Samani1,2, Safa Haghighat-Shishavan2, Myeong-Seong Kim2, Suk-Woo Lee2, Seyed Farshid Kashani-Bozorg1, and Kwang-Bum Kim2 * # E-mail: [email protected] 1 School of Metallurgy and Materials Engineering, College of Engineering, University of Tehran, Tehran 11155-4563, IR Iran. 2 Department of Materials Science and Engineering, Yonsei University, 134 Sinchon-dong, Seodaemoon-gu, Seoul 120-749, Republic of Korea. Keywords: N-doped holey graphene, Ru quantum dot, dicyandiamide, energy storage devices Herein, we report a simple, versatile, defect-engineered method to fabricate Ru quantum dots (Ru QDs) uniformly anchored on nitrogen-doped holey graphene (NHG) monolith.1 It uses in-situ pyrolysis of mixed glucose, dicyandiamide (DCDA), and RuCl3, followed by an acid treatment, and a final heat treatment to introduce in-plane holes of various sizes. Differently from the various conventional bottom-up (e.g. chemical vapor deposition) and top-down (e.g., chemical reduction of graphene oxide and liquid exfoliation of pristine graphite) synthesis strategies of graphene, we used another simple yet versatile single-step method to produce a highly conductive freestanding N-doped graphene (NG) monolith with Ru QDs grown through the plane of graphene. Specifically, the material was fabricated by calcinating glucose, an abundant and sustainable compound, and RuCl3 salt. It can produce graphene on the gram scale to meet the high demand for production. This method overcomes several other disadvantages of conventional processes, such as low yield, corrosive precursors, complex instruments, toxic reductants, and low tendency for dispersion.2 A novel transmission method in scanning electron microscopy was successfully implemented to directly visualize the holes with color contrast. A low accelerating voltage of 5 kV enabled prolonged observation without significant electron beam damage. The mechanisms of hole creation were examined in detail using various characterization techniques as well as control experiments. The Ru QDs had significant catalytic activity and resulted in larger in-plane holes through the graphene sheets. The mechanical strain and the chemical reactivity of Ru QDs significantly diminished the activation energy barrier for the oxidation of C=C bonds in the graphene structure. At the meeting, detailed synthesis of Ru quantum dot/N-doped holey graphene and its application as electrode materials for electrochemical energy storage devices will be discussed. References 1. Kwang Kim et al. , J. Mater. Chem. A, 2016 Accepted for publication 2. Kwang Kim et al. , Energy Environ. Sci., 2016, 9, 1270-1281 81 5.3.3 Nanowire Devices for Electrochemical Energy Storage Liqiang Mai*, Yunlong Zhao#, Chaojiang Niu# Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, Hubei, China Keywords: One-dimensional nanomaterials, electrochemical device, micropseudocapacitors One-dimensional nanomaterials can offer large surface area, facile strain relaxation upon cycling and efficient electron transport pathway to achieve high electrochemical performance. Hence, nanowires have attracted increasing interest in energy related fields. We designed the single nanowire electrochemical device for in situ probing the direct relationship between electrical transport, structure, and electrochemical properties of the single nanowire electrode to understand intrinsic reason of capacity fading. The results show that during the electrochemical reaction, conductivity of the nanowire electrode decreased, which limits the cycle life of the devices.1 Then, the prelithiation and Langmuir-Blodgett technique have been used to improve cycling properties of nanowire electrode. Recently, we have fabricated hierarchical MnMoO4/CoMoO4 heterostructured nanowires by combining "oriented attachment" and "self-assembly".2 The asymmetric supercapacitors based on the hierarchical heterostructured nanowires show a high specific capacitance and good reversibility with a cycling efficiency of 98% after 1,000 cycles. Furthermore, we fabricated Li-air battery based on hierarchical mesoporous LSCO nanowires and nonaqueous electrolytes, which exhibits ultrahigh capacity over 11000 mAh g-1.3 We also designed the general synthesis of complex nanotubes by gradient electrospinning, including Li3V2(PO4)3, Na0.7Fe0.7Mn0.3O2 and Co3O4 mesoporous nanotubes, which exhibit ultrastable electrochemical performance when used in lithium-ion batteries, sodium-ion batteries and supercapacitors, respectively.4 In addition, we fabricated all-solid-state 3D on-chip micropseudocapacitors with ultrahigh energy and power densities.5 Our work presented here can inspire new thought in constructing novel one-dimensional structures and accelerate the development of energy storage applications. Reference [1] L. Q. Mai, Y. J. Dong, L. Xu, C. H. Han. Nano Lett. 2010, 10, 4273; [2] L. Q. Mai, F. Yang, Y. L. Zhao, X. Xu, L. Xu, Y. Z. Lou. Nature Commun. 2011, 2, 381; [3] Y. L. Zhao, L. Xu, L. Q. Mai, C. H. Han, Q. Y. An, X. Xu, X. Liu, Q. J. Zhang. PNAS. 2012, 109, 19569; [4] C. J. Niu, J. S. Meng, X. P. Wang, C. H. Han, M. Y. Yan, K. N. Zhao, X. M. Xu, W. H. Ren, Y. L. Zhao, L. Xu, Q. J. Zhang, D. Y. Zhao, L. Q. Mai. Nature Commun. 2015, 6, 7402; [5] X. C. Tian, M. Z. Shi, X. Xu, M. Y. Yan, L. Xu, A. Minhas-Khan, C. H. Han, L. He, L. Q. Mai. Adv. Mater. 2015, 27, 7476. # Presenting Author Corresponding Author * 82 6.1.1 Effects of Spin States in Perovskite Solar Cells and Light-emitting Devices Bin Hu Beijing Jiaotong University, Beijing 100044, China Huazhong University of Science and technology, Wu Han 430074, China University of Tennessee, Knoxville, Tennessee 37996, USA Keywords: Spin states, organic/inorganic hybrid perovskites, perovskite solar cells, perovskite light-emitting diodes, Rashba effect Organic-inorganic hybrid perovskites are formed with three non-degenerate spin states J=3/2, J=1/2, and S=1/2 in the unite structure under the influence of spin-orbital coupling. Theoretically, different spin states possess very distinct charge recombination, dissociation, and transport rates, and consequently leading to different photovoltaic and light-emitting actions. Furthermore, different spin states are constructed with different wavefuntion arrangements, which give rise to largely different electrical and spin polarizations. Therefore, controlling spin states provide important opportunities to further advance perovskite solar cells and light-emitting devices. Recently, we found that optically operating spin states can increase both photocurrent and photovoltage in perovskite solar cells. This experimental result presents the first-hand evidence that spin states can influence the photovoltaic actions in perovskite solar cells. Fundamentally, we can see that the effects of spin states on photovoltaic actions are essentially controlled by the spin relaxation time, charge dissociation time, and charge extraction time. Our analysis indicates that spin relaxation can affect the dissociation and charge transport during the generation of photovoltaic actions, leading to the effects of spin states on photocurrent and photovoltage in both Sn-based and Pb-based perovskite solar cells. On the other hand, we observed that perovskite light-emitting devices can demonstrate low and high electroluminescence efficiencies when spin mixing between different spin states becomes in-operative and operative, respectively, at low and high injection currents. We found that the in-operative and operative spin mixing essentially result from monomolecular and bimolecular recombination to generate low and high electroluminescence efficiencies. Our studies show that spin mixing between different spin states can provide a unique method to control the electroluminescence efficiencies in perovskite light-emitting devices. This presentation will discuss the effects of spin states on photovoltaic and electroluminescence actions in perovskite solar cells and light-emitting devices. 83 6.1.2 High-efficiency Nondoped Deep Blue Light-emitting Materials Based on Bisphenanthroimidazole Derivatives Qing-Xiao Tong1*, Chun-Sing Lee2, Wen-Cheng Chen2 1 Departmen t of Chemistry, Shantou University, Guangdong, 515063, P. R. China, 2Center of Super-Diamond and Advanced Films (COSDAF), City University of Hong Kong, Hong Kong SAR, 999077, P. R. China Keywords: Phenanthroimidazole, Non-doped, Deep Blue, Organic Light-emitting Materials. Blue organic light-emitting materials have attracted much attention because of their significant applications in flat-panel displays and solid-state lighting. Especially in full-color displays, the blue emitter can not only effectively reduce the power consumption of the devices but also be utilized to generate emission of other colors by energy transfer to a suitable emissive dopant. However, high-performance blue emitters are still relatively rare. The intense interest in phenanthroimidazole (PI)-based blue-emitting materials stems from their attractive potential bipolar properties and excellent fluorescence efficiency. Molecular design of PI emitters and comprehensive studies of their photophysical properties and chemical structures are of great significance for developing high performance deep-blue emitters. We designed, synthesized several serials bisphenanthroimidazole derivatives and investigated their applications in nondoped deep blue light-emitting devices. Their devices efficiencies are the best or among the best comparing to those of the reported nondoped OLEDs with the corresponding color gamuts. Reference 1. Wen-Cheng Chen, Qing-Xiao Tong,* Chun-Sing Lee,* Sci. Adv. Mater., 2015, 7, 2193-2205. 2. Wen-Cheng Chen, Chun-Sing Lee*, Qing-Xiao Tong,* J. Mater. Chem. C, 2015, 3, 10957-10963. 3. Miao Chen, Qing-Xiao Tong,* Chun-Sing Lee*, et. al, Adv. Opt. Mater., 2015, 3, 1215-1219. 4. Ze-Lin Zhu, Qing-Xiao Tong,* Chun-Sing Lee*, et. al, J. Mater. Chem. C, 2016, 4, 6249-6255. 5. Wen-Cheng Chen, Qing-Xiao Tong,* Chun-Sing Lee*, et. al, Adv. Opt. Mater., 2014, 2, 626-631. * Qing-Xiao Tong 84 6.1.3 Highly efficient blue-green-emitting diodes with cationic iridium(III) complexes Dongxin Ma, Yong Qiu, Lian Duan* Email: [email protected]; Key Lab of Organic Optoelectronics and Molecular Engineering of Ministry of Education, Department of Chemistry, Tsinghua University, Beijing 100084, P. R. China Keywords: cationic iridium complexes, negative counter-ions, organic light-emitting diodes, solution process Cationic iridium(III) complexes with highly efficient luminescence of virtually all colors have emerged as phosphorescent emitters, which contain emissive coordinated iridium(III) cations and nonluminous negative counter-ions, for example, conventional small inorganic anions such as tetrafluoroborate ([BF4]-) and hexafluorophosphate ([PF6]-), or some bulky organic anions like tetraphenylborate derivatives. However, the charged nature and migration of these negative counter-ions always complicate the operation of devices, severely restricting the applications of cationic iridium(III) complexes in organic light-emitting diodes (OLEDs). Here we report a series of cationic iridium(III) complexes 1-4 with the same blue-green-emitting coordinated iridium(III) cation [Ir(ppy)2(pzpy)]+ (ppy is 2-phenylpyridine, pzpy is 2-(1H-pyrazol-1-yl) pyridine in Figure 1a) but four different-sized negative counter-ions [BF4]-, [PF6]-, tetrakis(pentafluorophenyl)borate ([B(5fph)4]-) and tetrakis[3,5-bis(trifluoromethyl)phenyl]borate ([BArF24]-), respectively. Their photophysical properties, electrochemical behaviors and thermal stability have been fully investigated, and the single-layer OLEDs are fabricated by solution process. By optimizing the doping concentrations of these cationic iridium(III) complexes thus controlling their anionic migration, we succeed in the preparation of efficient blue-green OLEDs, achieving the highest current efficiency of 17.1 cd A-1, an external quantum efficiency of 6.8 %, a maximum luminance of 14.2×103 cd m-2 and color coordinates of (0.21, 0.48) (see Figure 1b-c). To our knowledge, these values are among the best reported OLEDs based on ionic transition metal complexes as phosphorescent emitters in the blue-green region, indicating high promise of cationic iridium(III) complexes in flat panel displays and solid state lightings. Figure 1. (a) Chemical structures and the energy-level diagram of materials used in solution-processed OLEDs. (b-c) Current density and luminance versus voltage characteristics of single-layer devices based on different doping concentrations of complex 1. References: 1. Dongxin Ma, Taiju Tsuboi, Yong Qiu, Lian Duan. Adv. Mater. doi:10.1002/adma.201603253. 2. Dongxin Ma, Chen Zhang, Yong Qiu, Lian Duan. J. Mater. Chem. C, 2016, 4, 5731. 85 6.2.1 Conjugated Polymers as promising electrode materials for Li-ion Batteries Qichun Zhang1,2 1 School of Materials Science and Engineering, Nanyang Technological University, Singapore 639672 2 Division of Chemistry and Biochemistry, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore 637371 Email: [email protected] Key Words: Large azaacenes, synthesis, Characterization, fabrication, Li-ion batteries Electrode materials play a critical role in approaching high energy density and long cycle life lithium-ion batteries (LIBs). The increasing concern about the traditional inorganic electrode materials on resources and environmental issues has strongly inspired scientists to switch on searching green energy electrodes. Organic compounds are potentially sustainable and renewable materials as many of them can be obtained from natural products and biomass. Additionally, the properties of organic compounds can be tuned through the modification of the structures as well as the introduction of functional groups. In this talk, I will present our recent progress on the preparation of novel conjugated polymers and their application in Li-ion batteries. [1] J. Xie and Q. Zhang*, J. Mater. Chem. A. 2016, DOI: 10.1039/C6TA01069E. [2] P.-Y. Gu, Y. Zhao, J. Xie, N. Binte Ali, L. Nie, Z. J. Xu,* Q. Zhang* ACS Appl. Mater. Interfaces, 2016, 8:74647470. [3] J. Wu, X. Rui, C. Wang, W.-B. Pei, R. Lau, Q. Yan*, Q. Zhang* Adv. Energy Mater., 2015, 5:1402189 [4] J. Wu, X. Rui, G. Long, W. Chen, Q. Yan*, Q. Zhang*, Angew. Chem Int. Ed. 2015, 54: 7354-7358 86 6.2.2 Sub-2nm Thick Fluoroalkylsilane Self-Assembled Monolayer-Coated High Voltage Spinel Crystals as Promising Cathode Materials for Lithium Ion Batteries Nobuyuki Zettsua, b and Katsuya Teshima*a, b a Center for Energy and Environmental Science Shinshu University, 4-17-1 Wakasato, Nagano 3808553, Japan b Department of Materials Chemistry, Shinshu University, 4-17-1 Wakasato, Nagano 380-8553, Japan * corresponding author, e-mail: [email protected] High-voltage spinel (LiNi0.5Mn1.5O4) is considered one of the most promising cathode materials for use in Li-ion batteries for hybrid electric vehicles (HEVs) and plug-in hybrid electric vehicles (PHEVs) due to its high voltage plateau, at around 4.7 V. This results in its energy density (650 Wh·kg-1) being over 20% higher than those of conventional LiCoO2-, LiMn2O4-, and LiFePO4-based materials. However, the working potential of LiNi0.5Mn1.5O4 approaches the thermodynamic stability limit of carbonate-based electrolytes; hence, a systematic research approach is needed to enhance the compatibility of LiNi0.5Mn1.5O4 with electrolytes to improve the cycle life and safety characteristics. The main contribution of our paper is an examination of the benefits of the use of a sub-2nm thick fluoroalkyl-based self-assembled monolayer as a cathode-protecting layer in 5 V-class lithium ion batteries. As shown in Figure, it was revealed that a bare LiNi0.5Mn1.5O4- cathode had substantial capacity fade that dropped to 79% of the original capacity after 100 cycles at a rate of 1 C, which was entirely due to dissolution of Mn3+ from the spinel lattice via oxidative decomposition of the organic electrolyte. The capacity retention was maximally improved to 97% by coating of an ultrathin FAS-SAM on the LiNi0.5Mn1.5O4- cathode surface. Such surface protection with highly ordered fluoroalkyl chains insulated the direct contact with an organic electrolyte and led to increased tolerance to HF. Vapor-phase processing of FAS-SAM at atmospheric pressure allowed a dense and homogenous coating of the protecting layer on the LiNi0.5Mn1.5O4 cathode surface compared to conventional powder or thin film coating under vacuum. It should be noted that the thickness fraction of the FAS-SAM was less than 0.1% (1.34 nm) compared to the mean diameter of the LiNi0.5Mn1.5O4- crystal (1.01 m); therefore the FAS-SAM coating did not lose C rate capability due to increased charge transfer resistance. We believe that this contribution is theoretically and Figure. practically relevant because of the Cyclability of the FAS-SAM-coated LiNi0.5Mn1.5O4substantial improvements that such a cathode-based half-cells fabricated with different SAM simple modification makes to the device coating times, collected at a rate of 1 C between 3.5 and properties, including reduction in 4.8 V. capacity fade and enhancement of C rate capability.[1] [1] N. Zettsu et al., Sci. Rep., 6, 31999 (2016) 87 6.2.3 Charge-driven Synthesis of Straw-sheaf-like Cobalt Oxides with Excellent Cyclability and Rate Capability for Advanced Lithium-ion Batteries Xiao-Ying Lu 1*#, Bin Wang 2, Wai Kuen Au1 and Hongfan Guo3 Faculty of Science and Technology, Technological and Higher Education Institute of Hong Kong, Hong Kong, P.R. China. Email: [email protected] Fax: +852-21761554; Tel: +852-21761453. 2 Hong Kong Applied Science and Technology Research Institute, Hong Kong, P.R. China. 3 College of Chemical Engineering, Shenyang University of Chemical Technology, Shenyang, P.R. China. 1 Keywords: Cobalt oxide, Anode, Lithium-ion batteries, Charge-driven self-assembly and Cycling stability Transition metal oxides have been considered as promising high-capacity electrode materials for lithiumion batteries [1-2]. The architectures of electrode materials have significant effects on electrochemical performances in charge-discharge cycles for reversible lithium storage [3-4]. In this study, hierarchical strawsheaf-like cobalt oxides composed of numerous strongly tied nanoneedles has been successfully synthesized by a novel charge-driven self-assembly strategy with subsequent heat treatment. Zeta-potential measurement suggests that the positively charge polymers play important roles in the preferential crystal growth of cobaltbased materials for cobalt oxide anode materials. Impressively, owing to the unique physical characteristics, high specific capacity, superior cyclability and excellent rate capability of straw-sheaf-like cobalt oxides are demonstrated for electrochemical lithium storage by repeated charge-discharge cycles at high current densities. Electrochemical results indicate that reversible capacities as high as 842.9 and 723.4 mAh g-1 over 300 cycles are achieved with good cycling stability at current densities of 500 and 2000 mA g-1, respectively. In addition, a reversible capacity of 707 mAh g-1 can be still achieved even when evaluated at a high current density of 3000 mA g-1. Overall, the proposed synthesis strategy will be crucial to develop high-performance energy storage materials with novel hierarchical architectures for next generation lithium-ion batteries. # Presenting Author Corresponding Author * References 1. P. Poizot, S. Laruelle, S. Grugeon, L. Dupont and J. M. Tarascon, Nature, 2000, 407, 496-499 2. X. W. Lou, D. Deng, J. Y. Lee, J. Feng and L. A. Archer, Adv. Mater., 2008, 20, 258-262. 3. B. Wang, Y. Tang, X.-Y. Lu, S. L. Fung, K. Y. Wong, W. K. Au and P. Wu, Phys. Chem. Chem. Phys., 2016, 18, 4911-4923. 4. B. Wang, X.-Y. Lu and Y. Tang, J. Mater. Chem. A, 2015, 3, 9689-9699. 88 6.3.1 Epitaxial CaTi5O11 and TiO2-B Thin Films for High Rate Lithium-Ion Batteries Xiaoqing Pan Department of Chemical Engineering and Materials Science, Department of Physics and Astronomy, University of California - Irvine, Irvine, California 92697, USA. The bronze polymorph of titanium dioxide (TiO2-B) is interesting for many applications including high rate energy storage, solar cells, photocatalysis, thermoelectrics and sensing, owing to its uniquely layered structure and highly asymmetric unit cell. Although known to have advantages over anatase or rutile, high quality bronze phase TiO2-B specimens that demonstrate good electrochemical properties thus far have exclusively been nano-structured powders prepared by hydrothermal methods. We have recently discovered that Ca can stabilize the bronze structure, forming a variant phase CaTi5O11, which has then been successfully synthesized in epitaxial singlecrystalline thin films by pulsed laser deposition (PLD), a completely waterless process. Due to the near-perfect lattice match, the CaTi5O11 film can be used as a template layer to grow high quality, water-free TiO2-B films on top, which facilitates the synthesis and application of both materials on a wide variety of substrates, including SrTiO3, Nb:SrTiO3, LaAlO3, LSAT and SrTiO3 buffered Si. Lithium ion transport in the bronze structure is highly anisotropic. By utilizing substrates with a different orientation to align the more open channels with out-of-plane directions, extremely high rates of lithium ion transport, up to 600C (1C=335 mA g-1), with extraordinary structural stability has been achieved. In a battery half-cell using metallic lithium as counter electrode, the orientation-engineered CaTi5O11 film discharged to 155 mA h g-1 at a rate of 60C, corresponding to a time of 60 s to fully discharge the capacity, at the 100th cycle, delivering specific power of ~20 kW kg-1. Post-mortem examinations by x-ray diffraction (XRD) and transmission electron microscopy (TEM) confirmed that both the TiO2-B and CaTi5O11 structures were essentially unchanged after aggressively cycling for more than 60 days. The film microstructure and interfacial atomic structure were characterized by atomic resolution transmission electron microscopy. In addition, we have employed novel in situ TEM to study the Li-intercalation of the films. Revealed by TEM of electrochemical lithiation in TiO2-B, many defects were induced by strain relaxation upon Liinduced TiO2-B lattice expansion. Depending on Li intercalation direction in the crystal structure, either high-symmetry structural transformation or plain shears was generated. These results provide the basic knowledge needed to realize and utilize TiO2-B single crystals, while also supporting theoretical studies with determinate experimental data. 89 6.3.2 Enhancing the anode performance of antimony through nitrogen-doped carbon and carbon nanotubes Xia Liu, Zhihui Dai* Jiangsu Collaborative Innovation Centre of Biomedical Functional Materials and Jiangsu key Laboratory of Biofunctional Materials, School of Chemistry and Materials Science, Nanjing Normal University, Nanjing, 210023, P. R. China. Keywords: sodium-ion batteries; anode performance; antimony; nitrogen-doped carbon; nitrogen-doped carbon nanotubes * Corresponding Author: E-mail: [email protected], Fax: +86-25-85891051; Tel: +86-25-85891051 Antimony is a promising high-capacity anode material in sodium-ion batteries, but it generally shows poor cycling stability because of its large volume changes during sodium ion insertion and extraction processes. To alleviate or even overcome this problem, we develop a hybrid carbon encapsulation strategy to improve the anode performance of antimony through the combination of antimony/nitrogen-doped carbon (Sb/N-carbon) hybrid nanostructures and the carbon nanotube (CNT) network. When evaluated as an anode material for sodium-ion batteries, the as-synthesized Sb/N-carbon + CNT composite exhibits superior cycling stability and rate performance in comparison with Sb/N-carbon or Sb/CNT composite. A high charge capacity of 543 mA h g− 1 with initial charge capacity retention of 87.7% is achieved after 200 cycles at a current density of 0.1 A g − 1 . Even under 10 A g− 1, a reversible capacity of 258 mA h g− 1 can be retained. The excellent sodium storage properties can be attributed to the formation of Sb− N bonding between the antimony nanoparticle and the nitrogen-doped carbon shell in addition to the electronically conductive and flexible CNT network. The hybrid carbon encapsulation strategy is simple yet very effective, and it also provides new avenues for designing advanced anode materials for sodium-ion batteries. Scheme 1 Schematic illustration of the synthesis procedure for the Sb/N-carbon + CNT composite. Reference 1. Palomares, V.; Serras, P.; Villaluenga, I.; Hueso, K. B.; Carretero-Gonzá lez, J.; Rojo, T. Na-Ion Batteries. Energy Environ. Sci. 2012, 5, 5884− 5901. 2. Pan, H.; Hu, Y.-S.; Chen, L. Energy Environ. Sci. 2013, 6, 2338− 2360. 3. Kim, S. W.; Seo, D. H.; Ma, X.; Ceder, G.; Kang, K. Adv. Energy Mater. 2012, 2, 710− 721. 90 6.3.3 Composition and Interface Engineering of MoS2xSe2-2x Nanosheets for Superior Electrochemical Performance Jun Xu* School of Electronic Science & Applied Physics, Hefei University of Technology, Hefei 230009, P. R. China Keywords: MoX2, composition tuning, interlayer expansion, hydrogen evolution reaction, sodium storage performance Transition-metal dichalcogenides (MX2) with 2D covalently-bonded monolayers has wide potential applications in electrochemical energy storage and conversion owing to the 2D morphology, ultra-thin thickness, distinctive phase-engineering nature and composition-dependent properties. 1T-2H phase engineering, interlayer expansion, and chalcogen composition tuning of layered MoX2 nanosheets are key factors in optimizing their physical properties and electrochemical performance. In this talk, we report controllable synthesis of MoS2xSe2-2x nanosheets with expanded (002) interlayer spacing, tunable S/Se ratios and convertible 1T-2H phases. Influences of phase engineering, interlayer expansion and stoichiometry variation on hydrogen evolution reaction (HER) performance and sodium storage performance are investigated. (1) Assembled 1T-MoSe2 nanosheets possessing expanded (002) interlayer spacings as large as 1.17 nm with an 81% expansion is reported for the first time. The 1T-MoSe2 nanosheets exhibit striking kinetic metrics for HER performance with a low onset potential of 58 mV and a small Tafel slope of 78 mV dec−1.[1] (2) Hierarchical MoS2:C nanotubes assembled from 2D superstructure sheets consisting of alternative monolayers of MoS2 and carbon are prepared and demonstrated as a robust anode material for sodium ion batteries (SIBs) exhibiting superior rate and cycling performance. The MoS2:C superstructure nanotubes benefit for improving the electrical conductivity of MoS2 and providing expanded (002) interlayer spacing of 0.986 nm that facilitates fast Na+ insertion/extraction reaction kinetics.[2,3] (3) MoS2xSe2-2x nanotubes featuring controllable chalcogen compositions (0.06 x 1) and tunable (002) interlayer spacings are synthesized for optimized HER activities. The improved electrocatalytic performance of MoS2xSe2-2x (x=0.54) nanotubes is attributed to the chalcogen composition tuning and the interlayer distance expansion to achieve a benefitting hydrogen adsorption energy.[4] References [1] M. Jiang, J. Zhang, M. Wu, W. Jian, H. Xue, T.-W. Ng, C.-S. Lee, J. Xu, J. Mater. Chem. A 2016, 4, 14949–14953. [2] Z.-T. Shi, W. Kang, J. Xu, Y.-W. Sun, M. Jiang, T.-W. Ng, H.-T. Xue, D. Y.W. Yu, W. Zhang, C.-S. Lee, Nano Energy 2016, 22, 27−37. [3] Z.-T. Shi, W. Kang, J. Xu, L.-L. Sun, C. Wu, L. Wang, Y.-Q. Yu, D. Y. W. Yu, W. Zhang, C.-S. Lee, Small 2015, 11, 5667−5674. [4] J. Zhang, M.-H. Wu, Z.-T. Shi, M. Jiang, W.-J. Jian, Z. Xiao, J. Li, C.-S. Lee, J. Xu, Small 2016, 12, 4379−4385. 91 7.1.1 Non-fullerene acceptor-based polymer solar cells with high open-circuit voltage Hongzheng Chen Department of Polymer Science & Engineering, Zhejiang University, Hangzhou 310027, P. R. China Keywords: Non-fullerene, electron acceptor, polymer solar cells, open-circuit voltage. Though fullerene derivatives are being widely used as electron acceptors in polymer solar cells, their obvious drawbacks of limited chemical and energetic tunability, poor light-absorption, high-cost purification, and morphology instability have become the bottlenecks to further advancement of polymer solar cells. Therefore, the exploration of non-fullerene electron acceptors is motivated in recent years. With employing the efficient and expensive donors, many of the reported works focused solely on improving the performance of non-fullerene based polymer solar cells. The development of low-cost and practical non-fullerene bulk heterojunction (BHJ), especially those with low cost poly(3-hexylthiophene) (P3HT), gives generally the power conversion efficiencies (PCEs) less than 5%. In this presentation, I will propose a new design strategy to access novel non-fullerene acceptor with diketopyrrolopyrrole (DPP) chromophore that simultaneously addresses all of the above mentioned drawbacks in fullerene materials. The P3HT based solar cells using this new acceptor not only exhibit the PCE of 5.16% with an extremely high open-circuit voltage of 1.14 V, one of the highest values among the reported works using P3HT based fullerene-free BHJ, but also show superior thermal stabilities. Small molecule non-fullerene based tandem polymer solar cells are also demonstrated for the first time. A PCE of 8.48% is achieved with an ultra-high Voc of 1.97 V, which is the highest voltage value reported to date among the efficient tandem polymer solar cells. References 1. S. Li, W. Liu, M. Shi, J. Mai, T.-K. Lau, J. Wan, X. Lu, C.-Z. Li, and H. Chen, Energy & Environmental Science, 9(2016), 604. 2. S. Li, J. Yan, C.-Z. Li, F. Liu, M. Shi, H. Chen and T. P. Russell, J. Mater. Chem. A, 4(2016), 3777. 3. L. Zuo, C.-Y. Chang, C.-C. Chueh, S. Zhang, H. Li, A. K.-Y. Jen, and H. Chen, Energy & Environmental Science, 8(2015), 1712 4. W. Liu, S. Li, J. Huang, S. Yang, J. Chen, L. Zuo, M. Shi, X. Zhan, C.-Z Li, H. Chen, Adv. Mater., 2016 92 7.1.2 Ternary blends for large area flexible organic solar cells Yajie Zhang, Jianqi Zhang, Kun Lu, Zhixiang Wei# ,* National center for nanoscience and technology, Chinese Academy of Sciences, Beijing 100190, China Keywords: Organic solar cells, Ternary, Large area, Printing Significant progress has been achieved recently in the production of bulk heterojunction organic solar cells (OSCs) based on binary active layer composed of donor–acceptor (D-A)-type polymers or small molecules as donors and fullerene derivatives (e.g. PCBM) as acceptor.[1, 2] Compared with binary OSCs, ternary systems containing two donors and one acceptor (or one donor and two acceptors) can broaden the absorption range of active layers through complementary absorption of two donors, thereby providing a potentially effective route in achieving high Jsc and thus high efficiency. In this presentation, a ternary OSC is designed and fabricated, which contains a D–A-type polymer and a high-crystaline small molecule as donors and fullerene derivatives as acceptor. The small molecules increase the crystallinity of the donor phase, whereas the ratios of small molecules to polymers can tune the domain size of the ternary system. The PCE of the ternary OSCs is higher than that of binary systems based on small molecules or polymers [3]. By a further optimization of the ternary system, a PCE of 11% was obtained, which is among the highest values for OSCs.[4,5] A large area device with efficiency higher than 7% is demonstrated recently, which will lead to a potential application of the organic solar cells. [1] Y.J. Zhang, D. Deng, K. Lu, J.Q. Zhang, B.Z. Xia, Y.F. Zhao, J. Fang, Z.X. Wei, Adv. Mater. 2015, 27, 1071. [2] D. Deng, Y. J. Zhang, L. Yuan, C. He, K. Lu, Z. X. Wei, Adv. Energy Mater. 2014, 4, 1400538. [3] Y. J. Zhang, D. Deng, K. Lu, J.Q. Zhang, B.Z. Xia, Y. F. Zhao, J. Fang, Z. X. Wei, Adv. Mater. 2015, 27, 1071. [4] J. Q. Zhang, Y. J. Zhang, J. Fang, K. Lu, Z. Y. Wang, W. Ma, and Z. X. Wei, J. Am. Chem. Soc., 2015, 137, 8176. [5] D. Deng, Y. J. Zhang, J. Q. Zhang, Z. Y. Wang, L. Y. Zhu, J. Fang, B. Z. Xia, Z. Wang, K. Lu, W. Ma, Z. X. Wei, Nat. Cummun, 2016, 7, 13740 # Presenting Author Corresponding Author * 93 7.1.3 Photoconductive Cathode Interlayers for High Performance Organic Solar Cells Zengqi Xie* Institute of Polymer Optoelectronic Materials and Devices, State Key Laboratory of Luminescent Materials and Devices, South China University of Technology, Guangzhou 510640, P. R. China. E-mail: [email protected] Keywords: Photoconductivity, interlayer, perylene bisimide, zinc oxide, organic solar cells. Perylene bisimides (PBIs) were applied to modify ITO electrode and the work function of the electrode was decreased obviously, and thus it is suitable to be used as the cathode interlayer in the inverted polymer solar cells. A cross-linked thin film of PBI monomers was created on ITO electrode, which is insoluble in common organic solvents facilitating the solution procession of the bulk heterojunction active layer. The modified ITO was used as cathode in inverted polymer solar cells (i-PSCs) and enhanced device performance was obtained.1 Then, self-assembled PBI fibers was applied to modify the surface of ITO and Zinc oxide (ZnO) as cathode interlayers affording power conversion efficiency (PCE) as high as 9.17% and 9.43% respectively (PTB7:PC71BM as the active layers).2,3 Further, cathode interlayer based on cross-linked thin film on AZO afford a PCE of 10.35% (PTB7-Th:PC71BM as the active layer).4 Based on the interaction between PBI and ZnO, a highly photoconductive cathode interlayer was developed by doping 1wt% light absorber, i.e. PBI-H, into ZnO thin film, which absorbs a very small amount of light but shows highly increased conductivity of 2.0×10-3 S/m under sunlight. The photovoltaic devices based on this kind of photoactive cathode interlayer exhibit significantly improved device performance, which is rather insensitive to the thickness of the cathode interlayer over a broad range. A PCE as high as 10.5% was obtained by incorporation of the photoconductive cathode interlayer with the PTB7-Th: PC71BM active layer.5 Due to the advantage of highly electron extraction efficiency, the photoconductive cathode interlayer was successfully applied in ternary photovoltaic devices and a PCE over 11% was achieved in our lab (certified PCE 10.38%).6 The working mechanism of photoconductive cathode interlayer was deeply discussed in an aqueous processed system, including increased electron mobility and reduced work function under light irradiation. With these benefits, a PCE over 10% was achieved even the thickness of the interlayer was up to 100 nm and the thickness of the active layer was up to 300 nm.7,8 Finally, in a cross-linked film of PBI with electron withdrawing units, the stable PBI radical anions (PBI•-) were achieved by electrochemical reduction reaction. The device based on the anion state interlayer showed dramatically enhanced performance compared with the device based on the neutral state PBI interlayer. The results help us to understand the physics of PBI as the cathode interlayer in device.9 References (1) Feng, T.; Xiao, B.; Lv, Y.; Xie, Z. Q.; Wu, H. B.; Ma, Y. G. Chem. Commun. 2013, 49, 6283-6285. (2) Xie, Z. Q.; Xiao, B.; He, Z. C.; Zhang, W. Q.; Wu, X. Y.; Wu, H. B.; Würthner, F.; Wang, C.; Xie, F. Y.; Liu, L. L.; Ma, Y. G.; Wong, W.-Y.; Cao, Y. Mater. Horz. 2015, 2, 514-518. (3) Nian, L.; Zhang, W.Q.; Wu, S.P.; Qin, L.Q.; Liu, L.L.; Xie, Z.Q.; Wu, H.B.; Ma, Y.G. ACS Appl. Mater. Interfaces, 2015, 7, 25821-25827. (4) Wang, R.; Nian, L.; Yao, L.; Xie, Z. Q.; Liu, L. L.; Ma, Y.G. ACS Appl. Mater. Interfaces 2016, 8, 26463−26469. (5) Nian, L.; Zhang, W.Q.; Zhu, N.; Liu, L.L.; Xie, Z.Q.; Wu, H.B.; Würthner, F.; Ma, Y.G. J. Am. Chem. Soc., 2015, 137, 6995-6998. (6) Nian, L.; Gao, K.; Liu, F.; Kan, Y.; Jiang, X.; Liu, L. L.; Xie, Z. Q.; Peng, X. B.; Russell, T. P.; Ma, Y. G. Adv. Mater. 2016, 28, 8184–8190. (7) Nian, L.; Chen, Z.; Herbst, S.; Li, Q.; Yu, C.; Jiang, X.; Dong, H. L.; Li, F. H.; Liu, L. L.; Würthner, F.; Chen, J. W.; Xie, Z. Q.; Ma, Y. G. Adv. Mater. 2016, 28, 7521-7526. (8) Zhao, H. T.; Luo, Y.Q.; Xie, Z. Q.; Liu, L. L.; Ma, Y.G. Mater. Chem. Front. 2016, Submitted. (9) Ma, W. T.; Nian, L.; Luo, Y. Q.; Liu, L. L.; Xie, Z. Q.; Ma, Y. G. Unpublished results. 94 7.2.1 Functional Optical Nanostructures: Assembly, Properties and Applications Le He1*#, Xiaohong Zhang1 Institute of Functional Nano and Soft Materials, Soochow University, 199 Ren'ai Road, Suzhou Industrial Park, Suzhou, 215123, China 1 Keywords: Silicon, Nanocrystals, CO2 Reduction, Solar Energy, Heterogeneous Global warming and energy security are two major challenges currently facing human society. Thus there is a great need to develop technology capable of harnessing and securing environmentally sustainable energy supplies to replace fossil fuels and reduce CO2 emissions. Current clean, renewable, energy-generating methods that produce electricity from the sun and wind suffer from the problem of intermittency as well as the difficulty of storing electricity, as it has to be used essentially as it is produced. Hence there exists an urgent need to find a way of producing energy-rich fuels that can be transported and stored for use on demand. In this context, the purpose of our research is aimed at harnessing solar energy to make an energy rich portable fuel. This process means both fuel generation using (free) sunlight and carbon dioxide capture (to reduce global climate levels). To this end, we attempt to develop general strategies that allows for rational engineering of nanostructured solar fuel materials with desired structural, optical and electronic properties in order to greatly improve the conversion rate and efficiency in photoreduction of CO2. # Presenting Author Corresponding Author * 95 7.2.2 Interesting flowing of molten metal/alloy in a nanotube/nanowire Rujia Zou1, Qian Liu1, Zhenyu Zhang2, Junqing Hu1,#,* 1 State Key Laboratory for Modification of Chemical Fibers and Polymer Materials, College of Materials Science and Engineering, Donghua University, Shanghai 201620, China; 2Center of Super-Diamond and Advanced Films (COSDAF), Department of Physics and Materials Science, City University of Hong Kong Hong Kong, China Keywords: In-situ TEM; Metal molten; Migration; Devices, Dynamics In-situ transmission electron microscopy (TEM) has been demonstrated to be a very useful tool to discover new physical transformations associated with one-dimensional nanomaterials. So far, various kinds of physical phenomena occurring at the nanoscale, including melting, growth, and mass transport have been studied in real time using TEM, which provided new insights into the design, fabrication and engineering of nanodevices. Herein, we demonstrate interesting flowing of molten metal/alloy in a nanotube/nanowire, which include as follows: (i) Stability of CNT-based device. The molten electrode (e.g., Au, Ag, and Pt) due to Joule heating was flowing into the CNT channel by a resultant of the thermomigration and electromigration forces. The electrical performances of such a device are strongly affected by this process, often causing electrical shortening and even breakdown of pre-established devices. Dynamics analysis about the effects of the electromigration and thermomigration on the mass transportation of the liquid metal filling inside the CNT was carried out, and the destroying of the CNT devices may be avoided by selecting a CNT with a right length and controlling a bias. This study suggests that the electrode melting and its flow through the CNT channel may be one of the main reasons accounting for the unstable performance and the electrical breakdown and even catastrophic failure of the established CNT-based devices. (ii) Fabrication and engineering of the heterostructured devices. The migration of a molten Au/Ge alloy within a solid Ge nanowire has been in situ observed based on a two-terminal connected nanowire device. A theoretical model was proposed and the relevant dynamic mechanisms were discussed. It was found that the migration direction and stopping position of the Au/Ge alloy liquid both showed a bias dependence. This work supplied an important reference for the smart fabrication and engineering of the heterostructured devices. (iii) A nanoscale electrically/thermally driven switch. The melting point of Sn nanowire inside the Ga2O3 tube is found to be as low as 58 °C-far below the value of bulk Sn (231.89 °C), and its crystal phase (β-Sn) remains unchanged even at temperatures as low as -170 °C. The resistance demonstrates a sudden drop (rise) when two Sn nanowires contact (separate), due to the thermally driven motion of the liquid Sn fillings inside the tube. Thus this structure can be switched between its on and off states by controlling the motion, merging or splitting, of the Sn nanowire inside the tube, either electrically, by applying a current, or thermally, at a predetermined temperature. # Presenting Author: Junqing Hu, E-mail: [email protected] Corresponding Author: Junqing Hu, E-mail: [email protected] * 96 7.2.3 High-performance Wearable Supercapacitor Textiles Zijian Zheng*# Institute of Textiles and Clothing, The Hong Kong Polytechnic University, Hong Kong SAR Keywords: supercapacitor, textiles, wearable electronics, energy storage, polymer-assisted metal deposition. Wearable supercapacitor textiles are supercapacitors that made use of and/or shaped into textile fibers, yarns, and fabrics, which are inevitable energy storage devices for wearable electronic applications. To date, the major challenge in the development of wearable supercapacitors is how to improve the electrochemical properties of the device while acquiring high flexibility and durability under wearing conditions. Recently, our laboratory has developed several supercapacitor yarns and fabrics, which show record-high electrochemical performances of their kinds as well as excellent flexibility. These textile-based devices can be readily integrated into different textile forms by means of weaving, embroidery, and heat pressing for wearable applications. References: [1] Q. Huang, D. Wang, Z. J. Zheng*, Adv. Energy Mater. 2016, DOI: 10.1002/aenm.201600783. [2] L. Liu, Y. Yu, C. Yan, K. Li, Z. J. Zheng*, Nat. Commun. 2015, 6, 7260. [3] Y. Yu, C. Yan, Z. J. Zheng*, Adv. Mater. 2014, 26, 5508-5516. # Presenting Author Corresponding Author * 97 8.1.1 Molecular Orientation-Dependent Photovoltaic Performance in Organic Solar Cells Kilwon Cho Dept. of Chemical Engineering, Pohang University of Science and Technology, Pohang 37673 Korea Keywords: organic solar cell, molecular orientation, interface, photon harvesting, exciton dissociation Photovoltaic performance of organic solar cells is highly dependent on the anisotropic nature of optoelectronic properties of photoactive materials. Here, we demonstrate an approach for highly efficient planar heterojunction solar cells by tuning the molecular orientation of the organic semiconducting materials. A monolayer graphene inserted at anode interface served as a template for quasi-epitaxial growth of pentacene crystals with lying-down orientation, which was favorable for overall optoelectronic properties including light absorption, exciton diffusion, charge transport, and interfacial energetics. The lying-down orientation persisted until ~100 nm in thickness, significantly enhancing the photon harvesting within the photoactive layer due to its increased absorption range and exciton diffusion length. The resultant photovoltaic performance showed a remarkable increase in Voc, Jsc, FF and consequently a 5 times increment in power conversion efficiency than the devices without graphene layers. The effect of molecular orientation at donoracceptor interface was further investigated by using a planar heterojunction structure with orientationcontrolled P3HT thin films. Photophysical analyses revealed that the charge pair dissociation at the face-on interface was more efficient, which resulted in smaller geminate recombination loss and more efficient photocurrent generation. These results imply that the molecular orientation in photoactive layers is a critical factor that should be elaborately controlled for high performance organic solar cells. 98 8.1.2 Non-radiative recombination in organic solar cells Feng Gao IFM, Linköping University, Sweden Email: [email protected] Keywords: Organic solar cells, open-circuit voltage, recombination Compared with inorganic or perovskite photovoltaics, the key limiting factor for organic solar cells (OSCs) is large voltage loss, which is usually over 0.7 V. A significant contribution of the large voltage loss in OSCs is due to strong non-radiative recombination, which causes voltage loss of more than 0.35 V in most cases. The origin of the strong non-radiative recombination in OSCs has been puzzling the community for almost one decade, limiting rational design of materials to overcome this critical issue. In this study, we systematically investigate several exceptional OSC systems (including fullerene and nonfullerene electron acceptors), where the voltage loss is reduced to <= 0.7 V. We find that the quantum efficiency of electroluminescence in these systems have been significantly increased. Our work would pave the way to rational design of novel OSC materials for small voltage loss and high efficiency. 99 8.1.3 Metal Nanoparticle-assisted Crystallization of Perovskite Active Layer for High Performance Solar Cells Ali Asgher Syed#, Li Ning, Zhu Furong Department of Physics, Hong Kong Baptist University, Hong Kong Keywords: Solvent engineering; hole and electron extraction; charge collection efficiency. Both conventional and inverted perovskite solar cells (PSCs) have achieved high power conversion efficiencies. In order to gain a deeper understanding for growing better active layer in the solar cells, the crystallization process of perovskite needs to be examined in more depth. Growth of perovskite layer onto metal nanoparticles is a new approach which we have adopted for perovskite crystallization, layer growth, and the enhancement of charge collection and an overall power conversion efficiency (PCE) of the cells. By using solvent engineering approach for preparing all solution processable planar inverted PSCs, based on CH3NH3PbI3, our results reveal that adding a thin layer of silver nanoparticles to the cells leads to better perovskite crystallinity and hence the improvement in photocurrent density, open circuit voltage, favorable charge collection efficiency and thereby an improved PCE of ~14%. Whole fabrication was done at a low temperature of ≤120°C, making it more acceptable for large scale production at low cost. 100 8.1.4 Two-Dimension-Conjugated Polymer Donor Materials for Polymer Solar Cells Yongfang Li Institute of Chemistry, Chinese Academy of Sciences, China e-mail: [email protected] Abstract: Polymer solar cells (PSCs) have attracted great attention recently, because of the advantages of simple device structure, light weight and capability to be fabricated into flexible and semitransparent devices. The key photovoltaic materials of PSCs are conjugated polymer donors and the fullerene or non-fullerene acceptors. For broadening absorption and enhancing hole mobility of the polymer donor, we developed two-dimension (2D)-conjugated polymers with conjugated side chains, including 2D-conjugated polythiophene derivatives1 and D-A copolymers with narrow or medium bandgaps2. Recently, by side chain engineering of the medium bandgap 2D-conjugated D-A copolymers, the power conversion efficiency (PCE) of the PSCs with the 2D-conjugated polymer as donor and low bandgap A-D-A structured organic semiconductor ITIC as acceptor reached 9~11%35 . By further modification of the side chain isomerization of ITIC, the PCE of the non-fullerene PSCs was further improved to 11.77%6. The results indicate that the 2D-conjugated polymers are excellent donor materials for the PSCs with fullerene or non-fullerene acceptors. References: 1. J. H. Hou, Z. A. Tan, Y. Yan, Y. J. He, C. H. Yang, Y. F. Li, J. Am. Chem. Soc., 2006, 128, 4911-4916.. 2. Y. F. Li, Acc. Chem. Res. 2012, 45, 723–733. 3. H. J. Bin, Z.-G. Zhang, L. Gao, S. Chen, L. Zhong, L. Xue, C. Yang, Y. F. Li, J. Am. Chem. Soc., 2016, 138, 4657–4664. 4. L. Gao, Z.-G. Zhang, H. J. Bin, L. Xue, Y. Yang, C. Wang, F. Liu, T. P. Russell, Y. F. Li, Adv. Mater., 2016, 28, 8288–8295.. 5. Bin, H. J.; Gao, L.; Zhang, Z.-G.; Yang, Y.; Zhang, Y.; Zhang, C.; Chen, S.; Xue, L.; Yang, C.; Xiao, M.; Li, Y. F. Nature Commun, 2016, accepted. 6. Y. K. Yang, Z.-G. Zhang, S. Chen, H. J. Bin, L. Gao, L. Xue, C. Yang, Y. F. Li, J. Am. Chem. Soc., 2016, 138, 15011–15018. 101 8.2.1 High Efficiency Quantum Dot Sensitized Solar Cells Xinhua Zhong School of chemistry and molecular Engineering, East China University of Science and Technology, Shanghai 200237, China Email: [email protected] Keywords: Solar cells, Quantum dots, Sensitization A higher surface coverage of QD sensitizers on the oxide substrate is a “must” to improve the efficiencies of quantum dot sensitized solar cells (QDSCs). Due to the big size and lack of anchoring site on colloidal QD surface, the deposition of colloidal QD on TiO2 film electrode has being a bottleneck in the construction of high efficiency QDSCs. A capping ligand-induced selfassembly approach, wherein QDs capped with bifunctional linker ligands such as mercaptopropionic acid (MPA) are immobilized on TiO2 prompted by the affinity between carboxyl group and TiO2, has been developed to achieve fast, uniform, and dense deposition of colloidal QD on TiO2 electrode.1-3 Meanwhile, alloyed and type-II core/shell structured QD sensitizers with features of wide absorption range and high conduction band edge have been designed and prepared.4-7 Furthermore, the potential charge recombination inside QD, and at photoanode/electrolyte interfaces is substantially suppressed with the use of buffer layer and energetic barrier layers, consisting of a amTiO2/ZnS/SiO2 recipe onto QD sensitized TiO2 electrodes.[7,8] With the combination of high-quality QD sensitizers, effective deposition technique, and suppressed charge recombination, the power conversion efficiency (PCE) of QDSCs under simulated AM 1.5, full 1 sun illumination has been improved steadily from the level of 4-5% to a certified value of 11.6%.1-9 Figure 1. Zn-Cu-In-Se (ZCISe) based QDSCs and J-V curves under 1 full sun illumination. References: [1] Li W., Zhong, X., J. Phys. Chem. Lett. 2015, 6, 798. [2] Wang J. Mora-Sero I., Pan Z., Zhao K., Zhang H., Feng Y., Yang G., Zhong X., Bisquert J., J. Am. Chem. Soc. 2013, 135, 15913. [3] Pan Z., Mora-Sero I., Shen Q., Zhang H., Li Y., Zhao K., Wang J., Zhong X., Bisquert J. J. Am. Chem. Soc. 2014, 136, 9203. [4] Zhao K., Pan Z., Mora-Seró I., Cánovas E., Wang H., Song Y., Gong X., Wang J., Bonn M., Bisquert J., Zhong, X., J. Am. Chem. Soc. 2015, 137, 5602. [5] Du J., Du Z., Hu J.-S., Pan Z., Shen Q., Sun J., Long D., Dong H., Sun L., Zhong X., Wan L.-J., J. Am. Chem. Soc. 2016, 138, 4201 102 8.2.2 Engineering Light Absorption and Film Crystallization for High-Efficiency Perovskite Solar Cells Ming He and Zhiqun Lin#* School of Materials Science and Engineering, Georgia Institute of Technology, Atlanta, GA 30332, USA Keywords: perovskite solar cells, upconversion nanoparticles, meniscus-assisted solution printing Advances of metal halide perovskites in solar cells have been widely recognized. The power conversion efficiency (PCE) of perovskite solar cells has leaped from approximately 3 % to over 22 %. The photovoltaic performance of perovskite solar cells is highly correlated with chemical composition and film crystallization of perovskite photoactive layer. The chemical composition determines the spectral absorption range and the film crystallization influences the charge recombination. In this context, extending the spectral absorption of metal halide perovskite solar cells from visible into near-infrared (NIR) range renders the minimization of non-absorption loss of solar photons. Moreover, controlling the crystallization of perovskite films enables the reduction of the trap-assisted non-radiative charge recombination. Herein, we report two strategies for improving the photovoltaic performance of perovskite solar cells through engineering light absorption and film crystallization: (1) Monodisperse NaYF4:Yb/Er upconversion nanoparticles (UCNPs) were empolyed as the mesoporous electrode, enabling perovskite solar cells to operate under extended light absorption to NIR range (Figure 1a). Uniform NaYF4:Yb/Er UCNPs permanently tethered with hydrophilic polymer as surface ligands were rationally crafted by capitalizing on double hydrophilic star-like poly(acrylic acid)-blockpoly(ethylene oxide) (PAA-b-PEO) diblock copolymer as nanoreactor, in which the outer PEO blocks not only imparted the solubility of UCNPs but also rendered the tunability of film porosity during the manufacturing process. The incorporation of NaYF4:Yb/Er UCNPs as the mesoporous electrode led to a high efficiency of 17.8 %, which was further increased to 18.1 % upon the NIR irradiation. (2) Control over the crystallization of metal halide perovskite films is also crucial to pursuing high efficiency. We developed a robust strategy to manufacture large-grained FA0.85MA0.15PbI2.55Br0.45 perovskite film with good crystallization and preferred orientation by meniscus-assisted solution printing (MASP). Central to this strategy is the solvent evaporation-triggered outward convective flow that transported the perovskite solutes to the edge of the meniscus, promoting the formation of micrometer-scale perovskite grains with preferred crystal orientations (Figure 1b). The kinetics of grain growth was elucidated by in-situ optical microscopy tracking for further understanding the crystallization mechanism of perovskites during MASP, from which a two-stage, namely, quadratic followed by linear growth of perovskite crystallization was identified. The FA0.85MA0.15PbI2.55Br0.45 perovskite films prepared by the MASP exerted excellent optoelectronic properties such as long carrier lifetimes, low trap-state densities, and eventually high efficiencies approaching 20 % in planar solar cells. As such, these two strategies may open up avenues for the future development of perovskites for optoelectronic applications. Figure 1. (a) Scheme of the energy transfer process in CH3NH3PbI3 perovskite solar cells using NaYF4:Yb/Er upconversion mesoporous electrodes. (b) Schematic illustration of the meniscus-assisted solution printing (MASP) of large-grained perovskite film. # Presenting Author Corresponding Author * 103 8.2.3 Efficient Non-fullerene Organic Solar Cells with a Negligible Charge Separation Driving Force He Yan1, #* Department of Chemistry, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong Emails: [email protected] 1 Keywords: Organic Solar Cell, Temperature Dependent Aggregation, Non-fullerene, Low Voltage Loss, High Efficiency. Two major issues limiting the development of bulk heterojunction (BHJ) organic solar cells (OSCs) are the complicated morphology formed by the electron donor and electron acceptor and the high voltage loss. In this talk, I will present the effort of our group toward solving these key issues. Our methodology for targeting the first issue is through designing and synthesizing conjugated polymers with strong temperature dependent aggregation in solution. The success rate in terms of polymer synthesis and the power conversion efficiency of the resulting OSCs are dramatically improved through the use of this strategy, which enables us to achieve a record efficiency of 11.7%.1 In the meantime, our group has developed polymers and small molecular acceptors for efficient non-fullerene OSCs. More importantly, we find our high-performance non-fullerene device has an extremely low voltage loss,2 one of the smallest reported values for all OSCs. By carrying our detailed device physics studies, we demonstrate that our non-fullerene devices have fast charge separation and high electroluminescence quantum efficiency, despite a small driving force between the donor and acceptor molecules. Reference: 1. Zhao, J. et al. Efficient organic solar cells processed from hydrocarbon solvents. Nat. Energy 1, 15027 (2016). 2. Liu, J. et al. Fast charge separation in a non-fullerene organic solar cell with a small driving force. Nat. Energy 1, 16089 (2016). # Presenting Author Corresponding Author * 104 Abstract of Posters 105 P-01 Boosting the performances of Perovskite photodetectors by periodic nano-grating hole transporting layer Ning Li, Ali Asgher Syed and Furong Zhu* Department of Physics, Hong Kong Baptist University, Hong Kong Abstract: Perovskite materials has been intensively studied in the fields of solar cells, light emitting diodes as well as thin film transistors. They are also promising for applications in photodetectors due to high charge mobility, large absorption coefficient, and solution-based processes. In this work, we studied the effects of periodic nano-grating of PEDOT:PSS hole transporting layer (HTL) on the performances of perovskite photodetectors. The nano-grating structure of HTL was created by nano-imprinting method. As a result, grating induced internal light scattering effect favors the light absorption in the perovskite layer and improved contact area helps the charge extraction, resulting in improvements of the responsivity and response speed compared with planar structures. Our results also reveal that the perovskite photodiodes with periodic nano-grating HTL possess a less angular dependency on incident light angle. 106 P-02 Improved efficiency and stability of organic photovoltaic device using UV-ozone treated ZnO anode buffer Chiu-Yee Chan 1, Yu-Fang Wei 1, Hrisheekesh Thachoth Chandran 1, Chun-Sing Lee 1, 2 , Ming-Fai Lo 1, 2* and Tsz-Wai Ng 1, 2* 1 Center of Super-Diamond and Advanced Films (COSDAF), Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, P. R. China 2 City University of Hong Kong Shenzhen Research Institute, Shenzhen, People's Republic of China Keywords: ZnO buffer layer, organic photovoltaic devices, ultra-violet ozone, power conversion efficiency, stability Abstract We reported an efficient bulk-heterojunction solar cell of Boron subphthalocyanine chlorideFullerene with Ultra-violet (UV) ozone treated zinc oxide (ZnO) buffer layer at anode. By modifying the root mean square roughness of ZnO and UV ozone treated, the power conversion efficiency increases from 2.55% to 3.2 % under under AM1.5G illumination (100mWcm-2) as well as short circuit density and open circuit voltage. The improvement in absorbance increases the short-circuit density from 5.0 to 5.9 mA/cm2 and the high work function after UV ozone treatment which reduce the leakage current increases the Voc of solar cell from 0.9V to 1.06V. We also demonstrated that the device has a better stability since the reduction of work function under 1 day high vacuum storage. 107 P-03 Low-Temperature-Processed Flexible Organic-Inorganic Hybrid Heterojunction Rectified Diodes Ching-Hsiang Chang1#, Chao-Jui Hsu1, and Chung-Chih Wu1,2,3,a)* 1 Graduate Institute of Electronics Engineering, National Taiwan University, Taipei, Taiwan 2 Graduate Institute of Photonics and Optoelectronics, National Taiwan University, Taipei, Taiwan 3 Department of Electrical Engineering, National Taiwan University, Taipei, Taiwan a) [email protected] Keywords: flexible, Schottky barrier, heterojunction, PEDOT:PSS, n-InGaZnO In recent years, printed and flexible electronics have attracted much attention due to their various merits and unique features for emerging applications, such as radio frequency identification (RFID) tags and circuits for sensor networks and internet of things etc. For these emerging flexible electronic applications, high-performance diode rectifiers that can be readily fabricated on flexible plastic substrates at low temperatures are essential in their power transmission units. In this work, we report successful implementation of flexible PEDOT:PSS/n-InGaZnO organic-inorganic heterojunction diodes on plastics at low temperatures. High-conductivity p-type conducting polymer poly(3,4-ethylenedioxythiophene) polystyrene sulfonate (PEDOT:PSS) with a conductivity of ~1000 S/cm, a high work function (~5.1 eV), and high optical transparency was deposited by spin-coating as the bottom electrode. Then the semiconductive n-type aInGaZnO was deposited on top of PEDOT:PSS by sputtering at room temperature, followed by deposition of Mo top electrode. With the high work function of PEDOT:PSS and lower electron affinity of n-IGZO (~4.16 eV ), the Schottky barrier and Schottky diode characteristics were obtained with the PEDOT:PSS/n-IGZO hybrid heterojunction. The didoes on plastic substrates exhibited a low apparent turn-on voltage of 0.5, a high rectification ratio of up to 4.4 × 105 at ±1 V, a high forward current of 1 Acm−2 around 1 V and a decent ideality factor of 1.5, similar to characteristics of same diodes fabricated on glass substrates. (a) (b) (c) Figure 2. (a) Schematic device structure of the PEDOT:PSS/n-IGZO diodes. (b) The fabricated diodes on the plastic substrate. (c) J-V charateristics of the diodes on glass or plastic substrate (either flat or bent to a radius of curvature R = 2 cm) # Presenting Author Corresponding Author * 108 P-04 Anodic nanoporous SnO2 grown on Cu foils as superior binder-free Na-ion battery anodes Haidong Biana,b,#, Jie Zhanga, Muk-Fung Yuena,c, Wenpei Kanga,c, Yawen Zhana,c, Denis Y.W.Yua, Zhengtao Xub,*, Yang Yang Lia,c,d,* a Center of Super-Diamond and Advanced Films (COSDAF), City University of Hong Kong, Kowloon, Hong Kong, China b Department of Biology and Chemistry, City University of Hong Kong, 83 Tat Chee Avenue, Kowloon, Hong Kong, China c Department of Physics and Materials Science, City University of Hong Kong, Kowloon, Hong Kong, China d Centre for Advanced Structural Materials, City University of Hong Kong Shenzhen Research Institute, 8 Yuexing 1st Road, Shenzhen Hi-Tech Industrial Park, Nanshan District, Shenzhen, China * E-mail: [email protected], [email protected] Keywords: Na-ion batteries, cold rolling, anodization, nanoporous SnO2 We present a convenient, low-cost strategy to fabricate one-dimensional, vertically oriented nanoporous assembly of SnO2 upon a Cu substrate as a potentially promising anode system for Na-ion batteries application. The major novelty of the fabrication stage resides in anodizing a Sn/Cu bilayer film that is created by a facile cold-rolling procedure amenable to large-scale production. The open, nanoporous morphology of SnO2 facilitates the diffusion of electrolytes to access the SnO2 surface. The high porosity of the SnO2 phase also provides large void space to effectively accommodate the volume expansion/contraction during sodiation/desodiation. As a result, the 1-D nanoporous SnO2 thus assembled on the Cu substrate can be directly used as an effective electrode system for Na-ion storage--without the need for additives, dielivering a remarkable capacity of 326 mA h g-1 over 200 cycles at a current rate of 0.2 C. 109 P-05 First-Principles Design of Iron-Based Active Catalysts for Adsorption and Dehydrogenation of H2O Molecule on Fe(111), W@Fe(111), and W2@Fe(111) Surfaces Ming-Kai Hsiao,1 Bo-Ting Yao,1 Shin-Pon Ju,2,* and Hui-Lung Chen1,* 1 Department of Chemistry and Institute of Applied Chemistry, Chinese Culture University, Taipei, 111, Taiwan, 2 Department of Mechanical and Electro-Mechanical Engineering, National Sun Yat- sen University, Kaohsiung 80424, Taiwan Keywords: DFT, Catalysis, Fe(111), Dehydrogenation, H2O The adsorption and dehydrogenation of water on Fe(111), W@Fe(111), and W2@Fe(111) surfaces have been studied via employing the first-principles calculations method based on the density functional theory. The three adsorption sites of the aforesaid surfaces, such as top (T), 3-fold-shallow (S), and 3-fold-deep (D), were considered. The most favorable structure of all OHx (x = 0–2) species on the surfaces of Fe(111), W@Fe(111), and W2@Fe(111) have been thoroughly predicted and discussed. Our calculated results revealed that the adsorbed configurations of FeH2O(T-η1-O)-b, W@FeH2O(T-η1-O)-a, and W2@FeH2O(T-η1-O)-a possess energetically the most stable structure with their corresponding adsorption energies of -8.08, -13.37, and -18.61 kcal/mol, respectively. In addition, the calculated activation energies for the first dehydrogenation processes (HO-H bond scission) of H2O on Fe(111), W@Fe(111), and W2@Fe(111) surfaces, are 24.40, 12.62, and 9.97 kcal/mol, respectively. For second dehydrogenation processes (O-H bond scission), the corresponding activation energies of OH on Fe(111), W@Fe(111), and W2@Fe(111) surfaces are 39.35, 22.69, and 26.24 kcal/mol, respectively. Finally, the entire dehydrogenation courses on the varied Fe(111), W@Fe(111), and W2@Fe(111) surfaces are exothermic by 20.08, 41.35, and 59.30 kcal/mol, respectively. To comprehend the electronic properties of its nature of interaction between the adsorbate and substrate, we calculated the electron localization functions, local density of states, and Bader charges; the results were consistent and explicable. Corresponding Authors: *Shin-Pon Ju: [email protected] *Hui-Lung Chen: [email protected] 110 P-06 Highly Efficient Deep-Blue Electroluminescence from a Charge-Transfer Emitter with Stable Donor Skeleton Wen-Cheng Chen1*, Chun-Sing Leer1# Center of Super-Diamond and Advanced Films (COSDAF), City University of Hong Kong, Hong Kong SAR, PR China 1 Keywords: phenanthro[9,10-d]imidazole, donor-acceptor emitter, high stability, deep-blue OLED. Organic materials containing arylamines have been widely used as hole-transporting materials as well as emitters in organic light-emitting devices (OLEDs). However, it has been pointed out that the C-N bonds in these arylamines can easily suffer from degradation in excited states, especially in deep-blue OLEDs. In this work, phenanthro[9,10-d]imidazole (PI) is proposed as a potential donor with higher stability than those of arylamines. Using PI as the donor, a donor-acceptor type deep-blue fluorophore 1-phenyl-2-(4''-(1-phenyl-1Hbenzo[d]imidazol-2-yl)- [1,1':4',1''-terphenyl]-4-yl)-1H-phenanthro[9,10-d]imidazole (BITPI) is designed and synthesized. Results from UV-aging test on neat films of BITPI and other three arylamine compounds demonstrate that PI is indeed a more stable donor comparing to arylamine. OLEDs using BITPI as a emitter exhibits good device performances (EQE over 7%) with stable deep-blue emission (color index: (0.15, 0.13)) and longer operation lifetime than similarly-structured devices using arylamine-based emitters. Single-layer devices based on BITPI also show superior performances, which are comparable to the best results from the arylamine-based donor-acceptor emitters, suggesting that PI is a stable donor with good hole transport/injection capability. # Presenting Author Corresponding Author ([email protected]) * 111 P-07 High-Performance Color-Tunable Perovskite Light Emitting Devices through Structural Modulation from Bulk to Layered Film Ziming Chen1#, Chongyang Zhang1, Xiao-Fang Jiang1, Meiyue Liu1, Ruoxi Xia1, Tingting Shi1, Dongcheng Chen1, Qifan Xue1, Yu-Jun Zhao2, Shijian Su1, Hin-Lap Yip1#* and Yong Cao2 1 State Key Laboratory of Luminescent Materials & Devices, Institute of Polymer Optoelectronic Materials & Devices, South China University of Technology, P.R. China, 2 Department of Physics, South China University of Technology, P.R. China E-mail: [email protected] Keywords: Blue emission, perovskite LEDs, nanostructure modulation, layered perovskite. Organic-inorganic hybrid perovskite has been proved to be a promising material for light emitting devices (LEDs). Emission of organic-inorganic hybrid perovskites based on bulk, layered and quantum dot structure were reported. Based on nanostructure control, we successfully fabricated highly efficient perovskite LEDs from green to blue emission. Through adding small amount of 2-phenoxyethylamine (POEA) in CH3NH3PbBr3 precursor solution, the EQE of CH3NH3PbBr3 LED can enhanced from 0.06% to 2.82% (Fig.1) because adding POEA can passivate surface traps of CH3NH3PbBr3 crystal and help it become a purer phase with higher crystallinity. While loading large amount of POEA will change the bulk structure of perovskite to layered one because of the strong interaction between POEA molecules, resulting in a hypsochromic shift of emission from green to blue (Fig.1). In this case, we obtained a high-performance perovskite LED with EQE over 1% in sky-blue emission. In conclusion, through inducing POEA into CH3NH3PbBr3 precursor solution, we successfully revealed the relationship between perovskite structure change and optical properties, finding that nanostructure modulation could be a promising method to improve perovskite LED performance. [1] Fig. 1 EL spectra and EQE versus voltage characteristics of perovskite LEDs with different ratio of POEA. [1] Advanced Materials 2016, DOI: 10.1002/adma.201603157 # Presenting Author Corresponding Author * 112 P-08 The Detrimental Effect of Excess Mobile Ions in Planar CH3NH3PbI3 Perovskite Solar Cells Yuanhang Cheng#, Ho-Wa Li, Yuemin Xie, Xiuwen Xu, Sai Wing Tsang* Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, P. R. China. Keywords: perovskite solar cell, mobile ion concentration, photothermal deflection spectroscopy, transient photovoltage, stability The origin of the impact of mobile ion in perovksite solar cells (PVSCs) has recently become a hot topic under debate. Here, we investigate systematically the structural effect and various recombination pathways in PVSCs with different ion concentrations. By probing the transient ionic current in PVSCs, we extract mobile ion concentrations in a range of 1016 cm-3 to 1017 cm-3 depending on the processing conditions during a two-step process. The PVSC with the lowest ion concentration has both the highest efficiency over 15% and shelf-life over 1300 hours. Interestingly, in contrast to the commonly adopted models in literatures, we find that the crystal size and the bimolecular and trap-assisted recombination are not responsible to the large difference in photovoltaic performance. Instead, by using transient photocurrent and steady-state photoluminescence approaches, we find that the large reduction of shortcircuit current (Jsc) in mobile ion populated device is ascribed to the slow decay in photocurrent and the increasing amount of non-radiative recombination. In addition, we also find that the excess mobile ions trigger the deformation of perovskite to PbI2, which severely reduce the device lifetime. The results provide valuable information on the understanding of the role of excess mobile ion on the degradation mechanism of PVSCs. # Presenting Author: Yuanhang Cheng Corresponding Author : Sai Wing Tsang * 113 P-09 Edge-exposed Graphene Flexible Supercapacitor with Polymer Electrolyte Yeon Jun Choi1, Suk Woo Lee1, Geon-Woo Lee1, Byung-Hoon Park1, Tae-Ho Kim2, Dae Soo Jung3 and Kwang-Bum Kim1 E-mail: [email protected] 1 Department of Materials Science and Engineering, Yonsei University, 134 Sinchon-dong, Seodaemoon-gu, Seoul 120-749, Republic of Korea. 2 Center for Membranes, Korea Research Institute of Chemical Technology (KRICT), Daejeon 34114, Republic of Korea 3 Eco-Composite Materials Team, Korea Institute of Ceramic Engineering & Technology (KICET), Seoul 153801, Republic of Korea Keywords: Flexible supercapacitor, edge-exposed graphene, CNT bucky paper, solid polymer electrolyte Flexible energy storage devices have received increasing attention for their applications in emerging flexible and wearable electronics.1 Among various energy storage devices, supercapacitors (also called ultracapacitors or electrochemical capacitors) are considered as one of the most promising candidates to power flexible and wearable electronics owing to their high power density, long cycling life, and good operational safety.2 Realization of high-performance flexible supercapacitors requires consideration of electrochemical, mechanical, and interfacial properties of main components such as electrode, separator, and electrolyte. In this study, we designed and assembled a symmetric flexible supercapacitor based on edgeexposed graphene (EEG)-carbon nanotube (CNT) bucky paper and flexible solid polymer electrolyte. As an electrode material, EEG is a graphene with a high density of edge sites, therefore, high specific capacitance.3 Flexible EEG-CNT bucky paper was fabricated using vacuum filtration of a suspension of EEG and CNT. The assembled symmetric flexible supercapacitor shows a high capacitance per geometric area of 0.15 F cm-2 and an excellent capacitance retention of 98% over 50,000 cycles. In addition, the symmetric flexible supercapacitor has superior mechanical stability under repeated bending conditions. To be specific, the symmetric unit cell shows no decrease of specific capacitance after 5,000 bending cycles and specific capacitance retention of 90% over 50,000 cycles at highly bended state (bending radius : 3mm). More details about the electrochemical properties of the symmetric unit flexible supercapacitor will be discussed at the meeting. References 1. L. B. Hu et al., Nano Lett., 2010, 10, 708-714 2. J. R. Miller et al., Science, 2008, 321, 651-652 3. H. K. Kim et al., Energy Environ. Sci., 2016, 9, 1270-1281 114 P-10 Flexible fiber-shaped supercapacitor based on nickel-cobalt double hydroxide and pen ink electrodes on metallized carbon fiber 1 2 Libo Gao1# and Yang Lu1,2* Department of Mechanical and Biomedical Engineering, City University of Hong Kong, Hong Kong SAR, Kowloon 999077, Hong Kong; Center of Super-Diamond and Advanced Films (COSDAF), City University of Hong Kong, Kowloon, Hong Kong SAR, China * Author to whom correspondence should be addressed; E-Mail: [email protected] ; Tel.: 3442-4061. Keywords: fiber-shaped supercapacitor; nickel-cobalt double hydroxides; pen ink; nickel; carbon fiber Flexible fiber-shaped supercapacitors (FSSCs) recently are of extensive interest for portable and wearable electronic gadgets. Yet the lack of industrially flexible and cost-effective fibers with high conductivity and capacitance tremendously limits its civil practical application. To this end, here, we present pristine twisting carbon fibers (CFs) thread coated with a thin metallic layer via electroless deposition (ED) route, which exhibits exceptional conductivity with ~300% enhancement and superior mechanical strength (1.8 GPa). Subsequently, the commercial available conductive pen ink modified high conductive composite fiber uniformly covered with ultrathin nickel-cobalt double hydroxides (Ni-Co DHs) was introduced to fabricate flexible FSSC. The synthesized functionalized hierarchical flexible fiber exhibits high specific capacitance up to 1.39 F·cm-2 in KOH aqueous electrolyte. The asymmetric solid-state FSSC show maximum specific capacitance of 28.67 mF·cm-2 and energy density of 9.57 uWh·cm-2 at corresponding power density as high as 492.17 uW·cm-2 in PVA/KOH gel electrolyte, demonstrating its great potential in flexible electronic devices. Figure 1. Schematic illustration of fabrication the asymmetric fiber supercapacitor device. Figure 2. Electrochemical characterization of the asymmetric FSSC in solid PVA/KOH gel electrolyte. Acknowledgements: The authors gratefully acknowledge the funding support from Hong Kong RGC under the project # CityU 11216515. 115 P-11 Low-Light Photodetectors and Photovoltaics Based on Si/PEDOT:PSS Hybrid Devices Meng-Lin Tsai1,2,#, Libin Tang3, Lih-Juann Chen2,*, Shu Ping Lau3, Jr-Hau He1,* Computer, Electrical and Mathematical Sciences and Engineering, King Abdullah University of Science and Technology, Thuwal 23955-6900, Kingdom of Saudi Arabia, 2Department of Materials Science and Engineering, National Tsing Hua University, Hsinchu 30013, Taiwan, ROC, 3Department of Applied Physics, The Hong Kong Polytechnic University, Hung Hom, Kowloon, Hong Kong SAR. Email: [email protected]; [email protected] 1 Keywords: low-light, photodetector, solar cell, hybrid solar cell, omnidirectional Despite the massive improvement of traditional inorganic photodetectors and photovoltaic devices, the demand of light harvesting at low-light level has become increasingly important for the development of nextgeneration electronics. Traditional photodetectors usually suffer from high noise level at room temperature, therefore requires additional cooling systems for achieving low-light photodetection. Conventional solar cells also face the challenge of poor light harvesting at hazy or cloudy weather. Here we report an organic/inorganic hybrid device consisting of graphene quantum dot-modified poly(3,4ethylenedioxythiophene) polystyrene sulfonate spin-coated on Si with high responsivity, high detectability, omnidirectional light trapping capability, and fast operation speed at low-light level. We also carry out human tissue measurement, outdoor weather-dependent photovoltaic characterization, and indoor weak light photovoltaic characterization for demonstrating the potential of our low-light hybrid device for real-world applications. This advance provides a promising way for developing high performance low-light level photodetecting and photovoltaic devices in the future. Figure 1. (a) The schematic, SEM image, and fabrication process of the hybrid device. (b) TEM and high resolution TEM (inset) images of the GQD and a photograph of the GQD solution. (c) The diameter distribution of the sampled GQD measured from TEM images. Figure 3. (a) Schematic of the detection of 850 nm light propagating through human finger tissue. (b) Photo-todark current ratio (PDCR) of the hybrid device as a function of the 850 nm light propagation distance through human finger tissue. 116 Figure 2. (a)(b) 532 nm laser intensity-dependent responsivity and detectivity of the hybrid, micropyramidal Si, and planar Si devices measured at 0 V. (c) Schematic of angular dependent photodetection of the sun. (d) Enhancement of responsivity of the hybrid devices measured at 0 V under 850 nm light. (e)(f) The rise and fall time of the hybrid devices measured at 0 V under 850 nm light illumination. Figure 4. Current-voltage characteristics of the hybrid and micropyramidal Si devices at (a) 17:30 of a sunny day, (b) 13:00 of a cloudy day, and under (c) indoor LED illumination. P-12 High-Rate Li4Ti5O12/N-doped Reduced Graphene Oxide Composite for High Power Energy Storage Devices Jun Hui Jeong, Myeong-Seong Kim, Young-Hwan Kim, and Kwang-Bum Kima E-mail: [email protected] Department of Material Science and Engineering, Yonsei University, 50 Yonsei-ro, Seodaemun-gu, Seoul 03722, Republic of Korea Keywords: Lithium titanate; N-doped graphene; High-rate anode materials; High power Lithium ion batteries A Li4Ti5O12(LTO)/N-doped reduced graphene oxide (RGO) composite is proposed to inmprove the rate performance for high-rate lithium ion battery applications.1 The pore structure (both meso- and macro pores) is developed when RGO restacking is prevented, facilitating electrolyte ion diffusion to active sites.2,3 Uniform nitrogen doping on RGO sheets with high nitrogen contents provides additional free electrons to the sheets, resulting in increased electronic conductivity.4 The nitrogen content of the RGO sheets in the composite is 2.3 wt.%, which increases the electronic conductivity of the composite to 1.60 S cm-1. The specific surface area of the composite is increased to 35.8 m2 g-1. Thus, the composite structure with the Ndoped RGO sheets and porous secondary particles has high electrical conductivity and high ion accessibility. The LTO/N-doped RGO composite demonstrates excellent electrochemical performance with a high specific capacity of 117.8 mAh g-1 at 30 C and good cycle stability. References 1. J.H. Jeong et al., J. Power Sources, 2016, 336, 376-384 2. S-H. Park et al., Chem. Mater., 2015, 27, 457-465 3. M-S. Kim et al., Sci. Rep., 2016, 6, 29147 4. H-C. Youn et al., ChemSusChem., 2015, 8, 1875-1884 117 P-13 Enhanced Light Harvesting in Perovskite Solar Cells via Nanostructures Patterned Fullerene Passivation Layers Jian Wei1, #, Rui-Peng Xu 2, Jian-Xin Tang * Institute of Functional Nano& Soft Materials (FUNSOM), Soochow University Dushuhu Campus, No.199 Ren-Ai Road, Suzhou, P. R. China Keywords: perovskite solar cells, light harvesting, soft nanoimprinting Photovoltaic technology requires devices to efficiently carry out two processes: absorb light and covert the light into free charges rather than heat. Organic–inorganic lead halide perovskite solar cells are emerging as state-of-the-art photovoltaic devices because the hybrid perovskite materials potentially facilitate the photoelectric conversion process so that a more than 22% power conversion efficency has been obtained. However, it is still of great challenges to achieve maximum light trapping within the devices and then make the most of the light for photoelectric conversion. Based on the perovskite solar cells with a construction of glass/ITO/PEDOT:PSS/perovskite (CH3NH3PbI3-xClx)/PC61BM/Bphen/Ag, a simple and widely applicable scheme is put forward by incorporating soft nanoimprinted grating or quasirandom moth-eye nanostructures into fullerene passivation electron transporting layers as the light manipulation unit. Compared to the unpatterned device, the devices with grating and quasirandom moth-eye nanostructures exhibit a significant short circuit current enhancement of 6.6% and 11.2%, and the corresponding power conversion efficiencies increase from 14.39% to 15.36% and 16.23%, respectively. The effectiveness of this stratege is confirmd by absorption and external quantum efficiency measurements, wherein an improvement of the absorption spectrum over a broad wavelength range of 350-800 nm is observed. Theoretical simulations through finite difference time domain (FDTD) approach clearly exhibit that the scattering effect induced by nanostructures and the excited surface plasmon resonance (SPR) mode induced by the patterned metallic back electrode greatly enhance the energy flux densities in nanostructured layers, leading to more efficient light harvesting so as to higher device efficiencies. This light manipulation strategy can be a novel and efficient method for the performance enhancement study of perovskite solar cells. 118 P-14 Activated Graphene Microspheres for Supercapacitor Application Young-Hwan Kim and Kwang-Bum Kim E-mail: [email protected] Department of Materials Science and Engineering, Yonsei University, 134 Sinchon-dong, Seodaemoon-gu, Seoul 120-749, Republic of Korea. Keywords: Activation, N-containing carbon, Graphene, Supercapacitor Graphene has been extensively studied as an electrode material for supercapacitors due to its high electric conductivity, large specific surface area, and excellent chemical/mechanical stability.1,2 Due to the 2D nature of the graphene sheet, however, it tends to easily to form lamellar microstructures on a current collector during electrode fabrication. Restacking of the graphene sheets in the electrode greatly reduces the effective surface area of graphene and limits ion transport within the graphene electrode, which in turn leads to a decrease in the specific capacitance.3 Assemblies of graphene has been reported to convert 2D graphene sheets to a 3D structure of graphene could sustain its structure after being immersed in an electrolyte solution and was remarkably aggregation – resistant.4 In this study, we make 3D microsphere of graphene by using Ncontaining carbon and activate the produced 3D microsphere of graphene by potassium hydroxide. We report on activated graphene microspheres exhibited a large surface area of 1380 m2 g-1 and high micro-pore volume of 1.216 cm3 g-1 with a high specific capacitance of 254 F g-1 at 0.5 A g-1 and 226.7 F g-1 at 10 A g-1 in 1 M TEABF4/AN electrolyte. Detailed synthetic procedure, electrochemical properties of activated graphene microspheres will be discussed in the meeting. Figure (a) Cyclic Voltammograms of activated graphene microspheres at increasing potential scan rates from 10 mV s-1 to 500 mV s-1 (b) Galvanostatic charge/discharge profiles of activated graphene microspheres at increasing current density from 0.5 A g-1 to 10 A g-1 in 1 M TEABF4/AN electrolyte. References 1. K. S. Novoselov et al, Science, 2004, 306, 666. 2. C. Berger et al, Science, 2006, 312, 1191. 3. H. K. Kim et al, Energy Environ. Sci., 2016, 9, 1270. 4. S. H. Park et al, Chem. Mater., 2015, 27, 457. 119 P-15 Sn4P3 Nanotops Based Anodes for Sodium Ion Batteries Danni, Lan1#, Wenhui Wang1, Quan Li1* Department of Physics, The Chinese University of Hong Kong, Shatin, New Territory, Hong Kong 1 Keywords: Sodium ion batteries, anode, Tin phosphide Sodium ion batteries (SIBs) have been considered as a promising alternative to lithium ion batteries LIBs). The energy storage mechanism for SIBs is similar to that of LIBs, but the abundance of Na on earth makes it much cheaper than the Li counterparts. Suitable anodes with high specific capacity and appropriate redox potentials are requisite for high energy capacity sodium ion batteries. Among various material choices, Sn4P3 is a most promising anode material owing to its highest theoretical volumetric capacity (6650 mA h cm3 ), high gravimetric capacity (1132 mA h g-1) and relatively low redox potentials (~0.3 V-0.65 V vs. Na/Na+). Ball milling and solvothermal are the conventional fabrication methods for Sn4P3. However, the large size of Sn4P3 (when obtained by ball milling) or the P impurities left in the sample (when obtained by solvothermal) are detrimental to the anode performance. In the present work, a facile solution chemistry method is developed to grow phase pure Sn4P3 nanotops with controllable size. The detailed growth mechanism of the Sn4P3 nanotops will be discussed. The as-prepared Sn4P3 nanotops show good electrochemical performance when employed as SIB anode. This work is supported by RGC/GRF under project No. 14316716 # Presenting Author Corresponding Author * 120 P-16 On the Study of Exciton Binding Energy with Direct Charge Generation in Photovoltaic Polymers Ho-Wa Li1#, Zhiqiang Guan2, Yuanhang Cheng1, Taili Lui1, Qingdan Yang1, Chun-Sing Lee2*, Song Chen3*, Sai-Wing Tsang1* 1 Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, P. R. China, 2 Center of Super-Diamond and Advanced Films (COSDAF), Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, P. R. China, 3 Recording Head Operation, Seagate Technology LLC, Minneapolis, MN, 55435, USA Keywords: transport gap, exciton, binding energy, quantum efficiency, organic photovoltaics The excitonic effect in organic semiconductors plays a key role in determining the electronic devices performance. Strong exciton binding energy has been regarded as the detrimental factor limiting the further improvement in organic photovoltaic cells. Substantial photovoltage loss is accompanied with the dissociation of the Coulombic attraction of photo-generated electron-hole pairs. Despite the matter of importance, there is limited reported in measuring the exciton binding energy in organic photovoltaic materials. Conventional sophisticated approach using photoemission spectroscopy (UPS and IPES) requiring ultra-high vacuum that limits the wide access of the investigation. Here, we will demonstrate a facile approach for measuring the exciton binding energies of a wide range of organic semiconductors by photoconductivity. Quantitative values of the exciton binding energy in five prototypical photovoltaic polymers were obtained with concise photovoltaic device structure. And the extracted binding energies have excellent agreement with those determined by the conventional photoemission technique. The results would bring insight into the future development of reducing the excitonic effect for high efficiency organic photovoltaic cells. # Presenting Author Corresponding Author * 121 P-17 Rational Design of Hollow Carbon Nanofibers Inserted MnO Micro-Nano Spheres with Enhanced Electrochemical Performance for Li-Ion Batteries Huan-Huan Li, Jing-Ping Zhang* Faculty of Chemistry, National & Local United Engineering Laboratory for Power Batteries, Northeast Normal University, Changchun 130024, China. Keywords: lithium-ion batteries, MnO, anode materials, hollow carbon nanofibers. Manganese monoxide (MnO) has been proposed as a promising conversion anode material for lithium ion batteries (LIBs) because of its high theoretical capacity, comparatively low voltage hysteresis (<0.8 V), low cost and environmental friendliness. However, the inferior intrinsic electrical conductivity, poor ion transport kinetics, and obvious volume expansion/contraction of MnO greatly restrict its further application in LIBs.1-2 In this work, porous spherical MnO and hollow carbon nanofibers (HCNFs) composite (MnO/HCNFs) has been designed and synthesized by a facile hydrothermal method followed by a thermal reduction process. The MnO/HCNFs exhibites a unique porous cherry-like structure, which makes full use of the advantages of the rich porosity, micro-nano structure of MnO, and high conductivity of HCNFs. Firstly, the rich porosity throughout the entire MnO spheres increases active sites to store redox ions and enhance ionic diffusivity to primary MnO nanoparticles. Secondly, the three dimensional interconnected porous micro-nano structure is able to accommodate the volumetric changes and relieve the strains caused by the volume variation during the charge/discharge process, thus significantly enhancing the structural stability. Thirdly, the conductive HCNFs is favor for both transport of electrons and ions, contributing to decent redox kinetics. Due to the merits mentioned above, the MnO/HCNFs exhibited remarkable cycling performance (950/840 mAh g-1 after 200/500 cycles at 200/1000 mA g-1) and good rate capability (200 mA h g-1 at 6.4 A g-1) as anodes for LIBs. The realization of decent electrochemical performance without nanostructuring in a complex metal oxides expands the scope of cherry-like structured synthesis for other materials in energy storage use. Moreover, MnO/HCNFs synthesized in a facile and economical strategy in this work suggest that this material not only is structurally and electronically exceptional but merits consideration for a range of further applications. Scheme. Superior advantages of M-N/HCNFs compared to normal M-N structured materials. References 1. Poizot, P.; Laruelle, S.; Grugeon, S.; Dupont, L.; Tarascon, J. M. Nature 2000, 407, 496-499. 2. Li, X.; Xiong, S.; Li, J.; Liang, X.; Wang, J.; Bai, J.; Qian, Y. Chem. - Eur. J. 2013, 19, 11310-11319. * Corresponding Author: Jing-Ping Zhang; Email: [email protected]; Fax: 86-431-85099668. 122 P-18 Solution-Processed, Mercaptoacetic Acid-Engineered Quantum Dots Photocathode for Efficient Hydrogen Generation under Visible Light Irradiation Bin Liu,1,2 Xu-Bing Li,2 Li-Zhu Wu,*2 Chen-Ho Tung,*2 Wen-Jun Zhang *1 COSDAF, Department of Physics and Materials Science, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kong, China 2 Key Laboratory of Photochemical Conversion and Optoelectronic Materials, Technical Institute of Physics and Chemistry, the Chinese Academy of Sciences, Beijing, China 1 Keywords: photoelectrochemical, photocathode, quantum dots, hydrogen generation The production of clean fuels by solar energy conversion is an attractive solution to the looming energy crisis and greenhouse effect. Hydrogen (H2), with high specific enthalpy and benign combustion product, is considered to be an ideal candidate for such a fuel, particularly as it is produced by water splitting using sunlight. Recently, quantum dots (QDs) have appeared at the forefront of light-driven H2 production because their nanoscale physical properties are quite different from those of bulk materials. Unfortunately, all of the current systems are performed well only in the presence of large amounts of chemical sacrificial electron donors. To avoid the use of any sacrificial agent and generate H2 in an environmentally friendly manner, photoelectrochemical (PEC) production of H2 is an ideally clean and renewable mean that integrates solar energy collection and water reduction into a single photoelectrode. PEC studies involving QDs-sensitized photoelectrodes have focused almost exclusively on photoanodes, where photocurrents result from lightsimulated electron transfer from QDs into the conduction bands of an n-type semiconductor, such as TiO2. Conversely, QDs-based photocathodes, operated in an inverse mode of light-stimulated hole transfer from QDs into the valence band of a p-type semiconductor, are scarcely concerned to date. We describe here a simple, efficient and stable CdSe QDs/NiO photocathode engineered by molecular linker, mercaptoacetic acid (MAA), for H2 generation from neutral water. This protocol does not require any sacrificial reagent, external cocatalyst, protecting layer and buffer solution as well. Upon visible-light irradiation, photocurrent, as high as -60 μA/cm2, is achieved at a bias of -0.1 V vs. NHE in 0.1 M Na2SO4 (pH 6.8). Simultaneously, the photocathode evolves H2 consistently for 45 h with ~100% Faradic efficiency that is unprecedented in the field of sensitized photocathodes for H2 production. Mechanistic study reveals that the exceptional performance is derived from the efficient hole transfer process. Fig. 1 (a) The transient photocurrent responses to on-off illumination of photocathodes); (b) evolved H2 and charges passed through the outer circuit (dashed line); Acknowledgement. This work was supported by the Ministry of Science and Technology of China (2014CB239402, 2013CB834804 and 2013CB834505), the National Natural Science Foundation of China (21090343, 91027041 and 21390404), and the Chinese Academy of Sciences. References. [1] L.-Z. Wu, B. Chen, Z.-J. Li, C.-H. Tung, Acc. Chem. Res., 2014, 47, 2177. [2] B. Liu, X-B. Li, Y-J. Gao, Z. J. Li, Q-Y. Meng, C-H. Tung, L-Z. Wu, Energy Environ. Sci. 2015, 8, 1443. [3] J. Li, X. Gao, B. Liu, Q. Feng, X.-B. Li, M.-Y. Huang, Z. Liu, J. Zhang, C.-H. Tung, L.-Z. Wu, J. Am. Chem. Soc. 2016, 138, 3954. 123 P-19 Low temperature processed photoconductive cathode interlayer for inverted polymer solar cells Yinqi Luo1, Zengqi Xie1* 1 Institute of Polymer Optoelectronic Materials and Devices, State Key Laboratory of Luminescent Materials and Devices, South China University of Technology, Guangzhou 510640, P. R. China.Email: [email protected] Keywords: photoconductive, cathode interlayer, water soluble, zinc oxide, organic solar cells. We report an aqueous solution processed highly mobility cathode interfacial layer (CIL) for efficient inverted polymer solar cells (iPSCs) by doping ZnO with a water soluble perylene bisimide (PBI-SO3H). The easily formed strong interaction (chemical bonding) between ZnO and the -SO3H group facilitates the formation of uniform thin film even at relatively low temperature. PBI-SO3H greatly increases the electron mobility and conductivity of ZnO under light illumination due to photo induced electron transfer between them. As a result, the inverted polymer solar cell based on thieno[3,4-b]thiophene/benzodithiophene (PTB7):[6,6]-phenyl C71-butyric acid methyl ester (PC71BM) using ZnO:PBI-SO3H as an electron transporting layer delivered a power conversion efficiency (PCE) of 8.78%. Here, the ZnO:PBI-SO3H was treated under 150℃, which is a threshold for the procession on flexible substrate. Both the high conductivity and Low temperature processing of ZnO:PBI-SO3H interlayer are favorable for large-scale printable iPSCs. The work provides a promising candidate cathode interfacial material for efficient iPSCs. References (1) Nian, L.; Zhang, W.Q.; Wu, S.P.; Qin, L.Q.; Liu, L.L.; Xie, Z.Q.; Wu, H.B.; Ma, Y.G. ACS Appl. Mater. Interfaces, 2015, 7, 25821-25827. (2) Nian, L.; Zhang, W.Q.; Zhu, N.; Liu, L.L.; Xie, Z.Q.; Wu, H.B.; Würthner, F.; Ma, Y.G. J. Am. Chem. Soc., 2015, 137, 6995-6998. (3) Nian, L.; Gao, K.; Liu, F.; Kan, Y.; Jiang, X.; Liu, L. L.; Xie, Z. Q.; Peng, X. B.; Russell, T. P.; Ma, Y. G. Adv. Mater. 2016, 28, 8184–8190. (4) Nian, L.; Chen, Z.; Herbst, S.; Li, Q.; Yu, C.; Jiang, X.; Dong, H. L.; Li, F. H.; Liu, L. L.; Würthner, F.; Chen, J. W.; Xie, Z. Q.; Ma, Y. G. Adv. Mater. 2016, 28, 7521-7526. 124 P-20 Various morphologies of WO3 nanostructures fabricated by hydrothermal methods and its effects on photo-catalytic properties Soo-Min Park1,#, Sung-Myung Ryu1, Chunghee Nam1,2,* Department of Photonics and Sensors, Hannam University, Daejeon, Republic of Korea 2 Department of Unmanned System, Hannam University, Daejeon, Republic of Korea 1 Keywords: WO3 nanorods, oxide semiconductor, photo-catalyst, hydrothermal method Transition metal oxides have attracted much interest not only due to their fundamental scientific issues but also their various technological applications such as environment-, energy- and bio- materials. Tungsten oxides (WO3) among those oxides have wide-ranging applications such as, gas sensors, electrochromic for smart window, and photo-catalyst etc..[1-3] In this study, WO3 nanostructures have been synthesized by simple wet-chemical hydrothermal method at various temperatures using sodium tungstate (Na2WO4·2H2O) as a precursor material. In order to obtain various morphologies of WO3 nanostructures, we have added directional capping agents (citric acid and oxalic acid) during the preparation of solution, resulting in that structures and morphology of WO3 powders were obviously changed. The morphology and structure of synthesized WO3 samples were characterized by scanning electron microscopy (SEM), x-ray diffraction technique, and BET methods for surface area measurements. It was found that the capping agents have an essential influence on the morphology evolution due to NaCl limited concentration during synthesis of WO3 crystal. In addition, the optimal duration time for hydrothermal reaction is reduced, which is useful for mass-production of WO3 nano-powders. Finally, photo-catalytic properties were investigated by simple UVabsorption methods depending on the amount of UV exposure. The results will be presented in detail. [1] N. Xu, M. Sun, Y. W. Cao, J. N. Yao, and E. G. Wang, Appl. Surf. Sci. 157, 81 (2000) [2] Y. A. Yang, Y. W. Cao, P. Chen, B. H. Loo, and J. N. Yao, J. Phys. Chem. Solids. 59, 1667 (1998) [3] E. Rossinyol, A. Prim, E. Pellicer, J. Rodriguez, F. Peiro, A. Cornet, J. Ramon, B. Tian, T. Bo, and D. Zhao, Sens. Act. B 126 18 (2007) # Presenting Author Corresponding Author : [email protected] * 125 P-21 Efficient Thermally Activated Delayed Fluorescence OLEDs Based on Functional Phenylpyridinato Boron Complexes Yi-Jiun Shiu,a,# Yi-Ting Chen,b, Wei-Kai Lee,a Chung-Chih Wu,a,* Tzu-Chieh Lin,b Shih-Hung Liu,b Pi-Tai Chou,b* Chin-Wei Lu,c I-Chen Cheng,c Yi-Jyun Lien,c and Yun Chi,c,* a, Graduate Institute of Electronics Engineering and Department of Electrical Engineering, National Taiwan University, Taipei 10617, Taiwan b, Department of Chemistry, National Taiwan University, Taipei 10617, Taiwan c, Department of Chemistry, National Tsing Hua University, Hsinchu 30013, Taiwan E-mail: [email protected]; [email protected]; [email protected]; Keywords: boron, thermally activated delay fluorescence, N-donor, organic light emitting diodes, phenylpyridine Efficient light emitting materials are an indispensable component in the fabrication of organic light emitting diodes (OLEDs) for flat-panel display and solid state lighting applications. It is notable that the heavy transition-metal of phosphorescent emitters are capable to induce fast intersystem crossing (ISC) between the singlet (S1) and triplet (T1) excited states, giving electroluminescence with internal quantum efficiencies (ηint) of nearly 100%. Alternatively, there is a relatively new class of compounds, namely: thermally activated delayed fluorescence (TADF) emitters, which can also achieve unitary ηint without employment of the thirdrow transition-metal atoms. In general, TADF emitter can be enabled by reducing the spatial overlap between the HOMO and LUMO orbitals of molecules, for which the reduced electron exchange energy afforded the smaller energy gap between triplet (typically T1) and singlet (S1) states, defined as ET-S (T1-S1). The smaller ET-S facilitates the fast reverse intersystem crossing (RISC) from the non-emissive T1 to the emissive S1 excited state upon thermal activation, rendering effective harvest of triplet excitons to the singlet state for the generation of bright electroluminescence (fluorescence). A new series of functional phenylpyridinato boron complexes possessing thermally activated delay fluorescence (TADF) have been strategically designed and synthesized. These boron complexes utilize phenylpyridine as the electron acceptor (A) that links to carbazole or triphenyl amine as the electron donor (D) via a core boron atom, forming four-coordinate neutral boron complexes. The selection of boron to spatially separate donor and acceptor takes its advantage of facile functionalization. TADF properties of the resulting D-A functional materials in various solvents and solid hosts have been investigated via their emission spectra and associated relaxation dynamics. The results show that the operation of TADF is solvent polarity dependent in fluid states and solid host dependent. Some of these novel TADF emitters show high PLQYs in appropriate solid hosts and can be used to fabricate highly efficient blue-green to green TADF OLEDs showing EL efficiencies of up to (20.2%, 63.9 cdA-1, 66.9 lmW-1) and (26.6%, 88.2 cdA-1, 81.5 lmW-1), respectively. 126 2 P-22 Metal-oxide-semiconductor (MOS) photoanodes for photoelectrochemical water splitting devices Yuanyuan Shi1, Tingting Han1,2, Xiaoxue Song1#, Antonio Mio2, Luca Valenti2, Stefania Privitera2, Salvatore Lombardo2, Mario Lanza1* 1Institute of Functional Nano & Soft Materials, Soochow University, Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, 199 Ren-Ai Road, Suzhou, 215123, China 2Institute for Microelectronicsand Microsystems, National Research Council (IMM-CNR), 533 Stradale Primosole 95121 Catania, Italy * Corresponding author e-mail: [email protected] Keywords: MOS structure, Water splitting, Photoanode, Ageing mechanism, The metal-oxide-semiconductor (MOS) structure has been widely used in many different applications, ranging from microelectronics to photovoltaics. In this work we present a comprehensive explanation of the use of MOS devices in the field of water splitting, providing specific experimental details and guides about how to start in this field. MOS nanocomposites are promising candidates for transforming sunlight into clean chemical fuels, such as hydrogen. This approach is attractive because sunlight is intermittent and locationdependent, and chemical fuels can be stored and transported. One raising technology is to split water molecules into hydrogen and oxygen by electrolysis (see Eq. 1). To do so, the semiconductor is immersed in a liquid and illuminated, which produces a photocurrent that boost the electrolysis. When this happens, some chemical reactions appear at the liquid-semiconductor interface, which are: Overall water splitting: 2H2O O2 + 2H2 (Eq. 1) It is worth noting that a tandem water splitting cell contains two electrodes, a photoanode and a photocathode [1], where the OER and HER take place (respectively). The continuous generation of these chemical reactions at the surface of the semiconductor could corrode it, leading to performance decay. To avoid this problem some protective transition metal oxides (such as TiO2 [2, 3]) can be deposited at the interface (usually by ALD). Moreover, in order to accelerate the chemical reactions metallic catalysts need to be also evaporated or sputtered on top [2-5], leading to the effective MOS photoelectrode. Sometimes, metallic catalysts can also act as anti-corrosion layers, simplifying the manufacturing process. Here we will present our latest results using Ni/SiO2/n-Si photoanodes for water splitting [6, 7]. The cross sectional TEM image of a fresh 5 nm Ni/SiO2/n-Si photoanode, which exhibits the MOS structure of the sample layer by layer. Record activity and long stability have been obtained by using thin (below 10 nm) nickel layer on the n-Si surface with native SiO2 at alkaline conditions under illumination. The reliability and ageing mechanism of this kind of photoanodes have been explored combing a wide range of the nano and atomic scale tools with the long stability tests in photoanodes with different metal thicknesses. We observe that the degradation kinetics of the nickel coatings strongly depend on the thickness of the coating layer. The activity of the 2 nm nickel-coated silicon photoanode decays faster than thicker ones, due to prohibitive increase of SiO2 layer thickness plus contamination from the electrolyte. Above a thickness of 5 nm nickel coating, the performance of the samples decays due to the formation of holes on the nickel layer. References: [1] J. A. Turner, Science, 342, 811-812 (2013). [2] Y. W. Chen, J. D. Prange, S. Dühnen, Y. Park, M. Gunji1, C. E. D. Chidsey, P. C. McIntyre, Nat. Mater., 10, 539-544 (2011). [3] S. Hu, M. R. Shaner, J. A. Beardslee, M. Lichterman, B. S. Brunschwig, N. S. Lewis, Science, 344, 10051009 (2104). [4] A. G. Scheuermann, K. W. Kemp, K. Tang, D. Q. Lu, P. F. Satterthwaite, T. Ito, C. E. D. Chidsey, P. C. McIntyre, Energy Environ. Sci., 9, 504-516 (2016). [5] R. Fan, J. Min, Y. Li, X. Su, S. Zou, X. Wang, M. Shen, Appl. Phys. Lett., 106, 213901 (2105). [6] M. J. Kenney, M. Gong, Y. Li, J. Z. Wu, J. Feng, M. Lanza, H. Dai, Science, 342, 836-840 (2013). [7] T. Han, Y. Shi, X. Song, A. Mio, L. Valenti, F. Hui, S. Privitera, S. Lombardo, M. Lanza, J. Mater. Chem. A (2016, major revision). # Presenting Author *Corresponding Author 127 P-23 User Infrastructures for Energy Material Science at the Helmholtz Zentrum Berlin für Materialien und Energie HZB 1 Antje Vollmer1,*, # Helmholtz Zentrum Berlin für Materialien und Energie, Albert-Einstein-Str.15, 12489 Berlin, Germany Keywords: BESSY II, Energy Materials, Infrastructure. Modern societies are facing the urgent global challenge of a growing demand for energy and the sustainability of its supply. Meeting this challenge requires a tremendous effort in research, innovative solutions and smart applications. Scientists from around the world have accepted the task to develop and refine new scientific concepts and technologies to pave the way to clean and sustainable energy supply of tomorrow. The „Helmholtz Zentrum Berlin für Materialien und Energie“ has taken up the challenge of developing advanced materials for solar energy conversion and storage on one side and to provide outstanding infrastructure to a global user community on the other. By offering a variety of experimental possibilities HZB aims at contributing to a sustainable, economic and secure energy supply. With Synchrotron methods and dedicated laboratory infrastructures that allow guided materials design, synthesis and analysis, HZB targets the full chain from the discovery of basics principles in energy materials to the transfer of results to applications for the society. One of the infrastructures at BESSY II is EMIL@BESSYII, the Energy Materials In-situ Laboratory. In a concerted effort together with the Max Planck Society, EMIL@BESSYII will offer a pivotal, unique infrastructure for Energy Materials Research at HZB’s synchrotron light source. In addition to EMIL@BESSYII, a variety of dedicated experimental set-ups at BESSY II allow experiments on energy materials for applications in photovoltaics, energy conversion, energy storage and energy saving. Our new multi-user platform CoreLabs at HZB will complement the synchrotron infrastructures. CoreLabs are dedicated to research and development of new and improved materials for energy conversion and storage applications as well as energy-efficient future IT. They provide state-of-the-art laboratories and unique equipment and will serve the wider scientific community by offering services and user access to external academic and industrial partners. The X-ray CoreLab covers different modern X-ray diffraction methods focusing on in-situ studies of phase transitions and texture analysis. The microscopy CoreLab, participating in the ZEISS labs@loation program, conducts cutting-edge research on novel materials with the most modern ZEISS electron microscopes available. The HySPRINT CoreLab will focus on hybrid materials and components based on silicon and perovskite crystals used for energy conversion in photovoltaics as well as for solar hydrogen production (http://hz-b.de/corelabs). In this presentation the HZB infrastructures for Energy Material Science to the global user communities are presented and discussed. # Presenting Author Corresponding Author * 128 P-24 Enhanced cycle performance of Sn4P3 anode in Na-ion batteries using TiC Wenhui Wang #, Quan Li * Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, HongKong 1 Keywords: Sodium ion battery, Anode, Tin phosphide, TiC Sn4P3 is a most promising anode candidate for Na-ion battery, due to its high capacity (1132 mAh/g or 1192 Ah/L) and low average operating voltage (~0.5 V vs. Na/Na+). However, its cycle stability is limited by the low electronic conductivity of the binary Sn-P phases and the segregation of Sn upon cycling. In the present work, we show that enhanced cycling performance of Sn4P3 can be achieved by introducing TiC to the ball milled Sn4P3/TiC particles. With 30% TiC introduced, Sn4P3 can retain 94.5% of initial de-sodiation capacity over 100 cycles at current density of 100 mA/g. This is quite significant when comparing to a 17.4% remain in the case of Sn4P3 without TiC introduction. The optimization of TiC amount and mechanism for the cycling stability improvement will also be discussed. This work is supported by RGC/GRF under project No. 14316716 # Presenting Author Corresponding Author E-mail: [email protected] * 129 P-25 Studies of Charge Recombination and Collection Behaviors in Non-fullerene Based Organic Solar Cell Yiwen Wang#, Furong Zhu Department of Physics, Hong Kong Baptist University, Hong Kong Keywords: Non-fullerene acceptor; charge carrier mobility; bimolecular recombination. Fullerene derivative-based electron acceptors have been widely used for application in organic solar cells (OSCs), due to the advantages of high electron mobility, electron affinity and efficient charge transportation. However the fullerene-based acceptors have weak absorption in the visible light region and the limited room for tuning the energy level for realizing the desired energy level alignment with different polymer donors. In order to overcome these limitations, a variety of non-fullerene electron acceptors have been developed. A comprehensive analysis was carried out to study the charge recombination and collection in both conventional and inverted OSCs based on non-fullerene acceptor (ITIC). ITIC-based conventional and inverted configuration OSCs having power conversion efficiency (PCE) of 7.5% and 7.7% are obtained, with comparable performance of [6,6]-Phenyl-C71-butyric acid methyl ester (PC71BM)-based OSCs having PCE of 7.5% (conventional) and 7.9% (inverted). The results reveal that ITIC-based OSCs always show higher open circuit voltage (VOC) as compared to that of the PC71BM-based devices. The bimolecular recombination, charge collection at the organic/cathode interface and their impacts on VOC in ITIC-based OSCs are analyzed using the photo-induced charge extraction by linearly increasing voltage and light intensity-dependent current density–voltage characteristics measurements. 130 P-26 Theoretical Calculations of Electrochemical Activities of Cu-BHT Nanostructures on Catalyzing Hydrogen Evolution Reaction Huiying Yao1, Xing Huang2, Wei Hao3, Jia Zhu1#*, Shuzhou Li3*, Wei Xu2* Department of Chemistry, Beijing Normal University, Beijing, 100875 P. R. China 2 Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100190 P. R. China 3 School of Material Science and Engineering, Nanyang Technological University, 639798 Singapore *Email: [email protected], [email protected], [email protected] 1 Keywords: DFT, Hydrogen Evolution Reaction, Cu-BHT Hydrogen has been considered as a promising candidate of clean and sustainable energy for its high energy density, abundant resources and environmental friendly. One of the executable and convenient ways to obtain hydrogen is the electrocatalytic splitting of water through hydrogen evolution reaction (HER). Comparing with the well-known HER catalytic materials, the reported two-dimensional conjugated coordination polymer material Cu-BHT1 (BHT=benzenehexathiol) shows underestimated catalytic performance. Herein, we used density functional theory (DFT) to reveal various catalytic performances of electrodes covering by Cu-BHT nanostructures. Two kinds of crystal planes depending on the structure of CuBHT have been modeled: (0 0 1) and (1 0 0) surfaces. On (0 0 1), atomic hydrogen is more reliably adsorbed on atop site of S with Eads = 0.315 eV. While on (1 0 0) surface, it prefers to adsorbed above Cu with Eads = 0.256 eV. So far, it can be concluded that preferred adsorbed sites of atomic hydrogen and the strength of adsorption above same element both vary in different surfaces. Furthermore, we have studied the adsorption energy change along with increasing hydrogen coverage to give a better description of catalytic performance. It is expected to give helpful insights for improving the activity of metal organic material catalysts in experiment through controlling their surface morphologies. 1. Huang, X. et al. A two-dimensional p–d conjugated coordination polymer with extremely high electrical conductivity and ambipolar transport behaviour. Nat. Commun. 6:7408 131 P-27 Amorphous red P encapsulated in hollow porous carbon nanoshpere for sodium storage with exceptional long-term cyclic stability Shanshan Yao1, *, #, Jiang Cui1, Jang-Kyo Kim1 Department of Mechanical and Aerospace Engineering, The Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong, P. R. China. * Corresponding author: [email protected] (S. Yao) 1 Keywords: red P, HPCNS, vaporization-condensation, long lifespan, SIB. To satisfy the ever-growing demands of rechargeable battery market and large-scale application like smart grid energy storage, room-temperature sodium ion batteries (SIBs) have received much attention due to the abundant Na resource, low cost and similar electrochemistry of Na to Li.[1,2] Among a myriad of anode materials, phosphorus (P) has been considered a promising candidate for SIBs owing to the ultrahigh theoretical specific capacity of 2596 mAh g-1[3] and a relatively safe working potential of ~ 0.45 V vs. Na/Na+.[4] In this work, a facile and effective approach is developed to synthesize hollow, porous carbon nanosphere/phosphorus (HPCNS/P) composites as anodes for high performance SIBs where the red P s fully encapsulated within the hollow porous carbon nanosphere (HPCNS) matrix by vaporization-condensation. The strong chemical bonds formed between the HPCNSs and red P maintain excellent electrical contacts and stabilize the solid electrolyte interphase layer. The hierarchical mesopores of the HPCNS matrix not only enhance the electrolyte permeation and Na+ ion transport, but also effectively accommodate the volume expansion of red P upon sodiation. These ameliorating structural features give rise to exceptional structural stability of the electrode as proven by the in situ TEM examination. The HPCNS/P anode delivers an excellent reversible capacity of ~ 2000 mAh g-1 (based on the net mass of P) over 300 cycles at 0.1 A g-1 and excellent capacity retention of over 76 % after 1000 cycles at a high current density of 1.0 A g-1. The simple, versatile synthesis approach and the excellent electrochemical performance of HPCNS/P anodes shed new insights into rational design of insulating phosphorus-based SIB anodes with large volume expansion. Reference [1] H. Kim, H. Kim, Z. Ding, M. H. Lee, K. Lim, G. Yoon, K. Kang, Adv. Energy Mater. 2016, 1600943. [2] N. Yabuuchi, K. Kubota, M. Dahbi, S. Komaba, Chem. Rev. 2014, 114, 11636. [3] C. Zhang, X. Wang, Q. Liang, X. Liu, Q. Weng, J. Liu, Y. Yang, Z. Dai, K. Ding, Y. Bando, J. Tang, D. Golberg, Nano Lett. 2016, 16, 2054. [4] Y. Zhu, Y. Wen, X. Fan, T. Gao, F. Han, C. Luo, S. C. Liou, C. Wang, ACS Nano 2015, 9, 3254. 132 P-28 High efficiency hysteresis-free perovskite solar cells with a solution processed vanadium oxide (VOx) hole extraction layer Xiang Yao1)#, Xiong Gong1,2)* State Key Laboratory of Luminescent Materials & Devices, South China University of Technology, Guangzhou 510640, P. R. China. 2College of Polymer Science and Polymer Engineering, The University of Akron, OH 44325, USA. E-mail: [email protected], 1 Keywords: Vanadium oxide (VOx), Hole extraction layer, Perovskite solar cells, Solution-processed, Hysteresis-free. Perovskite hybrid solar cells (pero-HSCs) have attracted tremendous attention over the past few years due to distinct properties of the perovskite materials such as extremely long ambipolar carrier diffusion length, good electrical transport properties, high extinction coefficient, and broad adsorption range along with a tunable bandgap, etc.[1,2]To attain high performance for p-i-n perovskite hybrid solar cells (pero-HSCs), the design of hole extraction layer (HEL) and related interfacial engineering are big challenge. Vanadium oxide (VOx) is a low price material with superior thermal and chemical stability which is widely used as HEL in photovoltaic devices. The heating process higher than 300 °C is necessary for achieving a certain crystalline phase for enhancing the electrical conductivity of VOx in the previous works.[3] In our work, we report a simple way to fabricate a solution processed VOx film based on annealing treatment at 210 °C for 8 minutes in air. Further, the introduction of self-assembling monomolecular (SAM) surface modification on the VOx film have enhanced the hole extraction and reduced the change recombination due to the improvements in the perovskite crystallinity, and the reduction of pinholes and trap states of perovskite layer. The pero-HSCs with SAM surface modification have achieved a power conversion efficiency (PCE) of 14% Importantly, the peroHSCs with and without SAM surface modification displayed hysteresis-free. Scheme 1. the processing of solution processed VOx film based on annealing treatment Figure 1. J-V curves of the pero-HSCs W/ SAM and the pero-HSCs W/O SAM. Reference [1] Green MA, Ho-Baillie A, Snaith HJ. Nature Photonics. 2014, 7, 506. [2] Quilettes DW, Vorpahl SM, Stranks SD, Nagaoka H, Eperon GE, Ziffer ME, Snaith HJ, Ginger DS. Science. 2015, 6235, 683. [3] Xu W, Liu Y, Huang X, Jiang L, Li Q, Hu X, Huang F, Gong X, Cao Y. J Mater Chem C. 2016, 10, 1953 133 P-29 Color-tunable microwave synthesis of cadimum-free ZnS:Cu nanocrystals and potential application for LEDs Kui Zhang1,2, #, Shengmei Chen1, Juan Antonio Zapien1, * Center of Super-Diamond and Advanced Films (COSDAF), Department of Physics and Materials Science, City University of Hong Kong, Kowloon, Hong Kong, China, 2 Institute of Intelligent Machines, Chinese Academy of Sciences, Hefei, Anhui 230031, China 1 Keywords: semiconductor nanocrystals; light-emitting diode; microwave irradiation; photoluminescence Energy-efficient lighting has offered a promising option for energy saving because artificial lighting globally consumes about 20% of the total electrical energy in the world. Environmentally friendly lightemitting diodes (LEDs) with higher efficiencies, longer lifetimes, and fast response times are considered as promising light sources to replace the traditional ones such as incandescent or fluorescent lamps. Semiconductor nanocrystals (NCs) as potential converters for LEDs exhibit high photoluminescence quantum yields (PL QYs), low scattering and good color saturation, compared to traditional phosphors. The NC-LEDs have been successfully demonstrated by employing the combination of red and green light- emitting CdSe NCs on blue InGaN/GaN LEDs. However, the toxicity of the cadmium element and the significant selfabsorption and energy transfer in closely packed NCs with small Stokes shifts potentially hinders their ultimate research transformation and commercialization. Thus, it is necessary to develop the ideal NCs with low toxicity, high PL QY, and color-tunable emissions for LEDs. We have synthesized copper-doped zinc sulfide nanocrystals (ZnS:Cu NCs) by using MPA (3mercaptoprop ionic acid) as the stabilizer under microwave irradiation. TEM, XRD and photoluminescence measurements were employed to study the structure and optical properties of the ZnS:Cu NCs, respectively. It was found that by varying the microwave irradiation times, the size of nanocrystal could be changed and the luminescence could be tuned continuously within the range from 500 to 595 nm. Importantly, the LED device were successfully fabricated by integration of yellow and blue-green ZnS:Cu NCs. The experimental results indicated low toxic ZnS:Cu NCs could be suitable for solid state lighting. 1.6 Natural light (a) 1.4 Normalized PL intensity 1.2 (b) 500 513 525 540 555 580 595 nm UV light 1.0 Microwave irradiation time (min) 5 0.8 10 20 30 0.6 45 60 120 0.4 0.2 0.0 400 450 500 550 600 Wavelength (nm) 650 700 Figure. Photoluminescent spectra of ZnS:Cu NCs with color emission, as-prepared NCs-based LED, and the color coordination of the spectrum on the CIE 1931 color space. Reference: 1. Knowles, KE; Hartstein, KH; Kilburn, TB; Marchioro, A; Nelson, HD; Whitham, PJ; Gamelin, DR. Chem. Rev. 116, 10820 (2016). 2. Jang, E; Jun, S; Jang, H; Lim, J; Kim, B; Kim, Y. Adv. Mater. 22, 3076 (2010). 3. Yuan, X; Hua, J; Zeng, RS; Zhu, DH; Ji, WY; Jing, PT; Meng, XD; Zhao, JL; Li, HB. Nanotechnology 25, 435202 (2014). # Presenting Author: [email protected] * Corresponding Author : [email protected] 134 P-30 Increase the stability of TADF based OLED by using modified carbazole with tert-butyl and phenyl Lian Duan*, Yunge Zhang # Key Lab of Organic Optoelectronics and Molecular Engineering of Ministry of Education, Department of Chemistry, Tsinghua University, Beijing, 100084, P. R. China Keywords: TADF based OLED, stability, lifetime, modified carbazole. As the third-generation light emitters for organic light emitting diodes (OLEDs), thermally activated delayed fluorescence (TADF) materials have shown the prospect of commercialization. Albeit their high efficiency, the lifetimes of the devices with TADF emitters are still far from satisfaction. Adopting electron donors and acceptors with good stability are vital to prepare stable TADF emitters, which is crucial to the OLEDs’ lifetime. One of the most common used electron donors is carbazole, while the 3, 6-position of the carbazole tend to occur dimerization, hindering the long-term stability of the TADF emitters. Here, we modified the TADF molecule 2CzPN by introducing inert tert-butyl and phenyl groups to the 3, 6-position of carbazoles (named 2tBuCzPN and 2PHCzPN, respectively), and improved OLED efficiency along with enhanced OLED stability were achieved simultaneously. The data of cyclic voltammetry showed that compared with 2CzPN, the electrochemistry stability of 2tBuCzPN and 2PHCzPN were improved. Besides, 2tBuCzPN and 2PHCzPN exhibited much shorter excited-state lifetimes in doped thin films, because the substituents on the donors affected the molecular energy levels of the first singlet (S1) and triplet (T1) excited states in different ways, decreasing the energy gap between S1 and T1 (△EST). The OLEDs based on 2tBuCzPN and 2PHCzPN achieved improved maximum external quantum efficiency (EQE) of 17.0% and 14.0%, respectively (8.5% for 2CzPN), and longer lifetime with T50 of 7.6 h and 13.4 h at 500 cd/m2, respectively (1.7 h for 2CzPN). 0.00005 0.00005 0.0000 2CzPN-1cycle 2CzPN-2cycle 2CzPN-3cycle 2CzPN-4cycle 2CzPN-5cycle -0.0001 Current (A) Current (A) Current (A) 0.00000 2tBuCzPN-1cycle 2tBuCzPN-2cycle 2tBuCzPN-3cycle 2tBuCzPN-4cycle 2tBuCzPN-5cycle -0.00005 -0.00010 -0.0002 -1 1 Voltage (V) 0.00000 2PHCzPN-1cycle 2PHCzPN-2cycle 2PHCzPN-3cycle 2PHCzPN-4cycle 2PHCzPN-5cycle -0.00005 -0.00010 2 -1.5 -1.0 -0.5 1.0 Voltage (V) 1.5 2.0 -1.5 -1.0 -0.5 1.0 Voltage (V) 1.5 2.0 Figure 1. The cyclic voltammetry spectrum of 2CzPN, 2tBuCzPNtBu, and 2PHCzPNPH. 100 DPEPO-20%2CzPN DPEPO-30%2tBuCzPN DPEPO-30%2PHCzPN 2 500cd/m 10 Normalized Intensity EQE (%) Luminance (%) 10 1.0 DPEPO-0.3 2CzPN DPEPO-0.3 GPH DPEPO-0.4 GTBU 2tBuCzPN-30% 2PHCzPN-30% 2CzPN-20% 0.8 0.6 0.4 0.2 0.0 1 100 1000 Brightness (cd/m2) 1 10000 0 10 20 30 40 50 60 70 300 Time (h) 400 500 600 700 800 Wavelength (nm) Figure 2. The B-EQE, lifetime curve, and EL spectrum of 2CzPN, 2CzPNtBu, and 2CzPNPH. Table 1. The performance data of OLEDs. EQE Host:DPEPO Von PE EQE V PE λmax T50 500cd/m2 1000cd/m2 max 20%2CzPN 8.5% 5.5V 10 lm/W 4.1% 11.6V 2.7 lm/W 494nm 1.66h 30%2tBuCzPN 17% 4.2V 29 lm/W 7.7% 8.6V 8.3 lm/W 518nm 7.6h 30%2PHCzPN 14% 3.8V 33 lm/W 10% 9V 11 lm/W 532nm 13.4h 135 P-31 Hierarchical composite structure of few-layers MoS2 nanosheets supported by vertical graphene on carbon cloth for lithium ion battery and hydrogen evolution reaction electrodes Zhenyu Zhang, # Wenjun Zhang* Center of Super-Diamond and Advanced Films (COSDAF), and Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, People’s Republic of China. * [email protected] Keywords: Vertical graphene, few-layers MoS2 nanosheets, carbon cloth, hydrogen evolution reaction A hierarchical composite structure composed of few-layers molybdenum disulfide nanosheets supported by vertical graphene on conductive carbon cloth (MDNS/VG/CC) for high-performance lithium ion battery and electrochemical hydrogen evolution reaction (HER) is demonstrated in this work. In the fabrication, 3D vertical graphene is first prepared on carbon cloth by a micro-wave plasma enhanced chemical vapor deposition (MPCVD) and then few-layers MoS2 nanosheets are in-situ synthesized on the surface of the vertical graphene through a simple hydrothermal reaction. The vertical graphene can effectively increase conductivity and holding active material on current collector, contributing much better cycling performance than the electrode that without graphene. On the other side, this integrated catalyst exhibits an excellent HER electrocatalytic activity including an onset potential of 50 mV, an overpotential at 10 mA cm-2 (η10) of 78 mV, a Tafel slop of 53 mV dec-1, and an excellent cycling stability in acid solution. The excellent electrochemical performance on both sides can be ascribed to the abundant active edges provided by the vertical MoS2 nanosheets, the effective electron transport route provided by the graphene arrays on the conductive substrate and it offers robust anchor sites for MoS2 nanosheets and appropriate intervals for electrolyte infiltration. # Presenting Author Corresponding Author * 136 P-32 A Dual-Ion Battery Constructed with Aluminum Foil Anode and Mesocarbon Microbead Cathode in an Ionic Liquid Electrolyte Fan Zhang1,2,#, Bifa Ji2, Xuefeng Tong2, Maohua Sheng2, Yongbing Tang2,*, Chun-Sing Lee1,* Department of Physics and Materials Science, Center of Super-Diamond and Advanced Films (COSDAF), City University of Hong Kong, Hong Kong, SAR, China, 2 Functional Thin Films Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen 518055, China 1 Keywords: dual-ion battery, aluminum foil anode, mesocarbon microbead cathode, ionic liquid, alloying/intercalation. With the expansion of the market of portable electronics and electric vehicles, it is imperative to develop new-generation batteries with high performances. Dual-ion battery (DIB) has been proposed as a novel energy storage device with the merits of high safety and environmental friendliness over conventional lithium-ion batteries. The main difference of working mechanism between DIB and LIB is that both cations (typically Li+) and anion (such as PF6-) are involved in such DIB for charge transportation and storage, while conventional LIB involves only Li+ ion. Recently, we reported a novel DIB using an aluminum foil as anode which also enables the elimination of additional metal current collector and leads to further energy density enhancement and cost saving.[1] However, similar to most of DIBs, its cycling stability is still limited by decomposition of the organic electrolyte due to the high working voltages of DIBs. Additionally, organic solvents in the electrolyte can also co-intercalate into the graphite cathode forming Cn+(solv)yX−,[2] resulting in graphite exfoliation upon cycling. Herein, we report a novel dual-ion battery constructed with aluminum foil anode and mesocarbon microbead cathode (Al-MCMB) in an ionic liquid electrolyte with significantly enhanced cycling stability and rate performance. It was found that the Al-MCMB DIB has a reversible capacity of 98 mAh g-1 after 300 cycles at 0.5 C with negligible capacity decay at a high cut-off voltage of 4.8 V. More importantly, the energy density of the packaged cell is estimated up to 221 Wh kg-1 at the power density of 109 W kg-1 and remains 185 Wh kg-1 at 1141 W kg-1, among the best performance of DIBs. Fig.1 Schematic illustration of charge/discharge processes of the dual-ion battery using Al foil as anode and MCMB as cathode based on an ionic liquid electrolyte. References: [1] X. L. Zhang, Y. B. Tang, F. Zhang, C.-S. Lee, A novel aluminum-graphite dual-ion battery, Adv. Energy. Mater. 2015, 6, 1502588. [2] J. A. Read, A. V. Cresce, M. H. Ervin, K. Xu, Dual-graphite chemistry enabled by a high voltage electrolyte, Energy Environ. Sci. 2014, 7, 617. # Presenting Author: Fan Zhang *Corresponding Author: Chun-Sing Lee ([email protected]) and Yongbing Tang ([email protected]) 137 P-33 Epitaxy of Layered Orthorhombic SnS-SnSxSe(1-x) Core-Shell Heterostructures with Anisotropic Photoresponse Jing Xia and Xiang-Min Meng Key Laboratory of Photochemical Conversion and Optoelectronic Materials, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, 100190, P. R. China E-mail: [email protected] Keywords: physical vapor deposition, epitaxy, layered materials, heterostructure, anisotropic photoresponse Heterostructures are important functional units for modern electronic and optoelectronic devices such as bipolar transistors, light-emitting diodes, laser diodes, and photovoltaic cells.[1-4]In this talk, I will report synthesis of layered orthorhombic SnS-SnSxSe(1-x)core-shell heterostructures with well-defined geometry viaatwo-step thermal evaporation method.[5] Structural characterization reveals that the heterostructures of SnS-SnSxSe(1-x) are inplaneinterconnected and vertically stacked, constructed by SnSxSe(1-x) shell heteroepitaxially growing on/around the pre-synthesized SnS flake with an epitaxial relationship of (303)SnS//(033)SnSxSe(1-x), [010]SnS//[100]SnSxSe(1-x). On the basis of detailed morphology, structure and composition characterizations, a growth mechanism involving heteroepitaxial growth, atomic diffusion, as well as thermalthinning is proposed to illustrate the formation process of the heterostructures. In addition, a strong polarization-dependent photoresponse is found on the device fabricated using the as-prepared SnS-SnSxSe(1-x) core-shell heterostructure, enabling the potential use of the heterostructuresas functional components for optoelectronic devices featured with anisotropy. References: [1] [2] [3] [4] [5] H. Kroemer, P. IEEE. 1982, 70, 13. S. Nakamura, M. Senoh, T. Mukai, Appl. Phys. Lett. 1993, 62, 2390. J. Faist, F. Capasso, D. L. Sivco, C. Sirtori, A. L. Hutchinson, A. Y. Cho, Science 1994, 264, 553. J. Schrier, D. O. Demchenko, L. W. Wang, Nano Lett. 2007, 7, 2377. J. Xia, D. D. Zhu, X. Z. Li, L. Wang, L. F. Tian, J. Li, J. Y. Wang, X. Huang, X. M. Meng, Adv. Funct. Mater. 2016. 26. 4673-4679. 138 List of Participants 139 LIST OF PARTICIPANTS Last Name ADACHI ALI BAO BIAN CAO CHAN CHAN CHANG CHELORA VEETIL CHEN CHEN CHEN CHEN CHEN CHEN CHEN CHEN CHENG CHENG CHENG CHO CHOI CHU CUI CUI DAI DUAN FENG GAO GAO GONG HAN HE HE HE HE HE HU HU HU HUANG HYEON IMAHORI JEN JEONG JIANG JIANG KIM KIM KIM KOBAYASHI KOCH LAN LAN LEE First Name Chihaya Asgher Syed Bob Haidong Ke Chiu Yee Rocky Ka Lok Ching-Hsiang Jipsa Chin-Ti Hongzheng Hui-Lung Rui Shengmei Wen-Cheng Xiaodong Ziming Huiming Junye Yuanhang Kilwon Yeon Jun Fanghui Jiang Yi Zhihui Lian Ling Feng Libo Xiong Dong Bin Jr-Hau Le Z.R. Ryan Zhubing Bin Junqing Xiaoqing Yuan Taeghwan Hiroshi K-Y (Alex) Jun Hui Qing-Song Yang Jang kyo Kwang-Burn Young-Hwan Masayuki Norbert Danni Minhuan Chris Email [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] LEE Chun-Sing [email protected] LEE LEE Pui Kit Tae-Woo [email protected] [email protected] 140 Abstract Code Plenary3.1, 4.3.2 8.1.4, P-01 -5.3.1, P-04 -P-02 -P-03 -4.3.3 7.1.1 P-05 -P-29 6.1.2, P-06 4.2.1 P-07 1.3.1 -P-08, P-16 8.1.1 P-09 -5.2.2 Plenary1.1 6.3.2 4.1.1, 6.1.3, P-30 -8.1.2 P-10 4.3.1, P-28 --2.1.3, P-11 7.2.1 -3.3.2 6.1.1 7.2.2 P-34 -Plenary1.2 1.1.3 3.3.3 P-12 -4.1.2 2.3.2, 5.2.2, P-27 5.3.2, P-09, P-12, P-14 P-14 -3.1.2, 3.3.4 4.2.3, P-15 --4.2.4, 5.1.2, 6.1.2, P-02, P-06, P-16, P-32 5.2.1 3.3.1 Last Name LI LI LI LI LI LI LI LIANG LIN LIU LIU LIU LIU LIU LO LU LU LU LUO MA MA MAI MENG NAM NG OPITZ PAN QIN SHE SHEN SHIU SHRESTHA SO SONG SONG SONG SU SUN SUN TAM TANG TANG TANG THACHOTH CHANDRAN TIAN TONG TONG TSANG TSE TSUI TUNG VOLLMER WAN WANG WANG WANG WANG WANG WANG WANG WANG First Name Ho-Wa Huan-Huan Lain-Jong (Lance) Ning Quan Yangyang Yongfang Duoduo Zhiqun Bin Kevin Xiao-Ke Yunqi Bin Ming Fai Raymond Jian Xiaoying Yang Yinqi Chunqing Dongxin Liqiang Xiangmin Chunghee Tsz Wai Karen Andreas Xiao-Qing Chuanjiang Sandy Dong Yi-Jiun Lok Kumar Franky Li Weiguo Xiaoxue Zisheng Qian Xinying Ho Wan Jianxin Yongbing Zhiyong Email [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] Abstract Code P-08, P-16 5.2.3, P-17 1.2.1 P-01 4.2.3, P-15, P-24 5.3.1 8.1.3 -8.2.3 3.2.4 -5.1.2 2.1.1 P-18 P-02 1.3.2 6.2.3 P-10 P-19 -6.1.3 5.3.3 P-33 P-20 P-02 3.1.2 6.3.1 4.3.2 --P-21 1.2.3 3.1.1 1.3.3 3.2.3 P-22 ----4.1.3, P-13 4.2.4, P-32 3.2.1 Hrisheekesh [email protected] P-02 Yayuan Qing-Xiao Rui Sai-Wing Stephen Cheuk Hin Ace Wai Ching Wilson Chen-Ho Antje Lijun Aiwu Chunru Dan Hui Pengfei Wenhui Xun Yiwen [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] -6.1.2 -P-08, P-16 --Plenary2.1, P-18 P-23 Plenary4.1 -3.1.4 2.3.1 -5.1.3 P-15, P-24 2.2.2 P-25 141 Last Name WANG WEI WEI WONG WONG WONG WU WU XIAO XIE XIE XIN XU YAN YAN YANG YAO YAO YAO YAO YIN YIP YONG YOO YU YUEN ZAPIEN ZENG ZETTSU ZHAN ZHANG ZHANG ZHANG ZHANG ZHANG ZHANG ZHANG ZHANG ZHANG ZHANG ZHANG ZHANG ZHAO ZHAO ZHAO ZHENG ZHI ZHONG ZHU ZHU ZHU 142 First Name Ying Jian Zhixiang Fulung Ken-Tsung Wai-Yeung Raymond Chung-Chih Shuilin Xufen Yusheng Zengqi Caroline Jun Feng He Shihe Chenyi Huiying Shanshan Xiang Longwei Hin-Lap Angus Kijung Seunghyup Denis Muk Fung Juan Antonio Shanshan Nobuyuki Yawen Changjun Alex Fan Hua Jiaolong Jing-Ping Kui Qichun Rui Wen-Jun Xiaolu Yunge Zhenyu Fuwen Huijun Shaojing Zijian Chunyi Xinhua Daoben Furong Jia Email [email protected] [email protected] [email protected] [email protected] [email protected] Abstract Code 5.1.3 P-13 7.1.2 -3.1.3, 4.1.4 [email protected] 1.1.1 [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] [email protected] 4.1.4, P-03, P-21 -5.3.1 -7.1.3, P-19 -6.3.3 2.1.2 8.2.4 4.3.4 -P-26 P-27 P-28 4.2.2 1.1.2, P-07 2.2.1 5.1.1 5.2.1. P-04 P-04 P-29 5.3.1 6.2.2 5.3.1, P-04 -4.2.4, P-32 1.2.2 -5.2.3, P-17 P-29 6.2.1 -2.3.3, P-18, P-31 -P-30 2.3.3, 7.2.2, P-31 3.1.4 2.2.3 -7.2.3 5.2.4 8.2.1 Plenary3.2 3.1.5, 8.1.3, P-01, P-25 3.2.2, P-26 Notepapers 143 Notepapers 144 Notepapers 145 Notepapers 146 Notepape 147 Notepapers 148
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