22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Nanoparticles jet deposition of silicon, silicon-carbon and titania hierarchical nano-structures for energy applications G. Nava1,2, F. Fumagalli2 and F. Di Fonzo2 1 2 Dipartimento di Fisica, Politecnico di Milano, Piazza Leonardo da Vinci 32, 20133, Milan, Italy Center for Nano Science and Technology @PoliMI Istituto Italiano di Tecnologia, Via Giovanni Pascoli 70/3, 20133 Milan, Italy Abstract: A novel high rate and large area plasma based physical vapour deposition technique is presented for the fabrication of silicon, silicon-carbon and titania nanostructures for application in next generation lithium ion batteries and solar cells. The process, named Nanoparticles Jet Deposition (Nano-JeD), exploits the combination of a dusty non thermal plasma stage environment, providing ultra-high throughput, and a supersonic inseminated jet. Keywords: PECVD, supersonic nanoparticle inseminated jet, high rate, large area 1. General In the last decade the fields of energy production via renewable energy sources and effective energy storage represent very active areas of research. In the former field, dye sensitized solar cells (DSC) and nanocrystalline silicon thin films solar cells have been widely studied as promising and economical PV technology. In the first case, as proved by several experimental studies, enhanced performances compatible with commercial applications are achieved with the use of nanostructured materials, increasing the specific surface available for photoelectrochemical reactions, charge collection and charge transport, whereas for nanocrystalline silicon solar cells the lack of high rate production technique represent the main issue hindering a technological breakthrough [1, 2]. In the field of energy storage lithium-ion batteries are widely considered the most mature technology (long cycle life, high gravimetric and volumetric density), though still insufficient to fulfil the requirements for demanding applications, such as Pure Electic or Hybryd vehicles [3]. In the last few years intense research efforts have thus been invested in the development of new high capacity anode materials in order to boost the performances of this technology. Silicon – low cost and earthly abundant – has the highest theoretical capacity (4200 mAh/g) among the studied materials and represents the most appealing alternative to the commercially widespread graphite anodes (372 mAh/g) [4]. In particular the use of silicon nanostructures, composed by aggregates below the critical size for crack propagation (300 nm) and with an optimized system of voids to withstand the volume change upon lithiation (up to 300%), combined with carbon coatings that increase the stability of the solid electrolyte interface (SEI) has been proved by several works to be a suitable strategy to obtain superior cyclability and storage capacity [4-6]. The production of these optimized anode structures usually P-II-5-25 relies on complex multistep and low yield (45 mg/h) chemical synthesis methods, not suitable for large scale applications [7]. In the present work a novel large area (100 cm2), high yield (up to 200 mg/h) plasma-based deposition technique – named Nanoparticles Jet Deposition (NANO JeD) – is presented for single process fabrication of silicon, composite silicon-carbon and titania nanostructured materials, for application in lithiuim ion batteries anodes and dye sensitized solar cells phoanodes respectively. Gas phase self-assembled nanostructured films are obtained by coupling PECVD technique and nanoparticles inseminated sonic jet technique in a single reactor design. This novel process is based on the segmentation of the gas phase material synthesis in two separate steps: (i) precursor dissociation chemistry control in a non-thermal dusty plasma environment, allowing low temperature crystallization (mainly controlling over hydrogen dilution and coupled radiofrequency power in the discharge) and narrow size distribution synthesis of nanoclusters (controlled by the gas residence time in the discharge) [8]; (ii) nanoparticles nucleation and aggregation control by means of a sonic jet. The morphological properties of synthetized films range from aerogels through ordered dendritic nanostructures to compact films by controlling plasma process parameters and aerosol gas dynamic of the sonic jet flow field. Dense nanocrystalline silicon films are fabricated at high troughtput, exploiting the low temperature crystallization crystallization process preoviuosly discussed. Results concerning the control over silicon crystalline fraction and nanocrystals size tuning are presented. A nano-composite lithium ion battery anode (see Fig. 1. left), is fabricated, comprising of a bottom layer of hydrogenated carbon to improve the electrical contact and adhesion to the copper collector, an intermediate layer of hydrogenated amorphous silicon with a tree-like 1 nanostructured morphology for optimal volume adjustment upon swelling, and a top layer of hydrogenated carbon for the SEI stabilization. The nanocomposite anode is synthetized by alternating the use of acetylene (C 2 H 2 ) as the carbon precursor and silane (SiH 4 ) as the silicon precursor, all performed in an argon plasma. Preliminary characterizations of the above described design are presented. TiO 2 photoanodes (see Fig. 1 right) consisting of anatase single crystals assembled in quasi 1-D arrays of high aspect ratio hierarchical mesostructures are fabricated onto the F-doped SnO covered glass surfaces by self-assembly from the gas phase. Structural and morphological characteristics of TiO 2 nanostructured photoanodes can be optimized to achieve simultaneously high specific surface area for optimal dye uptake and broadband light scattering. As an example of the efficacy of the new process, we present the results of the first functional tests on DSC. [2] [2] [3] [4] [5] [6] Fig. 1. Left: Composite carbon-silicon-carbon material for application in lithium ion batteries anodes. Right: Nanostructured titania photoanode for application in dye sensitized solar cells. 2. References [1] L. Passoni, F. Ghods, P. Docampo, A. Abrusci, J. Martí-Rujas, M. Ghidelli, G. Divitini, C. Ducati, 2 [7] [8] [9] M. Binda, S. Guarnera, A. Li Bassi, C. Casari, H.J. Snaith, A. Petrozza and F. 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