Efficiency enhancement of solution processed single layer blue phosphorescent organic light emitting diodes by using Polyethylene glycol mono [4-(1,1,3,3tetramethylbutyl)phenyl] ether (Triton X-100) K.H. Yeoh1,a), K.L. Woon1,b) 1 Department of Physics, Faculty of Science, University Malaya, 50603 Kuala Lumpur, Malaysia Abstract We report on the efficiency enhancement of solution processed single layer blue phosphorescent organic light emitting diodes (PhOLED) by blending Triton X-100 into the electroluminescne (EL) layer. With 3.2wt% Triton X-100 blending, the power efficiency of the device can reach 8.5lm/W at brightness of 1000cd/m2, which corresponds to 2-fold increament compared to the similar PhOLED without Triton X-100 doping. The efficiency enhancement is attributed to the interfacial interaction between Al and the Triton X-100 which lowers the cathodic barrier injection of the PhOLED. Keyword: Organic light emitting diodes, Triton X-100 (2 li 1. INTRODUCTION Organic light emitting (OLED) diodes have attracted much attention lately due to its potential applications for large panel display and solid state lightings. Compared to vaccum deposition method, solution processed method is more promising because of its lower fabrication cost and compatibility of roll-to-roll processing. However this progress is heavily relied on the development of blue OLED because typically blue OLED has lower lifetime and efficiency due to the wide bandgap host that is required for the commonly used phosphorescent blue dopant e.g. Bis(4,6-difluorophenylpyridinato-N,C2)picolinatoiridium (FIrpic). Several groups have developed multi layer solution processed blue OLED that yield efficiency of 9 to 10lm/W at 1000cd/m2 [1,2]. In contrast to single layer OLED, the fabricating solution processed multi layer OLED is very challenging and high cost. The top layer need to form orthogonal film with the underneath layer. To date the development of multi layer OLED using wet process is fairly slow mainly hampered by the intermixing of the bottom layer with the top subsequent layer. For lighting application, a simple and low cost solution processed single layer OLED is highly desirable. In this paper, we report that high efficiency solution processed single layer PHOLED can be achieved by blending Triton X-100 as shown in Figure 1 into the EL layer. Our device shows 2 fold increament of luminous efficacy compared to the similar device without Triton X100 doping. i ) weight ratio (PVK:OXD-7:FIrpic:Triton X-100) where X is varied from 0 to 10. The EL layer was spin coated on to the PEDOT:PSS coated substrates to give a 70nm thick film and then baked at 80°C for 30 minutes. Following that, 1nm of Cs2CO3 and 100nm Al was vacuum deposited at base pressure of 2X10-6 mbar without breaking the vacuum. All the devices were encapsulated using UV curable epoxy and glass lid purchased from Ossila. The devices current density- voltage-luminance characteristics were measured using Konica Minolta Cs-200 and Keithley 276 source meter. Photocurrents of OLED were measured under illumination of a simulated AM1.5 light source at 100mW/cm2. Figure 1: Chemical structure of Triton X-100. The current density and brightness -applied voltage curve is shown in Figure 2. It is clearly shown that the current injection increases with Triton X-100 doping concentration. 2. EXPERIMENTAL AND RESULTS Indium tin oxide (ITO) coated glass substrates with sheet resistance 25Ω/□ were patterned using standard lithography method. The substrates were ultrasonically cleaned DI water, acetone, IPA and DI water for 10mintues, followed by oxygen plasma treatment for 5minutes. Next 50nm of poly(ethylenedioxythiophene):polystyrenesulfonate (PEDOT:PSS) (H. C. Starck, Clevios P VP Al 4083) was spin coated on the substrates and immediately baked in N2 environment for 7 minutes at 150°C. The chlorobenzne dissolved EL layer consists of poly(vinylcarbazole) ( PVK), 1,3-bis[(4-tertbutylphenyl) -1,3,4 oxidiazolyl] phenylene (OXD-7), FIrpic and Triton X-100, blended in 100:40:10:X a) b) Presenting author: [email protected] Corresponding author: [email protected] Figure 2: Current density, brightness – voltage (J-V) of blue PhOLED with Triton X-100 concentrations varied from 0wt% to 10wt% With 3.2wt% Triton X-100 doping, the device turn on voltage reduces to 3.5V at 1cd/m2 as shown in Figure 2. Figure 3 shows the power efficiency of the blue PhOLED at different brightness. The optimum Triton X-100 doping was 3.2wt% which gave 8.5lm/W at 1000cd/m2. The device efficiency varied between 7lm/W to 8.7lm/W from 100cd/m2 to 2500cd/m2. This variation is considerably small compared to the best solution processed single layer blue PhOLED device reported to date [3]. The efficiency enhancement is due to the interaction of lone pair oxygen atoms in Triton X-100 with Al which lead to the formation of Al3+ and consequently excessive negative charge is released at the cathode- emitting layer interface. These results in the formation of dipole at the cathode interface which effectively lower the cathode barrier for electron injection [4]. Figure 3: Power efficiency-brightness of the PhOLED with different concentrations of Triton X-100 doping. Figure 4: Photovoltaic characteristic of the blue PhOLED at 0wt% and 3.2wt% TritonX-100 doping. We measured the OLED’s photovoltaic response [3] and found that the open circuit voltage (VOC) for 3.5% TritonX doping is about 0.4V higher than the VOC of the control device as shown in Figure 4. This shows that Triton X100 has lower the effective work function of the cathode, which eases the electron injection. 3. SUMMARY In summary, we have demonstrated that the efficiency of a single layer solution processed blue PhOLED can be significantly enhanced by using a simple and low cost method by means of Triton X-100 doping. The efficiency enhancement is attributed to the dipole formation at the cathode interface due to the interaction of the lone pair oxygen atoms in the Triton X-100 with Al cathode. This simple and cost effective method will pave way towards large scale manufacturing of OLED for display and lighting applications. 4. REFERENCES 1. K. S. Yook , S. E. Jang , S. O Jeon , and J. Y. Lee, Adv. Mater. 22, 4479–4483 (2010). 2. E. Ahmed, T. Earmme and S.A. Jenekhe, Adv. Funct. Mater. 21, 3889–3899 (2011). 3. L. Li, J. Liu, Z. Yu, and Q. Pei, Appl. Phys Lett. 98, 201110 (2011). 4. X. Y. Deng, W. M. Lau, K. Y. Wong, K. H. Low, H. F. Chow and Y. Cao, Appl. Phys. Lett. 84, 3522-3524 (2004).
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