4 th Hybrid and Organic Photovoltaic Conference -Uppsala 2012 43 B10 - On the correlation between crystallinity and photophysics for donor polymers of interest for organic photovoltaic devices Ying Woan Soon, Safa Shoaee, Iain McCulloch, James R Durrant Imperial College London, Chemistry department, South Kensington campus, London, SW7 2AZ, GB Crystalline materials have been widely reported to give good charge carrier mobilities which can enhance charge transport.(1-2) Hence, in the field of OPV and OLED, highly crystalline materials have been considered as favourable for obtaining efficient devices. However, the fluorescence quenching associated with the process of ‘concentration quenching’ has been observed to be more efficient in crystalline materials.(3-4) This fluorescence quenching process is thought to be related to faster internal conversion, leading to a potential loss of device efficiency. In this study, photophysical properties of a range of conjugated donor-acceptor polymers with varying crystallinity are investigated using techniques including wide angled x-ray diffraction, single photon counting, and transient absorption spectroscopy (TAS). The more crystalline polymers are found to have shorter singlet and triplet lifetimes compared to the more amorphous polymers. This is consistent with the lack of triplet observation upon photoexcitation of the more crystalline polymers while high triplet yields are usually found in the amorphous polymers using microsecond TAS. Although amorphous polymers typically have lower charge mobilities than the more crystalline polymers, the longer singlet and triplet lifetimes of the amorphous polymers can potentially aid charge separation. Therefore, both the highly crystalline and amorphous polymers have different attributes that can compromise on the performance of OPV devices. Furthermore, the yield of polaron photogeneration in neat polymer films is found to be maximum in the semi-crystalline polymers. Recent high performing polymers in the literature such as poly[[4,8-bis[(2-ethylhexyl)oxy]benzo[1,2-b:4,5-b']dithiophene-2,6-diyl][3-fluoro-2-[(2ethylhexyl)carbonyl]thieno[3,4-b]thiophenediyl]] (PTB7) and poly[N-9”-hepta-decanyl-2,7carbazole-alt-5,5-(4’,7’-di-2-thienyl-2’,1’,3’-benzothiadiazole)] (PCDTBT) are found to be semicrystalline in our context. This finding can have direct implication on the future design of conjugated polymers for use in organic solar cells. References [1] Ma, W.; Yang, C.; Gong, X.; Lee, K.; Heeger, A.J. "Thermally Stable, Efficient Polymer Solar Cells with Nanoscale Control of the Interpenetrating Network Morphology".Adv.Funct.Mater.15, 1617-1622 (2005) [2] Mihailetchi, V.D.; Xie, H.X.; De Boer, B.; Koster, L.J.A.; Blom, P.W.M. "Charge transport and photocurrent generation in poly (3-hexylthiophene): Methanofullerene bulk-heterojunction solar cells".Adv. Funct. Mater. 16, 699-708 (2006) [3] Huignard, A.; Gacoin, T.; Boilot, J-P. "Synthesis and Luminescence Properties of Colloidal YVO4:Eu Phosphors".Chem. Mater.12,1090-1094 (2000) [4]Huang, H.; Xu, G.Q.; Chin, W.S.; Gan, L.M.; Chew, C.H."Synthesis and characterisation of Eu:Y2O3 nanoparticles". Nanotechnology 13, 318-323 (2002) © SEFIN 2012
4 th Hybrid and Organic Photovoltaic Conference -Uppsala 2012 44 B11 - Effect of crystallinity in P3HT:PCBM solar cells on bandgap trap states and apparent recombination order Donato Spoltore a , Wibren D. Oosterbaan a , Samira Khelifi b , John Clifford c , Aurelien Viterisi c , Emilio Palomares c , Marc Burgelman b , Laurence Lutsen a , Dirk Vanderzande a , Jean Manca a a, Institute for Materials Research (IMO-IMOMEC), Universiteit Hasselt, Wetenschapspark 1, Diepenbeek 3590, Belgium b, Department of Electronics and Information Systems (ELIS), University of Gent, Sint-Pietersnieuwstraat 41, Gent 9000, Belgium c, Institute of Chemical Research of Catalonia (ICIQ), Avda. Països Catalans 16, Tarragona 43007, Spain d, Institut Català de Recerca I Estudis Avançats (ICREA), Avda. Lluís Companys 23, Barcelona 80810, Spain In this work we investigate how varying the polymer crystalline fraction in nanofiber- P3HT:PCBM solar cells influences bandgap trap states and apparent recombination order. The recombination of charge carriers in polymer-fullerene solar cells is generally considered to be a second order non-geminate process. 1,2 It depends on the concentration of free electrons and free holes in the device through a recombination constant, which is proportional to the mobility. In the last few years recombination orders higher than two were found in P3HT:PCBM solar cells. 3-5 The most accepted explanation for this phenomenon stems from a multiple trapping model 6,7 which considers the recombination as a second order process with a recombination constant depending on the concentration of charge carriers. This is due to the dependence of mobility on the charge-carrier density caused by the presence of a tail of trapped states inside the gap: 8 the higher the number of traps the slower the mobility and the higher the apparent recombination order. In this work we varied, by temperature control of the nanofibers-P3HT casting dispersion, 9,10 the mass fraction of highly crystalline nanofibrillar P3HT to the total P3HT content in P3HT:PCBM solar cells. We show a clear correlation between the fraction of crystalline P3HT nanofibers, the apparent recombination order (measured with a transient photovoltage technique) 5,11 and the amount of traps in the bandgap (measured with an admittance spectroscopy technique). 12 References [1] Langevin, P. "Recombinaison et Mobilités des Ions dans les Gaz." Ann. Chim. Phys. 28, 433–530 (1903). [2] Pope, M.; Swenberg, C. E. "Electronic processes in organic crystals and polymers", Oxford University Press, USA, (1999). [3] Juška, G.; Genevičius, K.; Nekrasas, N.; Sliaužys, G.; Dennler, G. "Trimolecular recombination in polythiophene: fullerene bulk heterojunction solar cells". Appl. Phys. Lett. 93, 143303 (2008). [4] Deibel, C.; Baumann, A.; Dyakonov, V. "Polaron recombination in pristine and annealed bulk heterojunction solar cells". Appl. Phys. Lett. 93, 163303 (2008). [5] Shuttle, C. G.; O’Regan, B.; Ballantyne, A. M.; Nelson, J.; Bradley, D. D. C.; De Mello, J.; Durrant, J. R. "Experimental determination of the rate law for charge carrier decay in a polythiophene: Fullerene solar cell". Appl. Phys. Lett. 92, 093311 (2008). [6] Nelson, J. "Diffusion-limited recombination in polymer-fullerene blends and its influence on photocurrent collection". Phys. Rev. B 67, 155209 (2003). [7] Shuttle, C. G.; O’Regan, B.; Ballantyne, A. M.; Nelson, J.; Bradley, D.; Durrant, J. R. "Bimolecular recombination losses in polythiophene: Fullerene solar cells". Phys. Rev. B 78, 113201 (2008). [8] Shuttle, C. G.; Hamilton, R.; Nelson, J.; O'Regan, B. C.; Durrant, J. R. "Measurement of Charge-Density Dependence of Carrier Mobility in an Organic Semiconductor Blend". Adv. Funct. Mater. 20, 698–702 (2010). [9] Bertho, S.; Oosterbaan, W. D.; Vrindts, V.; D’Haen, J.; Cleij, T. J.; Lutsen, L.; Manca, J.; Vanderzande, D. "Controlling the morphology of nanofiber-P3HT:PCBM blends for organic bulk heterojunction solar cells". Organic Electronics 10, 1248–1251 (2009). [10] Bertho, S.; Oosterbaan, W. D.; Vrindts, V.; Bolsée, J.-C.; Piersimoni, F.; Spoltore, D.; D’Haen, J.; Lutsen, L.; Vanderzande, D.; Manca, J. V. "Poly (3-alkylthiophene) Nanofibers for Photovoltaic Energy Conversion". Adv. Mater. Res. 324, 32–37 (2011). [11] O'Regan, B. C.; Scully, S.; Mayer, A. C.; Palomares, E.; Durrant, J. "The Effect of Al 2O 3Barrier Layers in TiO 2/Dye/CuSCN Photovoltaic Cells Explored by Recombination and DOS Characterization Using Transient Photovoltage Measurements". J. Phys. Chem. B 109, 4616–4623 (2005). [12] Khelifi, S.; Decock, K.; Lauwaert, J.; Vrielinck, H.; Spoltore, D.; Piersimoni, F.; Manca, J.; Belghachi, A.; Burgelman, M. "Investigation of defects by admittance spectroscopy measurements in poly (3- © SEFIN 2012
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