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dc.contributor.authorShieh, Ji-Tingen_US
dc.contributor.authorLiu, Chiou-Huaen_US
dc.contributor.authorMeng, Hsin-Feien_US
dc.contributor.authorTseng, Shin-Rongen_US
dc.contributor.authorChao, Yu-Chiangen_US
dc.contributor.authorHorng, Sheng-Fuen_US
dc.date.accessioned2014-12-08T15:07:02Z-
dc.date.available2014-12-08T15:07:02Z-
dc.date.issued2010-04-15en_US
dc.identifier.issn0021-8979en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.3327210en_US
dc.identifier.urihttp://hdl.handle.net/11536/5514-
dc.description.abstractThe microscopic states and performance of organic solar cell are investigated theoretically to explore the effect of the carrier mobility. With Ohmic contacts between the semiconductor and the metal electrodes there are two origins of carriers in the semiconductor: the photocarriers generated by photon absorption and the dark carriers diffused from the electrodes. The power efficiency of the solar cell is limited by the recombination of a carrier with either the photocarrier or a dark carrier. Near the short-circuit condition the photocarrier recombination in the semiconductor bulk decreases as the mobility increases. Near the open-circuit condition the dark carrier recombination increases with the mobility. These two opposite effects balance with one another, resulting in an optimal mobility about 10(-2) cm(2)/V s which gives the highest power conversion efficiency. The balance of the electron and hole mobilities are not necessary to maintain the optimal efficiency also because of the balance of the photocarrier and dark carrier recombination. The efficiency remains about the same as one carrier mobility is fixed at 10(-2) cm(2)/V s while the other one varies from 10(-1) to 10(-3) cm(2)/V s. For solar cell with a Schottky barrier between the semiconductor and the metal electrode there is no dark carrier recombination. The efficiency therefore always increases with the mobility. (C) 2010 American Institute of Physics. [doi: 10.1063/1.3327210]en_US
dc.language.isoen_USen_US
dc.titleThe effect of carrier mobility in organic solar cellsen_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.3327210en_US
dc.identifier.journalJOURNAL OF APPLIED PHYSICSen_US
dc.citation.volume107en_US
dc.citation.issue8en_US
dc.citation.epageen_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000277303200107-
dc.citation.woscount34-
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