% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Kirchartz:16868,
author = {Kirchartz, T. and Pieters, B. E. and Kirkpatrick, J. and
Rau, U. and Nelson, J.},
title = {{R}ecombination via tail states in polythiophene:fullerene
solar cells},
journal = {Physical review / B},
volume = {83},
number = {11},
issn = {1098-0121},
address = {College Park, Md.},
publisher = {APS},
reportid = {PreJuSER-16868},
pages = {115209},
year = {2011},
note = {The authors would like to thank K. Taretto and M. Soldera
(Uni. Neuquen) for discussion and inspiration in the early
stage of the work and C. Shuttle (UCSB) and J. Durrant
(Imperial College) for sharing the experimental data. In
addition, we want to thank R. Mackenzie, G. Dibb, A.
Maurano, and D. Credgington (Imperial College) for fruitful
discussions on modeling and charge extraction. T. K.
acknowledges partial support by an Imperial College Junior
Research Fellowship. J. N. acknowledges the support of the
UK Engineering and Physical Sciences Research Council
through the Supergen (EP/031088/1) and Nanotechnology Grand
Challenges (EP/F056710/1, EP/F056389/1) programmes.},
abstract = {State-of-the-art models used for drift-diffusion
simulations of organic bulk heterojunction solar cells based
on band transport are not capable of reproducing the voltage
dependence of dark current density and carrier concentration
of such devices, as determined by current-voltage and
charge-extraction measurements. Here, we show how to
correctly reproduce this experimental data by including an
exponential tail of localized states into the density of
states for both electrons and holes, and allowing
recombination to occur between free charge carriers and
charge carriers trapped in these states. When this
recombination via tail states is included, the dependence of
charge-carrier concentration on voltage is distinctly
different from the case of band-to-band recombination and
the dependence of recombination current on carrier
concentration to a power higher than 2 can be explained.},
keywords = {J (WoSType)},
cin = {IEK-5},
ddc = {530},
cid = {I:(DE-Juel1)IEK-5-20101013},
pnm = {Erneuerbare Energien},
pid = {G:(DE-Juel1)FUEK401},
shelfmark = {Physics, Condensed Matter},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000288896400006},
doi = {10.1103/PhysRevB.83.115209},
url = {https://juser.fz-juelich.de/record/16868},
}