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Comment on “Roles of donor and acceptor nanodomains in 6% efficient thermally annealed polymer photovoltaics” [Appl. Phys. Lett.90, 163511 (2007)]
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1.
1.K. Kim, J. Liu, M. A. G. Namoothiry, and D. L. Carroll, Appl. Phys. Lett. 90, 163511 (2007).
http://dx.doi.org/10.1063/1.2730756
2.
2.V. Shrotriya, G. Li, Y. Yao, T. Moriarty, K. Emery, and Y. Yang, Adv. Funct. Mater. 16, 2016 (2006).
http://dx.doi.org/10.1002/adfm.200600489
3.
3.Measurement principles for terrestrial PV solar devices with reference spectral irradiance data,” International Electrotechnical Commission Standard No. IEC 60904-3.
4.
4.K. O. Sylvester-Hvid, T. Ziegler, M. K. Riede, N. Keegan, M. Niggemann, and A. Gombert, J. Appl. Phys. 102, 054502 (2007).
http://dx.doi.org/10.1063/1.2775219
5.
5.H. Hoppe, N. Arnold, D. Meissner, and N. S. Sariciftci, Thin Solid Films 451-452, 589 (2004).
6.
6.M. Niggemann, T. Ziegler, M. Glatthaar, M. Riede, B. Zimmermann, and A. Gombert, Proc. SPIE 6197, 61970D (2006).
7.
7.H. Hoppe, S. Shokhovets, and G. Gobsch, Phys. Status Solidi (RRL) 1, R40 (2007).
8.
8.G. Li, V. Shrotriya, Y. Yao, and Y. Yang, J. Appl. Phys. 98, 043704 (2005).
http://dx.doi.org/10.1063/1.2008386
9.
9.J. B.B. A. J. Moulé and K. Meerholz, J. Appl. Phys. 100, 094503 (2006).
http://dx.doi.org/10.1063/1.2360780
10.
10.M. A. Green, K. Emery, Y. Hisikawa, and W. Warta, Prog. Photovoltaics 15, 425 (2007).
http://dx.doi.org/10.1002/pip.781
11.
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FIG. 1.

The best EQE of device D1 redrawn from Ref. 1 (dashed curve, claimed ) and the accumulated short circuit current density vs the upper wavelength limit of EQE, based on the standard spectrum with . The lower limit is fixed at . For the maximum attainable limit of is obtained (solid curve), which for example yields at a cutoff wavelength of . For the shown EQE from Ref. 1, the limit is (dash-dotted curve).

Image of FIG. 2.

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FIG. 2.

The simulated upper limit for calculated for an solar cell with varying P3HT:PCBM layer thickness assuming an internal quantum efficiency (IQE) of unity. The optical constants were derived from ellipsometric data obtained from an annealed blend with a ratio of 1:0.7 P3HT:PCBM. The approximate thickness that typically corresponds in our own solar cells is indicated.

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2008-02-20
2014-04-24

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Scitation: Comment on “Roles of donor and acceptor nanodomains in 6% efficient thermally annealed polymer photovoltaics” [Appl. Phys. Lett.90, 163511 (2007)]
http://aip.metastore.ingenta.com/content/aip/journal/apl/92/7/10.1063/1.2840155
10.1063/1.2840155
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