Unique Curve for the Radiative Photovoltage Deficit Caused by the Urbach Tail

Author(s):  
Juan Bisquert
Keyword(s):  
2017 ◽  
Vol 95 (24) ◽  
Author(s):  
Mohamed Moustafa ◽  
Anke Wasnick ◽  
Christoph Janowitz ◽  
Recardo Manzke

1983 ◽  
Vol 54 (2) ◽  
pp. 1048-1052 ◽  
Author(s):  
K. Solomon Harshavardhan ◽  
S. Rajagopalan ◽  
L. K. Malhotra ◽  
K. L. Chopra

2008 ◽  
Vol 245 (12) ◽  
pp. 2794-2799 ◽  
Author(s):  
G. M. Mamedov ◽  
M. Karabulut ◽  
A. O. Kodolbaş ◽  
Ö. Öktü

1975 ◽  
Vol 39 (3) ◽  
pp. 715-719 ◽  
Author(s):  
Yoshitaka Takubo ◽  
Takao Koda
Keyword(s):  

2010 ◽  
Vol 81 (15) ◽  
Author(s):  
M. Letz ◽  
A. Gottwald ◽  
M. Richter ◽  
V. Liberman ◽  
L. Parthier

1996 ◽  
Vol 420 ◽  
Author(s):  
Helmut Stiebig ◽  
Frank Siebke ◽  
Reinhard Carius

AbstractCPM and PDS spectra of a-Si:H yield identical shape of the Urbach tail, while the defect absorption measured by PDS differs significantly from CPM. In this work an analysis of CPM and PDS spectra of annealed and degraded films is presented. Numerical simulations of CPM and PDS data, taking into account optical transitions, capture and emission processes as well as the Fermi level, yield information on the energy distribution and the charge state of the defects. The simulations reveal the coexistence of defects in the D−, D+ and D0 states. The defect distribution is dominated by charged states as predicted by the defect-pool model. Good agreement between measured and simulated PDS and CPM spectra can be obtained in the case of a homogeneous defect density. It is shown that differences between CPM and PDS are due to different sensitivities of the techniques to charged and neutral defect states. Microscopic inhomogeneities may cause significant additional differences.


2007 ◽  
Vol 46 (4B) ◽  
pp. 2405-2408 ◽  
Author(s):  
Hirofumi Kakemoto ◽  
Tohru Higuchi ◽  
Hajime Shibata ◽  
Satoshi Wada ◽  
Takaaki Tsurumi

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