Charged defect states at silicon grain boundaries

1986 ◽  
Vol 60 (11) ◽  
pp. 3910-3915 ◽  
Author(s):  
F. J. Stützler ◽  
H. J. Queisser
1986 ◽  
Vol 10-12 ◽  
pp. 229-234 ◽  
Author(s):  
F.J. Stützler ◽  
L. Tapfer ◽  
H.J. Queisser

1994 ◽  
Vol 76 (4) ◽  
pp. 2260-2263 ◽  
Author(s):  
Mehmet Güneş ◽  
Christopher R. Wronski ◽  
T. J. McMahon

1980 ◽  
Vol 44 (20) ◽  
pp. 1365-1365
Author(s):  
C. H. Seager ◽  
G. E. Pike ◽  
D. S. Ginley

2021 ◽  
Vol 32 (7) ◽  
pp. 9509-9516
Author(s):  
Shobhit Saraswat ◽  
V. K. Tomar ◽  
V. K. Deolia ◽  
A. Sharma ◽  
A. Dahshan ◽  
...  

2016 ◽  
Vol 4 (41) ◽  
pp. 16191-16197 ◽  
Author(s):  
Yang Zhou ◽  
Feng Wang ◽  
Hong-Hua Fang ◽  
Maria Antonietta Loi ◽  
Fang-Yan Xie ◽  
...  

The bromine has the role of passivating defect states at grain boundaries and interfaces in mixed halide perovskite solar cells.


1994 ◽  
Vol 336 ◽  
Author(s):  
Mehmet Güneş ◽  
R. W. Collins ◽  
C. R. Wronski

ABSTRACTSteady-state photoconductivity, sub-bandgap absorption and electron spin resonance (ESR) Measurements were carried out on annealed and light soaked intrinsic hydrogenated Amorphous silicon (a-Si:H) films. The experimental results were modeled using detailed numerical Model. The defect densities derived from the sub-bandgap absorption in the light soaked films were correlated with the ESR spin densities. Selfconsistent fitting of the data was obtained using a gap state distribution which consists of positively charged defect states above, negatively charged defect states below and neutral defect states at about Midgap. Both the annealed and the light degraded states are modeled using the same distribution of gap states whose densities increase upon light soaking with a slight increase in the ratio of the neutral to charged defect densities. These results on intrinsic a-Si:H are consistent with those of charged defect Models.


1998 ◽  
Vol 507 ◽  
Author(s):  
Helmut Stiebig ◽  
Frank Siebke ◽  
Reinhard Carius ◽  
Josef Klomfaβ

ABSTRACTIn this work, gap states in doped and undoped a-SiGe:H alloys are examined by numerical simulations of sub-bandgap absorption spectra measured by the constant photocurrent method and photothermal deflection spectroscopy. Deconvolution methods, neglecting the condition of charge neutrality, can be used for a rough estimate of the defect density value but not for ob- taining detailed information on the distribution of gap states in undoped samples. Our numerical analysis uses adapted occupation statistics and takes into account the condition of charge neutrality. Good agreement between measured and simulated PDS and CPM spectra is obtained. For a certain composition, i.e. a certain bandgap, the investigation of doped films yields infor- mation on the density and the position of charged defect states in the bandgap. In addition, the density of neutral defect states can be derived from a comparison of CPM and PDS spectra. The results reveal the coexistence of charged and neutral defects. In doped as well as in undoped films, charged defect states dominate the defect density. In the investigated range of compo- sitions the defect distribution of a-SiGe:H is similar to those found in a-Si:H. The width of the defect distributions does not decrease with decreasing bandgap. No evidence for a different be- havior of Si- and Ge-related defect states can be found in sub-bandgap absorption spectra.


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