Effects of Sample Inhomogeneity and Geometry on Photoconductivity Decay

2009 ◽  
pp. 88-88-11 ◽  
Author(s):  
T Wang ◽  
TF Ciszek
1989 ◽  
Vol 161 ◽  
Author(s):  
W. O. Doggett ◽  
Michael W. Thelander ◽  
J. F. Schetzina

ABSTRACTA system has been developed for accurately measuring lifetimes for photo-induced excess current carriers in semiconductors using the transient photoconductivity decay method. The specifications of state-of-the-art equipment, considerations peculiar to the capture of fast transient pulses, and sophisticated statistical data analysis techniques are discussed. Experimental results are presented to demonstrate the capability of the system (a) to measure lifetimes in the 40-ns - 75-µs range for temperatures varying from 77K to 300K with 10% accuracy for single lifetime decays and 30% accuracy for individual effective lifetimes in a multi-component decay, and (b) to use a 300-ns lifetime photoconductor as a detector to measure nanosecond-time-scale structure of laser pulses. The predominant excess carrier lifetimes of HgCdTe samples grown at NCSU by photoassisted molecular beam epitaxy (PAMBE) ranged from 46 ns at 300K to 341 ns at 77K. CdTe samples and CdMnTe-CdTe superlattices exhibited a multi-component decay with the two longest components having effective lifetimes of 26 µs and 4 µs for CdTe and 75 µs and 10 µs for CdMnTe-CdTe. These values were relatively insensitive to temperature variation.


2017 ◽  
Vol 46 (8) ◽  
pp. 585-590 ◽  
Author(s):  
I. M. Anfimov ◽  
S. P. Kobeleva ◽  
A. V. Pylnev ◽  
I. V. Schemerov ◽  
D. S. Egorov ◽  
...  

2013 ◽  
Vol 47 (1) ◽  
pp. 174-177 ◽  
Author(s):  
V. V. Vainberg ◽  
V. M. Vasetskii ◽  
Yu. N. Gudenko ◽  
V. N. Poroshin ◽  
N. V. Baidus ◽  
...  

Author(s):  
R.J. Kumar ◽  
P.A. Losee ◽  
Can Hua Li ◽  
Joseph Seiler ◽  
I. Bhat ◽  
...  

1992 ◽  
Vol 283 ◽  
Author(s):  
P. Basmaji ◽  
V. Grivickas ◽  
G. I. Surdutovich ◽  
R. Vitlina ◽  
V. S. Bagnato

ABSTRACTThe structure of aged porous silicon (PS) has been investigated using reflectivity, photoluminescence (PL), optical absorption and photoconductivity decay. An optical anisotropy in a perpendicular to surface direction is observed for PS samples below a critical porosity of 70%. The photostability of the PL spectra imply three different structures of PS, these should be attributed to quantum size structures, polymeric type structures and fluor-related structures. The absorption edge is deconvoluted into a band-to-band absorption with energy ranging between Eg = 1.6–2 eV and an absorption shoulder at hu ≤ Eg. The high energy PL band around 2.3 eV resembles that of fluoroindate glass. The observed rapid lifetime at high injection level is attributed to excitonic Auger-type recombination.


2014 ◽  
Vol 1052 ◽  
pp. 181-187
Author(s):  
Yan Li Ding ◽  
Yue Zhao ◽  
Yue Feng ◽  
Xiao Yan Liang ◽  
Lin Jun Wang ◽  
...  

Photoluminescence of porous silicon (PS) prepared by different etched time was studied. The photoluminescence might originate from the recombination of carriers and surface states, which was proved by FTIR, Raman spectroscopy and SEM. Furthermore, the hydrogen-related groups on the PS surface could eliminate the surface states for the blue emission, but the quantities of surface states for the green emission were depended on the uncovered area on the PS surface. Moreover, the shape of photoconductivity curve was depended on the quantities of the surface states, which also was related to the uncovered area on the PS surface. In addition, the results of the microwave-detected photoconductivity decay measurement indicated thatthe defects on the PS surface increased with the increase of the etched time, which would be related to the increase of the depth of pores.


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