Reconciliation of Theory with Experiment for Defects in CdTe: The case of the Cadmium Vacancy

Author(s):  
Seán R. Kavanagh ◽  
Aron Walsh ◽  
David O. Scanlon
Keyword(s):  
2015 ◽  
Vol 1117 ◽  
pp. 19-22
Author(s):  
Artur Medvid ◽  
Aleksandr Mychko ◽  
Edvins Dauksta

The enhancement of CdZnTe crystal resistivity by λ=1064nm Nd:YAG laser radiation was shown. This effect is explained by compensation of cadmium vacancy (VCd) by indium atoms due to a laser-induced temperature gradient around Te inclusions. The temperature gradient is caused by the selective absorption of the laser radiation by the Te inclusions.


1971 ◽  
Vol 26 (1) ◽  
pp. 18-20 ◽  
Author(s):  
W. B. Alexander

AbstractMeasurements of electromigration in single crystals of cadmium have been made as a function of orientation. The resulting values for the effective charge numbers are Z =1.54 ± 0.15 and Z⊥=3.20±0.3.The results are also expressed in terms of the effective charges for the separate atomic jumps, (1) to a vacancy in the same basal plane and (2) to a vacancy in an adjoining plane. While the parallelism of these findings with those for zinc is apparent, there is one significant difference. In cadmium vacancy creation (and annihilation) tends to alter the c-axis dimension preferentially.


Author(s):  
L. Worschech ◽  
W. Ossau ◽  
F. Fischer ◽  
A. Waag ◽  
G. Landwehr
Keyword(s):  

1993 ◽  
Vol 47 (23) ◽  
pp. 15578-15580 ◽  
Author(s):  
P. Emanuelsson ◽  
P. Omling ◽  
B. K. Meyer ◽  
M. Wienecke ◽  
M. Schenk

1996 ◽  
Vol 161 (1-4) ◽  
pp. 134-138 ◽  
Author(s):  
L. Worschech ◽  
W. Ossau ◽  
F. Fischer ◽  
A. Waag ◽  
G. Landwehr
Keyword(s):  

1974 ◽  
Vol 14 (11) ◽  
pp. 1237-1240 ◽  
Author(s):  
B. Furgolle ◽  
M. Hoclet ◽  
M. Vandevyver ◽  
Y. Marfaing ◽  
R. Triboulet

Author(s):  
I. M. Kupchak ◽  
D. V. Korbutyak ◽  
N. F. Serpak

Using the density functional theory and the generalized gradient approximation, we calculated the atomic structure, the density of electronic states, and the optical absorption spectra of CdS quantum dots containing intrinsic defects — a cadmium vacancy VCd and an interstitial sulfur atom SI, and substitutional impurities — zinc and copper in place of the atom cadmium — ZnCd and CuCd, respectively. The calculations were performed for the Cd33S33 cluster corresponding to the so-called “magic” size of the quantum dot. This size has a minimum of dangling bonds at the surface and allows the using of such a cluster without the passivation. The structural relaxation during the formation of such defects and the distribution of the wave function of the state corresponding to the top of the valence band are analyzed in details. It has been shown that the cadmium vacancy forms local states in the band gap of CdS nanocrystals, and can serve as centers of radiative recombination. Other defects form energy levels in the depths of the valence band or near its top, but whose energy positions do not correspond to the band maxima in the experimental photoluminescence spectra of CdS quantum dots, both undoped and doped with zinc. The calculated optical absorption spectra demonstrate a strong peak in the region of fundamental absorption of CdS for a cluster containing a substitutional impurity of CuCd, in contrast to other systems where no such peaks are observed. In addition, the replacement of the cadmium atom with copper leads to a decrease in the number of chemical bonds to three and, accordingly, to the largest relaxation among the systems studied. This feature is caused by the crystal structure inhomogeneity of copper sulfide CuxS, which, depending on stoichiometry, can be either a semiconductor or a metal.


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