Magnetophotoluminescence of neutral acceptor states in InSb

2002 ◽  
Vol 80 (13) ◽  
pp. 2332-2334 ◽  
Author(s):  
J. A. H. Stotz ◽  
M. L. W. Thewalt
Keyword(s):  
Coatings ◽  
2019 ◽  
Vol 9 (7) ◽  
pp. 435 ◽  
Author(s):  
Halina Opyrchal ◽  
Dongguo Chen ◽  
Zimeng Cheng ◽  
Ken Chin

The effect of Cu on highly efficient CdTe thin solid film cells with a glass/TCO/CdS/CdTe structure subjected to CdCl2 treatment was investigated by low-temperature photoluminescence (PL). The PL of the CdS/CdTe junction in samples without Cu deposition revealed a large shift in the bound exciton position due to the formation of CdSxTe1−x alloys with Eg (alloy) ≅ 1.557 eV at the interface region. After Cu deposition on the CdTe layer and subsequent heat treatment, a neutral acceptor-bound exciton (A0Cu,X) line at 1.59 eV and two additional band-edge peaks at 1.54 and 1.56 eV were observed, indicating an increase in the energy gap value in the vicinity of the CdTe/CdS interface to that characteristic of bulk CdTe. These results may suggest the disappearance of the intermixing phase at the CdTe/CdS interface due to the presence of Cu atoms in the junction area and the interaction of the Cu with sulfur atoms. Furthermore, an increase in the intensity of CdS-related peaks in Cu-doped samples was observed, implying that Cu atoms were incorporated into CdS after heat treatment.


2000 ◽  
Author(s):  
ChihMing Wang ◽  
HorngYu Chang ◽  
Kien Wen Sun ◽  
ShyangYeu Wang ◽  
Chien-Ping Lee

1976 ◽  
Vol 18 (11-12) ◽  
pp. 1557-1560 ◽  
Author(s):  
D.S. Pan ◽  
D.L. Smith ◽  
T.C. McGill
Keyword(s):  

1976 ◽  
Vol 75 (1) ◽  
pp. 341-346 ◽  
Author(s):  
W. Wardzyński ◽  
K. Pataj

1997 ◽  
Vol 482 ◽  
Author(s):  
K. P. Koron ◽  
A. Wysmolek ◽  
J. M. Baranowskil ◽  
K. Pakul ◽  
J. P. Bergman ◽  
...  

AbstractPhotoluminescence connected with excitons and their phonon replicas in undoped homoepitaxial MOCVD grown GaN layers have been studied in the temperature range 2 - 100 K. It is shown that the coupling between LO phonons and neutral acceptor bound excitons (ABE) is much stronger than the coupling between LO phonons and neutral donor bound excitons (DBE). In spite that emission due the DBE no-phonon is one order of magnitude stronger than the ABE one, the predominant feature of the first LO phonon replica of the excitonic structures is related to the ABE. It is argued that this fact is connected with delocalization of the acceptor wavefunction in the k-space which leads to a higher number of interacting LO phonons in the first replica. On the other hand, the second LO phonon replica of the excitonic structures is predominantly connected with the DBE. In the case of two LO phonons interacting with bound excitons the k - conservation has not so direct influence. In addition, the temperature dependence of LO phonon replicas and their kinetics in ps regime are also reported.


1970 ◽  
Vol 41 (9) ◽  
pp. 3840-3843 ◽  
Author(s):  
K. L. Ashley ◽  
W. E. Ham ◽  
R. T. Brown

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