Stimulated emission due to the inelastic scattering from the heavy-hole exciton to the light-hole exciton in CuI thin films

2002 ◽  
Vol 92 (7) ◽  
pp. 3511-3516 ◽  
Author(s):  
I. Tanaka ◽  
M. Nakayama
1998 ◽  
Vol 57 (4) ◽  
pp. 2592-2595 ◽  
Author(s):  
H. Nishimura ◽  
K. Kitano ◽  
S. Kawase ◽  
M. Nakayama
Keyword(s):  

2000 ◽  
Vol 87-89 ◽  
pp. 257-259 ◽  
Author(s):  
I Tanaka ◽  
D Kim ◽  
M Nakayama ◽  
H Nishimura

2001 ◽  
Vol 94-95 ◽  
pp. 385-388 ◽  
Author(s):  
I. Tanaka ◽  
K. Mizoguchi ◽  
M. Nakayama

2019 ◽  
Vol 2019 ◽  
pp. 1-7
Author(s):  
Takuya Kawazu

Optical properties of GaAs/AlGaAs quantum wells (QWs) in the vicinity of InAlAs quantum dots (QDs) were studied and compared with a theoretical model to clarify how the QD strain affects the electronic states in the nearby QW. In0.4Al0.6As QDs are embedded at the top of the QWs; the QD layer acts as a source of strain as well as an energy barrier. Photoluminescence excitation (PLE) measurements showed that the QD formation leads to the increase in the ratio Ie-lh/Ie-hh of the PLE intensities for the light hole (lh) and the heavy hole (hh), indicating the presence of the valence band mixing. We also theoretically calculated the hh-lh mixing in the QW due to the nearby QD strain and evaluated the PLE ratio Ie-lh/Ie-hh.


2015 ◽  
Vol 29 (30) ◽  
pp. 1550213 ◽  
Author(s):  
Zhenhua Wu ◽  
Lei Chen ◽  
Qiang Tian

We use the fractional–dimensional approach (FDA) to study exciton binding energies in GaAs films on [Formula: see text] substrates. In this approach, the Schrödinger equation for a given anisotropic system is solved in a noninteger-dimensional space where the interactions are assumed to occur in an isotropic effective environment. The heavy-hole and light-hole exciton binding energies are calculated as functions of the film thickness and substrate thickness. The numerical results show that both the heavy-hole and light-hole exciton binding energies decrease monotonously as the film thickness increases. When the film thickness and the substrate thickness is relatively small, the change of substrate thickness has comparatively remarkable influence on both heavy-hole and light-hole exciton binding energies. As the substrate thickness increases, both the heavy-hole and light-hole exciton binding energies increase gradually. When the film thickness or the substrate thickness is relatively large, the change of substrate thickness has no significant influence on both heavy-hole and light-hole exciton binding energies.


2008 ◽  
Vol 14 (4) ◽  
pp. 1053-1057 ◽  
Author(s):  
Hsing-Chao Chen ◽  
Miin-Jang Chen ◽  
Mong-Kai Wu ◽  
Yung-Chen Cheng ◽  
Feng-Yu Tsai

2019 ◽  
Vol 30 (17) ◽  
pp. 175301
Author(s):  
A Artioli ◽  
P Rueda-Fonseca ◽  
K Moratis ◽  
J F Motte ◽  
F Donatini ◽  
...  

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