scholarly journals lntersubband Relaxation in Step Quantum Well Structures

VLSI Design ◽  
1998 ◽  
Vol 8 (1-4) ◽  
pp. 289-293
Author(s):  
J. P. Sun ◽  
H. B. Teng ◽  
G. I. Haddad ◽  
M. A. Stroscio ◽  
G. J. Iafrate

Intersubband relaxation due to electron interactions with the localized phonon modes plays an important role for population inversion in quantum well laser structures designed for intersubband lasers operating at mid-infrared to submillimeter wavelengths. In this work, intersubband relaxation rates between subbands in step quantum well structures are evaluated numerically using Fermi's golden rule, in which the localized phonon modes including the asymmetric interface modes, symmetric interface modes, and confined phonon modes and the electron – phonon interaction Hamiltonians are derived based on the macroscopic dielectric continuum model, whereas the electron wave functions are obtained by solving the Schrödinger equation for the heterostructures under investigation. The sum rule for the relationship between the form factors of the various localized phonon modes and the bulk phonon modes is examined and verified for these structures. The intersubband relaxation rates due to electron scattering by the asymmetric interface phonons, symmetric interface phonons, and confined phonons are calculated and compared with the relaxation rates calculated using the bulk phonon modes and the Fröhlich interaction Hamiltonian for step quantum well structures with subband separations of 36 meV and 50meV, corresponding to the bulk longitudinal optical phonon energy and interface phonon energy, respectively. Our results show that for preferential electron relaxation in intersubband laser structures, the effects of the localized phonon modes, especially the interface phonon modes, must be included for optimal design of these structures.

1988 ◽  
Vol 31 (3-4) ◽  
pp. 767-770 ◽  
Author(s):  
A. Seilmeier ◽  
H.-J. Hübner ◽  
M. Wörner ◽  
G. Abstreiter ◽  
G. Weimann ◽  
...  

1991 ◽  
Vol 58 (21) ◽  
pp. 2393-2395 ◽  
Author(s):  
Shunichi Muto ◽  
Tsuguo Inata ◽  
Atsushi Tackeuchi ◽  
Yoshihiro Sugiyama ◽  
Toshio Fujii

1997 ◽  
Vol 79 (17) ◽  
pp. 3226-3229 ◽  
Author(s):  
Y. J. Wang ◽  
H. A. Nickel ◽  
B. D. McCombe ◽  
F. M. Peeters ◽  
J. M. Shi ◽  
...  

1999 ◽  
Vol 25 (1-2) ◽  
pp. 163-166 ◽  
Author(s):  
P. Kinsler ◽  
R.W. Kelsall ◽  
P. Harrison

2016 ◽  
Vol 30 (26) ◽  
pp. 1650196 ◽  
Author(s):  
Zheng Li ◽  
Hailong Wang ◽  
Li Chen ◽  
Sha Chen ◽  
Qian Gong

Within the framework of effective mass approximation, the scattering rate via longitudinal optical (LO) phonon emission for an electron and the mean scattering rate via LO phonons emission for electrons initially in the first excited sub-band and finally in the ground sub-band in [Formula: see text] stepped quantum well (QW) is calculated adopting the shooting method and Fermi’s golden rule. The results show that the scattering rate and the mean scattering rate are highly dependent on alloy compositions, well width, initial electron energy, electron temperature and sub-band separation [Formula: see text] between the ground sub-band and the first excited sub-band. When [Formula: see text] is larger than the LO phonon energy, the scattering rate and the mean scattering rate increases with increasing Ga composition, decreasing As composition and increasing well width. However, when [Formula: see text] is smaller than the LO phonon energy, its change tendency is contrary. The scattering rate increases with decreasing initial electron energy if the separation between the initial electron energy and the ground state energy [Formula: see text] is not smaller than the LO phonon energy. The scattering rate and the mean scattering rate increases with rising electron temperature. The mean scattering rate reaches the maximum value when [Formula: see text] is equal to the LO phonon energy. The interruption in the scattering rate happens when the separation between the initial electron energy and [Formula: see text] is smaller than the LO phonon energy. The rapid decrease of the mean scattering rate happens when [Formula: see text] is smaller than the LO phonon energy if [Formula: see text] continues decreasing. In addition, both the scattering rate and the mean scattering rate show little change with different stepped layer widths.


2016 ◽  
Vol 18 (43) ◽  
pp. 29864-29870 ◽  
Author(s):  
A. K. Sivadasan ◽  
Chirantan Singha ◽  
A. Bhattacharyya ◽  
Sandip Dhara

Interface phonon (IF) modes of [AlN/GaN]20 and [Al0.35Ga0.65N/Al0.55Ga0.45N]20 multi-quantum well (MQW) structures are reported. The effect of variation in the dielectric constant of “barrier” layers periodically arranged in the MQWs is investigated.


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