The Bound Polaron Problem

2018 ◽  
pp. 195-221
Author(s):  
Ashok Chatterjee ◽  
Soma Mukhopadhyay
Keyword(s):  
2012 ◽  
Vol 11 (03) ◽  
pp. 1250026 ◽  
Author(s):  
CHENG-SHUN WANG ◽  
YU-FANG CHEN ◽  
JING-JIN XIAO

Properties of the excited state of strong-coupling impurity bound polaron in an asymmetric quantum dot are studied by using linear combination operator and unitary transformation methods. The first internal excited state energy, the excitation energy and the transition frequency between the first internal excited and the ground states of the impurity bound polaron as functions of the transverse and the longitudinal effective confinement lengths of the dot, the electron–phonon coupling strength and the Coulomb bound potential were derived. Our numerical results show that they will increase with decreasing the effective confinement lengths, due to interesting quantum size confining effects. But they are an increasing functions of the Coulomb bound potential. The first internal excited state energy is a decreasing function of the electron–phonon coupling strength whereas the transition frequency and the excitation energy are an increasing one of the electron–phonon coupling strength.


2008 ◽  
Vol 22 (12) ◽  
pp. 1923-1932
Author(s):  
JIA LIU ◽  
ZI-YU CHEN

The influence of a perpendicular magnetic field on a bound polaron near the interface of a polar–polar semiconductor with Rashba effect has been investigated. The material is based on a GaAs / Al x Ga 1-x As heterojunction and the Al concentration varying from 0.2 ≤ x ≤ 0.4 is the critical value below which the Al x Ga 1-x As is a direct band gap semiconductor.The external magnetic field strongly altered the ground state binding energy of the polaron and the Rashba spin–orbit (SO) interaction originating from the inversion asymmetry in the heterostructure splitting of the ground state binding energy of the bound polaron. How the ground state binding energy will be with the change of the external magnetic field, the location of a single impurity and the electron area density have been shown in this paper, taking into account the SO coupling. The contribution of the phonons are also considered. It is found that the spin-splitting states of the bound polaron are more stable, and, in the condition of weak magnetic field, the Zeeman effect can be neglected.


1973 ◽  
Vol 56 (1) ◽  
pp. 211-221 ◽  
Author(s):  
T. D. Clark ◽  
K. K. Bajaj

2016 ◽  
Vol 97 ◽  
pp. 298-302 ◽  
Author(s):  
Zhao-Hua Ding ◽  
Ying Zhao ◽  
Jing-Lin Xiao

2013 ◽  
Vol 34 (9) ◽  
pp. 1128-1134
Author(s):  
曹艳娟 CAO Yan-juan ◽  
闫祖威 YAN Zu-wei ◽  
石磊 SHI Lei

2011 ◽  
Vol 32 (1) ◽  
pp. 27-32
Author(s):  
王东民 WANG Dong-min ◽  
肖景林 XIAO Jing-lin

2008 ◽  
Vol 403 (23-24) ◽  
pp. 4338-4341
Author(s):  
Xiu-qing Wang ◽  
Jing-lin Xiao
Keyword(s):  

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