Influence of electron-phonon interaction in doped silicon crystals on the root-mean-square dynamic displacement of atoms

1977 ◽  
Vol 20 (9) ◽  
pp. 1128-1131
Author(s):  
M. D. Kapustina ◽  
V. A. Panteleev ◽  
T. Yu. Markova
1983 ◽  
Vol 119 (2) ◽  
pp. K139-K142 ◽  
Author(s):  
E. M. Gololobov ◽  
E. L. Mager ◽  
Z. V. Mezhevich ◽  
L. K. Pan

1967 ◽  
Vol 45 (4) ◽  
pp. 1421-1438 ◽  
Author(s):  
C. Y. Cheung ◽  
Robert Barrie

A calculation is made of the temperature dependence of the energy levels of shallow donor impurities in silicon. This temperature dependence arises from the electron–phonon interaction and we consider mixing only of the {1s}, {2s), and {2p0} electronic states. A comparison is made with experiment for the case of phosphorus-doped silicon.


2002 ◽  
Vol 13 (4) ◽  
pp. 491-494 ◽  
Author(s):  
A Tilke ◽  
L Pescini ◽  
A Erbe ◽  
H Lorenz ◽  
R H Blick

1983 ◽  
Vol 61 (7) ◽  
pp. 1017-1020 ◽  
Author(s):  
J. Daunay ◽  
Jac. Daunay ◽  
P. Bugnet

Measurements of light absorption on ZnSe single crystals, conducted from 80 K to room temperature, show that the forbidden band gap decreases with increasing temperature because of the electron–phonon interaction. It is established for temperatures ranging from 140 to 320 K that longitudinal optic (LO) and acoustic (A) phonons operate simultaneously and exclusively so that [Formula: see text]. The first term, resulting from the Franz–Keldysh effect applied to the mean square field produced by LO phonons, provides the value of this field. It reaches 105 V cm−1 at room temperature.


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