Abstract
The interaction between tunneling system inherent in amorphous solids is established to be responsible for the universal behavior of their kinetics and thermodynamic properties at low temperature. In this paper, we describe the relaxation mechanism induced by the interaction that falls down as R−3 at large distances. This interaction is either the electrostatic dipole-dipole one or is the elastic one between the point defects (the tunneling system). In the last case, the interaction is due to an indirect interaction induced by acoustic virtual phonon exchange. The relaxation becomes significant at sufficiently low temperature where phonons are substantially frozen out. We show that, in a realistic experimental situation, the measuring field strongly accelerates the interaction-stimulated relaxation. The characteristic temperature and field dependences of the relaxation rate are found when the rate is affected both by the interaction between tunneling systems and by the external field.
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From Pis’ma v Zhurnal Éksperimental’no\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l} \) i Teoretichesko\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l} \) Fiziki, Vol. 80, No. 7, 2004, pp. 583–592.
Original English Text Copyright © 2004 by Burin, Maksimov, Polishchuk.
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Burin, A.L., Maksimov, L.A. & Polishchuk, I.Y. Relaxation in glasses at low temperatures. Jetp Lett. 80, 513–522 (2004). https://doi.org/10.1134/1.1839302
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DOI: https://doi.org/10.1134/1.1839302