Two-particle bound state spectrum of transfer matrices for Gibbs fields (Fields on the two-dimensional lattice. Adjacent levels) |
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Authors: | E. L. Lakshtanov R. A. Minlos |
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Affiliation: | (1) Moscow State University, Moscow;(2) Institute for Problems of Information Transmission, Russian Academy of Sciences, Russia |
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Abstract: | ![]() This paper is a continuation of the authors paper published in no. 3 of this journal in the previous year, where a detailed statement of the problem on the two-particle bound state spectrum of transfer matrices was given for a wide class of Gibbs fields on the lattice  +1 in the high-temperature region (T 1). In the present paper, it is shown that for = 1 the so-called adjacent bound state levels (i.e., those lying at distances of the order of T– , > 2, from the continuous spectrum) can appear only for values of the total quasimomentum of the system that satisfy the condition | – jmult|<c/T2 (here c is a constant), where j/mult are the quasimomentum values for which the symbol { (k), k 1} has two coincident extrema. Conditions under which such levels actually appear are also presented.__________Translated from Funktsional nyi Analiz i Ego Prilozheniya, Vol. 39, No. 1, pp. 39–55, 2005Original Russian Text Copyright © by E. L. Lakshtanov and R. A. MinlosIn memory of A. N. ZemlyakovThe work of the second author was supported by the Russian Foundation for Basic Research (grant 02-01-00444) and also by the Presidential Foundation for Support to Scientific Schools (grant NSh-90.934.2003.1).Translated by V. M. Volosov |
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Keywords: | transfer matrices bound state Fredholm operator total quasimomentum adjacent level |
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