Multipolarons in a Constant Magnetic Field

The binding of a system of N polarons subject to a constant magnetic field of strength B is investigated within the Pekar–Tomasevich approximation. In this approximation, the energy of N polarons is described in terms of a non-quadratic functional with a quartic term that accounts for the electron–e...

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Bibliographic Details
Published inAnnales Henri Poincaré Vol. 15; no. 6; pp. 1037 - 1059
Main Authors Anapolitanos, Ioannis, Griesemer, Marcel
Format Journal Article
LanguageEnglish
Published Basel Springer Basel 01.06.2014
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ISSN1424-0637
1424-0661
DOI10.1007/s00023-013-0266-4

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Summary:The binding of a system of N polarons subject to a constant magnetic field of strength B is investigated within the Pekar–Tomasevich approximation. In this approximation, the energy of N polarons is described in terms of a non-quadratic functional with a quartic term that accounts for the electron–electron self-interaction mediated by phonons. The size of a coupling constant, denoted by α , in front of the quartic term is determined by the electronic properties of the crystal under consideration, but in any case it is constrained by 0 <  α < 1. For all values of N and B , we find an interval α N , B <  α <  1 where the N polarons bind in a single cluster described by a minimizer of the Pekar–Tomasevich functional. This minimizer is exponentially localized in the N -particle configuration space R 3 N .
ISSN:1424-0637
1424-0661
DOI:10.1007/s00023-013-0266-4