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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Published in | Annales Henri Poincaré Vol. 15; no. 6; pp. 1037 - 1059 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Basel
Springer Basel
01.06.2014
|
Subjects | |
Online Access | Get full text |
ISSN | 1424-0637 1424-0661 |
DOI | 10.1007/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
. |
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ISSN: | 1424-0637 1424-0661 |
DOI: | 10.1007/s00023-013-0266-4 |