Volume 94, Number 4, May 2011
|Number of page(s)||5|
|Section||Condensed Matter: Electronic Structure, Electrical, Magnetic and Optical Properties|
|Published online||05 May 2011|
Classical diamagnetism, magnetic interaction energies, and repulsive forces in magnetized plasmas
Department of Mechanics, KTH - SE-100 44 Stockholm, Sweden, EU
Accepted: 6 April 2011
The Bohr-van Leeuwen theorem is often summarized as saying that there is no classical magnetic susceptibility, in particular no diamagnetism. This is seriously misleading. The theorem assumes position-dependent interactions but this is not required by classical physics. Since the work of Darwin in 1920 it has been known that the magnetism due to classical charged point particles can only be described by allowing velocity-dependent interactions in the Lagrangian. Legendre transformation to an approximate Hamiltonian can give an estimate of the Darwin diamagnetism for a system of charged point particles. Comparison with experiment, however, requires knowledge of the number of classically behaving electrons in the sample. A new repulsive effective many-body force, which should be relevant in plasmas, is predicted by the Hamiltonian.
PACS: 75.20.-g – Diamagnetism, paramagnetism, and superparamagnetism / 52.25.Xz – Magnetized plasmas / 05.20.-y – Classical statistical mechanics
© EPLA, 2011
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