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Particle and spin motion in polarized media
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Particle and spin motion in polarized media
A.J. Silenko
Institute of Nuclear Problems, Belarusian State University, Minsk, Belarus
E-mail: silenko@inp.minsk.by
Abstract
Quantum mechanical equations of motion are obtained for particles and spin in
media with polarized electrons in the presence of external fields. The motion of elec-
trons and their spins is governed by the exchange interaction, while the motion of
positrons and their spins is governed by the annihilation interaction. The equations
obtained describe the motion of particles and spin in both magnetic and nonmag-
netic media. The evolution of positronium spin in polarized media is investigated.
Media with polarized electrons can be used for polarization of positronium beams.
1
1 Introduction
The quantum mechanical description of the motion of particles and spin in matter
is a very important problem. The classical theory of motion of particles and spin has
been developed in great detail (see [1, 2])). A quantum mechanical equation of motion of
relativistic particles in an electromagnetic field was derived by Derbenev and Kondratenko
[3]. The motion of the spin of relativistic particles in an electromagnetic field is described
by the Bargmann–Michel–Telegdi (BMT) equation [4]. The Lagrangian with an allowance
for terms quadratic in spin was obtained in [5, 6]. The corresponding equation of spin
motion was presented in [7]. The interaction between polarized particles and polarized
matter was analyzed in [8, 9].
In the present paper, we find quantum mechanical equations of motion of particles
and spin for relativistic particles with arbitrary spin that move in media with polarized
electrons in the presence of external fields. The system of units h? = c = 1 is used.
2 Hamiltonian for particles in polarized media
For particles with arbitrary spin, the Hamiltonian can be derived with the use of the
interaction Lagrangian L, obtained in [5, 6].
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