| Abstract: | The confinement mechanism proposed earlier and then applied successfully to meson spectroscopy by one of the authors is interpreted
in classical terms. For this aim the unique solution of the Maxwell equations, an analog of the corresponding unique solution
of the SU(3)-Yang-Mills equations describing linear confinement in quantum chromodynamics, is used. Motion of a charged particle
is studied in the field representing magnetic part of the mentioned solution and it is shown that one deals with the full
classical confinement of the charged particle in such a field: under any initial conditions the particle motion is accomplished
within a finite region of space so that the particle trajectory is near magnetic field lines while the latter are compact
manifolds (circles). An asymptotical expansion for the trajectory form in the strong field limit is adduced. The possible
application of the obtained results in thermonuclear plasma physics is also shortly outlined. |
