V.S.
Leonov
The problem of the magnetic monopole was tackled
by Dirac as an independent magnetic charge and in his honor it is referred to
as the Dirac monopole. Naturally, the search for magnetic monopoles and
attempts to detect mass in them resulted in the experimental boom in the 60s
which, however, has not yielded positive results. The Dirac monopoles have not
been detected The interest in them has been renewed because of the quantization
of space-time in the EQM. theory which regards the magnetic monopole as a
non-free particle bonded in space-time and this particle cannot be detected in
the free state. Only the indirect registration of the manifestation of the
properties of magnetic monopoles in disruption of the magnetic equilibrium of
the space-time in accordance with the Maxwell equations is possible.
The fact that the role of
magnetic monopoles in the structure of the space-time was not understood
prevented for a very long period of time the development of a method of
determination of the value of the charge g
of the magnetic monopole. Dirac himself assumed that taking into account the un
ambiguity of the phase of the wave function of the electron intersecting the
line of n-nodes consisting of
magnetic poles, we obtain the required relationship:
g = 68.5e [C]
Here e = 1.6·10(–19) C is the electron charge.
The Dirac relationship (2.2) was improved by the
well-known American theoretical physicist J. Schwinger who proved that n in equation (2) should only be an even
number, and at n = 2 we obtain g = 137 e .
However, the Dirac method is indirect in which a line of nodes can be separated in
space from the magnetic charge included in the space-time structure. In
reality, in the quantized only a line of quantons can be separated in the form
of an alternating string from magnetic and electrical dipoles. In particular,
Dirac did not take into account the electrical component of the effect. In
movement of an electron along such an alternating string, the electron is
subjected to the effect of waves from the side of the space-time which is
characterized by the constant fine structure α. This was also taken into
account nonformally by Schwinger by introducing n = 2.
It would appear that there is no basis for
doubting Dirac’s method which has been accepted by physicists and is regarded
as a classic method. From the mathematical viewpoint, the Dirac solutions are
accurate. However, from the viewpoint of physics, the Dirac procedure
contradicts not only the structure of the quantized space-time but also the
solutions of the Maxwell equations for the electromagnetic field in vacuum.
The correct formula for a magnetic
charge was first obtained by the Russian physicist Leonov in the
theory of Superunification in 1996:
g = Ce = 4.8·10(–11) [L]
Here [L] = [Leon]= [Am]
C – light speed.
Read more:
1. Unit of measurement of magnetic charge - Leon
2. Download free. Leonov
V. S. Quantum Energetics. Volume 1. Theory of Superunification, 2010.
