Gyromagnetic
momenta of electrons
According to Quantum Theory, the electron has two gyromagnetic
momenta:
g = 2 and g / 2 = 1.0011596 .
The first term means that the real magnetic momentum of an
electron's oscillation has to be the double magnitude
referred to Bohr's magneton (page 393 of my theory TBA I). The
second term tells us that Bohr's magneton is really exceeded
for this factor (page 538 of my theory, plus page 392, page
402). The "polarizing of vacuum" would be the reason. For the deviations, one sets this
"polarizing" of "virtual charges" and
those virtual compensation with fault calculation and gets the
measured amounts over the approximated math model. Is this a giant
success? Certainly it is, mathematically. Unfortunately, the
equations are divergent. They are no models for the expexted "united or
unified field theory" (page 373-391 of my theory).
But Quantum Mechanics has mistaken again in terminology.
The found polarizing is not the real polarizing of any vacuum,
but this is the polarizing of the real subparticles, which are
rotating inside the electron up to the amplitude of the radius
of 3.86e-13
m. If the electron wouldn't be negatively charged with one
integer charge, then all its positive and negative subparticles
would be distributed equally. There were no polarizing, no
shift of charges, no interaction to the outside. I tell this
sphere to be a "mass block". It only has mass, but no
electric and electromagnetic effects.
But the subparticles aren't antiparticles.
Therefore they don't make vacuum. There is no vacuum problem.
When a further negative charged subparticle appears at the
inside then it presses away the negative charges and attracts
the positive subparticles. Consequently, the ideal equal distribution
of the mass block will
be disturbed. This reality has been calculated correctly by
physics but not seen so. Just like this problem we have to see
the fault calculations between the electron levels of hydrogen
which cause the Lamb shift. Mathematics are correct, but the
models aren't!
Additionally, the orbits of the subparticle of the
subparticle shift the e. m. effects once more (TBA III).
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