Exploiting the magnetic and therefore gravitic properties of the Bi-IV dipole from Bernoulli analysis of ellipses.
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In the SU(2) algebra, inward and outward momentum waves
(caused by spherical rotation) are part of the Dirac spin-orbit
wave function. The spinor properties are part of the quantum
electron wave function. They involve parity (P), time (T), and
charge (C) inversion. CPT is an invariant, but it can
be violated:
The center-of-mass energy of amplitude reaches a maximum
value when w is just under 0.8(w_r), where w_r = Raman reso-
nance (rotation frequency). The energy amplitude of the quad-
rupole oscillations becomes "extremely large" while the fre-
quency of the quadrupole oscillation is close to zero.
This is where the ELF frequencies become important for the decom-
pressing quadrupole. The precessional 'wobble', or off-center
-of-mass causing off-Raman resonance oscillations between
positive and negative states, has oscillation frequency de-
termined by the ~0.9 detuning from the Raman resonance. This
phenomenon is a result of the Optical Bloch Equations result-
ing from a vortex cycling in and out of the Fermionic crystal
(driven by optical stirring of the pulse probe), whereas in the
aforementioned oscillating quadrupole, the 0.8(w_r) represents
the Rabi oscillations of an atom in a light field.
The "optical stirring" results from the scattering of ambient
photons through resonance with fringefield photons, whose effect
can be calculated from the "non-renormalizable" Lagrangian for
the resulting shell amplitudes and momenta. The trilinear inter-
action for bosonic exchange WOULD violate CPT invariance; this
suggests that there is a Lorenz (notice the missing "t" - this
is a different person than "LorenTz", See Note 1) invariant (not
covariant) of gravitational interaction that is not associated
with relativistic theory. Relativistic theory must be corrected
using the Dirac/Wigner solution (See Note 2).
NOTE 1:
The Lorenz Gauge (NOT LorenTz - He was only 14) was used
to develop a mathematical relationship between electromagnetic
sources and their potentials (e.g., D'Alembert's Equations,
which define the change in phase and potential minus the par-
tial derivative of the change in phase and potential w.r.t.
time, both over the speed of light squared being equal to the
negative of the density of electric charge over the electric
permittivity and the negative magnetic permeability times the
density of the electric current, respectively). Since one of
the options to the solution to Maxwell's equations that obey
the Lorenz gauge include using ADVANCED potentials, as well
as RETARDED potentials, then for curved spacetime, the re-
tarded potential at a given x location depends on the particle’s
history before the retarded time u; and the advanced potential
depends on the particle’s history after the advanced time v.
Since a polarized beam aimed at a polarized crystal can create
some field effect with charged particle/antiparticle pairs, the co-
herence can only be a "manufactured" one, if it is to be used
as a field harmonic with a decompressing fringefield.
NOTE 2:
Properties of non-relativistic quaternions include the unpair-
ed three-spin electron degeneration, that is, without an ex-
ternal magnetic field (earth's gravitational biofield), the
three unpaired spins give rise to four degenerate spin wave
functions. During resonance these four degenerate spin wave
functions are represented by the three degrees of spin fre-
edom with a fourth plus or minus time vector within the qua-
ternic conducting crystal. The three degrees of spin freedom
for the dual quaternic resonate by pulse chirping at the Fab-
ionacci Series of the Golden Mean and is a biquadratic opera-
tion of quaternions (between two conducting quaternic crys-
tals). The resultant repulsion of pole and antipole are tre-
ated as a specific velocity of frequency or phase propogation
and direction of vibration of the entire particle between two
repulsive nodes in space.
