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The
CAP extended Poincaré-group
has 2x10
+ 1x6 =
26 degrees of freedom instead of the
10 degrees of freedom of the continuous
complete SR Poincaré-group.
Any description of what we experience always has
causes and consequences. This is why the complete
SR symmetry-group, described with
Sμν
and Aμν,
will be given using
fermions (massive half integer
spins) as sources of
bosons
as force-fields.
The 10 degrees of freedom of the symmetrical tensor Sμν
are given by the spin˝ masses
as sources and the resulting spin2
gravitational field.
The 6 degrees of freedom of the anti-symmetrical tensor
Aμν
are given by the spin˝ charges
as sources and the resulting spin1
EM-field.
The Maxwell equations of the
EM-field don't specify this field completely. Only
after using so-called
gauge-symmetry the
EM-field is given completely. The
EM-field
has U(1)-gauge-symmetry, given
SR with the Lorentz gauge-symmetry.
The electroweak theory, a mixed gauge-theory,
is given by the U(1)xSU(2)
gauge-symmetry, in which the photon (the non-reducible description of the
spin1 EM-field) appears mixed (given by the
so-called
Weinberg-angle) with the massive
Z and W±
gauge-bosons. The only additional gauge-symmetry possible in our
4D-spacetime universe is the
SU(3) gauge-symmetry. This gauge-symmetry
represents non-reducible all spin3/2
quarks as intrinsic unstable particles, quarks
only appear combined as so-called
hadrons.
The compound spin˝
fermions are called
baryons and the compound
bosons are called
gluons (keeping quarks of
a
baryon together) and
mesons. Only the
anti-symmetrical actions, related
to electrical charge, have
gauge-symmetry, because the symmetrical actions, related
to mass, don't allow so-called gauge-symmetry. In the symmetrical case all contributions cancel.
Therefore the
gravitational field can't be described as a gauge-field! All other force fields
are all related to charge and must be described using gauge-symmetry.
So, the complete symmetry-group of our universe is given by the
CAP extended Poincaré-group,
i.e. Sμν
en Aμν,
and the U(1)x(SU(2)xSU(3) gauge-symmetry
related to the anti-symmetrical (charge related) actions.
As shown experimentally,
gravitation
curves 4D-spacetime.
This curvature can only be analyzed mathematically in linear
space-time.
This requires doubling of degrees of freedom (4 →
8), as Einstein solved using
Riemann's work. This is the fundamental reason
for the fact that the
curvature tensor, or
Riemann-Christoffel
tensor, has 20 degrees of
freedom, while the metric and the also 2-indices symmetrical
Ricci tensor only have 10
degrees of freedom. In 4D
curved space-time this is proven with the Bianchi
symmetry relations of the curvature tensor. According to
Einstein’s
C(omprehensive)A(ction)P(rinciple)
curvature must be taken into account in any description of physics.
So, also in any SR description
and also in every
QM
description!
The only way to double the amount of degrees of freedom in a linear
description is describing all non-reducible
representations of the complete symmetry-group, i.e. all
elementary particles, as harmonic oscillating point-particles in the 2D-plane
orthogonal to the observed direction of motion given by the
SR worldline. Characteristics
observed in QM also lead to this conclusion.
The position of an extended elementary particle is given with its
average position, i.e. the position on the
SR worldline. This is
also the position used in an
Euler-Lagrange description to obtain the
equations of motion. The particle itself, described exactly with a point-description
never is on its average
worldline, but oscillates harmonically in the
2D-plane orthogonal to this
worldline. The SR solutions
require B(oundary)C(onditions).
Bosons interact in the direction of motion only,
i.e. must be described with closed BC.
Fermions
are able to interact in all directions and as a result of that fact
can't be on the same space-time position together. So,
fermions
require open BC. Open
BC have one positive integer
degree of freedom extra. This is the
quantum number giving the particles family. The higher this
number, the higher the mass, because more interaction with the
gravitational field.
The only massless particles are the spin1
photon and the
spin2
graviton. All other particles always have speeds
v < c(lightspeed).
This is why paths of fermions allow
knots under transformations. I'm
not saying it'll actually happen (only maybe in a black hole),
but mathematical it is possible! Without fermions no resulting force-fields of
bosons, so all possible universes
require space that allows knots.
In 2004
Grisha Perelman showed that only in
3D-space, i.e.
4D-spacetime
knots are possible.
This description appears completely correct, so every possible
universe must have 4D-spacetime!.
Our universe is the result of a black hole in another universe turning into a singularity.
This singularity
was characterized with a first phase of the Big
Bang in which 3 elementary
particle families of fermions came to life. After the
Big Bang all
matter scattered from the singularity
in all 3D-spacelike directions,
with a constant total energy and total angular-momentum of our universe. The energy
density only decreases so the 3 particles families of
fermions
are a given fact of our universe. The singularity of the black hole in
the other universe terminates by vapourization into our universe.

Last change:
05-10-2009 19:54:16
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