On Mar 6, 9:36*am, "Jay R. Yablon" wrote:
Dear Friends:
I have added sections 12, 13 and 14 to the Kaluza-Klein paper which I
have earlier posted. *These sections examine the relationship between
the electrodynamics potentials and the gravitational potentials, and
connect to QED.
Most significantly, these three sections not only connect to the QED
Lagrangian, but, they show how the familiar QED Lagrangian density
L = -(1/4) F dot F - J dot A
emerges *in the linear approximation* of 5-dimensional Kaluza-Klein
gravitational theory.
Then, we go in the opposite direction, to show the QED Lagrangian
density / action for *non-linear* theory, based on the full-blown
apparatus of gravitational theory. *You may view this at:
http://jayryablon.files.wordpress.co...linear-qed.pdf
Again, focus on sections 12, 13 and 14.
Looking for constructive feedback.
When taking an axis to be time-like or space-like
there are some Coulomb gauge operations in QED
that statistically swamp errors separating
imaginaries and reals.
Note: if you know about complex numbers you
will notice that the space part enters as if
it were imaginary
R2 = (ct)2 + (ix)2 + (iy)2 + (iz)2 = (ct)2 + (ir)2
where i^2 = -1 as usual. This turns out to be the
essence of the fabric (or metric) of spacetime geometry
- that space enters in with the imaginary factor i relative to time.
http://www.nrao.edu/~smyers/courses/...edoflight.html
Is there a specific place we can look to see
how you preserve or otherwise substitute for that
QED mechanism absent any emission or absorbtion
phenomena that can be related to gravito-inertial
effects?
The probablity of a path, is not the path so
the notion of geometrical analysis with other
than Gauss's curve raises some red flags.
Sue...
http://en.wikipedia.org/wiki/Path_integral_formulation
--Grosche, Christian
http://arxiv.org/abs/hep-th/9302097
Thanks,
Jay.
____________________________
Jay R. Yablon
Email:
co-moderator: sci.physics.foundations
Weblog:http://jayryablon.wordpress.com/
Web Site:http://home.nycap.rr.com/jry/FermionMass.htm