*137. K. L. Narayana,”Physical
process of Gravitons and Gravy Quark in the interior
of
Supergravity Cosmic Stellar structures”, 72nd Session of Ind.
Sci. Cong.
January 5th, 1985 and
Arthur Eddington Centenary Symposium,
Vol.3, Nagpur, 23rd February 1984.
Physical
process of Gravitons and Gravy Quark in the interior OF
SUPERGRAVITY Cosmic Stellar structures
K.
L. Narayana
Physics Department, Shivaji
University,
KOLHAPUR – 416004 (INDIA)
Present
address: (Retd. Prof. of Physics, SU), 17-11-10, Narasimha Ashram,
Official
colony, Maharanipeta. P. O, Visakhapatnam – 530002.
A B S T R A C T
Supergravity
gauge theories have been cited to
establish
the nature of physical processes of constituents
of
cosmic stellar structures. In the
present paper I have
Shown
how the gravitational gauge potentials obtained to be
The
vectors Bba μ in the complex 4 D – space of O(5), in a
twenty
Spin-coefficients
formulation may be incorporated in a new
Gravitational
theory. Further (in the Yang-Mills similitude)
Gauge-spinorial
potentials F αβ together with their potentials
Bμ
are utilized to define a new M - derivative that transports
a
vector, along a time-like vector Uμ . This derivative
is
presented to lead to gauge-covariant collineations.
(GRG
Conference, Pune 1983). There are two-fold mechanisms
That
are implied by the present theory that govern the possible
Physical
processes. One involves terms that signify the
Interaction
of an iso-scalar field with Massive spinorial
particles.
The other is due to the breakdown of an enlarged
Symmetry
of gravitons and gravy quarks resulting in new physical
processes.
They are mediated by both the neutral fields and
Charged
spinorial currents. In particular a process like KL à
è
μe-
, i.e. mediated by a direct exchange of E Boson
corresponding
to neutral gauge current J [34] has been pointed out
in
the generator scheme of SL(2,C)/ SU(2). It is interesting to
note
that these processes transpire at high energies, and the
manifest
gauge potentials, are generated by local iso-spin
transformations
that mandate on a wave function defined at a
space-time
point x. (Edington Centenary Symposium, Nagpur 1984).
126.
K. L. Narayana, ”on Spinorial and Materialistic optical Cosmod tensor Invariants
and Cosmod Gravity”, 73rd Sess. Ind.
Sci. Cong. Delhi January 6th, Physics
Section, 1986 and 72nd Sess. of Ind.
Sci.Cong. Lucknow, Mathematics section,
January 6th, 1985.
ON
SPINORIAL AND MATERALISTIC OPTICAL
TENSOR
INVARIANTS AND COSMOD GRAVITY
K.
L. Narayana
Physics Department, Shivaji
University,
KOLHAPUR – 416004 (INDIA)
Present
address: (Retd. Prof. of Physics, SU),17-11-10,Narasimha Ashram,
Official
colony, Maharanipeta. P. O, Visakhapatnam – 530002.
A
B S T R A C T
Spinorial and
materialistic optical shear, rotation
and
deformation tensors are defined and the fundamental
equations,
employing these, for the propagation of a null
gravitational
field have been formulated in the Extended
Newman-Penrose
spin coefficient formalism. The four-
dimensional
0(5) gauge space of inhomogeneous SL(2,C) x
SU(2)
supergravity theory has been used. The theorem,
as
follows is enunciated. “If a small
spinorial-
cosmod”
object in a null geodesic congruence casts a
shadow
on a screen, all portions of the shadow hit the
screen
simultaneously, but the shape, size, orientation
and
spinorial (cosmod) polarization of the shadow depend
only
on the location of the screen, not on its world
velocity. The shadow is thus spinorial expanded, iso-
spinrotated
and cosmod sheared”.
Next cosmod
gravity, in the context of large number
Hypothesis
of Dirac has been shown to arrive at the number
0.354x10-39
with quantum cosmod gravity range formula
τ= ( n ћ/ (2 e 2
∇f
c2 )).
ACKNOWLEDGMENT
The author is indebted to Late Prof. K. R. Rao,
D.Sc. (Madras) D.Sc.(London) of
Andhra University, Waltair ( in the years 1932-1972) for
his interest and guidance
in promoting my research
endeavor.
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