QUANTUM
GRAVITATION.
The certificate of
the copyright ¹ 8493 – 30.09.2003ã.
The state
department of the intellectual property.
(has
translated daughter Olga)
For the first time the concept of gravitation of
classical laws of gravitation has been determined by
Within the framework of the Quantum Theory of
the Relativity, in technology of dynamical axioms, Quantum Gravitation is
created.
In
1. PROBLEMS OF THEORIES OF GRAVITATION.
Now gravitational interaction is well
investigated, submitted in mathematical models, and laws of gravitation are
used in practical calculations.
Problems of gravitation begin at definition of
mathematical true of laws of classical gravitation of
In classical gravitation of
F=GMm/R2, F=gm,
at overlapping the centers of cooperating weights
(R→0), forces of gravitation (F → ∞), and acceleration of
" free falling » (g→ ∞)
weights (m) is equal also, in a gravitational field grow indefinitely.
On the one hand laws of gravitation are valid
and reflect real gravitational interaction of weights. On the other hand in the
nature there are no infinite forces and is accelerated.
This fundamental problem of mathematical
true, in real laws of classical gravitation of
Infinite growth of acceleration of weight in a gravitational
field, gives indefinitely big speeds of this weight. However after creation of
the Special Theory of the Relativity it was found out, that speed of weight cannot exceed
speed of light . For Einstein imperfection of classical gravitation of
Already in the General Theory of the
Relativity dynamics of Criteria of Evolution in space of speeds had
relativistic limits. The classical law of gravitation of
F=GMm / R2(1-GM / Rc2), (GM / R)<<c2 .
This equation follows from the equation of
relativistic dynamics existential a component already in a gravitational field.
1).c2
– (1/2)(cx2 = GM/R) = (cY2
= Ï ≠ 0); 2). c2(1 –
GM/2R c2) = ( ÏY ≠ 0) = c2; 3). (X2/T2)(1 –
GM/2R c2) = (ÏY ≠ 0) = c4/c2,
4). X2(1 – GM/2R c2)
= ( ÏY ≠ 0) = c4/b2 = (F=Ï2)/(F/m)2, 5). F= m2/X2(1 – GM/2R c2), 6). m2 = GM2, (G)1/2
= cosαX
7). F= GM1M2 /
X2(1 – GM/2R
c2),
Such equation in turn, follows from the law of
preservation of full energy (E = mc2), which Einstein has taken for
a basis. With high accuracy of calculations, such equation gives a real
deviation of rays of light in a gravitational field of the Sun. In strict
mathematical trues it passes in òåíçîð Einstein in Riemann’s space,
PKT – (1/2)PgKT = kTKT
as the equation of the General Theory of the
Relativity.
Already distances of the centers of
weights could not approach up to zero (R≠0). And the space of speeds in a
gravitational field, with nonzero gravitational ( Ï ≠ 0) potential, could not
exceed speed of light
cx2 << c2 .
Problems of classical gravitation of
It is necessary to note, that tensor of Einstein it is
mathematical true of Riemann’s space in Einstein's conditions, as the
multiplication table. To change if it is impossible.
And with physical interpretation in a gravitational field, Einstein could think
up this mathematical true only. It is possible to argue on physical ideas or
conditions applications òåíçîðà Einstein. But nobody can already change this mathematical true of
"multiplication table", a potential field in Riemann’s space.
In a basis of mathematical true òåíçîðà Einstein Einstein's deep physical
idea – a difference of relativistic dynamics in two points of a potential field
submitted Riemann’s tensor lays. And on Einstein's (g
KT)1/2 = 1 conditions, one of them is resulted to
In it essence of
classical relativistic gravitation. And classical gravitation of
However this, not last in
RG
= GM / c2.
In a surface of such sphere R = RG which have named « a black hole »,
forces and acceleration of weight (m) in a gravitational field of such sphere,
again increase is boundless. Such forces are not present in the nature. If
force of gravitation indefinitely big, our planet already would be in the
nearest to " a black hole ». However we sit and
we read further.
Einstein has devoted this problem
whole clause (Å.t.2, page 514, 1939 year.). It has noted in particular: « …Shvarcshuldovsky’s singularity at r = 2GM / c2 , are absent
in the nature as the substance cannot be concentrated arbitrarily, otherwise
particles it is achieved speeds of light ». So the founder of classical
relativistic gravitation of the General Theory of the Relativity has told. In
technology of dynamical axioms, the mathematical true of such statement
consists that
RG/K = cosαX = (G)1/2
, RG < K , K = (Y2/Y0) , RG = Y0 ,
at presence of a constant(G), gravitational
interaction in this case, the radius of curvature of a trajectory K, always is
more than radius of sphere of gravitational radius RG. From here impossibility of radial speed limit of light in a
potential field of mass trajectories,
in mathematical trues.
Such problems of mathematical true R = RG
in Einstein's classical relativistic gravitation, and (R=0)in
classical gravitation of
Question, what laws of real
gravitation, without problems?
Presence of the specified problems in
mathematical trues of theories of gravitation defines
areas and conditions in which these theories of gravitation are void. In this
connection there is a set of the questions which are not having answers. For
example:
- that such the
center of weights (R=0)?
- what gravitation in
the center of weights or on a surface of sphere of gravitational radius if
forces of gravitation are not infinite? What laws of these forces of
interaction in the center of weights?
- that such
gravitation in general? What relationships of cause and effect of gravitation
with other fundamental forces of interaction, in uniform spaces - matters?
As a matter of fact, after creation of
classical gravitation of
c2 – (1/2)cx2 = (cY2 = Ï = gR),
This question has remained open, and not solved
in the theory.
2. The question quantum potential (Ï = gKT), fields of gravitation «
outside of a powerful matter », has remained open.
3. Program of Maxwell « … descriptions (the author -
uniform) a physical reality by means of fields », has remained not executed.
4. The question internal spaces - matters of
sphere of gravitational radius R<RG of a powerful matter, as well
as a sphere - point of an individual, indivisible charge, has remained open.
However the physical reality uniform spaces -
matters nevertheless comprises decisions of all these questions and problems.
With finding-out of laws of quantum
relativistic dynamics in « the Quantum Theory of the Relativity », there is an
opportunity to define mathematical trues of quantum
potential fields. As the component, speech about quantum potential fields with
existential components of Electromagnetic (Y+ = X-) and mass (Y- = X+) fields of
interaction separately, in uniform Y+ = X-), (Y- = X+) spaces - matters the question is quantum
relativistic dynamics existential. Thus there are conditions of transition from
one potential fields
to another’s.
Equations of Maxwell are mathematical true of
a special case of the integrated equations of Electro strong Interaction of
nucleons of a nucleus. (« Electro strong interaction of a nucleus
»). Then quantum relativistic gravitation should comprise mathematical trues:
- classical and
quantum relativistic dynamics with conditions of transitions,
- electro strong
interaction of nucleons of a nucleus,
mathematical true of
Einstein’s tensor in the General Theory of the Relativity, as special case
fixed (gKT
= const), (gKTC = 0), conditions in variable (quantum)
gravitational potentials (gKT ≠ const), (gKTC
≠ 0)
mathematical trues of laws of classical gravitation,
Except for it mathematical trues of quantum potential
fields of gravitation, should contain conditions of transition to
quantum potential fields of electric
charges without mutual exception in uniform spaces - matters. For example, the
indivisible quantum of a space - matter of a proton has weight which forms a
potential field of gravitation, and a
charge which is consequence of its potential electric field. And mathematical trues
of quantum potential fields should solve:
Problems of infinity and uncertainty laws of
classical gravitation (R → 0), in the center of weights or charges,
and relativistic gravitation (in a surface of sphere R → RG).
problems of sources
of a potential field of gravitation and a charge,
quantum character and
properties of such potential fields,
- conditions of
transition to classical potential gravitational and electric fields.
The decision of such problems and
tasks opens new prospects. These problems are solved behind frameworks of the
modern theories created in
2. QUANTUM
GRAVITATION.
In dynamical axioms uniform spaces - matters,
covariant dynamics vector a component of charging and mass fields is considered
in allocated directions of
For each of them in conditions of
Global and Local Invariancy, the uniform mathematical
true of classical and quantum relativistic dynamics is submitted.
In uniform consideration
relativistic of covariant dynamics vector a component of charging and mass fields
in allocated directions of Euclid’s space (in conditions of turns with
displacement within the limits of a dynamical corner of parallelism of
trajectories), the mathematical true of deformation of Euclid’s space is
submitted. Thus appears quantum a potential field, as consequence.
The fixed difference of such quantum
relativistic dynamics in two points (1 and 2) gives the fixed potential field
in mathematical true òåíçîðà Einstein. However the internal maintenance of such quantum or fixed
potential field, and physical essence of relativistic gravitation, as against
of Einstein’s tensor, it is opened in a full kind, including charging and mass
fields of substance as a whole. Causes and effects of such quantum or fixed
potential field are opened. In the General Theory of the Relativity the fixed
points of a potential field of large-scale quantums
of a space - matter of planets, stars, galaxies are
considered.
In separate consideration of
charging fields, in same mathematical true, the submitted transformations pass
in electromagnetic dynamics with mathematical true of equations of Maxwell.
Such equations give an induction of mass fields and an induction of
relativistic weights in variable fields of Strong and Gravitational
Interaction. They are similar to the equations of an induction of a magnetic
field in a variable electric field. Speech about the
equations of the gravitational waves similar to electromagnetic waves.
In both cases in a full kind, the
component uniform the spaces - matters, submitted in the theory of "
Electro strong interaction of a nucleus », with precisely certain conditions of
dynamics of electromagnetic and gravitationally-mass fields of interaction in
uniform spaces - matters the question is mathematical true the integrated equations
of dynamics vector.
Both conditions of the integrated
equations of dynamics, are submitted in a uniform case
Globally invariant uniform to a space - matter. Dynamics of such trajectories
in the closed contour, within the limits of dynamical corners of parallelism of
trajectories with quantum relativistic dynamics ,
gives quantum charging and mass potential fields within the limits of
corresponding constants of interaction.
In technology of dynamical axioms, Locally invariant conditions of quantum relativistic
dynamics in quantum charging and mass fields of interaction separately are
determined. By the example of quantums of a space -
matter of indivisible protons and an electrons,
Locally invariant conditions of quantum relativistic dynamics are considered.
These are conditions of the closed contours of trajectories, with a dynamical
corner of parallelism, within the limits of corresponding constants of
interaction. Such conditions in mathematical trues
give a quantum field of Strong Interaction of a proton and a quantum electric
field of an electron. In the same mathematical trues
conditions of formation of the charged and neutral quantums
of Strong Interaction of nucleons of a nucleus in electro strong Interaction
are considered. Levels of quantum gravitational fields, since a nucleus of
atoms are submitted.
Quantums of Strong Interaction of a nucleus
of planets, stars, the galaxies corresponding to their nuclear matter are
submitted. Already in the center any weight or a charge, (in conditions
of Local Invariancy, in technology of dynamical
axioms) the closed contours accordingly charging or mass trajectories (with
quantum relativistic dynamics take place within the limits of dynamical corners
of parallelism). The nonzero radius of
these closed contours, in mathematical trues, passes
in quantum dynamical "surface" of «a black hole ».
Thus, in strict mathematical trues solve fundamental problems of classical gravitation
of
The law of return squares of
distances follows from ratio in mathematical trues of
quantum relativistic dynamics for radial forces. It used by
In technology of dynamical axioms
limiting (hc) radiuses of action of such radial
gravitational forces of usual substance of atoms are submitted. Radial forces
deformed
Such forces in mathematical trues,
pass on the strength of classical gravitation of
Thus:
- the
submitted mathematical trues of a space - matter in
the dynamical axioms - facts, solve the specified problems as tasks. These
decisions have the coordinated models of all types of fundamental interaction
and their relationships of cause and effect.
- in these
mathematical trues conditions of transition between
types of fundamental interactions are shown.
- classical and
relativistic forces of gravitational fields are a special case of the general
quantum radial forces in power levels of physical vacuum.
- in mathematical trues problems of infinity and uncertainties of classical
and relativistic theories of gravitation are solved.
- power levels of
physical vacuum, with potential fields of radial forces of interaction in these
levels, on extremely big and extremely small distances Are submitted.