Articles and Publication Physics Quantum physics TEMPORAL REALITY OF PHYSICAL CONTINUUM
TEMPORAL REALITY
OF PHYSICAL CONTINUUM
© Oleg Orestovich
Feygin
Northeast Advanced Researches
Projects Agency
Institute of
Scientific & Technological Researches
Ukrainian
Academy of Sciences
Kharkov, Ukraine
Contact to author:
fond@online.kharkiv.com
http://www.geocites.com/fond_nauka
It is natural to count, that any new theory
including chronoquantum mechanics, represents in the basis only the relative
true, but it, certainly, does not give the foundation for the prior
non-recognition of new ideas brought by it and concepts. Chrono-physical
concepts of this or that shape, undoubtedly, will
undergo the further development, but most likely, their evolution will go aside
the further withdrawal from classical representations of a quantum mechanics. In
accordance with structurization of physical reality to become clearly, that the
development of new chronoquantum's representations
will be accompanied by origin of a lot of metaphysical
problems of the bound with the analysis the nature of
an enclosing material world. Similar problems directly or indirectly concern
connection between tools of observation of appearances
and parameters of microscopic
objects, and fundamental concepts of probability of the fresh wording principle
of causality.
In the present conferring the further
development of the conceptual plan of model
operations of processes temporally localizations
of microscopic objects in boundaries of the chosen existential continuums is
considered. Further properties of wave
functions, as solutions for analogs
of Schrödinger equations are comprehensively analyzed. Based on the
obtained outcomes comparisons and deductions about applicability of a principle
of superposition of chronoquantum's states
are made at temporally localizations
of microscopic objects on strict sequence chosen continuums.
Thus dualism of a phenomenological covariance of model build-ups discrete
temporalogy by engaging
of some reference procedures from mathematical methods of physics. The given
methods, first, include the homogeneous linearization at theoretical exposition
of dynamics of localization of the material microscopic objects. It is shown,
that model interpolation of special sections of a quantum mechanics and a field
theory can be reached by contextual installation of the linear quantum
functionals, the bound with properties of metric space, and a perfect vacuum.
Radiating from far-reaching analogies, in a
basis àòåìïîðàëüíîé concepts
of development of world around the extending model concept uniform
is possible to put fields from which it is possible to
deduce deductively properties of space - time in a continual approximation. The
given concept of discrete temporalogy concerns
to discharge is inductive synthesized conceptual platforms, being inherently,
one of subitems quantum chronodynamic, including the relativistic theory of
discrete chrono-field [7,
9, 11]. One of principal singularities of the new theory is representations
about structure uniform chrono-field, the continuous in an interior frame of
reference and discrete - continual for exterior observer.
The similar problematic enters in relativistic
quantum chronophysics /RQCP/.
Continuity RQCP will
consist in the complete correspondence of its paradigm to main principles of a
reference quantum mechanics, including adequate interpretation
the basic conceptual devices of field theories of a
perfect vacuum and fundamental particles. On epistemological essence, RQCP
supplements variability of the modern unifying
physical theories of space and time. In ontological plan, RQCP structurization's
accepts of
causal relationships, spreading them on all without elimination the material
appearances of an enclosing real.
For quantum mechanical processes by
boundary magnitudes Planck parameters, and as the following point of a temporal
dial, obviously serve, it is necessary to count a lifetime of the easiest
virtual particles. Given temporal distance determines
kinetics of localization of microscopic objects on chosen temporal
envelopes of an existential continuum /CTEEC/
[7 - 9]. Their existence can be connected, both with
cosmological aspects, and with a problematic of the virtual structures in a
perfect vacuum [1, 4].
The quantum mechanical exposition of behaviour of
microparticles is grounded on several fundamental deductions among which the
major are principles of a wave-corpuscle dualism and indeterminacy:
Δp Δx ~ ΔE Δt ~ h (e) h (t);
(1)
Where p
- impulse; x
- coordinate; E
- an energy; t
- time; h(e)
- chronoquantum; h(t)
- energyquantum. According to (1) velocity, as well as
impulse of a particle cannot have a defined value simultaneously with its
coordinates. However, the product of a velocity and time gives mechanics
transition of a microscopic object, as magnitude obviously smaller the Planck
length compared to a fundamental metric size of a mesh of space
[5]. Therefore lack at a particle of a velocity
simultaneously with coordinates means, that if the position of a particle is
localized in the present instant through chronoquantum
its coordinates will already not have any defined
value. In a frame of reference of the given localization there is only some
probability of a determination of a particle in this or that point of space,
hence, the concept of a trajectory loses the sense. Purely on other the
situation will look on the part of the extraneous "timeless" observer,
for it passage of a microscopic object to new parameters will mean its
localization in next CTEEC. The quantum mechanical undular psi-function, which
quadrate of the module gives a probability distribution of a determination of
microparticles in space, too interpretation in
chronophysics, as assigning probability of localization of a microscopic object
on chosen CTEEC. Accordingly, probability amplitudes CTEEC
- in an operational aspect [6] will look like
localizations
{T(b)} = <T(b)|T(a, b)|T(a)> = S
<T(b)|T(i)><T(i)|T(a, b)|T(j)><T(j)|T(a)>, <T(b)|T(a)> =
S <T(b)|T(b-a)><T(b-a)|T(a)>, <T(b)|T(a)>
= S <T(b)|T(i)><T(i)|T(a)>, <T(j)|T(i)>
= d(j,i), <T(b)|T(j)> = S <T(b)|T(i)><T(i)|T(j)>;
(2)
where T(a),
T(a, b),
T(b), T
(i), T
(j) -
the CTEEC of terminating, transitional and intermediate states, accordingly;
i =
a, b-a,
b, …, (b> a)
- sequence of the CTEEC; d
(j, i)
- a Kronecker's delta. Probability amplitudes of localization's processes in a
complex conjugate to amplitudes of inverse passages and from the point of view
of the nonrelativistic quantum mechanical analysis represent outcome of an
approximation for infinitesimal intervals of time.
In a classical quantum theory, the undular
psi-function defines a state of a system on all a time interval of its existence.
From here it is usually concluded, that the derivative on time from an undular
psi-function should be determined by a value of function:
dψ /dt = <L>ψ = (2π i
/ h) dS /dt = (2π
i / h) <H>ψ, ψ = const exp[ i S / h(e) h(t)], <L(d)>ψ
= Δψ / h(t) =
= [2π i / h(t) h(e)] ΔS / h(t) = [2π
i / h(t) h(e)] <H(d)>ψ. (3)
where <L>,
<H> and
S -
quantum mechanical analogs of operators of Lagrange, Hamilton and a mechanical
operation. Operationally - differential equalities (3) make one of the basic
groups of the equations of chronoquantum's mechanics.
At the complete identification of an aspect of a quantum mechanical Hamiltonian
it is possible to count, that the equations (3) determines undular psi-functions
of the given physical microsystem.
Discrete - temporal aspect of the relevant
quantum mechanical Lagrangians can be installed to similarly common quantum
mechanical principle of operational representation of physical quantities, at
passage to semiclassical exposition of some wave function In turn it can be is
interpreted as comparison to any microplants of a chronodynamic operator, a
defining requirement of its localization on chosen CTEEC. Relations (2) and (3)
also contain discrete-temporal a
pre-image of the basic analytical shapes of a quantum mechanics
- Schrödinger
equations in various representations.
To one of temporal's researches directions
is chronophysics a
perfect vacuum, the filled the subpartial virtual particles. Aspects of detailed
elaboration of solutions in the given problematic are bound to an extension of a
definition chronoquantum's Hamiltonian
of the free particles as
<H(d)> = const [h(t) h(e)]^2 <L(d)>.
(4)
It is obvious, that the generalized aspect
of the chronoquantum's mechanical equations
of an aspect (3) with Lagrangians (4) similarly classical fashion of a Schrödinger
equations for the free particle with the solutions linking wave-corpuscle
performances through chronoquantum's parameters.
In classical representations of a quantum mechanics, the wave function should be
the unique, the continuous, and terminating in all metric space.
The Schrödinger equations for the free
particle have the relevant terminating solutions including an ionization
continuum of energies. The bound particles obey terminating solutions at a
discrete energy distribution. At multiparticle ensemble of interdependent
microparticles, the complete gang of coordinates in multivariate configurational
space determines the wave function. Passing to chronoquantum's
mechanics, it is possible to note, that the ionization continuum of
microparticles corresponds them to localization in boundaries particular CTEEC
at determination of their world lines. It follows, as
from common principles õðîíîäèíàìè÷åñêîé
digitization of physical event's space and from
interpretation their
quantum mechanical analogs:
|T(b)> = S |T(i)>
C(i), C(i) = <T(i)|T(b)>, |T(a)> = S |T(i)>D(i),
D(i) = <T(i)|T(a)>,
<T(b)|T(A)T(B)|T(a)> = S
<T(b)|T(i)> <T(i)|T(A)|T(j)> <T(j)|T(B)|T(z)> <T(z)|T(a)>,
T(b) = S <T(i)|U(b
– a)|T(j)> T(a) = S {d(i, j) – const H[T(a)]
(b – a)} T(a); (5)
here C(i),
D(i) -
populations of base quantum mechanical embodyings in õðîíîêâàíòîâîì
representation for localizations on next CTEEC; Ò(À)
and Ò(Â)
- the chosen frame of references. The equations (5)
illustrate a principle of chrono-relativism, consisting in various levels of
identification of a microscopic object depending on a temporal aspect of
references. Formulas (2)
- (5) can be interpreted also in language of
psi-functions through concept of probability amplitude of localization of some
CTEEC. Accordingly, localization in next CTEEC will be featured the following
linear combination of psi-functions:
ψ = const(1) ψ(1) + const(2) ψ(2),
|ψ|^2 = |const(1)|^2 |ψ(1)|^2 + |const(2)|^2 |ψ(2)|^2 +
+ {const(1)* const(2) ψ(1)* ψ(2)* +
const(1) const(2)* ψ(1) ψ(2)*}. (6)
Formulas (6) determine a principle of
chronoquantum's states superposition, adequate to model representations about
properties of chrono-functions "to sew together" next CTEEC in uniform
chronodynamic's structure.
Nevertheless, it is possible to assume, that there is a group of temporal's
models where the given amplitude can vary depending on
a position of plant on direct of substantial time.
Thus, the amplitude of each complete localization will be proportional to
amplitudes of localizations on the next envelopes, increased on a series of the
weight coefficients similar to quantum numbers.
In the most common sense of the equation
(6) define regularities of quantum's chronodynamic. Radiating from earlier
obtained temporal reinterpretation [2,
3] the basic equations
of a quantum mechanics for transtemporal matrixes,
it is possible to enter correctly enough concepts about the one-dimensional
linearization of strictly sequential population developing CTEEC:
<T(b)|T(b-a)|T(a)> = <T(n+1)|T(n)|T(n-1)>
=> |T(b-a)> = S |T(n)><T(n)|T(b-a)> = S
|T(n)> C(n). (7)
It is known, that properties of the wave
functions, satisfying to solutions of a Schrödinger equations, have common
character, including uniqueness, a continuity and a finiteness. For
chronophysics, it means an identification of a frame of reference with some
chosen CTEEC. Then the Schrödinger equations for the free particle will
have terminating in all space CTEEC of
a solution at any positive and zero value of an energy, making the continuous
energy distribution.
In case of the bound particle, the quantum
theory predicts presence of a discrete spectrum, at a wave function of points of
multivariate configurational space. Here the direct analogy between processes on
strict sequence CTEEC is
observed.
Conceptually - logic connections between
next CTEEC are grounded on analog of a principle of superposition of
psi-functions. Owing to an operation of the given principle a Hamiltonian of the
linear wave equation of the made system at inverse of a frame. The operating
invariance of a specular reflection in quantum physics reduces in a spatial
parity conservation law of a quantum state. The spatial parity conservation law
determines inversion of psi-functions
with deviation them on even and odd. A spatial parity conservation law it is
partial regulates probability of a generation - dissipation of the made systems
with maintenance of a moment.
Together with a principle of an
indistinguishability of microscopic objects, quantum conservation laws govern
appearances of trans-localization, appearing for the detached onlooker as
temporal change of actual events. Relocating of adequate
microscopic objects in boundaries of the arbitrary dual system corresponds to
the following equality of analytical shapes:
ψ[j (1), j
(2)] = exp(i a) ψ[j (2), j
(1)] = exp(2 i a) ψ[j (1), j
(2)] = ± ψ[j (2), j
(1)],
ψ[j (1), j
(2)] ~ ψ{n[j (1)]} ψ{k[j
(2)]} ± ψ{n[j (2)]}
ψ{n[j (1)]}. (8)
where j
(1), j
(2) -
populations of coordinates and spins of microparticles. The relation (8) shows
that the system of two identical particles can be featured the symmetric
transformation by
psi-functions. In quantum terms, the symmetry of psi-functions is defined to a
spin of particles. To the particles possessing a half-integer spin,
antisymmetric psi-functions are compared, and with particles to an integer spin
- the symmetric.
The surveyed group of chronoquantum's
principles of continuum's
digitization should be spread and to a perfect vacuum,
for example in representation of Dirac. Under the theory of Dirac of property of
physical space were defined by vacuum as a world material background. In the
modern quantum mechanics, all fundamental particles are considered as quantums
of the relevant field structures that for a physical system of vacuum is
interpreted, as a population of fields without actual particles. It is known,
that under laws of a quantum mechanics for any field oscillations are
characteristic.
In case of a perfect vacuum, it will be
so-called "zero" oscillations accompanying with a birth and vanishing
of virtual particles, relevant to the nature of each concrete field. Realization
of the universal law of conservation of energy demands for the given virtual
particles of observance of fundamental property of specifically short lifetime.
According to principles of chronophysics, it can mean presence the temporal-virtual
localization, parting next CTEEC.
Macroscopic display of the virtual
properties of a perfect vacuum by probably only mediate fashion in effects of
Lamb detrusion of levels of lines of atoms, attractions of plates in vacuum, the
abnormal moment of magnet of electrons and interaction of quantums. Quantum
chronophysics it is
possible to count other important corollaries of appearances tunneling and
superconductivity.
The obtained outcomes (3 - 8) for linearization
of microobject's localization in view of influence of virtual particles of a
perfect vacuum will gain a final aspect:
<T(b)|X|T(b-a)|Y|T(a)> = <T(n+1)|T(n+1/2)|T(n)|T(n-1/2)|T(n-1)>;
(9)
where X
and Y
- factors of the virtual localization;
T(n+1/2) and
T(n-1/2) -
relevant the virtual CTEEC. Thus, the virtual properties of a perfect vacuum can
be featured in terms localizations,
switching it in the common plan of digitization.
The physics of virtual particles supposes their origin not only in vacuum. It is
considered, that they constantly arise and disappear near to fundamental
particles and at their interaction. Thus, the virtual partial electrocharges act
the virtual positrons and electrons, polarizing enclosing vacuum. Because of
polarization of vacuum around of charged particles, there is the bound with them
the structural pulsatory charged envelope reducing their effective charges that
is exhibited in macroscopic effects of interpartial interaction.
From point of view RQCP,
it can be interpreted, as the virtual localization of
quantum microscopic objects in borderline fields or in other methodological
approach, as a delocalization on the virtual CTEEC. Their participation in
processes of localization can
be presented as a modification of a spectrum of eigentones chrono-fields. Here
actual enough and debatable problem identification of the virtual processes on
terrain clearance makes axes of temporal events.
Radiating from principle terrain clearance virtual particles, it is possible to
assume, that their occurrence is bound to interaction of next envelopes CTEEC.
Further, it has been shown [6], which the
probability amplitude of the basic passage from one CTEEC in another is equal to
the total of products of amplitudes of the intermediate and terminating
localizations direct and conjugates representation:
{T(b)} = <T(b)|T(a, b)|T(a)> = S
<T(b)|T(i)> <T(i)|T(a, b)|T(j)> <T(j)|T(a)>,
<T(b)|T(a)> = S
<T(b)|T(b-a)> <T(b-a)|T(a)>, <T(b)|T(a)> = <T(a)|T(b)>*,
<T(b)|T(a ® 1, b ®
¥ )|T(a)> = <T(b)|T(S)|T(a)> = S
<T(i)|T(S)|T(j)>|T(a-1)> = <T(a-1, a)|T(a)>,
<T(b)|T(a-1)> = <T(b)|T(a-1, a)|T(a)>,
<T(i)|T(a-1)> = <T(i)|T(a-1, a)|T(a)>; (10)
where T(a),
T(a. b),
T(b), T(i),
T(j) -
the CTEEC of terminating, transitional and intermediate states, accordingly;
i =
a, b-a,
b, …, (b> a)
- sequence CTEEC. Probability amplitudes of localization's processes in a
complex conjugate to amplitudes of inverse passages and from the point of view
of the nonrelativistic quantum mechanical analysis represent outcome of an
approximation for infinitesimal intervals of time.
From relations (10) follows:
<T(i)|T(a-1)> = S
<T(i)|T(a-1, a)|T(j)><T(j)|T(a)>, T*(i, a-1) = S
T*(i, j),
|T(i)|^2 = const / {exp[ i E t / h(t) h(e)]} = =
IT[E(0), t(0)]|^2 / {exp[ i t / h(t)]}^[E / h(e)],
<T(b)|T(a)> = S
<T(b)|T(i)><T(i)|T(a)>, <T(j)|T(i)> = d(j,i), <T(b)|T(j)>
= S <T(b)|T(i)><T(i)|T(j)>,
|T(b)> = S |T(i)>C(i),
C(i) = <T(i)|T(b)>, |T(a)> = S |T(i)>D(i),
D(i) = <T(i)|T(a)>, <T(a)|T(b)> = S D(i)*
C(i), <T(b)|T(A)|T(a)> = S <T(b)|T(i)><T(i)|T(A)|T(j)><T(j)|T(a)>,
<T(b)|T(A)T(B)|T(a)> = S
<T(b)|T(i)> <T(i)|T(A)|T(j)> <T(j)|T(B)|T(z)> <T(z)|T(a)>;
(11)
Here C(i),
D(i) -
populations of base quantum mechanical embodyings in
chronoquantum's representation
for localizations on next CTEEC.
Identification of the complete population
strictly sequential localizations on CTEEC means terrain clearance determination
of world lines of the material plants. It follows from common principles to
digitization of physical events and can be interpretation, as chrono-relativism
consisting in various levels of identification of a microscopic object depending
on a temporal aspect of
reference frame. Thus, the amplitude of localization can vary depending on a
position of plant on direct of time
and will be proportional to probabilities of next envelopes, increased on a
series of weight coefficients:
T(b) = S <T(i)|U(b–a)|T(j)>
T(a); U[T(b), T(a)] = d(i, j) – const H[T(a)] (b–a),
T(b) = S {d(i,
j) – const H[T(a)] (b–a)} T(a), const [T(i) – T(i+1)] / h(t) = S
H[T(a)] T(i) <T(b)|T(b-a)|T(a)> = <T(n+1)|T(n)|T(n-1)> => |T(b-a)>
= S |T(n)> <T(n)|T(b-a)> = S
|T(n)> C(n); (12)
where U(a,
b) = <b|U|a> - a
matrix of trans-temporal localizations
of the material object. In the most common, sense of expression (11) and (12)
define of discrete-temporal interpretation the
basic equations of a quantum mechanics for trans-temporal
matrixes. Here there is a possibility enough correct
introduction of a conceptual means for covariant homogeneous - linearized
translations of the material plants of a microcosmos on strict sequence
developing CTEEC. Thus, following the entered nonconventional chrono-quantum
mechanical nomenclature, we shall consider, that the
probability amplitude trans-temporal passage
between strictly next localizations of analog of the same material plant on
population CTEEC will
make
P[U(a, b)] ~ const F* i / h(t); (13)
where F*
- the dimensionless energy potential of a quantum
microscopic object.
The carried out examination shows,
that the scientific - materialistic analysis of the modern state of a
problematic of harmony of quantum and cosmological appearances can be
successfully supplemented important semantic component RQCP. Basic building
blocks RQCP are model
plans of self-consistent interaction of quantum microscopic objects in temporal
boundaries of chronoquantum's magnitudes
and relevant to them principles of a relativistic covariance and conservation
laws. Special complexities in RQCP arise
at attempts discrete analysis of canonical relations of a relativistic quantum
theory of a field, but already prestress outcomes show their possibility of
interpretation on a
conceptual basis of discrete quantum temporalogy [10,
11].
In an inference it is necessary to note,
that examination problems of chronophysics has
the important heuristic value and can help with the analysis of shortages of old
theories and build-up new, more adequately fundamental physical regularities
formative a uniform pattern.
REFERENCES
1. Feygin O.O. Discrete - temporal model of
Universe // SciTecLibrary (2003). - http://www.sciteclibrary.ru/eng/catalog/pages/5159.html
2. Feygin O.O. Discrete principles of
quantum chronodynamic // Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/5200.html
3. Feygin O.O. Quantum-theoretical
chrono-discretization // Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/5201.html
4. Feygin O.O. Cosmological principles of
quantum chronophysics // Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/5296.html
5. Feygin O.O. Chronodynamic
reinterpretation of Planck’s lengths // Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/5348.html
6. Feygin O.O. Temporal quantum functionals
// Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/5658.html
7. Feygin O.O. Concepts of quantums
chronophysics // Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/5813.html
8. Feygin O.O. Mechanics of chrono-quantums
// Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/5978.html
9. Feygin O.O.
Quantum temporallogy // Ibid. - http://www.sciteclibrary.ru/eng/catalog/pages/6375.html
10. Feygin O.O. Model
linearization of quantum chronodynamic //
SciTecLibrary (2004). - http://www.sciteclibrary.ru/rus/catalog/pages/7015.html
11. Feygin O.O. Principles
of chronoquantum mechanics // Ibid. – http://www.sciteclibrary.ru/rus/catalog/pages/7016.html
Publishing date: April 20, 2004
Source: SciTecLibrary.ru
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