Articles and Publication Physics Quantum physics DISCRETE PRINCIPLES OF QUANTUM CHRONODYNAMIC
DISCRETE
PRINCIPLES OF QUANTUM CHRONODYNAMIC
© Oleg O.
Fejgin
Contact to the author: tor@3s.kharkov.ua
The concept Planck’s quantum of action plays
one of central roles in the modern theoretical physics. Quantum postulates are
bound to fundamental structure of space - time and conservation laws that forms
the periodic attempts their re-interpreting at build-up of new physical theories.
The present article prolongs a cycle of examinations on formalization of a
quantum nature of space - time and is interlinked to development of theoretical
models on a basis locally - discrete fashions [5].
Let us consider quantum-mechanical oscillator
with a discrete gang of energies of oscillations [1]:
Ei = i hn , i = 0, 1, 2, 3, n, (1)
where h-quantum of action, n -frequency. The
thermodynamic probability of their embodying will make [2]:
Wi = W0 exp (-ihn / kT), i
= 0, 1, 2, 3, n, (2)
where kT-thermodynamic temperature.
Let us enter the formal definition for
probability of microscopic event from the equation (2), as time localization
during some allocated interval [3]:
W(t) = W0 [exp (ht n )]-ih(e)/kT,
(3)
where expression
Wt = exp (htn ) (4)
defines probability of time localization, and for
quantity ht from the formula (1) follows:
ht = Ei / ihen or
h = he ht; (5)
Here ht and he-builders of
quantum of action, in other words chrono-quantum and energy-quantum.
Let us carry out similar reasoning’s for
extension of a definition an analytical view of factor W0 from the
equation (3), the given term is bound to probability of existential localization
with underloadly possible energy for a viewed physical micro system. Norming W0
on individual aggregate probability of all probable localizations gives:
W0 = 1 – Wt-h(e)/kT.
(6)
In view of the formula (6) expression (3) can
give the following view:
Wti = Wt-ih(e)/kT
– Wi-(i+1)h(e)/kT. (7)
The relation (7) can give quite particular
physical sense if to take into account, that equality (4) is the trivial shape:
Wt = exp (-ihtn ). (8)
Then the equation (7) transfers in
Wti = Wtih(e)/kT
– Wt(i+1)h(e)/kT. (9)
From the received formula follows, that the
probability of time localization of particular micro event is defined by a
difference of localizations of previous and subsequent events in chrono-quantum
gauge of their development. Transferring to a wave mechanics, we compare to the
arbitrary microscopic object a wave amplitude ψ, satisfying to a canonical
wave equation [3]:
Δψ + const ψ/l 2 = 0,
(10)
where l = const hthe [m (E-U)]-0,5-
a wave length of a microscopic object in mass m in energy representation.
Substitution of the given expression in the equation (10) gives:
Δψ + const m (E-U) ψ (hthe)-2
= 0. (11)
The received relation corresponds to the
reference shape of a stationary Schrödinger equation. Hence, if to follow
traditional interpretation intensity of a ψ-wave in each point of space
corresponds to probability of a presence of a microscopic object in the
allocated micro volume, referred to quantity of this micro volume. Thus, if to
start with re-interpreting quantum relations according to equality (5) and (8)
the basic principle of indeterminacy for coordinate x and an impulse p gets the
following view:
Δx Δp ~ he ht.
(12)
At the fixed mass of a microscopic object the
left-hand part of a relation (12) transfers in
Δx m Δv = mΔx Δdx/dt = mΔ2x
(iht)-1. (13)
Then, both parts of a relation (12) become
mΔ2x ~ he (iht)2.
(14)
Let us note that the shape of the equations (13)
and (14) corresponds to the linear nonrelativistic case of a motion of a
microscopic object. Operating with a principle of indeterminacy for coordinate,
and an impulse of some micro particle, it is possible to assume velocities that
from reasons of dimensionality there is a similar relation for energy E and time
[4]:
ΔE Δt ~ he ht.
(15)
Reference interpretation of the formula (15)
includes concept of indeterminacy of energy of the microscopic object,
determined by time of the given energy localization and re-interpreting at
quantum digitization as
Jhe iht ~ he ht.
(16)
The relation (16) determines probability of joint
localization of the normalized of energy flux ΔE = jhe allocated
conventionally in time interval Δt = iht. At a minimum of
potential energy, U~0 for a linearized problem of a motion of a microscopic
object on a restricted site probabilistic equation (11) transfers trajectories
in
d2ψ / dq2 + const Eψ
(heht)-2 = 0, (17)
Where the q-generalized coordinate. From the
theory of a harmonic analysis well known, those solutions of the equations of a
view (17) are logarithmic functions of type
ψ = ψ0 sin [const qE0,5
(heht)-1]. (18)
Taking into account boundary conditions of an
interval of a motion: ψ=0 at q=q0 it is gained:
Const q0 E0,5 (heht)-1
= i+1. (19)
Expression (19) defines requirements of
digitization for the nonrelativistic energy of a microscopic object as a gang of
i-quantum numbers:
E = const (i+1)2 (he ht)2
. (20)
Thus, consecutive application of a principle
chrono-quantum re-interpreting the basic postulates of a quantum mechanics gives
in original updating trivial solutions of a canonical Schrödinger equation. It,
in turn, corresponds to a new principle chrono-quantization to energy,
re-interpreting as determination of energy levels on temporal sequence of
chrono-quanta’s. Hence, determination of spectral energy of a micro particle
in time boundaries allocated chrono-quantum may transit with the most probable
quantity:
E0 = const (he ht
q0-1)2. (21)
It is necessary to note, that though values of a
zero-point energy at quantum micro particles essentially depend on character of
fields of forces at zero of thermodynamic temperature exists fundamental
chrono-quantum interval with terrain clearance probability of localization of
events.
REFERENCES
- Aspects of Quantum Theory / Ed. A. Salam, E.
Wigner. - Cambridge.: CUP, 1972.
- Audi M. The Interpretation of Quantum
Mechanics. - Chicago: USP, 1973.
- Slater J. C. Concepts and Development of
Quantum Physics. - N. Y.: DP, 1969.
- Fejgin O.O. About an Opportunity of Build-up
Universal Quantum Chronodynamic // Bulletin IPME.- No.3, 1984.
- Fejgin O.O. DISCRETE
- TEMPORAL MODEL OF UNIVERSE
Publishing date: May 20, 2003
Source: SciTecLibrary.ru
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