![Distinct values of ℰ in increasing order calculated from (9) with (5) and (1), using [18] algorithm for finding partitions (í µí± í µí± ) of integer í µí± into ≤ í µí± parts. The values of M and N are given on the graphs. The graphs represent complete set of distinct values of ℰ for the given values of M and N. The graphs demonstrate close to linear dependence of ℰ on "quantum number" in the vicinity of equilibrium ℰ = 0 for statistical ensembles with M=3. This is the characteristic feature of statistical ensemble of cardinality M=3. Away from equilibrium and close to the boundary of hyper-plane (1) the linear behavior is violated.](https://www.researchgate.net/profile/Sergei_Viznyuk2/publication/293992646/figure/fig1/AS:648988474761224@1531742318398/Distinct-values-of-E-in-increasing-order-calculated-from-9-with-5-and-1-using-18_Q320.jpg)
Content uploaded by Sergei Viznyuk
Author content
All content in this area was uploaded by Sergei Viznyuk on Apr 08, 2018
Content may be subject to copyright.
Content uploaded by Sergei Viznyuk
Author content
All content in this area was uploaded by Sergei Viznyuk on Apr 08, 2018
Content may be subject to copyright.
Content uploaded by Sergei Viznyuk
Author content
All content in this area was uploaded by Sergei Viznyuk on Apr 08, 2018
Content may be subject to copyright.
Content uploaded by Sergei Viznyuk
Author content
All content in this area was uploaded by Sergei Viznyuk on Dec 17, 2017
Content may be subject to copyright.
Content uploaded by Sergei Viznyuk
Author content
All content in this area was uploaded by Sergei Viznyuk on Jan 25, 2017
Content may be subject to copyright.
Content uploaded by Sergei Viznyuk
Author content
All content in this area was uploaded by Sergei Viznyuk on Jun 05, 2016
Content may be subject to copyright.
New QM framework
Sergei Viznyuk
Abstract
I propose a model wherein a system is represented by a finite sequence of
natural numbers. These numbers are thought of as population numbers in statistical
ensemble formed as a sample with replacement of entities (microstates) from some
abstract set. I derive the concepts of energy and of temperature. I show an analogy
between energy spectra computed from the model and energy spectra of some known
constructs, such as particle in a box and quantum harmonic oscillator. The presented
model replaces the concept of wave function with knowledge vector. I derive
Schrödinger-type equation for knowledge vector and discuss principal differences with
Schrödinger equation. The model retains major QM hallmarks such as wave-particle
duality, violation of Bell’s inequalities, quantum Zeno effect, uncertainty relations,
while avoiding controversial concept of wave function collapse. Unlike standard QM
and Newtonian mechanics, the presented model has the Second Law of
Thermodynamics built-in; in particular, it is not invariant with respect to time reversal.
As for prophecies, they will pass away; as for tongues,
they will cease; as for knowledge, it will pass away.
1 Corinthians 13:8
1. PREAMBLE
Physical properties, such as temperature, energy, entropy, pressure, and phenomena such as
Bose-Einstein condensation are exhibited not just by “real” physical systems, but also by virtual
entities such as binary or character strings [1, 2, 3], world wide web [4], business and citation
networks [5, 6], economy [7, 8, 9]. A characteristic quantum mechanical behavior has been
observed in entities as different as electrons, electromagnetic waves, and nanomechanical
oscillators [10].
There must be an underlying mechanism which accounts for the grand commonality in
observed behavior of vastly different entities. Scientists have recently discovered that various
complex systems have an underlying architecture governed by shared organizing principles [6].
The …present-day quantum mechanics is a limiting case of some more unified scheme… Such a
theory would have to provide, as an appropriate limit, something equivalent to a unitarily evolving
state vector [11].
There are two factors present in all theories. One is the all-pervading time, and the other is the
observer’s mind. A successful grand commonality model must explain the nature of time, specify
mechanism of how the physical reality projects onto the mind of observer, and relate time to that
projection. A grand commonality theory may not contain fundamental physical constants. Any
model containing such constants is deemed incomplete.
I call physical reality (i.e. the “real” world) the underlying system. The underlying system is
represented by its state vector . The measuring device defines the basis. Knowledge vector is
the state vector represented in the basis. The concept of knowledge vector may seem similar to
wave function in Niels Bohr interpretation whence the wave function is not to be taken seriously
as describing a quantum-level physical reality, but is to be regarded as merely referring to our
(maximal) “knowledge” of a physical system… [11]. In the presented framework, the action of the
measuring device does not affect the state of underlying system, only the knowledge vector. The
model does not exhibit the so-called measurement problem [12].
The state vector has an associated value of proper time [13] which serves as the ordering
parameter for different states of underlying system. State vector is completely defined by a finite
sequence of natural numbers . I call the population numbers of microstates from set
. I do not speculate what is microstate, or set , leaving them as abstract notions. I think of
sequence as a sample with replacement of microstates . I call such sample the
statistical ensemble. Henceforth the notion of physical reality is reduced to a sequence of natural
numbers which do not have to be physicalized in any way.
The proper time has been previously defined [13] as the ordering parameter for
the states of statistical ensemble:
, where
(1)
The proper time is quantized with time quantum . I combine this definition of
time with the following rule on time increments:
The positive direction of time change is when:
, where all are non-negative.
(2)
The negative direction of time change is when:
, where all are non-positive.
(3)
If and are such that some are positive and some are negative, then state
vectors and do not connect by timeline. There can be multiple timelines (histories)
connecting two state vectors, as well as none.
For the given state vector, a choice of observation basis defines the knowledge vector. An
observation basis associated with the measuring apparatus is the preferred basis, much discussed
recently [14].
Commonly, the [Schrödinger] equation is solved in time-forward manner: given known state,
find conditional probabilities of [future] measurement outcomes. Similarly, if same equation is
solved backward in time, one would find the past too is only defined in terms of conditional
probabilities, expressed as a modulus square of correlation function of two state vectors.
Any known fact from the past is deemed the artifact of the present state. What observer thinks
as the past, the present, or the future is represented by the knowledge vectors in the present. This
stance aligns with empirical evidence, e.g. from delayed-choice experiments [15], suggesting the
history is determined by the setup at present. Thus, there is only present. A statistical correlation
between knowledge vectors, having as correlation distance, is perceived as time evolution.
To further develop the model, I derive the notions of energy in Section 2, and of temperature
in Section 3. In Section 4 I derive the equation of motion for knowledge vector and discuss its
similarity and differences with Schrödinger equation. I define the concept of measurement. I touch
upon the notions of open/closed systems; conservation of energy; Bell’s inequalities; Haag’s
theorem; quantum Zeno effect; and the notion of memory. I show the condition for quantum vs.
classical behavior is the existence of predictable phase relationship between knowledge vectors.
2. ENERGY
The base tenet of the model is that the sequence completely defines the underlying
system. I call sequence the mode. Since mode is formed as a sample with replacement, the
[unconditional] probability of finding underlying system in a particular mode is given by the
multinomial probability mass function:
(4)
, where is the probability of sampling microstate from set . Within the context of the model
(5)
, where is the cardinality of set . I introduce functions as follows:
(6)
(7)
(8)
(9)
(10)
, where is gamma function,
is Shannon’s [16] entropy, and
is equilibrium microstate entropy [17]. With (7-9), I rewrite (4) as
(11)
From (11) the probability of observing statistical ensemble of N microstates in a particular mode
is determined solely by the value of . If I’m to use as a single independent
variable, I can write the probability mass function in domain as:
(12)
Here is the multiplicity (degeneracy) of the given value
1
, i.e. a number of ways
the same value of is realized by different modes with given parameters. There is no
analytic expression for, however, it is numerically computable. Table 1 contains ,
values calculated for several sets of parameters. Figures 1-2 show distinct
values of in increasing order for several values of parameter and probabilities (5) calculated
from (9), using algorithm [18] for finding partitions of integer into parts [19]. The
sum of over all distinct values of is the total number of modes. It is equal to the
number of ways to distribute indistinguishable balls into distinguishable cells:
(13)
, where sum is over all distinct values of . Figure 3 shows the total number of
distinguishable states of statistical ensemble, and the total number of distinct values as
1
For a case of statistical ensemble with microstate probabilities (5); the multiplicity of is the multiplicity of the
value of multinomial coefficient in (4) [80]
functions of for two sets of probabilities (5), calculated from (13) and (9) using algorithm [18].
The graphs demonstrate the following:
• For probabilities (5), the average degeneracy of levels approaches as.
This statement can be expressed as:
(14)
Here
sum represents the number of distinct values of for the given parameters. As
is not a smooth function of (see Table 1), there could be no true probability density
in domain. However, I shall derive pseudo probability density to be used in expressions
involving integration by in thermodynamic limit. To be able to use analytical math, I have to
extend (7-11) from discrete variables to continuous domain. I call
• Thermodynamic limit is the approximation of large population numbers:
(15)
In thermodynamic limit, I shall use Stirling’s approximation for factorials
(16)
With (5) it allows rewriting of (7-9) as
(17)
(18)
Figure 4 demonstrates function calculated for two sets of parameters using exact
expression (7) and approximate formula (17). In thermodynamic limit, is a smooth function of
approximated by positive semi-definite quadratic form of in the vicinity of its
minimum (10):
(19)
Knowing the covariance matrix [20] of multinomial distribution (4) allows reduction of (19) to
diagonal form. The covariance matrix, divided by is:
, where
;
(20)
The rank of is . If is a diagonal form of , the eigenvalues of are :
;
;
;
(21)
For equal probabilities (5),
. I transform to new discrete variables:
;
(22)
, where is matrix with columns as unit eigenvectors of corresponding to eigenvalues (21).
In case of and probabilities (5)
(23)
The eigenvector corresponding to eigenvalue is perpendicular to hyper-plane (1)
defined by in M-dimensional space of coordinates, while vector is
parallel to the hyper-plane. Therefore, in (22). I rewrite (19) in terms of new variables
as
(24)
I call the canonical variables of statistical ensemble, and the canonical state vector.
I call parameter the energy of statistical ensemble. If statistical ensemble of microstates is
divided into sub-ensembles of microstates as
(25)
, then, from (22,25), the relation between canonical vector of the larger system and vectors
of subsystems is:
(26)
I may also call the canonical momentum of the system. Relation (26) states the total momentum
of the system equals the sum of momenta of constituent parts. The expressions (22,24) lead to
the following time evolution laws for , with time defined as proper time (1):
;
;
(27)
;
, where designates the expectation value of . The canonical vector constitutes the knowledge
vector in the basis of eigenvectors of . As the basis is associated with an observer, basis vectors
may differ from eigenvectors of . If the basis is obtained from eigenvectors of via an
orthogonal transformation, linear form (26), and quadratic form (24) are preserved. Hence, I state
the conservation of energy law as follows: the energy of the system is conserved under orthogonal
transformations of the basis. In layman’s terms, it means the energy may change from one form
to another (e.g. from potential into kinetic), while total energy of the system is conserved under
such transformation. The conservation of energy law in this form differs from the common one
(Conservation of Energy, Wikipedia) which “… states that the total energy of an isolated system
remains … conserved over time”. From (27) it follows the expectation value of energy is
not conserved over time. However, in scenarios drawn from classical physics, the exponent in (27)
has much longer characteristic timescale than orthogonal transformation of observation basis. This
condition is equivalent to , i.e. to thermodynamic limit case.
Figure 5 demonstrates function calculated for two sets of parameters using
exact expression (9) and approximations (18), and (24). I plotted instead of to show
asymptotic behavior of (9) and (18) in comparison with quadratic form (24). Using (17) and (24)
I obtain multivariate normal approximation [20] to multinomial distribution (4) as
(28)
Figure 6 shows graphs of as a function of calculated for and four
sets of probabilities, using exact formula (4), and multivariate normal approximation (28).
In order to derive pseudo probability density in domain, I note that:
• In thermodynamic limit, the number of distinguishable states of statistical
ensemble having is proportional to the volume of –dimensional sphere of
radius. This statement can be expressed as
(29)
The sum in (29) is over all distinct values of which are less or equal than. The function
is determined from normalization requirement:
(30)
In order to convert from sums to integrals over continuous variable I define pseudo density
of distinguishable states of statistical ensemble as
(31)
The corresponding pseudo probability density is given by (12). The normalization
requirement for these functions becomes:
(32)
The value is obtained from (9) by having microstate with lowest probability
acquire maximum population: . From (9) as :
(33)
For probabilities (5):
(34)
From (33) as . That allows replacing in the upper limit of integral in (32)
with . I get [20] the expression for function in
(29) as:
(35)
Using (35) and (17) allows rewriting (29) as
(36)
, where
is the volume of –dimensional
sphere of radius .
The number of distinct values of in limit can be estimated from (36) and (14) as
(37)
From (37) one can approximately enumerate distinct energy levels by “quantum number” :
(38)
From (31) the pseudo density of distinguishable states of statistical ensemble is
(39)
I use condition (13) to define effective
value:
(40)
Figure 7 shows calculated from exact expressions (4), (9), and from formula (36).
From (11), (17), and (39), the pseudo probability density function of statistical ensemble in
thermodynamic limit is
(41)
, where is the probability density function of gamma [20] distribution with scale
parameter, and shape parameter
. I calculate moments of:
Mean:
(42)
Variance:
(43)
moment
about mean:
(44)
The sums in (42-44) are over all combinations of satisfying (1), i.e. over all partitions of N.
Expression (41) allows explicit calculation of all moments of in thermodynamic limit. From (41)
the mean value , the variance, and the third moment are:
(45)
(46)
(47)
Figure 8 shows calculations of mean value, the variance, and the third moment from the
exact expressions (42-44) for the moments, with (4) as probability mass function. It demonstrates
how these values asymptotically approach thermodynamic limit values (45-47) as, i.e.
as where is the proper time (1).
I shall demonstrate how the presented model correlates with some known constructs. Consider
one-dimensional quantum harmonic oscillator. Its energy levels [21] are given by:
(48)
, where is the base frequency, and . Energy levels (48) are equally-spaced. In my
model, similar pattern is exhibited by energy levels of statistical ensemble of cardinality ,
as shown on Figure 1. From (18) in thermodynamic limit approximation, the energy of statistical
ensemble can be written as:
(49)
, where
;
;
(50)
From above, the energy levels of statistical ensemble of cardinality are:
(51)
, where are Loeschian numbers (Sloane, OEIS sequence A003136). With (48) and (51), I can
write the comparison table of the first few energy levels of quantum harmonic oscillator in units
of , and of statistical ensemble of cardinality in units
:
quantum harmonic
oscillator
1
3
5
7
9
11
13
15
17
19
21
23
25
27
29
31
33
35
37
39
41
43
statistical ensemble
of cardinality
0
1
3
4
7
9
12
13
16
19
21
25
27
28
31
36
37
39
43
, where black boxes designate missing energy levels. In the second row, the energy levels shown
in shaded boxes are only realized for modes with ; and energy levels shown in
white boxes are realized for modes with. Here is the remainder of
division of by .
Consider another classic quantum mechanical example: particle of mass in a box of size .
Its energy levels [21] are given by:
;
(52)
In my model, similar energy spectrum is exhibited by statistical ensemble of cardinality ,
as shown on Figure 2. From (49), the energy levels of statistical ensemble of cardinality ,
in thermodynamic limit approximation, are:
;
(53)
, where
is to be considered as the effective mass of the particle.
(54)
Energy levels (53) with even are only possible when is even, and energy levels with odd are
only possible when is odd. With ½ probability the lowest energy level is , and with
½ probability it is , in units of .
3. THERMODYNAMIC ENSEMBLE
The statistical ensemble considered in previous section represents a single copy of
underlying system, with mode uniquely identifying the state. In this section, I consider
observation as a random pick of underlying system from a collection of systems, each represented
by its own statistical ensemble of cardinality . I call such collection of systems thermodynamic
ensemble. I designate the set of modes a system may occupy; the total number of systems,
and the number of systems in mode :
(55)
I designate the probability for a system to be in any mode with total population of
microstates . Then, from (11), the probability for a system to be in a mode is:
(56)
I consider systems in the same mode indistinguishable to the observer. Then the probability mass
function of distribution of modes among systems is
(57)
The objective is to find the most probable distribution . For standalone systems, the most
probable distribution is the one which maximizes (57), i.e.
(58)
Let’s consider systems to be part of some bigger system in a certain state. That imposes conditions
on distribution of modes among systems, so relations (45-47), (58) may no longer hold. I consider
one of the possible conditions and show how it leads to the notion of temperature. Let the state of
the bigger system be such that the average energy of the systems in thermodynamic ensemble is
, which may be different from the average energy of a standalone systems given by (45). Then:
(59)
To find the most probable distribution of modes , I shall maximize logarithm of (57) using
method of Lagrange multipliers [22, 23] with conditions (55) and (59):
(60)
From (60), (59), (55) I obtain the following equation involving Lagrange multipliers and :
(61)
, where is digamma function, and and are to be determined by solving (61) for :
(62)
, and by plugging from (62) into (59) and (55). In (62), is the inverse digamma function,
and
. The parameter is commonly known as temperature.
Since the number of systems in mode cannot be negative, expression (62) effectively
limits modes which can be present in most probable distribution to those satisfying
(63)
, where is Euler–Mascheroni constant. Using approximation [24]:
, I rewrite (62) as:
(64)
Presence of term in (64) leads to a computationally horrendous task of calculating and ,
because the summation in (55) and (59) has to be only performed for modes satisfying (63). I shall
leave the exact computation to a separate exercise, and make a shortcut, by ignoring term in
(64). This approximation is equivalent to Boltzmann’s postulate
2
[25] that the number of systems
in mode is proportional to
. The shortcut allows calculation of Lagrange multiplier
from (55):
, where
(65)
Using expression (39), the partition function in (65) can be evaluated as:
(66)
The equation (59) then becomes
(67)
Eq. (67) is the familiar relation [23] between average per-particle energy and temperature in
-dimensional ideal Maxwell-Boltzmann gas. Thermodynamic entropy can be evaluated
as:
(68)
, where
(69)
With expression (17) for , in thermodynamic limit, I rewrite (68) as
(70)
, where
(71)
2
While widely used, this postulate has rather unphysical consequence that there is a non-zero probability of finding a
system in a mode with arbitrary large energy. Another consequence is the divergence of partition function for some
constructs, e.g. hydrogen electronic levels [59].
To calculate I have to make an assumption on distribution. As a possible example, I
shall assume the number of microstates for a system in thermodynamic ensemble is
Poisson-distributed around mean value. Therefore, for , I can use expression for the
entropy of Poisson distribution [26]:
(72)
I also use the following:
(73)
With (72), (73) I finally obtain:
(74)
In case of , i.e. for degrees of freedom, the expression (74) turns into
equivalent of Sackur-Tetrode equation [27] for entropy of ideal gas. For thermodynamic entropy
of a standalone system, instead of (68-74) from (17) and (45) I have:
(75)
Thermodynamic entropy (74) per system in thermodynamic ensemble is larger than entropy (75)
of a standalone system by term (72) plus the temperature-related term. The increase in entropy by
happens because of the spread in values of , i.e. in age of the systems. The increase in entropy
by temperature-related term
is due to the spread in energies of the systems. The non-zero
thermodynamic entropy of a standalone system implies its state is unknown prior to observation,
for each observation. Using (1) I rewrite (75) in terms of proper time as:
, where
(76)
The expression for in (76) was derived in thermodynamic limit, i.e. when . When
(i.e. when ) . By comparing to (Figure 9) I see that fairly
close to except when is large enough, in which case thermodynamic limit approximation
for the given becomes less valid anyhow. Therefore, I can replace with in (76) and
obtain thermodynamic entropy of a standalone system as:
(77)
The [linear] relation between thermodynamic entropy and proper time (77) is the manifestation
of the Second Law of Thermodynamics (SLT). Previously, SLT has been demonstrated in the
context of time model [13] using numeric calculation of microstate entropy.
The expression for in (66) has been derived in thermodynamic limit approximation, i.e.
when . It means there must be large number of energy levels included in sum (65), i.e.
temperature cannot be too small. Therefore, the expressions (66-67) are only valid for ,
where is the characteristic difference between adjacent energy levels.
For statistical ensemble of cardinality the approximately evenly-spaced energy levels
(Figure 1) allow for more accurate expression for partition function. From (38) the characteristic
difference between energy levels in the limit is:
(78)
Figure 10 shows numeric calculation of the difference between adjacent energy levels
averaged over distinct states of statistical ensemble with the given value of , and .
If , the first 17 energy levels in units of
and their degeneracy:
0
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
0
3
9
12
21
21
27
36
39
39
48
57
57
63
63
75
81
1
6
6
6
6
6
6
6
6
6
6
6
6
6
6
6
6
If , the first 16 energy levels and their degeneracy:
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
1
4
7
13
16
19
25
28
31
37
43
49
52
61
64
67
3
3
6
6
3
6
3
6
6
6
6
9
6
6
3
6
The combined energy levels are thus given by (51). I can use (48) as approximation for the
combined energy levels (51) in expression for partition function (65) with degeneracy of each level
=6, and obtain the mean energy of modes for subsystems with given as [28]:
;
(79)
The relation
is commonly referred to as the average number of photons in a mode [29].
In my model, the notion of a photon is meaningless. The quantized energy levels (9,48,51) make
transitions between modes appear as absorption or emission of particles.
Formula (79) has been obtained using linear dependence (48) of energy levels on quantum
number , in , i.e. limit. Figure 1 shows approximation (48) holds reasonably well
when is not too large. From (14), the linearity (48) break down for
. Therefore, the
typical black-body spectrum can only be exhibited by relatively low-temperature systems, with
. A good example is the cosmic microwave background. The higher the temperature,
the more will the spectrum differ from that of black body, especially in region, where
spectral intensity would fall off steeper than black-body radiation as . Such deviation from
black-body radiation is already obvious in solar spectrum.
Zero-point energy term
in (79) is the subject of a hundred-year controversy [30, 31]. It
leads to the infinite energy density of the field in any volume of space, as there is no upper limit
on in conventional theory. In presented model, contrary to the conventional theory, term
cannot contribute more than
to the average energy (79), i.e. its contribution is within
standard deviation (46). The problem of infinite zero-point energy [30] does not exist within the
context of the model.
4. THE DYNAMICS OF KNOWLEDGE VECTOR
In this section, I discuss dynamics of knowledge vector in the context of time model (1). A
knowledge vector is defined in an observation basis associated with the measuring device. A
special interest presents knowledge vector as projection of canonical vector (22)
(80)
Transformation (80) preserves quadratic form (24) which means the components have
familiar from classical mechanics relation to energy. The orthogonal transformation in (80)
represents the measuring device. The state of measuring device has to reflect the state of underlying
system. Therefore, transformation depends on , and, possibly, proper time . Any
matrix can be expressed [32] as matrix of real skew-symmetric matrix :
, where
(81)
Any real skew-symmetric matrix can be reduced [32, 33] to a block-diagonal form by
transformation:
(82)
, where
, and are real
(83)
Plugging (82) into (81) I obtain from (80):
(84)
, where
(85)
I re-write (84) as
(86)
, where I introduced new knowledge vector , and new state vector . Vector
is the state vector represented in eigenbasis of the measuring device. Action of operator
on vector in (86) constitutes transformation by the measuring device. I define eigenspaces of the
measuring device as 2D subspaces formed by pairs of eigenvectors corresponding to eigenvalues
in (83). In eigenbasis, the action of the measuring device is reduced to rotations in 2D
orthogonal eigenspaces, as evident from (85).
As I mentioned earlier, the rank of matrices , and of vectors is . Therefore,
transformation (86) takes especially simple form in case of :
, where
, and
(87)
When the transformation is trivial: if then ; if then .
Transformation (87) can be expressed in complex notation using real components :
, where
, and
(88)
In case of one can convert to complex notation by combining pairs of real ,
components corresponding to 2D eigenspaces in (85) into complex numbers as in (88). In case of
even there will be one real-only component left un-transformed. In complex notation, (85)
can be written as a Lie group unitary matrix :
for even :
, where
(89)
, and for odd
(90)
Transformation (86) can now be expressed in complex notation as:
(91)
In complex notation, matrix (85) takes diagonal form and becomes
matrix (89-90). Operating with unitary matrices in diagonal form is easier than with orthogonal
matrix (85). The complex notation is a technique to make some math easier to handle, not to create
new physics out of thin air.
Consider scenario where eigenspaces of the measuring device do not depend on time or on
state vector of underlying system, i.e.
in (86). That deems a valid expectation if
measuring device is to provide consistent results. It means, e.g., the orientation of polarizer does
not depend on time, or on the polarization of incident light. Then, from (27),
.
Assuming analytic :
(92)
, where, for even :
(93)
, and for odd :
(94)
, where
(95)
If eigenspace component , the underlying system is in a state characterized by the
symmetry with respect to rotations within 2D eigenspace of the measuring device. Therefore,
the eigenspace component will not rotate if , i.e. null vector has no phase. Thus,
. In the vicinity of, is approximated by a positive quadratic form
on . The only such form is the eigenspace component of energy:
, where
, and
(96)
, and is a constant of proportionality which I’m tempted to call Planck’s constant. No model is
complete if it contains underived physical constants. To obtain an expression for , I note that in
a case of and , there are canonical vectors possible, from (22):
(97)
The phase difference between these vectors is
. Thus, for underlying system with and
, the proper time (1) increment corresponds to a phase increment
. The energy (9) of underlying system with and is
.
Thus, in proper time scale of the system with , the value of the Planck’s constant is:
;
(98)
A classical measuring device, such as the wall clock, is coupled into environment via various
interactions, electromagnetic, gravitational, etc. Effectively, it is part of the whole universe. Its
proper time is the universe’ proper time, defined by the total population number (1) of microstates
in statistical ensemble representing the universe. In universe’ proper time scale (98) becomes:
;
(99)
From (99) it follows, the Planck’s constant ought to decrease with time . Although, given
the number is likely to be very large, the decrease
might not be detectable.
Since the time increments
also decrease, the product
stays the same. The
decrease in the value of is negated by the slowing time. It is not clear if such decrease can be
detected at all given all measurements of Planck’s constant [34], in effect, are measurements of
the product or
. The dimensionless value (99) of Planck’s constant does not expound
the observable timescales, which are to be determined from empirical evidence.
Unlike (91), the equation (92) with (93-95) only contains reference to knowledge vector , and
no reference to the state vector of underlying system. The linearity of (92) means the expected
past and the future of knowledge vector are unambiguously defined in the present. The expectation
that the current state contains information about the past gives rise to the concept of memory. The
past or the future are the knowledge vectors defined in the present and related by transformation:
(100)
The measurement device performing transformation (100) maintains phase relationship
(coherence) between knowledge vectors. I call it a quantum device.
Equation (92) is similar to Schrödinger equation where H-matrix , and where are
the characteristic frequencies. The notable difference is that (92) incorporates measurement
apparatus, as it describes the expected evolution of knowledge vector as rotations within 2D
eigenspaces of the measuring device. The Schrödinger equation describes evolution of wave
function as if it exists as some sort of physical reality outside of measurement apparatus.
Schrödinger himself believed wave function is a physical reality, a density wave [35]. It is rather
common in physics community [36], and others (see e.g. Tangled up in Entanglement by L.M.
Krauss and response by D. Chopra) to assume the evolution of wave function according to
Schrödinger equation is independent of the observer, i.e. independent of representation.
The expectation of the equivalence of different representations is born out of assumption of
realism, i.e. of observed system existing and possessing properties independent of observer. If
different representations are not equivalent, physicists are confronted with the choice of preferred
basis [14]. The assumption of realism led to a number of theories alternative to Copenhagen
Interpretation, such as many worlds [37] and pilot wave [38]. The Copenhagen Interpretation
maintains underlying system does not have definite properties prior to being measured. In different
representations, objects may demonstrate contradictory behavior, as in interference experiments
[15] where objects behave either as waves, or as classical particles depending on configuration of
measuring apparatus. If device maintains phase relationship between knowledge vectors, the
observed object exhibits wave-like behavior. Without phase relationship between knowledge
vectors, classical behavior is observed, as I show below. The corresponding experimental setups
provide examples of [unitarily] non-equivalent representations. It is trivial to prove there could be
no unitary transformation from quantum to a classical behavior. Consider a system in a pure
quantum state. Its density matrix satisfies . If unitary transformation , such as time
propagator
, is applied to , then density matrix in the new basis is
. It is easy to see that , i.e. the system remains in a pure quantum state. It will also be
true in case of time-dependent , i.e. no [coherent] coupling of external fields can force a pure
quantum system to transform into a classical, or a mixed state. The existence of non-equivalent
representations has been proven by Haag [39] but its significance is still not fully appreciated.
The measurement result is [usually] a finite scalar value. It’s natural to assume it is an analytic
scalar function of knowledge vector with minimum at =0. Due to above-
mentioned symmetry of state, in the vicinity of , is approximated by a positive
semi-definite quadratic form on , diagonal in device eigenbasis:
(101)
, where index spans eigenspaces of the measuring device; is the operator matrix of observable;
are eigenvalues of ; are eigenspace components of energy (96); are device calibration
constants. For any observable, there exists a device eigenbasis in which the operator matrix of
the observable is diagonal. In real number notation, matrix must be positive semi-definite in
order for the observed values to be real non-negative numbers. In complex notation (91), the
eigenvalues of come in complex-conjugate pairs. In this case in (101) is the real part of the
eigenvalue. In canonical basis (22), the device is defined by a symmetric matrix ,
where matrix defines eigenspaces, as in (85), and diagonal matrix defines eigenvalues.
The quadratic form approximation is invalid under higher energies. However, the rightmost
side of (101) is expressed in terms of energy eigenspace components, not as a quadratic form on
knowledge vector. It is conceivable the rightmost side of (101) is not an approximation. It may be
valid for the whole range of energy values, including region of higher energies, where linear
dependence of on quantum number breaks down (Figure 1).
If operator matrix of observable is diagonal in eigenbasis of device , and operator matrix
of observable is diagonal in eigenbasis of device , and if devices and have different
eigenspaces, then matrices and do not commute. Hence, the generalized uncertainty principle
[21] applies if observables and are measured in eigenbasis of some third device :
(102)
The canonical state vector can be expressed as a sum (26) of canonical state vectors. Similar
decomposition of the knowledge vector can be used for input to quadratic form (101):
(103)
, where are eigenspace phases (89) of vectors ;
;
. The decomposition is selected from possible decompositions of
by the measuring device, through entanglement with underlying system. Device acts as a filter,
only entangling with modes which match device modes. In device eigenbasis, such modes are
the knowledge vectors . I will also call them medium oscillators.
Depending on the context, knowledge vectors in (103) may bear different meaning.
In time-correlation measurement, vector is viewed as state vector before-transition, and vector
– as after-transition. In case of spatial correlation, vector may be viewed as observer Alice,
and vector – as observer Bob. The expression (103) simplifies for , with :
, where
(104)
The variance of the measurement scalar (104) is:
(105)
Signal (104) does not include transitions to or from . Therefore, it is impossible to
harvest zero-point energy or detect a zero-energy state with scalar measurement. A narrow-band
device would have
, where is the number of knowledge vectors
in superposition . If a single transition does not change significantly the energy of a
given mode, I can also assume , with . These
assumptions are equivalent to thermodynamic limit approximation. I then rewrite (104-105) as:
(106)
(107)
Given ; , I evaluate in (106) via linear expansion near initial values
; :
(108)
In a case of temporal correlations, ; . With (92-96), I rewrite (108) in the vicinity
of initial state as:
(109)
, where is the transition time; is the complex gradient of scalar phase:
, where
(110)
For a device to detect transition , signal must vary more than its standard deviation .
The detection fidelity is characterized by a change from statistical mean, expressed in terms of a
number of standard deviations. In [40] the half-life threshold was used – the decrease of the signal
by half from its initial value . For superposition in (106-107), it corresponds
to . The detection fidelity in this case is , i.e. the probability the change
was due to transition is 84%, and probability that it happened due to statistical error is 16%.
For ; ; from (106-107):
(111)
(112)
Signal (111) decreases by half from its initial value =, when
. Therefore,
the half-life detection threshold satisfies energy-time uncertainty relation in a form of Mandelstam-
Tamm bound [41]:
(113)
I call the superposition of knowledge vectors , coherent within interval , if the
difference is an analytic function of in the interval. I call
the transition rate.
For the coherent superposition of knowledge vectors, with , the transition rate
. This result is referred to as Zeno paradox [42]. It is the characteristic feature of
measurement with quantum device.
The non-zero transition rate arises from de-coherence of knowledge vectors through random
phase dispersion caused by various mechanisms, e.g. by:
1. Rayleigh scattering [43, 44]
2. Brownian motion [45, 46]
3. Dispersive media [47, 48]
4. Recombination of electron-hole pairs in semiconductors [49]
A transition changes energy (48) by with equal probability in either direction. The
case of , where , is equivalent to consecutive transitions in the same direction.
I call device which undergoes multiple transitions at random within any given interval a
classical device. In time the phases of knowledge vectors in (106) undergo a number
of positive and negative increments with equal probability The resultant increments are
binomially distributed with mean , and variance
.
Here, is the mean free time between transitions, i.e. de-coherence time. In between transitions,
the phase difference changes according to (109). It gives rise to the variance in phase
, and to the variance in phase difference
.
Figure 11 shows numeric calculation of (106), with binomially distributed phases . The
calculation established the following:
(114)
The exponential decay (114) is the characteristic feature of a classical process. From (114), the
transition rate in limit:
(115)
The half-life threshold (113), in this case, changes to:
, given
(116)
From (116), , where is the object’s decay time. The expression (116)
establishes relation between de-coherence and decay times. Quantum de-coherence has received
an extensive coverage in last decades. A link between de-coherence and decay has been suggested
[50]. De-coherence between knowledge vectors is not unlike the spontaneous collapse of wave
function, a subject of a number of collapse theories [51].
Consider a photodetector measuring intensity of incident radiation. A knowledge vector (a
medium oscillator) is formed when a set of elements (e.g. electron-hole pairs) on the surface of
photodetector entangle through some medium, e.g. through electromagnetic field. An analog of
such entanglement is a Cooper pair in superconductor, mediated by phonon interaction. The
surface area which encloses a set of elements in entangled state is limited by the coherence radius
, where is the speed of light, is the refractive index of the material. If is the
number of entangled elements per unit area of the detector; is the dimensionless scattering
rate; is the scattering frequency within [rad/s] spectral width, then, the de-coherence
time is evaluated as:
(117)
Combining (117) with (115), I obtain transition rate:
(118)
In equilibrium, the loss of a number of oscillators in a particular mode is compensated by the
radiation-stimulated induction into the mode of the same number of oscillators. The energy balance
equation is:
(119)
, where is the spectral radiance of incident radiation; is the efficiency of conversion of the
incident radiation into oscillator energy; is the number of medium oscillators per unit surface
area of the detector. I have to subtract zero-point energy term
from the ensemble-average
energy in (119), because an oscillator cannot lose energy in the ground state. From (79,119):
(120)
The term in square brackets can be considered as pertaining to the incident radiation, and
parameters outside the brackets as properties of the detector. Then, (120) can be split into formula
for the spectral radiance, and formula for the detector efficiency:
(121)
(122)
, where
can be interpreted as the number of entangled elements making up one oscillator.
The Planck’s formula for the spectral energy density readily follows from (121):
(123)
5. DISCUSSION
The presented model bears familiar hallmarks of quantum physics. Consider e.g. wave-particle
duality. The particle properties result from discreteness of probability mass function (4), of energy
spectrum (Table 1), of proper time (1), of measurement scalar (101,103,106). The discrete values
of measurement scalar may be associated with observable states of underlying system. The choice
of observation basis (i.e. the experimental setup) can make quantum leaps between observable
values look like emission and absorption of particles.
Wave properties result from superposition of knowledge vectors in the measurement
scalar (103,106). The superposition should rather be called decomposition, as the knowledge
vector of underlying system is decomposed into a sum of eigenvectors of the measuring
device. For a simple case , the expression for the measurement scalar (111) is identical
to the intensity distribution in interference pattern in a double-slit experiment.
Consider another QM hallmark: violation of Bell’s inequalities [52]. The violation of Bell’s
inequalities can be understood without invoking the concept of wave function collapse. In a typical
experiment [53, 54] two entangled particles represent the same underlying system, which is being
observed via two spatially separated devices and . An observer Alice is attached to device ,
and observer Bob is attached to device . If Alice and Bob did not communicate via conventional
channel, neither of them would know the result of the other. The statistical correlation can only
be detected when knowledge vectors and converge to form the resultant observation (111).
The target of experiments on violation of Bell’s inequalities is the function in (111). It shows
double-slit experiment is about as good experiment on violation of Bell’s inequalities as any other.
Confusion of statistical correlation with causality in this context led some minds to bewilderment
about spooky action at a distance [55].
Consider the concept of measurement in conventional QM theory. If measurement has
been performed at time , and the result is , the expectation value at time is given by:
, where
; is Hamiltonian,
(124)
, and is the state of the system at . Is the system considered closed or open? Conventional
theory would imply the system is closed, as only a closed system can be described by a state vector.
If the system is closed, it has to be in energy eigenstate. If is also an energy eigenstate, then
from (124), , i.e. a closed system ought to be static. The conventional theory
handles this paradox by considering system quasi-closed, i.e. initially described by a state vector,
but with -matrix having off-diagonal terms. Then is not a true Hamiltonian of the system but
so-called interaction Hamiltonian, and is not an eigenstate of .
According to Heisenberg picture of QM formalism, the measurement
is obtained from measurement via unitary transformation of observation basis.
Since the result of the measurement at is one of the eigenvalues of operator , the state
of the system at has to be one of the eigenstates of . Attempts to understand this fact
have needlessly led Copenhagen School to the concept of wave function collapse. If are
eigenvectors of , corresponding to eigenvalues , then
(125)
, where I converted to eigenbasis of -matrix. It allows rewriting (125) as
(126)
, where are eigenvalues of . Coefficients are all real because
their transpose by indices is equal to their adjoint. Hence, I rewrite (126) as:
(127)
From (127) it is clear that [42, 56], which can also be demonstrated if
(127) is broken into power series of near :
(128)
, where are commutator brackets. If the system was in state at
then the probability to find it in state at is:
, where
(129)
From (127-129) it follows that
;
leading to what is
perceived as quantum Zeno effect.
The eigenvalues of -matrix are not true energy levels of the system because -matrix is
not a true Hamiltonian. They can also be defined up to an arbitrary constant, as only the difference
matters for the dynamics of the system. The subtraction of a constant from eigenvalues of
-matrix in (127-129) doesn’t change the expectation value . Such technique is called re-
normalization. The re-normalization [30] is used in conventional theory to “resolve” various
ultraviolet catastrophes, including problem of infinite zero-point energy density resulting from
term in (79). The problem with that approach is that term in (48,79) already refers to
the difference between energy levels. Therefore, renormalization cannot possibly help here. Other
problem with conventional theory is that it does not comply with Second Law of Thermodynamics
(SLT), as Neumann’s entropy [57] is invariant under unitary transformations. The SLT trumps any
other law in physics, so any theory or model which is not compliant with SLT is faulty.
In the presented model, the canonical state vector (22) of underlying system has an associated
value of time (1). The multiple possible histories of underlying system are represented by the
sequences of statistical ensembles arranged by time progression rule (2,3). The progression
rule (2,3) results in increase of entropy (77) with time. In thermodynamic limit, the time
progression of underlying system is approximated by rather featureless exponential decline (27).
The observational diversity is rooted not in dynamics of underlying system, but in the dynamics
(91-92) of observation basis.
This work has been motivated, in part, by:
• a perception of a common mechanism which might account for similar traits in vastly different
entities
• an apprehension that modern science mostly operates within confinement of a primitive
realism, which presents the world as a collection of solids of various shapes, liquids, gases,
and progressively more exotic objects, all the way to the not quite defined notions of dark
energy and dark matter, purported to make up 95% of the “reality”; with all those things
existing somewhere “out there” beyond the tip of our noses
• a sense of contradiction between assumption of causal relationships which modern physics
strives to establish, and probabilistic nature of observation outcome, implying there is no such
thing as causality, just correlation
References
[1]
W. Wislicki, "Thermodynamics of systems of finite sequences," J. Phys. A: Math. Gen.,
vol. 23, no. 3, p. L121, 1990.
[2]
C. Frenzen, "Explicit mean energies for the thermodynamics of systems of finite
sequences," J. Phys. A: Math. Gen., vol. 26, no. 9, p. 2269, 1993.
[3]
S. Viznyuk, "Thermodynamic properties of finite binary strings," arXiv:1001.4267 [cs.IT],
2010.
[4]
R. Albert and A.-L. Barabási, "Statistical mechanics of complex networks," Rev. Mod.
Phys., vol. 74, pp. 47-97, 2002.
[5]
G. Bianconi and A.-L. Barabási, "Bose-Einstein condensation in complex networks,"
arXiv:cond-mat/0011224 [cond-mat.dis-nn], 2000.
[6]
A.-L. Barabási and E. Bonabeau, "Scale-Free Networks," Scientific American, vol. 288,
pp. 50-59, 2003.
[7]
M. Bouchaud, "Wealth Condensation in a simple model of economy," Physica A
Statistical Mechanics and its Applications, vol. 282, p. 536, 2000.
[8]
T. Garrett, "Thermodynamics of long-run economic innovation and growth,"
arXiv:1306.3554 [q-fin.GN], 2013.
[9]
S. Sieniutycz and P. Salamon, Finite-Time Thermodynamics and Thermoeconomics,
Taylor & Francis, 1990.
[10]
J. Chan, T. Alegre, A. Safavi-Naeini, J. Hill, A. Krause, S. Groeblacher, M. Aspelmeyer
and O. Painter, "Laser cooling of a nanomechanical oscillator into its quantum ground
state," arXiv:1106.3614 [quant-ph], 06 2011.
[11]
R. Penrose, "On Gravity's Role in Quantum State Reduction," General Relativity and
Gravitation, vol. 28, no. 5, pp. 581-600, 1996.
[12]
A. Bassi and G. Ghirardi, "Dynamical Reduction Models," arXiv:quant-ph/0302164, 04
2003.
[13]
S. Viznyuk, "Time as a parameter of statistical ensemble," arXiv:1110.3296 [physics.gen-
ph], 2011.
[14]
T. Wang and D. Hobill, "Is the Preferred Basis selected by the environment?,"
arXiv:1412.2852 [quant-ph], 2014.
[15]
X.-s. Ma, J. Kofler and A. Zeilinger, "Delayed-choice gedanken experiments and their
realizations," arXiv:1407.2930v3 [quant-ph]., 2016.
[16]
C. Shannon, "A Mathematical Theory of Communication," The Bell System Technical
Journal, vol. 27, pp. 379-423, 623-656, 1948.
[17]
S. Viznyuk, "Shannon's entropy revisited," arXiv:1504.01407 [cs.IT], 03 2015.
[18]
K. Yamanaka, S. Kawano and K. Y., "Constant Time Generation of Integer Partitions,"
IEICE Transactions on Fundamentals of Electronics, Communications and Computer
Sciences, Vols. E90-A, no. 5, pp. 888-895, 2007.
[19]
S. Viznyuk, "OEIS sequence A210237," 2012. [Online]. Available:
https://oeis.org/A210237. [Accessed 21 04 2015].
[20]
C. Forbes, M. Evans, N. Hastings and B. Peacock, Statistical Distributions, Fourth Edition,
Hoboken, NJ, USA: John Wiley & Sons, Inc., 2010.
[21]
D. J. Griffiths, Introduction to Quantum Mechanics, 2nd ed., Pearson Education, Inc.,
2005.
[22]
I. Vapnyarskii, "Lagrange multipliers," in Encyclopedia of Mathematics, Springer, 2001.
[23]
K. Huang, Introduction to Statistical Physics, Taylor & Francis, Inc., 2001.
[24]
M. S. I. A. Abramowitz, "6.3 psi (Digamma) Function," in Handbook of Mathematical
Functions with Formulas, Graphs, and Mathematical Tables, New York: Dover, 1972, p.
258–259.
[25]
L. Landau and E. Lifshitz, Statistical Physics, vol. 5, Elmsford: Pergamon Press, Ltd.,
1980.
[26]
R. Evans, J. Boersma, N. M. Blachman and A. Jagers, "The Entropy of a Poisson
Distribution: Problem 87-6," SIAM Review, vol. 30, no. 2, p. 314–317, 1988.
[27]
K. Huang, Statistical Mechanics, John Wiley & Sons, 1987.
[28]
"Planck's law," [Online]. Available: https://en.wikipedia.org/wiki/Planck%27s_law.
[Accessed 20 06 2015].
[29]
C. Kittel and H. Kroemer, Themal physics, W. H. Freeman, 1980.
[30]
P. Jordan and W. Pauli, "Zur Quantenelektrodynamik ladungsfreier Felder," Zeitschrift für
Physik, vol. 47, no. 3, pp. 151-173, 1928.
[31]
G. Grundler, "The zero-point energy of elementary quantum fields," arXiv:1711.03877
[physics.gen-ph], Novermber 2017.
[32]
D. Youla, "A normal form for a matrix under the unitary congruence group," Canad. J.
Math, vol. 13, pp. 694-704, 1961.
[33]
T. Voronov, "Pfaffian," in Concise Encyclopedia of Supersymmetry, Springer Netherlands,
2003, pp. 298-298.
[34]
R. Steiner, "History and progress on accurate measurements of the Planck constant,"
Reports on Progress in Physics, vol. 76, no. 1, 2012.
[35]
J. Bell, "Against 'measurement'," Physics World, August 1990.
[36]
N. Mermin, "The Ithaca Interpretation of Quantum Mechanics," arXiv:quant-ph/9609013,
17 09 1996.
[37]
B. S. DeWitt, "Quantum mechanics and reality," Physics Today, pp. 30-35, 1970.
[38]
D. Bohm, "A suggested interpretation of the quantum theory in terms of hidden variables,"
Phys. Rev., vol. 85, pp. 166-179, 1952.
[39]
R. Haag, "On Quantum Field Theories," Dan. Mat. Fys. Medd., vol. 29, no. 12, pp. 1-37,
1955.
[40]
L. Mandelstam and I. Tamm, "The uncertainty relation between energy and time in non-
relativistic quantum mechanics," Journal of Physics, vol. 9, no. 4, pp. 249-254, 1945.
[41]
S. Deffner and S. Campbell, "Quantum speed limits: from Heisenberg's uncertainty
principle to optimal quantum control," arXiv:1705.08023 [quant-ph], 16 10 2017.
[42]
S. E. Misra B., "The Zeno's paradox in quantum theory," Journal of Mathematical
Physics, vol. 18, no. 4, pp. 756-763, 1977.
[43]
H. Uys, M. Biercuk, A. VanDevender, C. Ospelkaus, D. Meiser, R. Ozeri and J. Bollinger,
"Decoherence due to Elastic Rayleigh Scattering," Phys.Rev.Letters, vol. 105, p. 200401,
2010.
[44]
M. Schlosshauer, Decoherence and the quantum-to-classical transition, Springer, 2007.
[45]
J. Paz, "Decoherence in Quantum Brownian Motion," arXiv:gr-qc/9402007, 02 1994.
[46]
K. Hornberger, "Introduction to Decoherence Theory," Lect. Notes Phys., pp. 221-276,
2009.
[47]
C. Antonelli and e. al, "Sudden Death of Entanglement Induced by Polarization Mode
Dispersion," Phys.Rev.Letters, vol. 106, no. 8, p. 080404, 02 2011.
[48]
S. Salemian and S. Mohammadnejad, "Analysis of Polarisation Mode Dispersion Effect on
Quantum State Decoherence in Fiber-based Optical Quantum Communication," in
Proceedings of the 2011 11th International Conference on Telecommunications
(ConTEL), Graz, 2011.
[49]
Y. Jho, X. Wang, D. Reitze, J. Kono, A. Belyanin, V. Kocharovsky and G. Solomon,
"Cooperative recombination of electron-hole pairs in semiconductor quantum wells under
quantizing magnetic fields," Phys.Rev. B, vol. 81, pp. 155314-1, 2010.
[50]
S. Viznyuk, "Gravity-induced decay," 2016. [Online]. Available:
https://www.academia.edu/21674738/Gravity-induced_decay.
[51]
G. Ghirardi, "Collapse Theories," 2016. [Online]. Available:
https://plato.stanford.edu/entries/qm-collapse/.
[52]
J. Bell, "On the Einstein Podolsky Rosen Paradox," Physics, vol. 1, no. 3, pp. 195-200,
1964.
[53]
A. Aspect, P. Grangier and G. Roger, "Experimental Tests of Realistic Local Theories via
Bell's Theorem," Physical Review Letters, vol. 47, no. 7, pp. 460-463, 1981.
[54]
B. Hensen, H. Bernien, A. Dreau and e. all, "Loophole-free Bell inequality violation using
electron spins separated by 1.3 kilometres," Nature, vol. 526, no. 686, October 2015.
[55]
A. Einstein, N. Rosen and B. Podolsky, "Can Quantum-Mechanical Description of
Physical Reality Be Considered Complete," Phys. Rev., vol. 47, p. 777, 1935.
[56]
S. A. Koshino K., "Quantum Zeno effect by general measurements," arXiv:quant-
ph/0411145, 3 2005.
[57]
J. Von Neumann, Mathematical Foundations of Quantum Mechanics, Princeton University
Press, 1955.
[58]
"Digamma function," [Online]. Available:
http://en.wikipedia.org/wiki/Digamma_function. [Accessed 21 04 2015].
[59]
S. J. Strickler, "Electronic Partition Function Paradox," Journal of Chemical Education,
vol. 43, no. 7, pp. 364-366, 1966.
[60]
S. Viznyuk, "Condensation into ground state in binary string models," arXiv:1012.5318
[cs.IT], 2010.
[61]
D. Ward and S. Volkmer, "How to Derive the Schrodinger Equation,"
arXiv:physics/0610121 [physics.hist-ph], 2006.
[62]
L. Kish, "Zero-point energy in the Johnson noise of resistors: Is it there?,"
arXiv:1504.08229 [physics.gen-ph], 2015.
[63]
N. Sloane, "OEIS sequence A003136," 1991. [Online]. [Accessed 2015].
[64]
"Unitary matrix," [Online]. Available: https://en.wikipedia.org/wiki/Unitary_matrix.
[Accessed 10 07 2015].
[65]
"Hermitian matrix," [Online]. Available: https://en.wikipedia.org/wiki/Hermitian_matrix.
[Accessed 10 07 2015].
[66]
"Orthogonal matrix," [Online]. Available:
https://en.wikipedia.org/wiki/Orthogonal_matrix. [Accessed 10 07 2015].
[67]
"Skew-symmetric matrix," [Online]. Available: https://en.wikipedia.org/wiki/Skew-
symmetric_matrix. [Accessed 10 07 2015].
[68]
B. J.S., "On the Einstein Podolsky Rosen Paradox," Physics, vol. 1, no. 3, pp. 195-200,
1964.
[69]
"Conservation of energy," [Online]. Available:
https://en.wikipedia.org/wiki/Conservation_of_energy. [Accessed 19 07 2015].
[70]
"Planck time," [Online]. Available: https://en.wikipedia.org/wiki/Planck_time. [Accessed
20 07 2015].
[71]
"Heisenberg picture," [Online]. Available:
https://en.wikipedia.org/wiki/Heisenberg_picture. [Accessed 25 07 2015].
[72]
J. Bell, Speakable and unspeakable in quantum mechanics, Cambridge: University Press,
1989.
[73]
D. Chopra, "Physics May Stonewall, But Reality Doesn't," 2015. [Online]. Available:
https://www.deepakchopra.com/blog/article/5438.
[74]
"Temperature," 1 03 2016. [Online]. Available: https://en.wikipedia.org/wiki/Temperature.
[75]
"Copenhagen Interpretation," 10 2016. [Online]. Available:
https://en.wikipedia.org/wiki/Copenhagen_interpretation.
[76]
"Copenhagen Interpretation," 2016. [Online]. Available:
https://en.wikipedia.org/wiki/Copenhagen_interpretation.
[77]
"Cool Cosmos at IPAC, NASA," 1 3 2016. [Online]. Available:
http://coolcosmos.ipac.caltech.edu/cosmic_classroom/light_lessons/thermal/temperature.ht
ml.
[78]
C. Wu, E. Ambler, R. Hayward, D. Hoppes and R. Hudson, "Experimental test of parity
conservation in beta decay," Phys. Rev., vol. 105, no. 4, pp. 1413-1415, 1957.
[79]
S. Viznyuk, "Gravity-induced decay," 2016. [Online]. Available:
https://www.academia.edu/21674738/Gravity-induced_decay.
[80]
S. Viznyuk, "OEIS sequence A210238," 2012. [Online]. Available:
http://oeis.org/A210238. [Accessed 21 04 2015].
[81]
S. Viznyuk, "OEIS sequence A213008," 2012. [Online]. Available:
https://oeis.org/A213008. [Accessed 21 04 2015].
[82]
P. Busch, "The Time-Energy Uncertainty Relation," arXiv:quant-ph/0105049, 2007.
[83]
P. G. Giacosa F., "Influence of the measurement on the decay law: the bang-bang,"
arXiv:1411.2255v1 [quant-ph], 11 2014.
[84]
C. Unnikrishnan, "End of Several Quantum Mysteries," arXiv:1102.1187v1 [quant-ph], 2
2011.
[85]
T. Padmanabhan, "Thermodynamical Aspects of Gravity: New insights," arXiv:0911.5004
[gr-qc], 11 2009.
[86]
T. Jacobson, "Thermodynamics of Spacetime: The Einstein Equation of State," arXiv:gr-
qc/9504004, 4 1995.
[87]
D. Fixen, "The Temperature of the Cosmic Microwave Background," arXiv:0911.1955
[astro-ph.CO], 11 2009.
[88]
D. Haddad, F. Seifert, L. Chao, A. Possolo, D. Newell, J. Pratt, C. Williams and S.
Schlamminger, "Measurement of the Planck constant at the National Institute of Standards
and Technology from 2015 to 2017," Metrologia, vol. 54, no. 5, pp. 633-641, 2017.
0.000000
1
0.000000
1
0.000000
1
0.000000
1
0.001998
2
0.003328
6
0.008299
20
0.036368
42
0.007992
2
0.009972
3
0.016598
30
0.072735
210
0.017982
2
0.009994
3
0.024828
30
0.107827
105
0.031968
2
0.013311
6
0.024966
30
0.109103
140
0.049951
2
0.023262
6
0.033127
20
0.110476
105
0.071930
2
0.023328
6
0.033196
20
0.144194
420
0.097905
2
0.029951
6
0.033265
20
0.145567
42
0.127878
2
0.039846
3
0.041495
120
0.146843
420
0.161847
2
0.040023
3
0.049521
20
0.180562
105
0.199813
2
0.043196
6
0.050072
20
0.181935
840
0.241778
2
0.043329
6
0.057889
60
0.183211
105
0.287740
2
0.053246
6
0.058024
30
0.213187
140
0.337700
2
0.063064
6
0.058162
30
0.215653
105
0.391659
2
0.063396
6
0.058302
60
0.218302
1260
0.449618
2
0.069775
6
0.066188
60
0.220951
105
0.511576
2
0.069997
6
0.066393
30
0.223804
140
0.577534
2
0.083198
6
0.066601
60
0.249555
210
0.647492
2
0.089556
3
0.074556
60
0.250928
210
0.721452
2
0.090154
3
0.074696
20
0.253394
630
[…]
[…]
[…]
[…]
[…]
[…]
[…]
[…]
640.1354
2
952.5446
6
929.0220
30
333.7789
105
644.8379
2
955.9414
3
929.4275
60
334.1844
210
649.6592
2
956.3468
6
930.8138
20
335.5707
42
654.6150
2
957.7331
6
934.0276
20
337.6184
140
659.7260
2
962.0473
6
934.7208
60
338.3115
210
665.0203
2
963.1459
6
935.8194
20
339.4101
42
670.5388
2
968.1543
3
940.4212
30
342.8495
105
676.3459
2
968.8474
6
941.1144
20
343.5426
42
682.5595
2
974.9556
6
946.8165
20
348.0859
42
689.4673
2
981.7580
3
953.2134
5
353.3277
7
Table 1
, value pairs calculated from (9) for four sets of parameters using [18]
algorithm for finding partitions of integer into parts. For each partition I
calculated the value of and multiplicity of multinomial coefficient in (4) [80].
Finally, for each distinct value of produced the results for the
table. I display the first 20 and the last 10 records from the table.
0
5
10
15
20
25
30
010 20 30 40 50 60 70 80 90 100
0
100
200
300
400
500
600
700
800
900
1,000
0 10,000 20,000 30,000 40,000 50,000 60,000 70,000
M=3 N=30
Figure 1
Distinct values of in increasing order calculated from (9) with (5) and (1), using
[18] algorithm for finding partitions of integer into parts. The values of
M and N are given on the graphs. The graphs represent complete set of distinct values
of for the given values of M and N. The graphs demonstrate close to linear
dependence of on “quantum number” in the vicinity of equilibrium for
statistical ensembles with M=3. This is the characteristic feature of statistical
ensemble of cardinality M=3. Away from equilibrium and close to the boundary of
hyper-plane (1) the linear behavior is violated.
M=3 N=900
0
20
40
60
80
100
120
140
010 20 30 40 50 60 70 80 90 100
0
20
40
60
80
100
120
140
0 10,000 20,000 30,000 40,000 50,000
M=2 N=200
M=7 N=70
Figure 2
Distinct values of in increasing order calculated from (9) with (5) and (1), using [18]
algorithm for finding partitions of integer into parts. The values of M and
N are given on the graphs. The graphs represent complete set of distinct values of
for the given values of M and N.
1
10
100
1000
10000
100000
1000000
10000000
100000000
1E+09
1E+10
110 100 1000 10000
Figure 3
The total number of distinguishable states of statistical ensemble (curves 1, 3),
and the total number
of distinct values (curves 2, 4) as functions of for two
sets of probabilities:
1. for
2.
for
3. for
4.
for
The values on curve 1 are by factor greater than on curve 2 as. The
values on curve 3 are by factor greater than on curve 4 as.
Using Stirling’s approximation for large in formula (13) one can see the curves grow
proportionally to as
(1)
(2)
(3)
(4)
Figure 4
Function calculated for two sets of probabilities.
Blue lines were calculated using exact formula (7). Red lines
were calculated using thermodynamic limit approximation (17)
Figure 5
Values of calculated as a function of with probabilities (5) for
four sets of parameters:
1.
2.
3.
4.
Blue lines were calculated using exact formula (9). Green dash lines were
calculated using thermodynamic limit approximation (18). Red lines were
calculated using quadratic form (24) approximation. For a given value of
the values were distributed proportionally to corresponding
probabilities. For large value of the blue lines and green
dash lines overlap closely as seen on curves 1 and 3. For small values of
the thermodynamic limit approximation is not accurate, and blue lines differ
from green dash lines as seen on curves 2 and 4. Red lines overlap with blue
lines in close proximity to the minimum (10) of.
(1)
(2)
(3)
(4)
(1)
(2)
(3)
(4)
Figure 6
Values of calculated as a function of for
and four sets of probabilities
1.
2.
3.
4.
Blue lines were calculated using exact formula (4). Red lines
were calculated using multivariate normal approximation (28).
For the given value of the distribution of values is
proportional to the corresponding probabilities
1.E+00
1.E+01
1.E+02
1.E+03
1.E+04
1.E+05
1.E+06
1.E+07
1.E+08
1.E+09
1.E+10
1.E+11
0.001 0.01 0.1 1 10 100 1000
(3)
(2)
(1)
Figure 7
The number of distinguishable states of statistical ensemble having
as a function of for three sets of the parameters and probabilities (5):
1.
2.
3.
4.
Solid lines are the results of calculation using exact formulas (4) and (9). Dash
lines represent thermodynamic limit approximation (36). The graphs
demonstrate thermodynamic limit provides the better approximation the larger is
the ratio
. Solid lines level off close to because density of states per
interval decreases near due to non-spherical -domain boundary of
hyper-plane (1). The boundary is defined by
First three moments of plotted as dots vs. total number N of microstates for
three sets of probabilities. The value of the third moment is reduced by a
factor of 2 to show its asymptotic behavior comparing with the first two moments.
(4)
0.0
0.5
1.0
1.5
2.0
2.5
3.0
110 100 1000
Figure 8
The mean value, the variance, and the third moment vs. total number N of
microstates for three values of and probabilities (5). The graphs have been
calculated using exact expressions (42-44) with probability mass function (4). The
value of the third moment is reduced by a factor of 2 to show its asymptotic
behavior comparing with and . For each set of parameters, the curves
approach values as
Figure 9
Comparison of in (76) with
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.90
1.00
110 100 1000
Figure 10
Difference between adjacent energy levels (9), averaged over distinct states of
statistical ensemble with the given value of , and . The curve is
approximated by (78) as
Figure 11
Blue line is a calculation of measurement scalar (106), with binomially distributed phases
, as a function of time . The red line is a plot of formula (114). The plots have been
produced using GNU Octave (MATLAB) code http://phystech.com/download/ph.m
with the following parameters:
• number of knowledge vectors in superposition ;
• mean free time between transitions of a knowledge vector :
• characteristic frequency
The plots have been normalized to . As the number of knowledge vectors increases
the blue curve smoothers and becomes identical with red curve.
