Cyclic mechanicsThe principle of cyclicity
Vasil PenchevAssociate Professor, Doctor of Science,
Bulgarian Academy of Science
[email protected]://www.scribd.com/vasil7penchev
http://vsil7penchev.wordpress.com
The mutual transformation between mass, energy, time, and quantum information
Notations:Quantities:Q โ quantuminformationS โ entropyE โ energyt โ timem โ massx โ distance
Constants:h โ Planck c โ light speedG โ gravitationalk โ Boltzmann
๐๐โ๐ฌ๐
โ๐
G
Skquantuminformation []
Quantum information in terms of quantum temperature and the Bekenstein bound
๐ธ๐=๐บ๐
๐ฌ๐= ๐๐ป ๐โค๐ ฯ๐ฤง๐ ๐ ๐
๐ธ๐=๐บ๐ ๐๐ฤง
=๐บ๐
๐ฌ๐โค๐ ฯ๐ฤง๐ ๐ ๐=
๐ ฯ๐ฤง๐ ๐
Here are the corresponding radiuses of spheres, which can place (2) the energy-momentum and
(1) the space-time of the system in question
The transformation in terms of quantum measure
Notations:Quantities:Q โ quantuminformationE โ energyt โ timem โ massx โ distance
Constants:h โ Planck c โ light speedG โ gravitationalk โ Boltzmann
๐
Q๐ธ๐๐ธ๐
quantuminformation
The universe as a single qubit ...and even as a single bit
YIN
โ0โโ1โYANG
A qubit A bit
?No,
the Kochen-Speckertheorem
the axiom of choice,Yes
QUANTUM INVARIANCE
Quantummechanics
Generalrelativity
The universe as an infinite cocoonof light = one qubit
Space-time
Energy-momentum
Light coneAll the universe can arise trying to divide
one single qubit into two distinctive parts, i.e. by means of quantum invariance
The Kochen-Speckertheorem stars as Yin
The axiom of choicestars as Yang
Minkowski space
Mass at rest as another โJanusโ between the forces in nature
Banach spaceEntanglement
GravityPseudo-Riemannianspace
Weakinteraction
Stronginteraction
ElectromagnetismMinkowski
spaceGroupsrepresented in Hilbertspace
Mass atrest
?The โStandard
Modelโ
The Higgs mechanism? ?
?
How the mass at rest can arise bya mathematical mechanism
The universe as a cocoon of light
Space-time
Energy-momen-tum
The Kochen-Specker theoremEntanglement=
m Quantum invariance
The mass at restis a definite masslocalized in a definite spacedomain
= The mass at rest The axiom of choice
Mass at rest in relativity and wave-particle duality
Minkowski spaceRelativity
Hilbert spaceWave-particle duality
The lightcone
๐
๐๐ ๐
spacedual space
๐ ๐๐
Any qubit in Hilbert space
The qubit corresponding
in its dual space
๐ ๐๐
๐ ๐ธ๐
๐ ๐ ๐ฌ๐ด๐ ๐บ๐ป
๐ ๐๐
Wave function as gravitational fieldand gravitational field as wave function
Gravitationalfield
Wavefunction
Infinity
Wholeness
+
Actual infinity=
How to compare qubits, or a quantum definition of mass at rest
Hilbert spaceWave-particle duality
spacedual space
๐ ๐๐
Any qubit in Hilbert space
The qubit corresponding
in its dual space
๐ ๐๐
๐ ๐ธ๐
๐ ๐ ๐ฌ๐ด๐ ๐บ๐ป
๐ถโ ๐โก๐๐๐๐๐๐๐๐๐๐๐๐Mass at rest means
entanglement
How the mass at rest can arise bya mathematical mechanism
The universe as a cocoon of light
Space-timeEnergy-
momen-tum The Kochen-
Specker theoremEntanglement=
m Quantum invariance
Mass at restarises if a biggerEM qubit (domain)must be insertedin a smaller STqubit (domain)
= The mass at rest The axiom of choice
๐ฌ๐ด
๐ฌ๐ดโ๐บ๐ป
Mass at rest and quantum uncertainty: a resistless conflict
โAt restโ means:
Consequently, the true notions of โrestโ and โquantum uncertaintyโ are inconsistent
probability speed
Generalized
Internal External
Observers
Whole
Mass at rest and quantum uncertainty:a vincible conflict
The quantity is a power. According to generalrelativity this is the power of gravitational energy, and to quantum mechanics an additional degree offreedom or uncertainty:
Quantum mechanics General relativity
Gravitationalfield with the power p(t) in any point:
๐ท ๐(๐๐)๐ ๐๐ท ๐
The Bekenstein bound as a thermody-namic law for the upper limit of entropy
The necessary and sufficient condition for the above equivalence: (โfrequency). This means that the upper bound is reached for radiation, and any mass at rest decreases the entropy proportionally to the difference to the upper limit:
โด Mass at rest represents negentropy information
The Bekenstein bound as a function of two conjugate quantities (e.g. t and E)
where
๐บ๐=๐๐ ๐๐โ๐๐
:
That is the quantum uncertainty (ะฏ)
as a rest mass ()
The generalized observeras any โpointโ or any relation (or even ratio) between any internal andany external observer
About the โnewโ invariance to the generalized observer
Quantum mechanicsSpecial & general relativity
All classical mechanics and science
System An(y) exter-nal observer
relativityspeed
Reference frame
System
An(y) internal observer
probability
Any internal observer
Any external observer
System
Cyclicity from the โgeneralized observerโ
Any internal observer
System
Any external observer
The generalizedobserver
The universe
Any internal observer ยฟ
Any external observer
The generalized observer
The generalized observer is (or the process of) the cyclic return of any internal observer into itself as an external
observer All physicallaws shouldbe invariantto thatcyclicity, or to โthe generalizedobserverโ
Also:
General relativity as the superluminal generalization of special relativity
Minkowski space where:โ โ means its imaginary region, and โ โ its real one. The two ones are isomorphic, and as a pair are isomorphic to two dual Hilbert spaces.Gravitational energy by the energy to an externalobserver or to an internal one :
The curvature in โ โ can be represen-red as a second speed in โ โ. Then theformer is to the usual, external observer,and the latter is to an internal one
Cyclicity as a condition of gravity
A space-timecycle
Gravity =( ) โ ( )S โ actionP โ powerE โ energy
h โ homebodyt โ travellerg - gravity
Cyclicity as the foundation of conservation of action
๐บ๐=๐บ๐๐๐๐ ๐๐๐๐๐๐๐ ๐๐๐๐๐๐โ
๐ ๐=๐๐
The universe
Simultaneity of all points
The Newtonabsolute time
and space
CIclIcIty
Simultaneity of quantum entities
Apparatus
Entangle-ment
CIclIcIty
Mathematical and physical uncertaintyCertainty Uncertainty Independence
Set theory Any element of any set (the
axiom of choice)
Any set Disjunctive sets
Logic Bound variable
Free variable
Independent variables
Physics (relativity)
Force Degree of freedom
Independent quantities
Quantum mechanics
The measured value of a conjugate
Any two conjugates
Independent quantities
(not conjugates)
General relativity is entirely a thermodynamic theory!
The laws of thermodynamicsThe Bekenstein bound
GeneralRelativityโ
Since the Bekenstein bound is a thermodynamic law, too, a quantum one for the use of this impliesthat the true general relativity is entirely a thermody-namic theory! However if this is so, then which is the statistic ensemble, to which it refers?
To any quantum whole, and first of all, to the universe, represented as a statistic ensemble!
Cycling and motion
The universe
Mechanical motionof a mass point in it
Cycle 1 = Phase 1
Cycle 3
Cycle 2 = Phase 2
ACTION CONSERVATION
Energy conservation
Time conservation
General relativity is entirely a thermodynamic theory!
The laws of classicalthermodynamics
The Bekenstein bound
GeneralRelativityโ
A quantum thermodynamic law
A quantum wholeunorderable in
principle โA relevant
well-ordered,statistical ensemble: SPACE-TIME
โ
The statistic ensemble of general relativity
Quantum information = = Action =
Energy (Mass) โจ Space-Time (Wave Length)
A quantumwhole
SPACE-TIMEdifferentenergy โ
momentum and rest mass
in any point in general
The axiomof choice
The Kochen-Speckertheorem
Einsteinโs emblem:
The question is: What is the common fundament of energy and mass?Energy conservation defines the energy as such: The rest mass of a particle can vanish (e.g. transforming into photons), but its energy never! Any other funda-ment would admit as its violation as another physicalentity equivalent to energy and thus to mass?!
However that entity has offered a long time ago, and that by Einstein himself and another his famous
formula, , Nobel prized
The statistic ensemble of general relativityThe Bekenstein bound
Informationas pure energy
(photons) = max entropy
A domain of space-time asan โideal gasโof space-time
points
OR A body with nonzero mass as
informational โcoagulateโ
Informationas a nonzero rest mass
(a body) <max entropy
๐ฌ=๐๐๐The particular case if
Information -โIโ๐๐๐ฌ=๐๐๐๐๐โ๐๐ฐ
The general case: or - speed of body time, which is 1 in the particular case above
Reflections on the information equation:
๐๐๐ฌ=๐๐๐๐๐โ๐๐ฐ
๐ฌ๐๐
=๐๐๐
๐๐โ๐๐ ๐๐ฌ๐
๐
The information equation for the Bekenstein bound:
For action:
For momentum:
For energy:The information equation for the โlight timeโ:
๐ฌ=๐๐ท ๐๐
๐โ๐ฌ๐
The distinction between energy and rest mass
If one follows a space-time trajectory (world line),then energy corresponds to any moment of time,
and rest mass means its (either minimal or average)constant component in time
Energy (mass)
Time๐๐
๐ฌ๐๐ฌ๐
๐ฌ๐๐๐ ๐๐ ๐๐
... ... ... ...๐๐ ๐๐
The laws of classical thermodynamics
Gravitational field as a limit, to which tends the statistical ensemble of an ideal gas
Gravitational field
Differential representation
An infinitelysmall volumeof an ideal gas
The Bekenstein bound (a quantum law)
A back transformationto the differen-tials of mecha-nical quantities
The rehabilitated aether, or:Gravitational field as aether
A point under infinitelylarge magnification
A finite volumeof an ideal gas
Space-time ofgeneral relativity
as
aether
The laws of classical thermodynamics
The Bekenstein bound (a quantum law)
The gas into the pointpressuretemperature
momentumenergy
The back transformation
An additional step consistent with the โthermodynamicโ general relativity
A finite volumeof ideal field
The universeas a whole
A cyclical structure
The infinity of ideal field ===
===A point in it
=
The cyclicity of the universe by the cyclicality of gravitational field
The universeTwo โsuccessiveโ
points in it๐๐๐๐
๐๐๐๐๐๐
, - two successive cycles
โHilbert
Dual
Hilbert
space As to the universe,
as to any point in itby means of
the axiom of choice andthe Kochen โ Specker theorem
โLightโ โLightโ
The cyclicity of gravitational and of quantum field as the same cyclicity
The universe
A point in it
GeneralrelativityGravity
Quantummechanics
The StandardModelStrong,
electromagne-tic, and weak
interaction
?
?
gravityQuantum??
Gravitational and quantum field as an ideal gas and an ideal โanti-gasโ accordingly
Dual
Hilbert
space
Hilbert
The universe
A point in it
All the space-time
Pseudo-Riemannian
space
A volume ofideal gas orideal field
Quantum field
Gravitationalfield
Specific gravity as a ratio of qubits
Conjugate A
Conj
ugat
e B Quantum uncertainty
Gravity as if determines the quantum uncertaintybeing a ratio of conjugates
Quantum mechanics General relativity
An โideal gasโ composed of mass points (
๐ ๐๐
๐ ๐๐ฌ
isuncertain
Qubits
The gas constant R of space-timeThe axiom of choice needs suitable fundamental
constants to act physically:
How much to (or per) how many?
The Boltzmann constant Avogadroโs number ?โ
Quantum mechanics General relativity
In Paradise: No choice
On earth: Choices, choices ...
โ๐ฒ๐ฉ
๐ต ๐จ
Paradise on earth!An ideal gas (aether) of
space-time points:
๐น=๐ฒ ๐ฉ.๐ต ๐จ
Time as entropy: โrelicโ radiation as a fundamental constant or as a variable
Seen โinsideโ:Our immense andexpanding universe
determined bythe fundamental
constants
Seen โoutsideโ:A black hole
among many onesdetermined by
its physical parameterslike mass, energy, etc.
๐บ๐๐๐๐ ๐๐๐๐๐ ๐บ๐๐๐๐ ๐๐๐๐๐
๐ซ๐๐๐๐๐๐๐๐๐๐๐ ๐๐๐๐๐โ๐+Energy (D) flow(D) +Energy (S) flow(S)
๐บ๐๐๐๐ ๐๐๐๐=๐บ๐=๐๐๐
= ๐๐ช๐ด๐ฉ .
๐๐๐
=( ๐๐ช๐ด๐ฉ )๐๐=๐
Horizon
How much should the deceleration of time be?
The ideal gas equation is:
๐=๐๐=(๐ต๐ฒ ยฟยฟ๐ฉ /๐ฒ๐)๐ฌ๐ ยฟ๐บ๐=๐ต๐๐ฒ ๐=
๐ฒ ๐ฉ
๐ต ๐จ๐ต
๐๐ =๐ฒ๐ฉ
๐ช๐ด๐ฉ๐
๐๐ =๐ฒ๐ฉ
๐ช๐ด๐ฉ๐ =๐=
๐๐๐
The โSupreme Poleโ (the Chinese Taiji ๅคชๆฅต )
The universe
Any separatepoint in it
The Einstein and Schrรถdinger equation:the new cyclic mechanics
The Einstein equation Schrรถdingerโs equation
Space & Time= โ0โ Info
d(Info)=d(Energy)Pseudo-Riemannian
space-time โ 0 info
d(Information) = d(Energy of gravity)
Cyclic mechanics: Conservation of information
actIon
The Great Pole
The universeAny and all points in it