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Page 1: Cyclic mechanics

Cyclic mechanicsThe principle of cyclicity

Page 2: Cyclic mechanics

Vasil PenchevAssociate Professor, Doctor of Science,

Bulgarian Academy of Science

[email protected]://www.scribd.com/vasil7penchev

http://vsil7penchev.wordpress.com

Page 3: Cyclic mechanics

The mutual transformation between mass, energy, time, and quantum information

Notations:Quantities:Q โˆ’ quantuminformationS โˆ’ entropyE โˆ’ energyt โˆ’ timem โˆ’ massx โˆ’ distance

Constants:h โˆ’ Planck c โˆ’ light speedG โˆ’ gravitationalk โˆ’ Boltzmann

๐’•๐’‰โ†”๐‘ฌ๐’„

โ†”๐’Ž

G

Skquantuminformation []

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Quantum information in terms of quantum temperature and the Bekenstein bound

๐‘ธ๐Ÿ=๐‘บ๐Ÿ

๐‘ฌ๐Ÿ= ๐Ÿ๐‘ป ๐Ÿโ‰ค๐Ÿ ฯ€๐’Œฤง๐’„ ๐’™  ๐Ÿ

๐‘ธ๐Ÿ=๐‘บ๐Ÿ ๐’•๐Ÿฤง

=๐‘บ๐Ÿ

๐‘ฌ๐Ÿโ‰ค๐Ÿ ฯ€๐’Œฤง๐’„ ๐’™  ๐Ÿ=

๐Ÿ ฯ€๐’Œฤง๐’•  ๐Ÿ

Here are the corresponding radiuses of spheres, which can place (2) the energy-momentum and

(1) the space-time of the system in question

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The transformation in terms of quantum measure

Notations:Quantities:Q โˆ’ quantuminformationE โˆ’ energyt โˆ’ timem โˆ’ massx โˆ’ distance

Constants:h โˆ’ Planck c โˆ’ light speedG โˆ’ gravitationalk โˆ’ Boltzmann

๐’‰

Q๐‘ธ๐Ÿ๐‘ธ๐Ÿ

quantuminformation

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The universe as a single qubit ...and even as a single bit

YIN

โ€œ0โ€โ€œ1โ€YANG

A qubit A bit

?No,

the Kochen-Speckertheorem

the axiom of choice,Yes

QUANTUM INVARIANCE

Quantummechanics

Generalrelativity

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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

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Mass at rest as another โ€œJanusโ€ between the forces in nature

Banach spaceEntanglement

GravityPseudo-Riemannianspace

Weakinteraction

Stronginteraction

ElectromagnetismMinkowski

spaceGroupsrepresented in Hilbertspace

Mass atrest

?The โ€œStandard

Modelโ€

The Higgs mechanism? ?

?

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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

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Mass at rest in relativity and wave-particle duality

Minkowski spaceRelativity

Hilbert spaceWave-particle duality

The lightcone

๐’•

๐’Ž๐’— ๐’‘

spacedual space

๐‘Ÿ ๐‘†๐‘‡

Any qubit in Hilbert space

The qubit corresponding

in its dual space

๐‘Ÿ ๐‘†๐‘‡

๐‘Ÿ ๐ธ๐‘€

๐’Ž ๐’“ ๐‘ฌ๐‘ด๐’“ ๐‘บ๐‘ป

๐’Ž ๐’‘๐’—

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Wave function as gravitational fieldand gravitational field as wave function

Gravitationalfield

Wavefunction

Infinity

Wholeness

+

Actual infinity=

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How to compare qubits, or a quantum definition of mass at rest

Hilbert spaceWave-particle duality

spacedual space

๐‘Ÿ ๐‘†๐‘‡

Any qubit in Hilbert space

The qubit corresponding

in its dual space

๐‘Ÿ ๐‘†๐‘‡

๐‘Ÿ ๐ธ๐‘€

๐’Ž ๐’“ ๐‘ฌ๐‘ด๐’“ ๐‘บ๐‘ป

๐œถโ‰ ๐Ÿโ‰ก๐’†๐’๐’•๐’‚๐’๐’ˆ๐’๐’†๐’Ž๐’†๐’๐’•Mass at rest means

entanglement

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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

๐‘ฌ๐‘ด

๐‘ฌ๐‘ดโ†’๐‘บ๐‘ป

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Mass at rest and quantum uncertainty: a resistless conflict

โ€œAt restโ€ means:

Consequently, the true notions of โ€œrestโ€ and โ€œquantum uncertaintyโ€ are inconsistent

probability speed

Generalized

Internal External

Observers

Whole

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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:

๐‘ท ๐’Š(๐’•๐’Š)๐’• ๐’Š๐‘ท ๐’Š

Page 16: Cyclic mechanics

The Bekenstein bound as a thermody-namic law for the upper limit of entropy

The necessary and sufficient condition for the above equivalence: (โˆ’frequency). 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:

โˆด Mass at rest represents negentropy information

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The Bekenstein bound as a function of two conjugate quantities (e.g. t and E)

where

๐‘บ๐ŸŽ=๐Ÿ’๐…๐Ÿ๐’Œโˆ’๐’Ž๐ŸŽ

:

That is the quantum uncertainty (ะฏ)

as a rest mass ()

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The generalized observeras any โ€œpointโ€ or any relation (or even ratio) between any internal andany external observer

About the โ€œnewโ€ 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

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Cyclicity from the โ€œgeneralized 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 โ€œthe generalizedobserverโ€

Also:

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General relativity as the superluminal generalization of special relativity

Minkowski space where:โ€œ โ€œ means its imaginary region, and โ€œ โ€œ 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€œ โ€œ can be represen-red as a second speed in โ€œ โ€œ. Then theformer is to the usual, external observer,and the latter is to an internal one

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Cyclicity as a condition of gravity

A space-timecycle

Gravity =( ) โ€“ ( )S โ€“ actionP โ€“ powerE โ€“ energy

h โ€“ homebodyt โ€“ travellerg - gravity

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Cyclicity as the foundation of conservation of action

๐‘บ๐’Š=๐‘บ๐’†๐’‘๐’†๐’“ ๐’‚๐’–๐’๐’Š๐’•๐’๐’‡ ๐’†๐’๐’†๐’“๐’ˆ๐’šโ‡”

๐’• ๐’Š=๐’•๐’†

The universe

Simultaneity of all points

The Newtonabsolute time

and space

CIclIcIty

Simultaneity of quantum entities

Apparatus

Entangle-ment

CIclIcIty

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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)

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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!

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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

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General relativity is entirely a thermodynamic theory!

The laws of classicalthermodynamics

The Bekenstein bound

GeneralRelativityโ‡’

A quantum thermodynamic law

A quantum wholeunorderable in

principle โ‡’A relevant

well-ordered,statistical ensemble: SPACE-TIME

โ‡’

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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

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Einsteinโ€™s 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

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The statistic ensemble of general relativityThe Bekenstein bound

Informationas pure energy

(photons) = max entropy

A domain of space-time asan โ€œideal gasโ€of space-time

points

OR A body with nonzero mass as

informational โ€œcoagulateโ€

Informationas a nonzero rest mass

(a body) <max entropy

๐‘ฌ=๐’Ž๐’„๐ŸThe particular case if

Information -โ€œIโ€๐’•๐Ÿ๐‘ฌ=๐’•๐Ÿ๐’Ž๐’„๐Ÿโˆ’๐’‰๐‘ฐ

The general case: or - speed of body time, which is 1 in the particular case above

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Reflections on the information equation:

๐’•๐Ÿ๐‘ฌ=๐’•๐Ÿ๐’Ž๐’„๐Ÿโˆ’๐’‰๐‘ฐ

๐‘ฌ๐’—๐Ÿ

=๐’Ž๐’„๐Ÿ

๐’—๐Ÿโˆ’๐Ÿ๐…๐’Œ๐‘ฌ๐ŸŽ

๐’„

The information equation for the Bekenstein bound:

For action:

For momentum:

For energy:The information equation for the โ€œlight timeโ€:

๐‘ฌ=๐Ÿ๐œท ๐’Ž๐’„

๐Ÿโˆ’๐‘ฌ๐ŸŽ

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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)

Time๐’Ž๐ŸŽ

๐‘ฌ๐ŸŽ๐‘ฌ๐Ÿ

๐‘ฌ๐’๐’•๐ŸŽ ๐’•๐Ÿ ๐’•๐’

... ... ... ...๐’Ž๐ŸŽ ๐’Ž๐ŸŽ

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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

Page 33: Cyclic mechanics

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

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An additional step consistent with the โ€œthermodynamicโ€ general relativity

A finite volumeof ideal field

The universeas a whole

A cyclical structure

The infinity of ideal field ===

===A point in it

=

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The cyclicity of the universe by the cyclicality of gravitational field

The universeTwo โ€œsuccessiveโ€

points in it๐’๐Ÿ๐’๐Ÿ

๐’•๐’๐Ÿ๐’•๐’๐Ÿ

, - two successive cycles

โ‡”Hilbert

Dual

Hilbert

space As to the universe,

as to any point in itby means of

the axiom of choice andthe Kochen โ€“ Specker theorem

โ€œLightโ€ โ€œLightโ€

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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??

Page 37: Cyclic mechanics

Gravitational and quantum field as an ideal gas and an ideal โ€œanti-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

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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 โ€œideal gasโ€ composed of mass points (

๐’“ ๐Ÿ๐’•

๐’“ ๐Ÿ๐‘ฌ

isuncertain

Qubits

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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 Avogadroโ€™s number ?โ‡”

Quantum mechanics General relativity

In Paradise: No choice

On earth: Choices, choices ...

โ‡”๐‘ฒ๐‘ฉ

๐‘ต ๐‘จ

Paradise on earth!An ideal gas (aether) of

space-time points:

๐‘น=๐‘ฒ ๐‘ฉ.๐‘ต ๐‘จ

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Time as entropy: โ€œrelicโ€ radiation as a fundamental constant or as a variable

Seen โ€œinsideโ€:Our immense andexpanding universe

determined bythe fundamental

constants

Seen โ€œoutsideโ€:A black hole

among many onesdetermined by

its physical parameterslike mass, energy, etc.

๐‘บ๐’‘๐’†๐’†๐’…๐’•๐’Š๐’Ž๐’†๐Ÿ ๐‘บ๐’‘๐’†๐’†๐’…๐’•๐’Š๐’Ž๐’†๐Ÿ

๐‘ซ๐’†๐’„๐’†๐’๐’†๐’“๐’‚๐’•๐’Š๐’๐’ ๐’•๐’Š๐’Ž๐’†๐Ÿโˆ’๐Ÿ+Energy (D) flow(D) +Energy (S) flow(S)

๐‘บ๐’‘๐’†๐’†๐’…๐’•๐’Š๐’Ž๐’†=๐‘บ๐’•=๐’•๐’•๐ŸŽ

= ๐’‰๐‘ช๐‘ด๐‘ฉ .

๐Ÿ๐’•๐ŸŽ

=( ๐’‰๐‘ช๐‘ด๐‘ฉ )๐’•๐ŸŽ=๐Ÿ

Horizon

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How much should the deceleration of time be?

The ideal gas equation is:

๐’=๐’‘๐’™=(๐‘ต๐‘ฒ ยฟยฟ๐‘ฉ /๐‘ฒ๐’–)๐‘ฌ๐’• ยฟ๐‘บ๐’–=๐‘ต๐’‰๐‘ฒ ๐’–=

๐‘ฒ ๐‘ฉ

๐‘ต ๐‘จ๐‘ต

๐Ÿ๐’• =๐‘ฒ๐‘ฉ

๐‘ช๐‘ด๐‘ฉ๐’‰

๐Ÿ๐’• =๐‘ฒ๐‘ฉ

๐‘ช๐‘ด๐‘ฉ๐’‰ =๐‚=

๐Ž๐Ÿ๐…

The โ€œSupreme Poleโ€ (the Chinese Taiji ๅคชๆฅต )

The universe

Any separatepoint in it

Page 42: Cyclic mechanics

The Einstein and Schrรถdinger equation:the new cyclic mechanics

The Einstein equation Schrรถdingerโ€™s equation

Space & Time= โ€œ0โ€ 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


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