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Friday, 16 May 2025

Stochastic Meaning Theory 4 Energy of Language For ZHANG Taiyan and Wenshi 1908

 Stochastic Meaning Theory 4

 

Energy of Language

For ZHANG Taiyan and Wenshi 1908

 

TANAKA Akio

 

1

Domain     Λ∈R3

Substantial particles     N-number m-mass 

Particles are assumed to Newton dynamics.

Place coordinate of particle i in N-number particles     ri∈Λ

Momentum of particle     pi∈R3

State at a moment     γ = (r1, …, rN, p1, …, pN)

Set of state γ     PΛ, N ≃ΛN ×R3N⊂R6N

PΛ, N is called phase space.

2

Volume     V

Particles     n- mol

Energy     U  

Parameter space     E

Point of E     ( U, V, n )

3

Subspace     PΛ, N ( U )

Volume of PΛ, N ( U )     WΛ, N ( U )

4

Adiabatic operation      ( U, V, n ) →  ( U’, V’, n’ )

Starting state of γ∈PΛ, N

Ending state of γ∈PΛ’, N

Map of time development    f

5

Volume of PΛ’, N ( U’ )     WΛ’, N ( U’ )

Volume of f (PΛ, N ( U ) ) is equivalent to WΛ, N ( U ).

f (PΛ, N ( U ) ) is subspace of PΛ’, N ( U’ )

WΛ, N ( U ) ≤ WΛ’, N ( U’ )

6

Equilibrium state     ( U, V, n )

Another equilibrium state       ( U’, V’, n’ )

Two volume of equilibrium states are seemed to be one state at phase space     WΛ, N ( U ) WΛ’, N’ ( U’ )

Operation of logarithm of equilibrium state at phase space     S ( U, V, n ) = k log WΛ, N ( U ) , (k ; arbitrary constant)

7

Phase space     2n- dimension

Differential 2-form    ω

Local coordinate     qi, pi

ω = ∑ni=1d qi, ∧dpi

ω is called symplectic form.

2n- dimensional manifold     M

Pair    (M, ω)

(M, ω) that satisfies the next is called symplectic manifold.

(i) dω = 0

(ii) ωn ≠0

Phase space is expressed by symplectic manifold.

8

Hamiltonian system

Coordinate    ( q, p ) = (q1, …, qn, p1, …, pn )

Phase space     R2n

C1 class function     H = (q, p, t )

 = ( 1≤i ≤n )

 = ( 1≤i ≤n )

9

An assumption from upper 8

H : = Sentence

q : = Place where word exists

p : = Momentum of word

t : = Time at which sentence is generated

10

Equilibrium state of sentence     H

Another equilibrium state of sentence     H’

Adiabatic process of language     H → H’

Entropy of language     S

H → H’ ⇔ S (H ) ≤ S (H’ )

 

[References]

Warp Theory / Tokyo October 24, 2004

Quantum Warp Theory Warp / Tokyo December 31, 2005

 

To be continued

Tokyo July 24, 2008

Sekinan Research Field of Language

www.sekinan.org

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