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
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 )
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
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