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Stochastic Meaning Theory 5 Language as Brown Motion For ZHANG Taiyan 2 / August 12, 2008

Stochastic Meaning Theory 5

Language as Brown Motion
For ZHANG Taiyan 2

TANAKA Akio

[A]
1
Abstractive space     Ω
σ additive family that consists of subset of Ω     F
Measure that is defined over F     P
P satisfies P (Ω ) = 1. 
P      probability measure over ( Ω, F )
Ω      sample space     
( Ω, F , P )     Probability space
Element of Ω     sample ω
Element of F     event A
Probability that event A occurs     probability P ( A )
Real number valued Borel measurable function over Ω     random variable X = X ( ω )
Random variable is integrable.
Mean (Expectation) of X     E[X] = ∫Ω X ( ω ) P ( dω )
2
Measurable space     ( S, S )
X : ( Ω, F ) → ( S, S )
X is measurable.
X      S-value random variable.
Random variable     X1, …, Xd
X : = (X1, …, Xd )     Rd-value random variable
3
Rd-value random variable     X
E[X i 2] < ∞
E[(X - E[X])2]     variance
4
S-value random variable.     X
PX : = P ( X ∈A ), A∈S     distribution
5
Real number space     R
Borel set family over R    B ( R )
Probability measure over ( R, B ( R ) )     μ
6
Rd-value random variable     X
ψX (ξ ) : = E[eiξ・X], ξ∈Rd     characteristic function
7
Lebesgue measure     dx
Mean     m∈R
Variance     v >0
Measure over R     μ ( dx ) = e -(x-m)2 / 2v dx /     Gauss distribution ( normal distribution)
8
(2p – 1 ) !! : = (2p – 1 ) ・(2p – 3 ) … 3・1
E[X2p] = (2p – 1 ) !! v p     moment of X
9
Event     A, B∈F
When (A∩B) = P(A) P(B), A and B are independent each other.
10
Integrable and independent random variable     X, Y
Product XY     integrable
E[XY] = E[X]E[Y]
11
Time     t
t ∈[0, ∞)
Family of Rd-value random variable ≥    X = ( Xt ) t ≥ 0     d-dimensional stochastic process
∀ω∈Ω
When Xt (ω) is continuous as function of t., d-dimensional stochastic process is called to be continuous.
12
σ additive family     Ft
Ft  ⊂F
0 ≤ s ≤ t
F s  ⊂Ft
(Ft  ) = (Ft  ) t ≥ 0   increase information system
13
d-dimensional stochastic process     X = ( Xt ) t ≥ 0    
∀t ≥ 0
Xt : Ω → Rd  is Ft – measurable.
X = ( Xt ) t ≥ 0 is (Ft ) – adapted.
14
Mapping ( t, ω) ∈([0, ∞)×Ω, B([0, ∞)]×F) ↦ Xt ( ω) ∈( Rd, B ( Rd ) )
When the mapping is measurable, X = ( Xt ) t ≥ 0  is called to be measurable.
15
X = ( Xt )
Ft0 = Ft0,X : = σ ( XS ; s≤t )
16
Probability space      ( Ω, F , P )    
Stochastic process defined over  ( Ω, F , P )      (Bt)t ≥ 0 = (Bt(ω)) t ≥ 0
(Bt)t ≥ 0 that satisfies the next, it is called Brownian motion.
(i) P ( B0 = 0  ) = 1
(ii) For ∀ω∈Ω, Bt (ω) is continuous on t.
(iii) For 0 = t0<∀t1<…<tn, ∀n∈N, {Bti-Bti-1} satisfies the next.
a) {Bti-Bti-1} are independent each other.
b) {Bti-Bti-1} are followed by mean 0 and variance ti-ti-1 of Gauss distribution.
17
(Existence theorem)
Over adequate probability space, there exists Brownian motion.
18
Ω = W0
F = B ( W0 )
Brownian motion has the next.
(i)Bt ( w ) = Wt
(ii) w = ( wt ) t ≥0 ∈W 0
Measure over ( W0, B ( W0 ) )      P
P is called Wiener measure.
19
d-dimensional Brownian motion     B = ( Bt ) t ≥ 0
d×d orthogonal matrix     A
ABt     d-dimensional Brownian motion
Sphere     S : = δ B (0, r),  B (0, r) = {|x| ≤ r }
Hitting time     σS (ω) : = inf{t >0; Bt ∈S }
Hitting place    BσS (ω)
Distribution of BσS (ω)      uniform stochastic measure
20
d-dimensional Brownian motion     B = ( Bt ) t ≥ 0
x∈Rd
Brownian motion from x     ( x + Bt ) t ≥ 0
W  d = B ( W d )
Space     (W d, W d )
Distribution over  (W d, W d )     Px
Mean on Px     Ex [ ・ ]
Probability space     (W d, W d , Px )
Stochastic process over (W d, W d , Px )    Bt ( w ), w∈W d ; Bt ( w ) = wt
Sub σ additive family of W d     Ft0 =σ (Bs ; s≤t ) , Ft = Ft0 ⋁ N, t≥0 ; N : = {N∈W d ; Px (N) = 0, ∀x ∈Rd }
Ft* = Ft+ : = ∩s>t Fs
Shift operator over W d     θs : W d → W d , s≥0 ; (θs (w) ) t : = wt+s
Bt ∘  θs  = Bt+s
21
(Markov property)
∀x∈Rd
∀s≥0
∀Y = Y (w) : W d –measurable bounded function over W d
Ex[Y∘θs ・1A] = Ex[EBs(w)[Y]∘θs ・1A] , ∀A∈F s
By conditional mean
Ex[Y∘θs | Fs] (w) = EBs(w)[Y
Px-a.s.w
22
(Blumenthal’s 0-1 law)
When A∈F0 ( = F0* ), Px (A) = 0 or 1
23
Random variant of 1-dimensional Brownian motion starting from the origin     B
σ (0,∞) : = inf {t >0; Bt∈(0,∞) }
A = {σ(0,∞) = 0 }
A ∈F0*
P (σ(0,∞) = 0 ) = 0 or 1
t↓0
P (σ(0,∞) = 0 ) = 1
From symmetry of Brownian motion Bt = -Bt

[B]
Language that has Brownian motion     LB
LB has actual language and imaginary language.

[References]
Mirror Theory For the Structure of Prayer / Dedicated to the Memory of CHINO Eiichi / Tokyo June 5, 2004
Mirror Language / Tokyo June 10, 2004
Guarantee of Language / For LÉVI-STRAUSS Claude / Tokyo June 12, 2004
Actual Language and Imaginary Language / To LÉVI-STRAUSS Claude / Tokyo September 23, 2004


To be continued
Tokyo August 12, 2008
Sekinan Research Field of Language

Stochastic Meaning Theory 4 Energy of Language For ZHANG Taiyan and Wenshi 1908 / July 24, 2008

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