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a
b
15
1
0.9
10
0.8
5
0.7
0.6
0
0.5
−5
0.4
0.3
−10
0.2
−15
0.1
−20
0
−8
−6
−4
−2
0
2
4
6
0
200
400
600
800
1000
1200
1400
1600
1800
2000
x
k (iterations)
Fig. 7.1 ( a ) Wiener random walk ( b ) Solution of Schrödinger's equation: Shifted Gaussians that
give the probability density function of a stationary diffusion process ( continuous curves )andthe
approximation of the p.d.f. by symmetric triangular possibility distributions ( dashed lines )
(or decrements), then according to the CLT it must follow a Gaussian distribution.
Thus one obtains:
Ef w .t/gD0 while EΠw .t/ Ef w .t/g 2
D 2 t
(7.5)
7.2.3
Outline of Wiener Process Properties
Wiener's process is a stochastic process that satisfies the following conditions:
1. w .0/ D 0
2. The distribution of the stochastic variable w .t/ is a Gaussian one with a p.d.f.
.x;t/ which satisfies the following relation
@ 2 .x;t/
@x 2 ;.x;0/D ı.x/
@.x;t/
@t
2
2
(7.6)
D
For a limited number of time instants t 1 <t 2 < <t n the stochastic variables
w .t j / w .t j1 / are independent.
3. It holds that Ef w .t/gD0 and EfΠw .t/ w .s/ 2
D 2 .t s/g for all 0st.
4. w .t/ is a continuous process
The standard Wiener process evolves in time according to the following relation
p hN.0;1/
(7.7)
w .t C h/ D w .t/ C
The Wiener process actually describes a diffusion phenomenon and the associated
p.d.f. of stochastic variable is given by
p 2t e x 2
1
.x;t/ D
(7.8)
2t
 
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