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Time-Continous Stochastic Processes 0. Time Continous Stochastic Processes

1. The document discusses time-continuous stochastic processes and their properties such as stationarity and ergodicity. 2. It defines correlation functions including the autocorrelation function (ACF) and cross-correlation function (CCF), and describes their characteristics for stationary processes. 3. The power density spectrum (PDS) is introduced as the Fourier transform of the ACF, and properties such as the average process power are described.

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0% found this document useful (0 votes)
69 views10 pages

Time-Continous Stochastic Processes 0. Time Continous Stochastic Processes

1. The document discusses time-continuous stochastic processes and their properties such as stationarity and ergodicity. 2. It defines correlation functions including the autocorrelation function (ACF) and cross-correlation function (CCF), and describes their characteristics for stationary processes. 3. The power density spectrum (PDS) is introduced as the Fourier transform of the ACF, and properties such as the average process power are described.

Uploaded by

Huy Du
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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0.

Time-Continous
Time
Continous Stochastic Processes
process X(t)

single realisation of

X(t) : sample function x(t)

A process is stationary, if the ensemble averages (moments,


autocorrelation function, cross-correlation function,
probability density functions) are independent of time.
If you can calculate the expected values of a process
by averaging one sample function in time domain
instead of averaging an ensemble of sample functions
functions,
then the process is ergodic.
An ergodic process is always stationary too ,
but a stationary process need not to be ergodic.
We will only
y consider ergodic
g
p
processes on the next slides.
0-1

Correlation Functions

Time-Continous
Time
Continous Stochastic Processes
process X (t ) , function g ( X (t )) :

moments

E{g ( X (t ))} = g (x ) p X ( x ) dx = lim

1st moment:

E{ X } =

T /2
1
T

g (x(t )) dt

T / 2

x p (x ) dx =
X

2nd moment:

{ } x

E X2 =

p X ( x ) dx

variance:

E X X

}= E{ X } (E{ X })
2

= =
2
X

0-2

Power Density Spectrum

2
X

p X ( x ) dx

Correlation Functions of Continous Processes


autocorrelation function (ACF) of a complex-valued process X(t):

rXX ( 1 , 2 ) = E X ( 1 ) X ( 2 ) = E{( X R ( 1 ) jX I ( 1 )) ( X R ( 2 ) + jX I ( 2 ))}


stationary processes: 1 t , 2 t +
autocovariance function:

{[

(t + ) X ]} = rXX ( ) X
c XX ( ) = rXX ( )

c XX ( ) = E X (t )

zero mean processes

rXX ( ) = E X (t ) X (t + )

] [X

cross correlation function (CCF) of two processes X(t) and Y(t):


cross-correlation

rXY ( 1 , 2 ) = E X ( 1 ) Y ( 2 )
0-3

stationary rXY

( ) = E{X (t ) Y (t + )}

Correlation Functions

Correlation Functions of Continous Processes


characteristics of ACF

(
)
r

=
r
XX
XX ( )

real processes

rXX ( ) = rXX ( )

max{rXX ( )} = rXX (0 )

{
(
)
(
)
(
)
(
)
rXX 0 = E{X t X t } = E X t }

zero mean

ACF is even

rXX (0) = X2

characteristics of CCF

rXY ( ) = rYX ( )

real processes

c XY ( ) = rXY ( ) X Y

rXY ( ) = rYX ( )

cross-covariance

uncorrelated processes: c XY ( ) = 0 rXY ( ) = X Y


orthogonal processes:
0-4

rXY ( ) = 0

uncorr. processes with


Correlation Functions

or

Y = 0

Power Density Spectrum


(Power Density Spectrum, PDS)

definition (Wiener-Khintshine theorem)

S XX ( j ) = F{ rXX ( )} =

j
r
(

)
e
d
XX

explanation of plausibility:
see slide 9

ACF is conjugate even power density spectrum is real

process average power (zero mean):


Var{X (t )} =

2
X

1
2

XX

( j ) d

= rXX (0)

white noise: PDS is a constant ( infinite power only a model)


S XX ( j ) = N 0 / 2 with - < <

rXX ( ) = F1{N 0 / 2} = N 0 / 2 0 ( )
0-5

Power Density Spectrum

Definition of Wiener-Khintschine : explanation of


plausibility
x(t ) if T t T
xT (t ) =
finite sample function:
X T ( j )
otherwise
0
T

finite energy:

xT (t ) dt =
2

average power:

1
2

X T ( j ) d
2

Theorem of Parseval

T
1
2T

xT (t ) dt =
2

1
2

1
2T

X T ( j ) d PDS of sample func.


2

definition: PDS of the ergodic process X(t)


mean off a sample
l ffunction
ti with
ith iinfinite
fi it llength
th :

S XX ( j ) = lim

0-6

1
2T

X T ( j )

Power Density Spectrum

Definition of Wiener-Khintschine : explanation of


plausibility

S XX ( j ) = F{rXX ( )} = rXX ( ) e j d

Wiener-Khintschine:

ergodic processes: rXX ( ) = lim

S XX ( j )
T

= lim

0-7

1
2T

lim

1
2T

(
)
(
)
(t ) X (t + )}
{
x
t

x
t
+

dt

E
X
T
T

e
d =
(
)
(
)
x
t

x
t
+

dt
T T

x ( t ) x ( t + )e

T T

1
2T

1
dtd = Tlim
2T

j
(
t
)
(
t

)
d dt
x
x
+
e
T T

Power Density Spectrum

Definition of Wiener-Khintschine : explanation of


plausibility

67
8

j
+ j t
(
)
(
)
x
t
x
t
+

e
e
T
T

= lim 21T
T

4
6
47
8
( t + )

d dt

(substitution: = t + ; d = d )
T

= lim 21T
T

0-8

j t
j
1
(
)
(
)
x
t
e
dt

x
e
=
( )

lim
T
T
T
T
2T X T j
T
14
4244
3 1442443
X T j
X T ( j )

Power Density Spectrum

(see slide 8)

Response of a linear system to a random input signal


random input signal : X (t )
h(t )
random output signal : Y (t )

impulse response:

(Energy-) ACF :

rhhE ( ) = h (t ) h(t + ) dt = h( ) h ( )

ACF of the output:

rYY ( ) = rXX ( ) rhhE ( ) = rXX ( ) h( ) h ( )

CCF off ini / output:


t t rXY ( ) = rXX ( )
PDS of output process:

h( )

SYY ( j ) = S XX ( j ) H ( j )

no phase information!

Cross-power density spectrum: S XY ( j ) = S XX ( j ) H ( j )


((between input
p and output)
p )
0-9

Response of a Linear System

Response of a linear system to a random input signal


white noise as input signal of a linear system:

rYY ( ) = N 0 / 2 0 ( ) rhhE ( ) = N 0 / 2 rhhE ( )

SYY ( j ) = N 0 / 2 H ( j )

rXY ( ) = N 0 / 2 0 ( ) h( ) = N 0 / 2 h( )

S XY ( j ) = N 0 / 2 H ( j )
0-10

Response of a Linear System

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