ft makes the new yorker, october 4, 2010 page 71

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FT makes the New Yorker, October 4, 2010 page 71

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FT makes the New Yorker, October 4, 2010 page 71. The Fourier transform.  regularity conditions Functions, A(  ), -  <  <   |A(  )|d  finite FT. a(t) =  exp{it  )A(  )d  -  <  <  Inverse A(  ) =(2 ) -1  exp{-i  t} a(t) dt - PowerPoint PPT Presentation

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Page 1: FT makes the New Yorker, October 4, 2010 page 71

FT makes the New Yorker, October 4, 2010 page 71

Page 2: FT makes the New Yorker, October 4, 2010 page 71

The Fourier transform. regularity conditions

Functions, A(), - < <

|A()|d finite

FT. a(t) = exp{it)A()d - < <

Inverse A() =(2)-1 exp{-it} a(t) dt

unique

C()= A() + B()

c(t) = c(t) + b(t)

2 1

Page 3: FT makes the New Yorker, October 4, 2010 page 71

Convolution (filtering).

d(t) = b(t-s) c( s)ds

D() = B()C()

Discrete FT.

a(t) = T-1 exp{i2ts/T} A(2s/T) s, t = 0,1,...,T-1

A(2s/T) = exp {-i2st/T) a(t)

FFTs exist

Page 4: FT makes the New Yorker, October 4, 2010 page 71

Dirac delta.

g() () d = g(0)

exp {it}() d = 1

inverse

() = (2)-1 exp {-it}dt

Heavyside function H() = signum ()

() = dH()/d

Page 5: FT makes the New Yorker, October 4, 2010 page 71

Mixing. Stationary case unless otherwise indicated

cov{dN(t+u),dN(t)} small for large |u|

|pNN(u) - pNpN| small for large |u|

hNN(u) = pNN(u)/pN ~ pN for large |u|

qNN(u) = pNN(u) - pNpN u 0

|qNN(u)|du <

cov{dN(t+u),dN(t)}= [(u)pN + qNN(u)]dtdu

Page 6: FT makes the New Yorker, October 4, 2010 page 71

Power spectral density. frequency-side, , vs. time-side, t

/2 : frequency (cycles/unit time)

fNN() = (2)-1 exp{-iu}cov{dN(t+u),dN(t)}/dt

= (2)-1 exp{-iu}[(u)pN+qNN(u)]du

= (2)-1pN + (2)-1 exp{-iu}qNN(u)]du

Non-negative, symmetric

Approach unifies analyses of processes of widely varying types

Page 7: FT makes the New Yorker, October 4, 2010 page 71

Examples.

Page 8: FT makes the New Yorker, October 4, 2010 page 71
Page 9: FT makes the New Yorker, October 4, 2010 page 71

Spectral representation. stationary increments - Kolmogorov

)(}exp{/)(

)(1}exp{)(

N

N

dZitdttdN

dZiittN

})(){(},cov{ increments orthogonal

)()()}(),(cov{order of spectrumcumulant

...),...,()...()}(),...,({)()}({

)()(dZ valued,-complex random, :

111...11

N

YX

NNNN

KKNNKKNN

NN

NN

YXEYX

ddfdZdZK

ddfdZdZcumdpdZE

dZZ

Page 10: FT makes the New Yorker, October 4, 2010 page 71

Filtering.

dN(t)/dt = a(t-v)dM(v) = a(t-j )

= exp{it}A()dZM()

with

a(t) = (2)-1 exp{it}A()d

dZN() = A() dZM()

fNN() = |A()|2 fMM()

Page 11: FT makes the New Yorker, October 4, 2010 page 71

Association. Measuring? Due to chance?

Are two processes associated? Eg. t.s. and p.p.

How strongly?

Can one predict one from the other?

Some characteristics of dependence:

E(XY) E(X) E(Y)

E(Y|X) = g(X)

X = g (), Y = h(), r.v.

f (x,y) f (x) f(y)

corr(X,Y) 0

Page 12: FT makes the New Yorker, October 4, 2010 page 71

Bivariate point process case.

Two types of points (j ,k)

Crossintensity. a rate

Prob{dN(t)=1|dM(s)=1}

=(pMN(t,s)/pM(s))dt

Cross-covariance density.

cov{dM(s),dN(t)}

= qMN(s,t)dsdt no () often

Page 13: FT makes the New Yorker, October 4, 2010 page 71

Spectral representation approach.

b.v. of ,)()()}(),(cov{

)(}exp{/)(

)(}exp{/)(

NMMNNM

N

M

FddFdZdZ

dZitdttdN

dZitdttdM

Page 14: FT makes the New Yorker, October 4, 2010 page 71

Frequency domain approach. Coherency, coherence

Cross-spectrum.

duuquif MNMN )(}exp{21)(

Coherency.

R MN() = f MN()/{f MM() f NN()}

complex-valued, 0 if denominator 0

Coherence

|R MN()|2 = |f MN()| 2 /{f MM() f NN()|

|R MN()|2 1, c.p. multiple R2

Page 15: FT makes the New Yorker, October 4, 2010 page 71

where

A() = exp{-iu}a(u)du

fOO () is a minimum at A() = fNM()fMM()-1

Minimum: (1 - |RMN()|2 )fNN()

0 |R MN()|2 1

AAfAfAfff MMNMMNNNOO

Proof. Filtering. M = {j }

a(t-v)dM(v) = a(t-j )

Consider

dO(t) = dN(t) - a(t-v)dM(v)dt, (stationary increments)

Page 16: FT makes the New Yorker, October 4, 2010 page 71

Proof.

0 Take

0

sderivative second andfirst Consider

1

1

MNMMNMNN

MMNM

OO

MMNMMNNNOO

ffffffA

f

AAfAfAfff

Coherence, measure of the linear time invariant association of the components of a stationary bivariate process.

Page 17: FT makes the New Yorker, October 4, 2010 page 71

Regression analysis/system identification.

dZN() = A() dZM() + error()

A() = exp{-iu}a(u)du

Page 18: FT makes the New Yorker, October 4, 2010 page 71

Empirical examples.

sea hare

Page 19: FT makes the New Yorker, October 4, 2010 page 71

Mississippi river flow

Page 20: FT makes the New Yorker, October 4, 2010 page 71
Page 21: FT makes the New Yorker, October 4, 2010 page 71
Page 22: FT makes the New Yorker, October 4, 2010 page 71

Partial coherency. Trivariate process {M,N,O}

]}||1][||1{[/][ 22| ONMOONMOMNOMN ffffff

“Removes” the linear time invariant effects of O from M and N

Page 23: FT makes the New Yorker, October 4, 2010 page 71
Page 24: FT makes the New Yorker, October 4, 2010 page 71
Page 25: FT makes the New Yorker, October 4, 2010 page 71

Time series variants.

details later

continuous time case

Mixing.

cov{Y(t+u),Y(t)} = cYY(u)

small for large |u|

|cYY(u)|du <

Page 26: FT makes the New Yorker, October 4, 2010 page 71

Power spectral density. frequency-side, , vs. time-side, t

/2 : frequency (cycles/unit time)

fYY() = (2)-1 exp{-iu}cov{Y(t+u),Y(t)}

= (2)-1 exp{-iu}cYY(u)du -<<

Non-negative, symmetric

Approach unifies analyses of processes of widely varying types

Things in the frequency domain look the same

Page 27: FT makes the New Yorker, October 4, 2010 page 71

Spectral representation.

Y(t) = exp{it}dZY() - < t <

ZY() random, complex-valued conj{ZY()} = ZY(-)

E{dZY()} = ()cNd

cov{dZY(),dZY()}=(-)f NN()dd

cum{dZY(1),...,dZY(K)} = ...

Page 28: FT makes the New Yorker, October 4, 2010 page 71

Filtering.

Yt) = a(t-v)X(v)dv

= exp{it}A()dZX()

with

a(t) = (2)-1 exp{it}A()d

dZY() = A() dZX()

fYY() = |A()|2 fXX()

Page 29: FT makes the New Yorker, October 4, 2010 page 71

Bivariate time series case.

(X(t),Y(t)) - < t <

Cross-covariance function. general case

cov{X(s),Y(t)}

= cXY(s,t)

Page 30: FT makes the New Yorker, October 4, 2010 page 71

Spectral representation approach.

b.v. of ,)()()}(),(cov{

)(}exp{/)(

)(}exp{/)(

NMXYYX

Y

X

FddFdZdZ

dZitdttdY

dZitdttdX

FXY(.): cross-spectral measure

Page 31: FT makes the New Yorker, October 4, 2010 page 71

Frequency domain approach. Coherency, coherence

Cross-spectrum.

f XY()= (2)-1 exp{-iu)c XY(u)du -< <

complex-valued

Coherency.

R XY() = f XY()/{f XX() f YY()}

0 if denominator 0

Coherence.

|RXY()|2 = |f XY()| 2 /{fXX() fYY()|

|RXY()|2 1, c.p. multiple R2

Page 32: FT makes the New Yorker, October 4, 2010 page 71

Regression analysis/system identification.

dZY() = A() dZX() + error()

A() = exp{-iu}a(u)du

Page 33: FT makes the New Yorker, October 4, 2010 page 71

Partial coherency. Trivariate process {X,Y,O}

]}||1][||1{[/][ 22

| OYXOOYXOXYOXYffffff

“Removes” the linear time invariant effects of O from X and Y