Extremes of supOU processes Vicky Fasen August 16, 2005 - - PowerPoint PPT Presentation

extremes of supou processes
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Extremes of supOU processes Vicky Fasen August 16, 2005 - - PowerPoint PPT Presentation

Extremes of supOU processes Vicky Fasen August 16, 2005 fasen@ma.tum.de Graduate Program Applied Algorithmic Mathematics Munich University of Technology http://www-m4.ma.tum.de/pers/fasen/ Vicky Fasen p. 1/22 Overview


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SLIDE 1

Extremes of supOU processes

Vicky Fasen August 16, 2005

fasen@ma.tum.de

Graduate Program ”Applied Algorithmic Mathematics” Munich University of Technology

http://www-m4.ma.tum.de/pers/fasen/

Vicky Fasen – p. 1/22

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SLIDE 2

Overview

  • Introduction

◮ i. d. i. s. r.m ◮ SupOU process ◮ Class of convolution equivalent tails ◮ Model assumptions of this talk

  • Extremal behavior
  • Conclusion

Vicky Fasen – p. 2/22

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SLIDE 3
  • i. d. i. s. r. m

Definition A stochastic process Λ = {Λ(A) : A ∈ B(R+ × R)} is called an i. d. i. s. r. m. (infinitely divisible independently scattered random measure) on R+ × R, if for disjoint sets (An)n∈N in B(R+ × R),

  • Λ

  • n=1

An

  • =

  • n=1

Λ(An) a. s. (r. m.)

  • (Λ(An))n∈N is an independent sequence

(i. s.)

  • Λ(A) is infinitely divisible for every A ∈ B(R+ × R)

(i. d.)

Vicky Fasen – p. 3/22

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SLIDE 4
  • i. d. i. s. r. m

We consider only i. d. i. s. r. m. with characteristic function E[exp (iuΛ(A))] = exp(Π(A)ψ(u)) for u ∈ R, A ∈ B(R+ × R+), where

  • ψ is the cumulant generating function of a Lévy process

with generating triplet (m, σ2, ν) E[exp (iuL(t))] = exp (tψ(u))

  • Π(dω) = π(dr) × λ(dt) for ω = (r, t) ∈ R+ × R, where λ is

the Lebesgue measure and π is a probability measure on R+ (m, σ2, ν, π) are called the generating quadruple of Λ

Vicky Fasen – p. 4/22

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SLIDE 5
  • i. d. i. s. r. m

We consider only i. d. i. s. r. m. with characteristic function E[exp (iuΛ(A))] = exp(Π(A)ψ(u)) for u ∈ R, A ∈ B(R+ × R+), where

  • ψ is the cumulant generating function of a Lévy process

with generating triplet (m, σ2, ν) E[exp (iuL(t))] = exp (tψ(u))

  • Π(dω) = π(dr) × λ(dt) for ω = (r, t) ∈ R+ × R, where λ is

the Lebesgue measure and π is a probability measure on R+ (m, σ2, ν, π) are called the generating quadruple of Λ Λ is called Lévy random field

Vicky Fasen – p. 4/22

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SLIDE 6

Compound Poisson random measure

Let ν be finite. Then N =

  • k=1

ε(Rk,Γk,Zk) where

  • (Rk) i. i. d. with d. f. π
  • (Γk) jump times of a Poisson process with intensity µ = ν(R)
  • (Zk) i. i. d. with d. f. ν/µ

is a Poisson random measure with intensity π(dr) × dt × ν(dx) Λ(A) =

  • R

x dN(A, x) =

  • k=1

Zk 1{(Rk,Γk)∈A} is a compound Poisson random measure

Vicky Fasen – p. 5/22

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SLIDE 7

Compound Poisson random measure

Let ν be finite. Then N =

  • k=1

ε(Rk,Γk,Zk) where

  • (Rk) i. i. d. with d. f. π
  • (Γk) jump times of a Poisson process with intensity µ = ν(R)
  • (Zk) i. i. d. with d. f. ν/µ

is a Poisson random measure with intensity π(dr) × dt × ν(dx) Λ(A) =

  • R

x dN(A, x) =

  • k=1

Zk 1{(Rk,Γk)∈A} is a Lévy jump field

Vicky Fasen – p. 5/22

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SLIDE 8

Compound Poisson random measure

Let ν be finite. Then N =

  • k=1

ε(Rk,Γk,Zk) where

  • (Rk) i. i. d. with d. f. π
  • (Γk) jump times of a Poisson process with intensity µ = ν(R)
  • (Zk) i. i. d. with d. f. ν/µ

is a Poisson random measure with intensity π(dr) × dt × ν(dx) Λ(R+ × [0, t]) =

  • k=1

Zk 1{(Rk,Γk)∈R+×[0,t]} =

N(t)

  • k=1

Zk

Vicky Fasen – p. 5/22

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SLIDE 9

Underlying Lévy process

Let Λ be an i. d. i. s. r. m. We denote by L = (L(t))t∈R the underlying driving Lévy process with L(t) = Λ(R+ × [0, t]) L has the characteristic triplet (m, σ2, ν)

Vicky Fasen – p. 6/22

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SLIDE 10

supOU process

Definition The supOU process (superposition of Ornstein-Uhlenbeck processes) Y is defined by Y (t) =

  • R+×R

e−r(t−s) 1[0,∞)(t − s) dΛ(r, s) where

  • |x|≥2

log |x| ν(dx) < ∞

  • λ−1 =
  • R+

r−1 π(dr) < ∞

Vicky Fasen – p. 7/22

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SLIDE 11

Special cases

  • Λ a compound Poisson random measure

(Λ(A) = ∞

k=1 Zk 1{(Rk,Γk)∈A}):

Y (t) =

  • R+×R

e−r(t−s) 1[0,∞)(t − s) dΛ(r, s) =

N(t)

  • k=−∞

e−Rk(t−Γk)Zk

  • OU-process: π(λ) = 1: Y (t) =

t

−∞

e−λ(t−s) dL(s)

  • π discrete with π(λk) = pk and ∞

k=1 pk = 1. Then

Y (t) =

  • k=1

t

−∞

e−λk(t−s) dLk(s) where (Lk) are independent Lévy processes with characteristic triplet (pkm, pkσ2, pkν)

Vicky Fasen – p. 8/22

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SLIDE 12

Properties of a supOU process

  • (m, σ2, ν) determines the marginal distribution:

mY = 1 λ

  • m +
  • |y|>1

y |y| ν(dy)

  • σ2

Y = σ2

2λ νY [x, ∞) = 1 λ ∞

x

ν [y, ∞) y dy

  • π determines the correlation function ρ:

ρ(h) = λ ∞ r−1e−hr π(dr)

  • e. g. π(dr) = Γ(2H + 1)−1r2He−r dr for r > 0, H > 0, then

ρ(h) = (h + 1)−2H for h ≥ 0

Vicky Fasen – p. 9/22

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SLIDE 13

Properties of a supOU process

  • (m, σ2, ν) determines the marginal distribution:

mY = 1 λ

  • m +
  • |y|>1

y |y| ν(dy)

  • σ2

Y = σ2

2λ νY [x, ∞) = 1 λ ∞

x

ν [y, ∞) y dy λ−1 =

  • R+ r−1 π(dr)
  • π determines the correlation function ρ:

ρ(h) = λ ∞ r−1e−hr π(dr)

  • e. g. π(dr) = Γ(2H + 1)−1r2He−r dr for r > 0, H > 0, then

ρ(h) = (h + 1)−2H for h ≥ 0

Vicky Fasen – p. 9/22

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SLIDE 14

Properties of a supOU process

  • (m, σ2, ν) determines the marginal distribution:

mY = 1 λ

  • m +
  • |y|>1

y |y| ν(dy)

  • σ2

Y = σ2

2λ νY [x, ∞) = 1 λ ∞

x

ν [y, ∞) y dy

  • π determines the correlation function ρ:

ρ(h) = λ ∞ r−1e−hr π(dr)

  • e. g. π(dr) = Γ(2H + 1)−1r2He−r dr for r > 0, H > 0, then

ρ(h) = (h + 1)−2H for h ≥ 0

Reference: Barndorff-Nielsen (2001), Barndorff-Nielsen and Shephard (2001)

Vicky Fasen – p. 9/22

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SLIDE 15

Examples

200 400 600 800 1000 1200 1400 1600 1800 2000 10 20 30 40 supOU process 200 400 600 800 1000 1200 1400 1600 1800 2000 10 20 30 40 OU process

Vicky Fasen – p. 10/22

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SLIDE 16

Class of convolution equivalent tails S(γ)

Let F be a d. f. on R with F(x) < 1 for every x ∈ R. F belongs to the class S(γ), γ ≥ 0, if (i) F belongs to the class L(γ), γ ≥ 0, i. e. for all y ∈ R locally uniformly lim

x→∞F (x + y)/F (x) = e−γy

(ii) lim

x→∞F 2∗(x)/F (x) = 2

  • R

eγx dF (x) < ∞ The class γ = 0 is called subexponential d. f. s denoted by S Examples:

  • γ = 0: stable-, Weibull-, loggamma-, Pareto distribution
  • γ > 0: generalized inverse Gaussian distribution

Vicky Fasen – p. 11/22

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SLIDE 17

Properties of S(γ)

Let F be infinitely divisible with Lévy measure ν and γ ≥ 0. Then F ∈ S(γ) ⇔ ν (1, ·] ν(1, ∞) ∈ S(γ) ⇔ lim

x→∞

F (x) ν(x, ∞) =

  • R

eγx F (dx)

Vicky Fasen – p. 12/22

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SLIDE 18

Model

In this talk we restrict our attention to a supOU process driven by a positive compound Poisson random measure, i. e. Zk is positive and ν(R) < ∞. Y (t) =

N(t)

  • k=−∞

e−Rk(t−Γk)Zk a) L(1) ∈ S(γ) ∩ MDA(Λ): lim

n→∞nP(L(1) > anx + bn) = e−x

b) L(1) ∈ S(γ) ∩ MDA(Φα) = Rα: lim

n→∞nP(L(1) > anx) = x−α

Vicky Fasen – p. 13/22

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SLIDE 19

Overview

  • Introduction
  • Extremal behavior

◮ Tail behavior of Y ◮ Tail behavior of M(h) ◮ Point process behavior ◮ Running maxima

  • Conclusion

Vicky Fasen – p. 14/22

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SLIDE 20

Representation

If L(1) ∈ L(γ) then P(L(1) > x) = c(x) exp

x 1 a(y) dy

  • ,

x > 0, where a, c : R+ → R+ lim

x→∞ c(x) = c > 0

a is absolutely continuous lim

x→∞ a(x) = 1

γ lim

x→∞ a′(x) = 0

Vicky Fasen – p. 15/22

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SLIDE 21

Tail behavior of Y (t)

lim

x→∞ a(x)/x = 0

lim

x→∞ a(x) = 1/γ

a) L(1) ∈ S(γ) ∩ MDA(Λ): P(Y (t) > x) ∼ 1 λ a(x) x EeγY (t) EeγL(1)P(L(1) > x) for x → ∞ b) L(1) ∈ S(γ) ∩ MDA(Φα): P(Y (t) > x) ∼ 1 λαP(L(1) > x) for x → ∞

Vicky Fasen – p. 16/22

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SLIDE 22

Tail behavior of M(h)

Let h > 0 and M(h) = sup0≤t≤h Y (t) a) L(1) ∈ S(γ) ∩ MDA(Λ): P(M(h) > x) ∼ hEeγY (t) EeγL(1)P(L(1) > x) for x → ∞ b) L(1) ∈ S(γ) ∩ MDA(Φα): P(M(h) > x) ∼ [h + (λα)−1]P(L(1) > x) for x → ∞

Vicky Fasen – p. 17/22

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SLIDE 23

Example: OU-Weibull Process

L(t) = N(t)

k=1 Zk,

Y (t) = N(t)

k=−∞ e−λ(t−Γk)Zk

20 40 60 80 100 120 140 160 180 200 5 10 15 20 25 30

Path of a OU−Weibull−process, p=0.5

Y(Γk)=Zk+Y(Γk) −ZK

Vicky Fasen – p. 18/22

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SLIDE 24

Example: OU-Weibull Process

Y (Γk) > aTx + bT ⇐ ⇒ a−1

T (Y (Γk) − bT) > x

20 40 60 80 100 120 140 160 180 200 5 10 15 20 25 30

Path of a OU−Weibull−process, p=0.5

Y(Γk)=Zk+Y(Γk) −ZK

sT tT

uT(x) =aTx+bT

Vicky Fasen – p. 18/22

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SLIDE 25

Example: OU-Weibull Process

κT =

  • k=1

ε Γk

T ,a−1 T (Y (Γk)−bT )

,

I = [s, t) × (x, ∞)

20 40 60 80 100 120 140 160 180 200 5 10 15 20 25 30

Path of a OU−Weibull−process, p=0.5

Y(Γk)=Zk+Y(Γk) −ZK

sT tT

uT(x) =aTx+bT κT([s,t)×(x,∞)) =3

Vicky Fasen – p. 18/22

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SLIDE 26

Point process behavior

a) L(1) ∈ S(γ) ∩ MDA(Λ) : ∞

k=1 ε(sk,Pk) ∼ PRM(dt × e−x dx) ∞

  • k=1

ε(T −1Γk,a−1

T

(Y (Γk)−bT )) T→∞

= ⇒

  • k=1

ε(sk,Pk+γYk) b) L(1) ∈ Rα: ∞

k=1 ε(sk,Pk) ∼ PRM(dt × αx−α−1 dx) ∞

  • k=1

ε(T −1Γk,a−1

T

Y (Γk)) T→∞

= ⇒

  • k=1

  • j=0

ε(sk,exp (−RkΓk,j)Pk)

Vicky Fasen – p. 19/22

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SLIDE 27

Point process behavior

a) L(1) ∈ S(γ) ∩ MDA(Λ) : ∞

k=1 ε(sk,Pk) ∼ PRM(dt × e−x dx) ∞

  • k=1

ε(T −1Γk,a−1

T

(Y (Γk)−bT )) T→∞

= ⇒

  • k=1

ε(sk,Pk+γYk) b) L(1) ∈ Rα:

Motivation: Y (Γk + t) = N(Γk+t)

i=−∞

e−Ri(Γk+t−Γi)Zi Y (Γk + t) ≈ e−RktZk Y (Γk+j) ≈ e−Rk(Γj+k−Γk)Zk

  • k=1

ε(T −1Γk,a−1

T

Y (Γk)) T→∞

= ⇒

  • k=1

  • j=0

ε(sk,exp (−RkΓk,j)Pk)

Vicky Fasen – p. 19/22

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SLIDE 28

Running maxima

Let M(T) = sup0≤t≤T Y (t). a) L(1) ∈ S(γ) ∩ MDA(Λ): lim

T→∞P(a−1 T (M(T ) − bT) ≤ x) = exp(−Ee−γY (t)e−x)

b) L(1) ∈ S(γ) ∩ MDA(Φα): lim

T→∞P(a−1 T M(T ) ≤ x) = exp(−x−α)

Vicky Fasen – p. 20/22

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SLIDE 29

Conclusion

Extension Y (t) =

  • R+×R

f(r, t − s) dΛ(r, s)

  • Kernel functions f : R+ × R+ → R+ with f(r, 0) = f + and

f(r, s) < f + for r ∈ supp(π), s > 0, which are non-increasing in both coordinates and lims→∞ f(r, s) = 0 for r ∈ supp(π)

  • L(1) ∈ S:

◮ any kernel function with a finite number of extremes ◮ neglecting the assumption, that Λ is a positive

compound Poisson random measure Remark

  • The long memory property has no influence on the extremal

behavior

Vicky Fasen – p. 21/22

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SLIDE 30

References

Fasen, V. (2005) Extremes of regularly varying Lévy driven mixed moving average processes, to appear in J. Appl. Probab. Fasen, V. (2005) Extremes of subexponential Lévy driven moving average processes, submitted for publication. http://www-m4.ma.tum.de/pers/fasen/

Vicky Fasen – p. 22/22