On maximal inequalities for stable stochastic integrals
Ald´eric Joulin
Universit´e de La Rochelle (France)
Workshop
“Stochastic and harmonic analysis of processes with jumps”
2-9 May 2006 - Angers
Content
1 Motivations
2 Pruitt’s truncation method
3 Large range estimates
4 Small range estimates
5 Application to first crossing problems
Motivations
Z α-stable process, H predictable integrable.
Our aim: to understand the behavior of H · Z as α is “close to 2”, i.e. to give upper bounds on:
- Large range: P sup
t∈[0,1]
Z t 0
HsdZs
≥ x
!
, x large.
- Small range: P sup
t∈[0,1]
Z t 0
HsdZs ≥ x
!
, x small.
Main difficulties:
- Absence of close formulae for stable densities.
- Infinite variance ⇒ classical maximal inequalities fail.
Motivations
Pruitt ’81. Regularity of paths of L´evy processes. In the SαS case:
P sup
t∈[0,1]
|Zt| ≥ x
!
≤ D1
α(2 − α)xα, xα> D1 α(2 − α). Optimal in x since behavior similar to ν ({|x |, ∞}).
Linear explosion as α → 2.
Proof: Truncation of the jumps + Doob’s maximal inequalities.
Motivations
Gin´e-Marcus ’83. To derive a CLT for stable stochastic integrals. Generalization of Pruitt’s result: for any
xα > D2kHkαα α(2 − α)2,
P sup
t∈[0,1]
Z t 0
HsdZs
≥ x
!
≤ D2
α(2 − α)2xα Z 1
0
E|Ht|αdt.
Optimal in x .
H ∈ Lα(Ω × [0, 1]) is sufficient.
Explosion of quadratic order as α → 2.
Motivations
Hult-Lindskog ’06. Extremal behavior of L´evy-type stochastic integrals:
P sup
t∈[0,1]
Z t
0
HsdZs
≥ x
!
∼x →∞ Dα
αxα Z 1
0
E|Ht|αdt.
Uniform integrability assumption E supt∈[0,1]|Ht|α+p < ∞.
Dα bounded in α ⇒ No explosion phenomenon !
⇒ loss of information from asymptotic to non-asymptotic estimates.
Motivations
Natural question: is it possible to avoid the explosion of the upper bound as α → 2 and to involve at the same time optimal bounds in terms of the deviation level x and the Lα-norm of H ? I do not know.
Our purposes: to conserve the optimal rate x−α and:
- to weaken the speed of explosion in Gin´e-Marcus’ estimate, with the same optimal Lα-norm.
- to avoid the explosion as α is close to 2, at the price of stronger integrability assumptions on H.
Pruitt’s truncation method
Z α-stable with characteristics (b, 0, ν), where ν stable L´evy measure:
ν(dy ) = c−1{y <0}+ c+1{y >0} dy
|y |α+1. L´evy-Itˆo decomposition with truncation level R:
Zt = bRt + Z t
0
Z
|y |≤R
y ˜µ(dy , dt) + Z t
0
Z
|y |>R
y µ(dy , dt)
= drift + L2-martingale Zt(R−) + compound Poisson Zt(R+).
Pruitt’s truncation method
Construction of stable stochastic integrals:
H ∈ L2(Ω × [0, 1]).
Xt := A(R)t + Xt(R−)+ Xt(R+), with A(R)t := bR
Z t 0
Hsds, Xt(R−):= H·Zt(R−), Xt(R+) := H·Zt(R+).
Pruitt’s truncation method
Crucial point: the truncation level R is chosen at the end of the proofs, depending on:
the deviation level x . a suitable Lp-norm kHkp.
Large range estimates (1)
Proposition
Underlying driving Z SαS. Then
P sup
t∈[0,1]
|Xt| ≥ x
!
≤ D
(2 − α)xα Z 1
0
E|Ht|αdt, xα ≥ DkHkαα 2 − α .
Large range estimates (1)
Remark
Optimal in the deviation level x and the Lα-norm of H.
Linear explosion (instead of quadratic) as α → 2:
⇒ generalization of Gin´e-Marcus’ estimate.
Proof: adaptation to stable stochastic integrals of
Bass-Levin-Vondracek’s method + choice of truncation level R = x .
Large range estimates (2)
For non-explosion as α is close to 2, we need the tricky inequality:
P sup
t∈[0,1]
|Xt| ≥ x
!
≤ P sup
t∈[0,1]
|A(R)t | ≥ x/2
! (1)
+P sup
t∈[0,1]
|Xt(R−)| ≥ x/2
! (2)
+P sup
t∈[0,1]
|Xt(R+)| > 0
!
≤ (1) + (2) + K αRα.
⇒ Reduced to bound suitably (2), avoidingR
|y |≤Ry2ν(dy )
Large range estimates (2)
Theorem
H ∈ Lα+p(Ω × [0, 1]), p ∼ 2 − α. Then for xα ≥ K kHkαα+p
(2 − α)β , β := βα+p > 2 :
P sup
t∈[0,1]
|Xt| ≥ x
!
≤ M xα
Z 1 0
E|Ht|α+pdt
α/(α+p)
.
Large range estimates (2)
Remark
Optimal in x and no longer explosion as α → 2.
Price to pay compared to Gin´e-Marcus’ estimate:
- H ∈ Lα+p and not only in Lα.
- Restriction on the range of validity of x (β > 2).
Proof: moment estimates + choice of truncation level R = x /kHkα+p.
Small range estimates
Theorem
Underlying driving Z SαS, H bounded. Then for any > 0 and any x ∈ (0, xα,),
P sup
t∈[0,1]
Xt ≥ x
!
≤ (1 + ) exp −Kα
x
kHk∞,α
α/(α−1)! .
Small range estimates
Remark
Different behaviors as x is small or large. What about intermediate range ?
As α → 2, recover the Gaussian case ?
Small range estimates
Corollary
Yes: choosing a suitable weight in the stable L´evy measure and taking limit as α → 2 yields
P sup
t∈[0,1]
Bt≥ x
!
≤ exp −x2/2 , x > 0.
Application to first crossing problems
Z SαS. Stable (recurrent) O.U. process of parameter λ > 0:
Xt(λ):=
Z t 0
e−λ (t−s)dZs, t ≥ 0, X0(λ )= 0.
First passage times: if x > 0, define
Tx(λ ):= inf{t ≥ 0 : |Xt(λ)| ≥ x}, Tcurv := inf{t ≥ 0 : |Zt| ≥ x(1 + λαt)1/α}.
By Alili-Patie’s transform: Tx(λ )
(d )= λ α1 log (1 + λαTcurv).
Maximal inequalities for X(λ ) ⇒ Estimates on Tx(λ )
⇒ Estimates on Tcurv.
Application to first crossing problems
Theorem
Estimates on first crossing times:
P (Tcurv > r ) ≤ exp
− K1
λxα log (1 + λαr )
, r > 0, x > 0,
P (Tcurv≤ r ) ≤ K2log (1 + λαr )
λxα , 0 < r < r0(α, x , λ).
L. Alili and P. Patie.
On the first crossing times of a Brownian motion and a family of continuous curves.
C. R. Math. Acad. Sci. Paris, 340(3):225–228, 2005.
E. Gin´e and M.B. Marcus.
The central limit theorem for stochastic integrals with respect to L´evy processes.
Ann. Probab., 11(1):58–77, 1983.
H. Hult and F. Lindskog.
Extremal behavior of stochastic integrals driven by regularly varying L´evy processes.
To appear in Ann. Probab., 2006.
W.E. Pruitt.
The growth of random walks and L´evy processes.
Ann. Probab., 9(6):948–956, 1981.
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