Heat kernels of unimodal Levy processes with weak scaling conditions
Heat kernels of unimodal Levy processes with weakscaling conditions
Michał Ryznar
Wrocław University of Science and Technology, Poland
The 3rd Conference on Nonlocal Operators and Partial DifferentialEquations
Będlewo, June 27, 2016.
The presentation is based mostly on a joint project with K. Bogdan, T.Grzywny.
Heat kernels of unimodal Levy processes with weak scaling conditions
Definitions
A (Borel) measure on Rd is called isotropic unimodal, if on Rd \ {0} it isabsolutely continuous with respect to the Lebesgue measure, and has afinite radial nonincreasing density function.
Heat kernels of unimodal Levy processes with weak scaling conditions
Definitions
A (Borel) measure on Rd is called isotropic unimodal, if on Rd \ {0} it isabsolutely continuous with respect to the Lebesgue measure, and has afinite radial nonincreasing density function.
A Levy process X = (Xt, t > 0) is a stochastic process with values in Rd,
which has stationary and idependent increments and cad-lag paths:
Xt1 −Xt0 , . . . , Xtn −Xtn−1 are independent for any 0 6 t0 6 . . . 6 tn.
Xt+h −Xt has the same distribution as Xh, t, h > 0
Heat kernels of unimodal Levy processes with weak scaling conditions
Definitions
A (Borel) measure on Rd is called isotropic unimodal, if on Rd \ {0} it isabsolutely continuous with respect to the Lebesgue measure, and has afinite radial nonincreasing density function.
A Levy process X = (Xt, t > 0) is a stochastic process with values in Rd,
which has stationary and idependent increments and cad-lag paths:
Xt1 −Xt0 , . . . , Xtn −Xtn−1 are independent for any 0 6 t0 6 . . . 6 tn.
Xt+h −Xt has the same distribution as Xh, t, h > 0
X = (Xt, t > 0) is called unimodal isotropic if all its one-dimensionaldistributions pt(dx) are isotropic unimodal.
Heat kernels of unimodal Levy processes with weak scaling conditions
Definitions
A (Borel) measure on Rd is called isotropic unimodal, if on Rd \ {0} it isabsolutely continuous with respect to the Lebesgue measure, and has afinite radial nonincreasing density function.
A Levy process X = (Xt, t > 0) is a stochastic process with values in Rd,
which has stationary and idependent increments and cad-lag paths:
Xt1 −Xt0 , . . . , Xtn −Xtn−1 are independent for any 0 6 t0 6 . . . 6 tn.
Xt+h −Xt has the same distribution as Xh, t, h > 0
X = (Xt, t > 0) is called unimodal isotropic if all its one-dimensionaldistributions pt(dx) are isotropic unimodal.
We call the transition density pt(x, y) = pt(y − x) = p(t, x, y) the heatkernel.Ttf(x) = f(x+ y)pt(y)dy form a semigroup on various function spaces.
Heat kernels of unimodal Levy processes with weak scaling conditions
Characteristic function
E ei〈ξ,Xt〉 =
∫
Rd
ei〈ξ,x〉pt(dx) = e−tψ(ξ), ξ ∈ R
d.
Isotropic unimodal Levy processes are characterized by Levy-Kchintchineexponents of the form ([Watanabe 1983])
ψ(ξ) = σ2|ξ|2 +∫
Rd
(1− cos 〈ξ, x〉) ν(|x|)dx, (1)
with nonincreasing ν and σ > 0. N(dx) = ν(|x|)dx is called the Levymeasure of the process.
N(dx) = limt→0
pt(dx)
t
Heat kernels of unimodal Levy processes with weak scaling conditions
Characteristic function
E ei〈ξ,Xt〉 =
∫
Rd
ei〈ξ,x〉pt(dx) = e−tψ(ξ), ξ ∈ R
d.
Isotropic unimodal Levy processes are characterized by Levy-Kchintchineexponents of the form ([Watanabe 1983])
ψ(ξ) = σ2|ξ|2 +∫
Rd
(1− cos 〈ξ, x〉) ν(|x|)dx, (1)
with nonincreasing ν and σ > 0. N(dx) = ν(|x|)dx is called the Levymeasure of the process.
N(dx) = limt→0
pt(dx)
t
If e−tψ(ξ) ∈ L1 then
pt(ξ) =1
(2π)d
∫
Rd
e−i〈ξ,x〉e−tψ(x)dx 6 pt(0).
Heat kernels of unimodal Levy processes with weak scaling conditions
Examples
Isotropic stable processes: ν(x) = c|x|−d−α
Truncated α-stable processes: ν(r) = c r−d−α1(0,1)(r).
Heat kernels of unimodal Levy processes with weak scaling conditions
Examples
Isotropic stable processes: ν(x) = c|x|−d−α
Truncated α-stable processes: ν(r) = c r−d−α1(0,1)(r).
Subordinate Brownian motions:Let Tt be a subordinator (positive and increasing one-dimensional Levyprocess) without drift; Ee−λTt = e−tϕ(λ), where (Bernstein function)
ϕ(λ) =
∫ ∞
0
(1− e−λs)µ(ds).
Let B(t) be an independent Brownian motion with ψ(ξ) = |ξ|2. ThenB(Tt) has an absolutely continuous Levy measure N(dx) = ν(x)dx, where
ν(x) =
∫ ∞
0
gs(x)µ(ds),
and gs(x) = (4π s)−d/2e−
|x|2
4s is the Gaussian kernel.
Heat kernels of unimodal Levy processes with weak scaling conditions
Generators
Af(x) = σ2∆+ p.v.∫
Rd
(f(x+ y)− f(x)) ν(|x|)dx, f ∈ C2(Rd)
Heat kernels of unimodal Levy processes with weak scaling conditions
Generators
Af(x) = σ2∆+ p.v.∫
Rd
(f(x+ y)− f(x)) ν(|x|)dx, f ∈ C2(Rd)
Fractional Laplacian: α-stable isoperimetric process
∆α/2f(x) = p.v. cd,α
∫
Rd
(f(x+ y)− f(x)) 1
|x|d+α dx
Heat kernels of unimodal Levy processes with weak scaling conditions
Generators
Af(x) = σ2∆+ p.v.∫
Rd
(f(x+ y)− f(x)) ν(|x|)dx, f ∈ C2(Rd)
Fractional Laplacian: α-stable isoperimetric process
∆α/2f(x) = p.v. cd,α
∫
Rd
(f(x+ y)− f(x)) 1
|x|d+α dx
A = I − (I −∆)α/2: relativistic α-stable isoperimetric process
Af(x) = p.v. cd,α
∫
Rd
(f(x+ y)− f(x)) K(d+α)/2(|x|)|x|(d+α)/2 dx
Heat kernels of unimodal Levy processes with weak scaling conditions
Topics
Heat kernels estimates and weak scaling.
Heat kernels of unimodal Levy processes with weak scaling conditions
Topics
Heat kernels estimates and weak scaling.
Exit times. Estimates of the mean exit time and surviaval probability forsmooth sets.
Heat kernels of unimodal Levy processes with weak scaling conditions
Topics
Heat kernels estimates and weak scaling.
Exit times. Estimates of the mean exit time and surviaval probability forsmooth sets.
Heat kernels for the killed process on exiting a set. Estimates.
Heat kernels of unimodal Levy processes with weak scaling conditions
Our goal:Estimates for pt(x) in terms of the symbol ψ of the process (or ψ
∗)
Heat kernels of unimodal Levy processes with weak scaling conditions
Our goal:Estimates for pt(x) in terms of the symbol ψ of the process (or ψ
∗)
Example: Cauchy, isotropic 1-stable process, ψ(x) = |x|.
pt(x) = Cdt
(t2 + |x|2)(d+1)/2 for x ∈ Rd.
Heat kernels of unimodal Levy processes with weak scaling conditions
Our goal:Estimates for pt(x) in terms of the symbol ψ of the process (or ψ
∗)
Example: Cauchy, isotropic 1-stable process, ψ(x) = |x|.
pt(x) = Cdt
(t2 + |x|2)(d+1)/2 for x ∈ Rd.
Below f ≈ g means that there is a constant c > 0 such thatc−1g 6 f(x) 6 cg(x). This c is called the comparability constant.
Heat kernels of unimodal Levy processes with weak scaling conditions
Our goal:Estimates for pt(x) in terms of the symbol ψ of the process (or ψ
∗)
Example: Cauchy, isotropic 1-stable process, ψ(x) = |x|.
pt(x) = Cdt
(t2 + |x|2)(d+1)/2 for x ∈ Rd.
Below f ≈ g means that there is a constant c > 0 such thatc−1g 6 f(x) 6 cg(x). This c is called the comparability constant.
Example: isotropic α-stable process, ψ(x) = |x|α, 0 < α < 2.
pt(x) ≈ min{t−d/α,t
|x|d+α } for x ∈ Rd.
Heat kernels of unimodal Levy processes with weak scaling conditions
Our goal:Estimates for pt(x) in terms of the symbol ψ of the process (or ψ
∗)
Example: Cauchy, isotropic 1-stable process, ψ(x) = |x|.
pt(x) = Cdt
(t2 + |x|2)(d+1)/2 for x ∈ Rd.
Below f ≈ g means that there is a constant c > 0 such thatc−1g 6 f(x) 6 cg(x). This c is called the comparability constant.
Example: isotropic α-stable process, ψ(x) = |x|α, 0 < α < 2.
pt(x) ≈ min{t−d/α,t
|x|d+α } for x ∈ Rd.
t−d/α =(
ψ−1(1/t))d,
t
|x|d+α =tψ(1/|x|)|x|d = ctν(x)
Heat kernels of unimodal Levy processes with weak scaling conditions
Our goal:Estimates for pt(x) in terms of the symbol ψ of the process (or ψ
∗)
Example: Cauchy, isotropic 1-stable process, ψ(x) = |x|.
pt(x) = Cdt
(t2 + |x|2)(d+1)/2 for x ∈ Rd.
Below f ≈ g means that there is a constant c > 0 such thatc−1g 6 f(x) 6 cg(x). This c is called the comparability constant.
Example: isotropic α-stable process, ψ(x) = |x|α, 0 < α < 2.
pt(x) ≈ min{t−d/α,t
|x|d+α } for x ∈ Rd.
t−d/α =(
ψ−1(1/t))d,
t
|x|d+α =tψ(1/|x|)|x|d = ctν(x)
pt(x) ≈ min{
[
ψ−1(1/t)]d,tψ(1/|x|)|x|d
}
Heat kernels of unimodal Levy processes with weak scaling conditions
Recall pt(x) is radially decreasing. Easy observation:
pt(2r)(|B2r| − |Br|) 6 P(r 6 |Xt| 6 2r) 6 pt(r)(|B2r| − |Br|)
Heat kernels of unimodal Levy processes with weak scaling conditions
Recall pt(x) is radially decreasing. Easy observation:
pt(2r)(|B2r| − |Br|) 6 P(r 6 |Xt| 6 2r) 6 pt(r)(|B2r| − |Br|)
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r)
Heat kernels of unimodal Levy processes with weak scaling conditions
Recall pt(x) is radially decreasing. Easy observation:
pt(2r)(|B2r| − |Br|) 6 P(r 6 |Xt| 6 2r) 6 pt(r)(|B2r| − |Br|)
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r)
pt(r) > c(d, κ)r−dP(r 6 |Xt| 6 κr), κ > 1
Heat kernels of unimodal Levy processes with weak scaling conditions
Recall pt(x) is radially decreasing. Easy observation:
pt(2r)(|B2r| − |Br|) 6 P(r 6 |Xt| 6 2r) 6 pt(r)(|B2r| − |Br|)
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r)
pt(r) > c(d, κ)r−dP(r 6 |Xt| 6 κr), κ > 1
There are many results about heat kernel estimates-usually assumptions are interms of Levy measures (Chen, Kaleta, Kumagai, Kim, Knopova, Mimica,Schilling, Song, Sztonyk and many others).
Heat kernels of unimodal Levy processes with weak scaling conditions
Recall pt(x) is radially decreasing. Easy observation:
pt(2r)(|B2r| − |Br|) 6 P(r 6 |Xt| 6 2r) 6 pt(r)(|B2r| − |Br|)
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r)
pt(r) > c(d, κ)r−dP(r 6 |Xt| 6 κr), κ > 1
There are many results about heat kernel estimates-usually assumptions are interms of Levy measures (Chen, Kaleta, Kumagai, Kim, Knopova, Mimica,Schilling, Song, Sztonyk and many others).
In our approach we derive estimates using the symbol ψ (ψ∗ ) and theassumptions will be formulated in terms of ψ.Let ψ∗(u) := sup|x|6u ψ(x), for u > 0.
Proposition
ψ(x) 6 ψ∗(|x|) 6 π2 ψ(x) for x ∈ Rd. (2)
Heat kernels of unimodal Levy processes with weak scaling conditions
Proposition
For r > 0 we have
P(|Xt| > r) 62e
e− 1(2d+ 1)(
1− e−tψ∗(1/r))
.
Heat kernels of unimodal Levy processes with weak scaling conditions
Proposition
For r > 0 we have
P(|Xt| > r) 62e
e− 1(2d+ 1)(
1− e−tψ∗(1/r))
.
Recall
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r) 6 Cdtψ∗(2/r)r−d 6 10Cdtψ
∗(1/r)r−d
Heat kernels of unimodal Levy processes with weak scaling conditions
Proposition
For r > 0 we have
P(|Xt| > r) 62e
e− 1(2d+ 1)(
1− e−tψ∗(1/r))
.
Recall
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r) 6 Cdtψ∗(2/r)r−d 6 10Cdtψ
∗(1/r)r−d
Corollary
There is C = C(d) such that
pt(x) 6 Ctψ∗(1/|x|)/|x|d for x ∈ Rd \ {0}.
Heat kernels of unimodal Levy processes with weak scaling conditions
Proposition
For r > 0 we have
P(|Xt| > r) 62e
e− 1(2d+ 1)(
1− e−tψ∗(1/r))
.
Recall
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r) 6 Cdtψ∗(2/r)r−d 6 10Cdtψ
∗(1/r)r−d
Corollary
There is C = C(d) such that
pt(x) 6 Ctψ∗(1/|x|)/|x|d for x ∈ Rd \ {0}.
Example: isotropic α-stable process, ψ(x) = |x|α, 0 < α < 2.
pt(x) 6 Ct/|x|d+α for x ∈ Rd \ {0}.
Heat kernels of unimodal Levy processes with weak scaling conditions
The method of proof of the estimates of P(|Xt| > r).
For reasons which shall become clear in the proof of the next result, we choosethe following parametrization of the tails:
ft(ρ) = P(|Xt| >√ρ) = P(|Xt|2 > ρ), ρ > 0, t > 0. (3)
Consider the Laplace transform of ft:
Lft(λ) =∫ ∞
0
e−λρft(ρ)dρ, λ > 0.
Heat kernels of unimodal Levy processes with weak scaling conditions
The method of proof of the estimates of P(|Xt| > r).
For reasons which shall become clear in the proof of the next result, we choosethe following parametrization of the tails:
ft(ρ) = P(|Xt| >√ρ) = P(|Xt|2 > ρ), ρ > 0, t > 0. (3)
Consider the Laplace transform of ft:
Lft(λ) =∫ ∞
0
e−λρft(ρ)dρ, λ > 0.
Lemma
There is a constant C1 = C1(d) such that
C−111
λ
(
1− e−tψ∗(√λ))
6 Lft(λ) 6 C11
λ
(
1− e−tψ∗(√λ))
, λ > 0.
Heat kernels of unimodal Levy processes with weak scaling conditions
Proof.
By Fubini’s theorem, for integrable functions h, k:∫
Rd
h(x)k(x)dx =
∫
Rd
h(x)k(x)dx
Heat kernels of unimodal Levy processes with weak scaling conditions
Proof.
By Fubini’s theorem, for integrable functions h, k:∫
Rd
h(x)k(x)dx =
∫
Rd
h(x)k(x)dx
Ee−λ|Xt|2
=
∫
Rd
e−λ|x|2
pt(x)dx = (4π)−d/2∫
Rd
e−tψ(x√λ)e−|x|
2/4dx.
Heat kernels of unimodal Levy processes with weak scaling conditions
Proof.
By Fubini’s theorem, for integrable functions h, k:∫
Rd
h(x)k(x)dx =
∫
Rd
h(x)k(x)dx
Ee−λ|Xt|2
=
∫
Rd
e−λ|x|2
pt(x)dx = (4π)−d/2∫
Rd
e−tψ(x√λ)e−|x|
2/4dx.
λLft(λ) = E(1− e−λ|Xt|2
)
= 1−∫
Rd
e−λ|x|2
pt(x)dx = (4π)−d/2∫
Rd
(
1− e−tψ(x√λ))
e−|x|2/4dx.
Heat kernels of unimodal Levy processes with weak scaling conditions
By the result of Hoh, 1998’,
ψ(su) 6 ψ∗(su) 6 2(s2 + 1)ψ∗(u), s, u > 0. (4)
Heat kernels of unimodal Levy processes with weak scaling conditions
By the result of Hoh, 1998’,
ψ(su) 6 ψ∗(su) 6 2(s2 + 1)ψ∗(u), s, u > 0. (4)
Note that1− e−bt 6 b(1− e−t), t > 0, b > 1, (5)
Heat kernels of unimodal Levy processes with weak scaling conditions
By the result of Hoh, 1998’,
ψ(su) 6 ψ∗(su) 6 2(s2 + 1)ψ∗(u), s, u > 0. (4)
Note that1− e−bt 6 b(1− e−t), t > 0, b > 1, (5)
1− e−tψ(x√λ)
6 1− e−2t(|x|2+1)ψ∗(
√λ)
6 2(|x|2 + 1)(
1− e−tψ∗(√λ))
λLft(λ) = (4π)−d/2∫
Rd
(
1− e−tψ(x√λ))
e−|x|2/4dx
6
(
1− e−tψ∗(√λ))
∫
Rd
2(|x|2 + 1)(4π)−d/2e−|x|2/4dx
Heat kernels of unimodal Levy processes with weak scaling conditions
On the other hand, if |x| > 1, then
ψ(
x√λ)
> ψ∗(
|x|√λ)
/π2 > ψ∗(√
λ)
/π2
by (2). Thus,
λLft(λ) = (4π)−d/2∫
Rd
(
1− e−tψ(x√λ))
e−|x|2/4dx
> (4π)−d/2∫
Bc1
e−|x|2/4dx
(
1− e−tψ∗(√λ)/π2)
>
(
1− e−tψ∗(√λ))
π−2(4π)−d/2∫
Bc1
e−|x|2/4dx,
where we use (5).
Heat kernels of unimodal Levy processes with weak scaling conditions
Upper bound for ft(r) = P(|Xt| >√r) ??
Heat kernels of unimodal Levy processes with weak scaling conditions
Upper bound for ft(r) = P(|Xt| >√r) ??
The upper bound for Lft(λ) immediately provides the upper bound for ft(r)since ft(r) is decreasing.
Heat kernels of unimodal Levy processes with weak scaling conditions
Upper bound for ft(r) = P(|Xt| >√r) ??
The upper bound for Lft(λ) immediately provides the upper bound for ft(r)since ft(r) is decreasing.
ft(1/λ)(1− e−1) 6 λ
∫ 1/λ
0
e−λrft(r)dr 6 λLft(λ) 6 Cd
(
1− e−tψ∗(√λ))
Heat kernels of unimodal Levy processes with weak scaling conditions
Upper bound for ft(r) = P(|Xt| >√r) ??
The upper bound for Lft(λ) immediately provides the upper bound for ft(r)since ft(r) is decreasing.
ft(1/λ)(1− e−1) 6 λ
∫ 1/λ
0
e−λrft(r)dr 6 λLft(λ) 6 Cd
(
1− e−tψ∗(√λ))
Lower bound??
Heat kernels of unimodal Levy processes with weak scaling conditions
Upper bound for ft(r) = P(|Xt| >√r) ??
The upper bound for Lft(λ) immediately provides the upper bound for ft(r)since ft(r) is decreasing.
ft(1/λ)(1− e−1) 6 λ
∫ 1/λ
0
e−λrft(r)dr 6 λLft(λ) 6 Cd
(
1− e−tψ∗(√λ))
Lower bound??
The lower bound for Lft(λ) + some type of weak scaling condition for thesymbol (WUSC) give the lower bound for ft(r). This argument is still simpleyet requires more effort than the upper bound.
Heat kernels of unimodal Levy processes with weak scaling conditions
Upper bound for ft(r) = P(|Xt| >√r) ??
The upper bound for Lft(λ) immediately provides the upper bound for ft(r)since ft(r) is decreasing.
ft(1/λ)(1− e−1) 6 λ
∫ 1/λ
0
e−λrft(r)dr 6 λLft(λ) 6 Cd
(
1− e−tψ∗(√λ))
Lower bound??
The lower bound for Lft(λ) + some type of weak scaling condition for thesymbol (WUSC) give the lower bound for ft(r). This argument is still simpleyet requires more effort than the upper bound.
WUSC implies some type of scaling property for Lft(λ).
Heat kernels of unimodal Levy processes with weak scaling conditions
Improvement of the general upper bound
Let
K(r) =1
r2
∫
|x|<r|x|2ν(dx) r > 0.
Proposition
For r > 0 we haveP(r/2 6 |Xt| 6 r) 6 CdtK(r).
pt(r) 6 C(d)r−dP(r/2 6 |Xt| 6 r) 6 CdtK(r)
rd
We always haveK(r) 6 cdψ
∗(1/r)
Example: ψ(x) = log(1 + |x|2). Then ν(x) ≈ 1|x|d , |x| < 1.
Hence K(r) ≈ 1, r < 1 while limr→0 ψ∗(1/r) =∞
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Scaling conditions
Let φ : [0,∞)→ [0,∞).
φ ∈WLSC(α, θ, c) if α > 0, θ > 0 and c ∈ (0, 1] exist, such that
φ(λθ) > cλαφ(θ) for λ > 1, θ > θ,
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Scaling conditions
Let φ : [0,∞)→ [0,∞).
φ ∈WLSC(α, θ, c) if α > 0, θ > 0 and c ∈ (0, 1] exist, such that
φ(λθ) > cλαφ(θ) for λ > 1, θ > θ,
equivalently
infy>x>θ
φ(y)
φ(x)
(
x
y
)α
> 0,
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Scaling conditions
Let φ : [0,∞)→ [0,∞).
φ ∈WLSC(α, θ, c) if α > 0, θ > 0 and c ∈ (0, 1] exist, such that
φ(λθ) > cλαφ(θ) for λ > 1, θ > θ,
equivalently
infy>x>θ
φ(y)
φ(x)
(
x
y
)α
> 0,
equivalently
φ(x)x−α
is comparable to a non-decreasing function on [θ,∞).
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Scaling conditions
Let φ : [0,∞)→ [0,∞).
φ ∈WLSC(α, θ, c) if α > 0, θ > 0 and c ∈ (0, 1] exist, such that
φ(λθ) > cλαφ(θ) for λ > 1, θ > θ,
equivalently
infy>x>θ
φ(y)
φ(x)
(
x
y
)α
> 0,
equivalently
φ(x)x−α
is comparable to a non-decreasing function on [θ,∞).The scaling condition WLSC is global if we can set θ = 0
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
φ ∈WUSC(α, θ, C) if α < 2, θ > 0 and C > 1 exist, such that
φ(λθ) 6 Cλαφ(θ) for λ > 1, θ > θ,
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
φ ∈WUSC(α, θ, C) if α < 2, θ > 0 and C > 1 exist, such that
φ(λθ) 6 Cλαφ(θ) for λ > 1, θ > θ,
equivalently
supy>x>θ
φ(y)
φ(x)
(
x
y
)α
<∞,
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
φ ∈WUSC(α, θ, C) if α < 2, θ > 0 and C > 1 exist, such that
φ(λθ) 6 Cλαφ(θ) for λ > 1, θ > θ,
equivalently
supy>x>θ
φ(y)
φ(x)
(
x
y
)α
<∞,
equivalently
φ(x)x−α
is comparable to a non-decreasing function on [θ,∞).
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
φ ∈WUSC(α, θ, C) if α < 2, θ > 0 and C > 1 exist, such that
φ(λθ) 6 Cλαφ(θ) for λ > 1, θ > θ,
equivalently
supy>x>θ
φ(y)
φ(x)
(
x
y
)α
<∞,
equivalently
φ(x)x−α
is comparable to a non-decreasing function on [θ,∞).The scaling condition WUSC is global if we can set θ = 0
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Examples:ψ(θ) = θα + θβ , 0 < α < β < 2 has global WLSC(α), WUSC(β):
ψ(θ)θ−α = 1 + θβ−α is increasing
This symbol corresponds to the sum of two independent isotropic stableprocesse with indices α, β, respectively
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Examples:ψ(θ) = θα + θβ , 0 < α < β < 2 has global WLSC(α), WUSC(β):
ψ(θ)θ−α = 1 + θβ−α is increasing
This symbol corresponds to the sum of two independent isotropic stableprocesse with indices α, β, respectively
ψ(θ) = (θ2 + 1)α/2 − 1, 0 < α < 2 has global WLSC(α), but only localWUSC(α).
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Examples:ψ(θ) = θα + θβ , 0 < α < β < 2 has global WLSC(α), WUSC(β):
ψ(θ)θ−α = 1 + θβ−α is increasing
This symbol corresponds to the sum of two independent isotropic stableprocesse with indices α, β, respectively
ψ(θ) = (θ2 + 1)α/2 − 1, 0 < α < 2 has global WLSC(α), but only localWUSC(α).
ψ(θ)θ−α = (θ−2 + 1)α/2 − θ−α is increasing
and
ψ(θ)θ−α ≈ 1, θ > 1
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Lemma
C = C(d) exists such that if ψ∈ WUSC(α, θ, C) anda = [(2− α)C]
2
2−αCα−22 , then
P(|Xt| > r) > a(
1− e−tψ∗(1/r))
, 0 < r <√a/
θ.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Lemma
C = C(d) exists such that if ψ∈ WUSC(α, θ, C) anda = [(2− α)C]
2
2−αCα−22 , then
P(|Xt| > r) > a(
1− e−tψ∗(1/r))
, 0 < r <√a/
θ.
The Lemma above follows from the following result due to Zhale 2009’
Lemma
Let g > 0 be nonincreasing, β > 0 and Lg ∈WUSC(−β, θ, C). There isb = b(β,C) ∈ (0, 1) such that
g(r) >b
2ebr−1Lg(r−1), 0 < r < b/θ.
We apply the lemma to ft(r) = P(|Xt| >√r) and then use the estimates for
Lf . First using the lower and the upper bounds for the Laplace transformtogether with WUSC(α, θ, C) condition for ψ we prove that Lf hasWUSC(α/2− 1) property.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Theorem (Bogdan, Grzywny and Ryznar, 2014’, JFA)
If ψ ∈WLSC(α, θ, c), then there is C∗ = C∗(d, α, c) such that
pt(x) 6 C∗min
{
[
ψ−(1/t)]d,tψ∗(1/|x|)|x|d
}
if tψ∗(θ) < π−2.
If ψ ∈WLSC(α, θ, c)∩WUSC(α, θ, C), then c∗ = c∗(d, α, c, α, C),r0 = r0(d, α, c, α, C) exist with
pt(x) > c∗min
{
[
ψ− (1/t)]d,tψ∗(1/|x|)|x|d
}
, tψ∗(θ/r0) < 1 and |x| <r0θ.
Here ψ−(r) = inf{s : ψ∗(s) > r} is the generalized inverse of thenondecreasing function ψ∗.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Theorem (Bogdan, Grzywny and Ryznar, 2014’, JFA)
If ψ ∈WLSC(α, θ, c), then there is C∗ = C∗(d, α, c) such that
pt(x) 6 C∗min
{
[
ψ−(1/t)]d,tψ∗(1/|x|)|x|d
}
if tψ∗(θ) < π−2.
If ψ ∈WLSC(α, θ, c)∩WUSC(α, θ, C), then c∗ = c∗(d, α, c, α, C),r0 = r0(d, α, c, α, C) exist with
pt(x) > c∗min
{
[
ψ− (1/t)]d,tψ∗(1/|x|)|x|d
}
, tψ∗(θ/r0) < 1 and |x| <r0θ.
Here ψ−(r) = inf{s : ψ∗(s) > r} is the generalized inverse of thenondecreasing function ψ∗.If WLSC holds, then (at least for small t):
pt(0) =1
(2π)d
∫
e−tψ(x)dx ≈[
ψ− (1/t)]d.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Corollary
There is C = C(d) such that
ν(x) 6 Cψ∗(1/|x|)|x|−d.
If ψ ∈WLSC(α, θ, c)∩WUSC(α, θ, C) and |x| < r0/θ, then
ν(x) > c∗ψ∗(1/|x|)|x|−d.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Corollary
There is C = C(d) such that
ν(x) 6 Cψ∗(1/|x|)|x|−d.
If ψ ∈WLSC(α, θ, c)∩WUSC(α, θ, C) and |x| < r0/θ, then
ν(x) > c∗ψ∗(1/|x|)|x|−d.
Corollary
If ψ ∈ WLSC(α,0,c)∩WUSC(α,0,C), then
pt(x) ≈ min{
[
ψ−(1/t)]d,tψ∗(1/|x|)|x|d
}
, t > 0, x ∈ Rd.
Example. Xt = X(α)t +X
(β)t , 0 < β < α < 2. X
(α)t , X
(β)t idependent
isotropic stable and ψ(ξ) = |ξ|α + |ξ|β . (Chen, Kumgai 2008’)
pt(x) ≈ min{
(1/t)d/α ∧ (1/t)d/β , t
|x|d+α +t
|x|d+β
}
, t > 0, x ∈ Rd.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Theorem (Bogdan, Grzywny and Ryznar, 2014’, JFA)
Let Xt be an isotropic unimodal Levy process in Rd with transition density p,
Levy-Khintchine exponent ψ and Levy measure density ν. The following areequivalent:
(i) WLSC and WUSC [global WLSC and WUSC ] hold for ψ.
(ii) For some r0 ∈ (0,∞) [r0 =∞] and a constant c,
pt(x) > ctψ∗(|x|−1)|x|d , 0 < |x| < r0, 0 < tψ∗(|x|−1) < 1.
(iii) For some r0 ∈ (0,∞) [r0 =∞] and a constant c,
ν(x) > cψ∗(|x|−1)|x|d , 0 < |x| < r0.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Theorem (Kulczycki and Ryznar, 2016’, TAMS)
Let X be an isotropic Levy process in Rd such that ν(r) is nonincreasing,absolutely continuous such that −ν′(r)/r is nonincreasing. Then its transitiondensity pt(x) = pt(|x|) satisfies
∣
∣
∣
d
drpt(r)∣
∣
∣6 c(d)
1 ∧ tψ∗(1/r)rd+1
, t, r > 0.
If additionally ψ satisfies WLSC(α, θ0, c), then
∣
∣
∣
d
drpt(r)
∣
∣
∣6 c(d, α)
r
c(d+2)/α+1
(
[ψ−(1/t)]d+2 ∧ tψ∗(1/r)
rd+2
)
, tψ∗(θ0) 6 1/π2.
If additionally ψ satisfies WLSC(α, θ0, c) and WUSC(α, θ0, C), then we have
∣
∣
∣
d
drpt(r)∣
∣
∣> c∗r
(
[ψ−(1/t)]d+2 ∧ tψ∗(1/r)
rd+2
)
, tψ∗(θ0/r0) 6 1, r < r0/θ0,
where c∗ = c∗(d, α, α, c, C), r0 = r0(d, α, α, c, C). Note that if the scalingconditions are global, that is θ0 = 0, then the last two estimates hold for allt, r > 0.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Let X be an isotropic Levy process in Rd such that ν(r) is nonincreasing,absolutely continuous such that −ν′(r)/r is nonincreasing.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Let X be an isotropic Levy process in Rd such that ν(r) is nonincreasing,absolutely continuous such that −ν′(r)/r is nonincreasing.
Then there exists a Levy process X(d+2)t in Rd+2 with the characteristic
exponent ψ(d+2)(ξ) = ψ(|ξ|), ξ ∈ Rd+2 and the radial, radially nonincreasing
transition density p(d+2)t (x) = p
(d+2)t (|x|) satisfying
p(d+2)t (r) =
−12πr
d
drpt(r), r > 0.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Let X be an isotropic Levy process in Rd such that ν(r) is nonincreasing,absolutely continuous such that −ν′(r)/r is nonincreasing.
Then there exists a Levy process X(d+2)t in Rd+2 with the characteristic
exponent ψ(d+2)(ξ) = ψ(|ξ|), ξ ∈ Rd+2 and the radial, radially nonincreasing
transition density p(d+2)t (x) = p
(d+2)t (|x|) satisfying
p(d+2)t (r) =
−12πr
d
drpt(r), r > 0.
The estimates of the gradient of pt enabled analysis of gradients of harmonicfunctions with respect to the process X. In a joint paper with T. Kulczycki(2015’) we showed that the gradient of a positive harmonic function exists andwe derived its estimates from above.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Symbols which do not have weak scaling properties
Slowly varying: e.g.
ψ(x) = log(1 + |x|α)β , 0 < α 6 2, 0 < β 6 1
Various asymptotics and estimates were recently obtained by T. Grzywny,B. Trojan and M.R (2016) under some additional assumptions on thesymbol or its derivative. One of the main difficulties here is the fact thatvery often p(t, 0) =∞.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Symbols which do not have weak scaling properties
Slowly varying: e.g.
ψ(x) = log(1 + |x|α)β , 0 < α 6 2, 0 < β 6 1
Various asymptotics and estimates were recently obtained by T. Grzywny,B. Trojan and M.R (2016) under some additional assumptions on thesymbol or its derivative. One of the main difficulties here is the fact thatvery often p(t, 0) =∞.2-regularly varying: e.g.
ψ(x) =|x|2
log(1 + |x|α) , 0 < α 6 2
This case seems to be even more difficult than the one above. There areworks by A. Mimica (2015), A. Mimica ad P. Kim (2016) where somecases were treated.
Heat kernels of unimodal Levy processes with weak scaling conditions
Consequence of scaling
Symbols which do not have weak scaling properties
Slowly varying: e.g.
ψ(x) = log(1 + |x|α)β , 0 < α 6 2, 0 < β 6 1
Various asymptotics and estimates were recently obtained by T. Grzywny,B. Trojan and M.R (2016) under some additional assumptions on thesymbol or its derivative. One of the main difficulties here is the fact thatvery often p(t, 0) =∞.2-regularly varying: e.g.
ψ(x) =|x|2
log(1 + |x|α) , 0 < α 6 2
This case seems to be even more difficult than the one above. There areworks by A. Mimica (2015), A. Mimica ad P. Kim (2016) where somecases were treated.
Both cases are far from being explored to that extent as regularly varyingsymbols with indices strictly between 0 and 2.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Survival probability. Dirichlet heat kernel.
The first exit time from open D ⊂ Rd:
τD = inf{t > 0 : Xt /∈ D}
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Survival probability. Dirichlet heat kernel.
The first exit time from open D ⊂ Rd:
τD = inf{t > 0 : Xt /∈ D}
Transition density of the process killed on leaving D (Dirichlet heat kernel):
pD(t, x, y) = p(t, x, y)− Ex[τD < t; p(t− τD, XτD , y)],
where p(t, x, y) = pt(y − x).
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Survival probability. Dirichlet heat kernel.
The first exit time from open D ⊂ Rd:
τD = inf{t > 0 : Xt /∈ D}
Transition density of the process killed on leaving D (Dirichlet heat kernel):
pD(t, x, y) = p(t, x, y)− Ex[τD < t; p(t− τD, XτD , y)],
where p(t, x, y) = pt(y − x).
We have Px(Xt ∈ B, τD > t) =∫
BpD(t, x, y)dy.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Survival probability. Dirichlet heat kernel.
The first exit time from open D ⊂ Rd:
τD = inf{t > 0 : Xt /∈ D}
Transition density of the process killed on leaving D (Dirichlet heat kernel):
pD(t, x, y) = p(t, x, y)− Ex[τD < t; p(t− τD, XτD , y)],
where p(t, x, y) = pt(y − x).
We have Px(Xt ∈ B, τD > t) =∫
BpD(t, x, y)dy.
In particular, pD yields the probability of surviving time t:
Px(τD > t) =
∫
pD(t, x, y)dy.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Survival probability. Dirichlet heat kernel.
The first exit time from open D ⊂ Rd:
τD = inf{t > 0 : Xt /∈ D}
Transition density of the process killed on leaving D (Dirichlet heat kernel):
pD(t, x, y) = p(t, x, y)− Ex[τD < t; p(t− τD, XτD , y)],
where p(t, x, y) = pt(y − x).
We have Px(Xt ∈ B, τD > t) =∫
BpD(t, x, y)dy.
In particular, pD yields the probability of surviving time t:
Px(τD > t) =
∫
pD(t, x, y)dy.
Green function: GD(x, y) =∫∞0pD(t, x, y)dt.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Known results about estimates of Dirichlet HeatKernels
Zhang (2002) - smooth domains, BM
Varopulos (2003) - Lipschitz domains, BM
Chen, Kim, Song (2010), bounded smooth domains, isotropic stableprocesses
Bogdan, Grzywny, Ryznar (2010), Lipschitz domains, isotropic stableprocesses
Chen, Kim, Song (2012-2014) - smooth domains, subclasses of SBM andLevy processes comparable with SBM
Kim, Song, Vondracek (2014) - halfspace, subclasses of SBM
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Known results about estimates of Dirichlet HeatKernels
Zhang (2002) - smooth domains, BM
Varopulos (2003) - Lipschitz domains, BM
Chen, Kim, Song (2010), bounded smooth domains, isotropic stableprocesses
Bogdan, Grzywny, Ryznar (2010), Lipschitz domains, isotropic stableprocesses
Chen, Kim, Song (2012-2014) - smooth domains, subclasses of SBM andLevy processes comparable with SBM
Kim, Song, Vondracek (2014) - halfspace, subclasses of SBM
Below f ≈ g means that there is a constant c > 0 such thatc−1g 6 f(x) 6 cg(x). This c is called the comparability constant.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Upper bound
Lemma
pD(t, x, y) 6 pt/3(0)Px(τD > t/3)Py(τD > t/3).
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Upper bound
Lemma
pD(t, x, y) 6 pt/3(0)Px(τD > t/3)Py(τD > t/3).
Proof. By the semigroup property
pD(t, x, y) =
∫ ∫
pD(t/3, x, z)pD(t/3, z, w)pD(t/3, w, y)dzdw
6 pt/3(0)
∫
pD(t/3, x, z)dz
∫
pD(t/3, w, y)dw.
6 pt/3(0)Px(τD > t/3)Px(τD > t/3).
Under some conditions (eg. WLSC) for small t and x close to y we havept/3(0) ≈ pt(x− y).Also Px(τD > t/3) ≈ P
x(τD > t), t small. The lemma is sufficient (almost) forthe sharp upper bound for points which distance is small relatively to time(V 2(|x− y|) 6 t).
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Lemma
Consider open D1, D3 ⊂ D such that dist(D1, D3) > 0. LetD2 = D \ (D1 ∪D3). If x ∈ D1, y ∈ D3 and t > 0, then
pD(t, x, y) 6 Px(XτD1 ∈ D2) sup
s<t, z∈D2p(s, z, y)
+ (t ∧ ExτD1) sup
u∈D1, z∈D3ν(|z − u|) ,
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Lemma
Consider open D1, D3 ⊂ D such that dist(D1, D3) > 0. LetD2 = D \ (D1 ∪D3). If x ∈ D1, y ∈ D3 and t > 0, then
pD(t, x, y) 6 Px(XτD1 ∈ D2) sup
s<t, z∈D2p(s, z, y)
+ (t ∧ ExτD1) sup
u∈D1, z∈D3ν(|z − u|) ,
The lemma above is used for points which are relatively far away from eachother t 6 V 2(|x− y|) and close to the boundary. Its application requires goodcontrol of the exit distribution and mean exit time. Recall that in the previouslecture we studied the estimates in the case of a ball.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Mean exit time.
Denote Br = B(0, r).We will be interested in estimating ExτBr , in particular at points which areclose to the boundary. The knowledge of the rate of decay of the mean exittime provides the rate decay of harmonic functions in a smooth domain (withrespect to the generator), which continuously vanish outside a part of thecomplement of a domain. This property is known as Boundary HarnackPrinciple. They also play important role in estimating the Dirichlet heat kernels.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Mean exit time.
Denote Br = B(0, r).We will be interested in estimating ExτBr , in particular at points which areclose to the boundary. The knowledge of the rate of decay of the mean exittime provides the rate decay of harmonic functions in a smooth domain (withrespect to the generator), which continuously vanish outside a part of thecomplement of a domain. This property is known as Boundary HarnackPrinciple. They also play important role in estimating the Dirichlet heat kernels.
In the case of a Brownian motion we know that |Bt|2 − d · t is a martingale , sostopping at τBr we have
r2 − d · ExτBr = Ex(
|BτBr |2 − d · τBr
)
= Ex|B0|2 = |x|2.
ExτBr =
1
d(r2 − |x|2), |x| 6 r.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Mean exit time.
Denote Br = B(0, r).We will be interested in estimating ExτBr , in particular at points which areclose to the boundary. The knowledge of the rate of decay of the mean exittime provides the rate decay of harmonic functions in a smooth domain (withrespect to the generator), which continuously vanish outside a part of thecomplement of a domain. This property is known as Boundary HarnackPrinciple. They also play important role in estimating the Dirichlet heat kernels.
In the case of a Brownian motion we know that |Bt|2 − d · t is a martingale , sostopping at τBr we have
r2 − d · ExτBr = Ex(
|BτBr |2 − d · τBr
)
= Ex|B0|2 = |x|2.
ExτBr =
1
d(r2 − |x|2), |x| 6 r.
In the case of ψ(ξ) = |x|α, 0 < α < 2 (isotropic α-stable ) Getoor 1990’proved that
ExτBr = Cd,α(r
2 − |x|2)α/2, |x| 6 r.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Symmetric processes
Let Xt, t > 0, - a symmetric Levy process in Rd, d ∈ N; with the characteristic
exponent
ψ(x) = 〈x,Ax〉+∫
Rd
(1− cos 〈x, z〉)N(dz), x ∈ Rd,
where A - a symmetric and non-negative definite matrix, N - a symmetric Levymeasure
(∫
Rd(1 ∧ |z|2)N(dz) <∞
)
.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Symmetric processes
Let Xt, t > 0, - a symmetric Levy process in Rd, d ∈ N; with the characteristic
exponent
ψ(x) = 〈x,Ax〉+∫
Rd
(1− cos 〈x, z〉)N(dz), x ∈ Rd,
where A - a symmetric and non-negative definite matrix, N - a symmetric Levymeasure
(∫
Rd(1 ∧ |z|2)N(dz) <∞
)
.
The classical result of Pruitt 1981’ provides a constant C = C(d)
C−1
h(r)6 E
0τB(0,r) 6C
h(r), r > 0,
where
h(r) =TrA
r2+
∫
Rd
(
1 ∧ |z|2
r2
)
N(dz).
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Symmetric processes
Let Xt, t > 0, - a symmetric Levy process in Rd, d ∈ N; with the characteristic
exponent
ψ(x) = 〈x,Ax〉+∫
Rd
(1− cos 〈x, z〉)N(dz), x ∈ Rd,
where A - a symmetric and non-negative definite matrix, N - a symmetric Levymeasure
(∫
Rd(1 ∧ |z|2)N(dz) <∞
)
.
The classical result of Pruitt 1981’ provides a constant C = C(d)
C−1
h(r)6 E
0τB(0,r) 6C
h(r), r > 0,
where
h(r) =TrA
r2+
∫
Rd
(
1 ∧ |z|2
r2
)
N(dz).
Let ψ∗(r) = sup{ψ(x) : |x| 6 r}. Then
1
8(1 + 2d)ψ∗(r−1) 6 h(r) 6 2dψ∗(r−1)
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
One-dimensional case, symmetric process
Theorem (Grzywny, Ryznar, 2012’, PMS)
There is an absolute constant C such that for every symmetric Levy process inR which is not compound Poisson,
C−1√
ψ∗( 1r−|x| )ψ
∗( 1r)6 E
xτ(−r,r) 6C
√
ψ∗( 1r−|x| )ψ
∗( 1r), |x| < r.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
One-dimensional case, symmetric process
Theorem (Grzywny, Ryznar, 2012’, PMS)
There is an absolute constant C such that for every symmetric Levy process inR which is not compound Poisson,
C−1√
ψ∗( 1r−|x| )ψ
∗( 1r)6 E
xτ(−r,r) 6C
√
ψ∗( 1r−|x| )ψ
∗( 1r), |x| < r.
The upper bound is a consequence of the formula of the Green function for ahalf-line.Let V (r) = 1√
ψ∗(1/r), r > 0. Then the above estimate can be rewritten as
Exτ(−r,r) ≈ V (r − |x|)V (r), |x| < r,
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
d-dimensional case and unimodal isoperimetric process
The upper bound for a d-dimensional ball follows immediately from theone-dimensional result since a ball can be included in a tangent strip.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
d-dimensional case and unimodal isoperimetric process
The upper bound for a d-dimensional ball follows immediately from theone-dimensional result since a ball can be included in a tangent strip.
Corollary
There is absolute constant C such that for all r > 0 and x ∈ Rd we have
ExτBr 6
C√
ψ∗( 1r−|x| )ψ
∗( 1r), |x| < r.
The lower bound is much more difficult to obtain and requires precise estimatesof the genarator of the process on suitable test functions.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
d-dimensional case and unimodal isoperimetric process
The upper bound for a d-dimensional ball follows immediately from theone-dimensional result since a ball can be included in a tangent strip.
Corollary
There is absolute constant C such that for all r > 0 and x ∈ Rd we have
ExτBr 6
C√
ψ∗( 1r−|x| )ψ
∗( 1r), |x| < r.
The lower bound is much more difficult to obtain and requires precise estimatesof the genarator of the process on suitable test functions.
Theorem (Bogdan, Grzywny, Ryznar, 2015’, PTRF)
If Condition H holds, then there is C = C(d) such that for r > 0,
C
Hr
1√
ψ∗( 1r−|x| )ψ
∗( 1r)6 E
xτBr , |x| < r.
Here Hr > 1 is increasing in r and in many situations we may show that it isbounded uniformly: H∞ <∞.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Assumption H
Each of the following situations imply H:
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Assumption H
Each of the following situations imply H:
1. X is a subordinate Brownian motion governed by a special subordinator.In this case Hr = 1.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Assumption H
Each of the following situations imply H:
1. X is a subordinate Brownian motion governed by a special subordinator.In this case Hr = 1.A function φ is a special Bernstein function if it is a Bernstein functionand λ
φ(λ)is also a Bernstein function.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Assumption H
Each of the following situations imply H:
1. X is a subordinate Brownian motion governed by a special subordinator.In this case Hr = 1.A function φ is a special Bernstein function if it is a Bernstein functionand λ
φ(λ)is also a Bernstein function.
2. σ > 0. That is the process has a non-trivial Brownian part.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Assumption H
Each of the following situations imply H:
1. X is a subordinate Brownian motion governed by a special subordinator.In this case Hr = 1.A function φ is a special Bernstein function if it is a Bernstein functionand λ
φ(λ)is also a Bernstein function.
2. σ > 0. That is the process has a non-trivial Brownian part.
3. Scale invariant Harnack inequality holds.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Assumption H
Each of the following situations imply H:
1. X is a subordinate Brownian motion governed by a special subordinator.In this case Hr = 1.A function φ is a special Bernstein function if it is a Bernstein functionand λ
φ(λ)is also a Bernstein function.
2. σ > 0. That is the process has a non-trivial Brownian part.
3. Scale invariant Harnack inequality holds.For instance: d > 3 and s−βψ(s) is almost increasing on (θ,∞) for someβ > 0.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Assumption H
Each of the following situations imply H:
1. X is a subordinate Brownian motion governed by a special subordinator.In this case Hr = 1.A function φ is a special Bernstein function if it is a Bernstein functionand λ
φ(λ)is also a Bernstein function.
2. σ > 0. That is the process has a non-trivial Brownian part.
3. Scale invariant Harnack inequality holds.For instance: d > 3 and s−βψ(s) is almost increasing on (θ,∞) for someβ > 0.d > 1 and s−βψ(s) is almost increasing and s−γψ(s) is almost decreasingon (θ,∞) for some β > 0 and γ < 2.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Uniform estimate
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Uniform estimate
If X is a subordinate Brownian motion governed by a special subordinator then
C(d)−1√
ψ∗( 1r−|x| )ψ
∗( 1r)6 E
xτBr 6C(d)
√
ψ∗( 1r−|x| )ψ
∗( 1r), |x| < r.
ψ(x) = φ(|x|2), where φ(r) and r/φ(r) are Bernstein functions.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Uniform estimate
If X is a subordinate Brownian motion governed by a special subordinator then
C(d)−1√
ψ∗( 1r−|x| )ψ
∗( 1r)6 E
xτBr 6C(d)
√
ψ∗( 1r−|x| )ψ
∗( 1r), |x| < r.
ψ(x) = φ(|x|2), where φ(r) and r/φ(r) are Bernstein functions.
(at least for d > 3)If ψ has global WLSC condition then the above two sided estimate is true (atleast for d > 3) but the constant on the left-hand side possibly dependent onthe process.For example for truncated isotropic stable processes, ν(x) = 1
|x|d+α 1{|x|<1},
ψ(x) ≈ |x|α ∧ |x|2, 0 < α < 2:
ExτBr ≈
[
(r − |x|)α/2 + (r − |x|)] [
rα/2 + r]
, |x| < r.
The same estimate for relativistic α-stable processes,ψ(x) = (|x|2 + 1)α/2 − 1, 0 < α < 2.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
D is of class C1,1 at scale r if D ⊂ Rd, D is open, non-empty, r > 0 and for
every Q ∈ ∂D there are balls B(x′, r) ⊂ D and B(x′′, r) ⊂ Dc tangent at Q.
Theorem
Let ψ ∈WLSC ∩WUSC. Open and bound D is C1,1 at scale r. Then forx ∈ R
d,
ExτD ≈
1√
ψ∗(1/δD(x))ψ∗(1/r)
The comparability constant depends on r, d, ψ and diamD.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
D is of class C1,1 at scale r if D ⊂ Rd, D is open, non-empty, r > 0 and for
every Q ∈ ∂D there are balls B(x′, r) ⊂ D and B(x′′, r) ⊂ Dc tangent at Q.
Theorem
Let ψ ∈WLSC ∩WUSC. Open and bound D is C1,1 at scale r. Then forx ∈ R
d,
ExτD ≈
1√
ψ∗(1/δD(x))ψ∗(1/r)
The comparability constant depends on r, d, ψ and diamD.
Under certain conditions (global weak scaling)
ExτD ≈
1√
ψ∗(1/δD(x))ψ∗(1/r)
with the comparability constant dependent on d, ψ and rdiamD.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Heat kernel on bounded smooth domains
Theorem (Bogdan, Grzywny, Ryznar, 2014, SPA)
Let ψ satisfy WLSC and WUSC. There is r0 = r0(d, ψ) > 0 such that for0 < r < r0 and bounded D ⊂ R
d of class C1,1 with localization radius r andν(diamD) > 0, we have for all x, y ∈ R
d, t > 0,
pD(t, x, y) ≈ Px(τD > t/2)Py(τD > t/2)p
(
t ∧ V 2(r), x, y)
and
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Heat kernel on bounded smooth domains
Theorem (Bogdan, Grzywny, Ryznar, 2014, SPA)
Let ψ satisfy WLSC and WUSC. There is r0 = r0(d, ψ) > 0 such that for0 < r < r0 and bounded D ⊂ R
d of class C1,1 with localization radius r andν(diamD) > 0, we have for all x, y ∈ R
d, t > 0,
pD(t, x, y) ≈ Px(τD > t/2)Py(τD > t/2)p
(
t ∧ V 2(r), x, y)
and
Px (τD > t) ≈ e−λ1(D)t
(
V (δD(x))√t ∧ V (r)
∧ 1)
.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Heat kernel on bounded smooth domains
Theorem (Bogdan, Grzywny, Ryznar, 2014, SPA)
Let ψ satisfy WLSC and WUSC. There is r0 = r0(d, ψ) > 0 such that for0 < r < r0 and bounded D ⊂ R
d of class C1,1 with localization radius r andν(diamD) > 0, we have for all x, y ∈ R
d, t > 0,
pD(t, x, y) ≈ Px(τD > t/2)Py(τD > t/2)p
(
t ∧ V 2(r), x, y)
and
Px (τD > t) ≈ e−λ1(D)t
(
V (δD(x))√t ∧ V (r)
∧ 1)
.
Here λ1(D) denotes the smallest eigenvalue of the compact semigroupgenerated by pD(t, x, y).
Recall that V (r) = 1√ψ∗(1/r)
, where ψ is the symbol of the process.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Heat kernel on bounded smooth domains
Theorem (Bogdan, Grzywny, Ryznar, 2014, SPA)
Let ψ satisfy WLSC and WUSC. There is r0 = r0(d, ψ) > 0 such that for0 < r < r0 and bounded D ⊂ R
d of class C1,1 with localization radius r andν(diamD) > 0, we have for all x, y ∈ R
d, t > 0,
pD(t, x, y) ≈ Px(τD > t/2)Py(τD > t/2)p
(
t ∧ V 2(r), x, y)
and
Px (τD > t) ≈ e−λ1(D)t
(
V (δD(x))√t ∧ V (r)
∧ 1)
.
Here λ1(D) denotes the smallest eigenvalue of the compact semigroupgenerated by pD(t, x, y).
Recall that V (r) = 1√ψ∗(1/r)
, where ψ is the symbol of the process.
Extends results obtained by Chen, Kim, Song in the case of subordinateBrownian motions governed by complete subordinators with weak scalingconditions.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Bounded smooth domains
Let ψ satisfy global WLSC and WUSC.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Bounded smooth domains
Let ψ satisfy global WLSC and WUSC. For every r > 0:
pB(0,r)(t, x, y) ≈ e−λ1(Br)t(
V (r − |x|)√t ∧ V (r)
∧ 1)(
V (r − |y|)√t ∧ V (r)
∧ 1)
p(t∧V 2(r), x, y),
where the comparability constant depends only on d and ψ.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Bounded smooth domains
Let ψ satisfy global WLSC and WUSC. For every r > 0:
pB(0,r)(t, x, y) ≈ e−λ1(Br)t(
V (r − |x|)√t ∧ V (r)
∧ 1)(
V (r − |y|)√t ∧ V (r)
∧ 1)
p(t∧V 2(r), x, y),
where the comparability constant depends only on d and ψ. Moreover
c1(d)
V 2(r)6 λ1(Br) 6
c2(d)
V 2(r)
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Bounded smooth domains
Let ψ satisfy global WLSC and WUSC. For every r > 0:
pB(0,r)(t, x, y) ≈ e−λ1(Br)t(
V (r − |x|)√t ∧ V (r)
∧ 1)(
V (r − |y|)√t ∧ V (r)
∧ 1)
p(t∧V 2(r), x, y),
where the comparability constant depends only on d and ψ. Moreover
c1(d)
V 2(r)6 λ1(Br) 6
c2(d)
V 2(r)
A consequence of the above estimate and intrinsic ultracontractivity of PDt(Grzywny 2008’) is:
Corollary
Let φr1 be the (positive) eigenfunction corresponding to λ1(Br). There isc = c(d, ψ) such that
c−1V (r − |x|)rd/2V (r)
6 φr1(x) 6 cV (r − |x|)rd/2V (r)
, x ∈ Rd.
IU: pB(0,r)(t, x, y) ≈ φr1(x)φr1(y)e−λ1(Br)t, t→∞
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2014’, SPA)
Let ψ ∈WLSC(α, 0)∩WUSC(α, 0) and d > α. Let D be a C1,1 at scale R1 andsuch that Dc ⊂ BR2 . For all x, y ∈ R
d and t > 0 we have
pD(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
(
V (δD(x))√t ∧ V (R1)
∧ 1)
with comparability constants C = C(d, ψ,R2/R1).
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2014’, SPA)
Let ψ ∈WLSC(α, 0)∩WUSC(α, 0) and d > α. Let D be a C1,1 at scale R1 andsuch that Dc ⊂ BR2 . For all x, y ∈ R
d and t > 0 we have
pD(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
(
V (δD(x))√t ∧ V (R1)
∧ 1)
with comparability constants C = C(d, ψ,R2/R1).
In particular for D = (BR1)c comparability constants depend only on d and ψ.
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
1 ∧ δα/2
D(x)
1∧t1/2 , if α < d,
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
1 ∧ δα/2
D(x)
1∧t1/2 , if α < d,
1 ∧ log(1+δ1/2
D(x)
log(1+t1/2), if α = d = 1,
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
1 ∧ δα/2
D(x)
1∧t1/2 , if α < d,
1 ∧ log(1+δ1/2
D(x)
log(1+t1/2), if α = d = 1,
δα−1D
(x)∧δα/2D(x)
(t1/α∨δD(x))α−1∧ (t1/α ∨ δD(x))α/2, if α > d = 1,
with comparability constants C = C(d, α).
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
1 ∧ δα/2
D(x)
1∧t1/2 , if α < d,
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
1 ∧ δα/2
D(x)
1∧t1/2 , if α < d,
1 ∧ log(1+δ1/2
D(x)
log(1+t1/2), if α = d = 1,
Heat kernels of unimodal Levy processes with weak scaling conditions
Exit time
Exterior domains
Theorem (Bogdan, Grzywny, Ryznar, 2010’, AoP)
Let ψ(ξ) = |ξ|α, α ∈ (0, 2), and D = B(0, 1)c. For all x, y ∈ Rd and t > 0 we
havepB(0,r)
c(t, x, y) ≈ Px(τD > t)Py(τD > t)p(t, x, y),
and
Px(τD > t) ≈
1 ∧ δα/2
D(x)
1∧t1/2 , if α < d,
1 ∧ log(1+δ1/2
D(x)
log(1+t1/2), if α = d = 1,
δα−1D
(x)∧δα/2D(x)
(t1/α∨δD(x))α−1∧ (t1/α ∨ δD(x))α/2, if α > d = 1,
with comparability constants C = C(d, α).