Sheet 11

Prof. Leif Döring, Felix Benning
course: Wahrscheinlichkeitstheorie 1semester: FSS 2022tutorialDate: 16.05.2022dueDate: 10:15 in the exercise on Monday 16.05.2022
Exercise 1 (Canonical Continuous Process).

Suppose X=(Xt)t0 is a continuous stochastic process on some probability space (Ω,𝒜,) and X its law on C([0,). Define

  • Ω~:=C([0,)), 𝒜~:=(C([0,))) and ~:=X,c

  • X~:=id:C([0,))C([0,)) with X~t:=πt(X~).

Show that (X~t)t0 is a continuous stochastic process on (Ω~,𝒜~,~), which has the same finite dimensional marginals (same law) as X.

Solution.

Due to X~(ω)C([0,)) for all ω, we have

X~s(ω) =πs(X~(ω))=X~(ω)(s)
X~(ω)(t)=X~t(ω)st,

for all ωΩ~, so (X~t)t0 is a continuous stochastic process. Now the law of X~ is

X~(B)=~(X~B)=X~=id~(B)=X,c(B).

And by definition t1,,tnX,c:=t1,,tnX, therefore we have that the finite dimensional marginals are the same

t1,,tnX~ =t1,,tnX.
Exercise 2 (Modification vs. Indistinguishable).
  1. (i)

    Let X,Y be stochastic processes. Show the implications (i)(a)(i)(b)(i)(c) for

    1. (a)

      X and Y are indistinguishable

    2. (b)

      X is a modification of Y

    3. (c)

      X and Y have the same finite dimensional distributions

    Solution.

    (i)(a)(i)(b) We have for all tE

    {XtYt}{sE:XsYs}N

    where N is a measurable zero set as X and Y are indistinguishable. Therefore {XtYt} is a zero set and we have (Xt=Yt)=1. So by definition X is a modification of Y.

    (i)(b)(i)(c) For every t we have Xt=Yt almost surely. So for a finite set {t1,,tn} we can just take the union of zero sets to get (Xt1,Xtn)=(Yt1,Ytn) almost surely. But this implies that the distributions are also equal and by Prop. 8.1.14 we only need to check the finite dimensional distributions are equal (i.e. t1,,tnX=t1,,tnY). ∎

  2. (ii)

    If X is a modification of Y and both X and Y are continuous on a Polish space (E,d), then X and Y are indistinguishable.

    Solution.

    Let Q be the countable dense subset of E, then as X is a modification of Y we have

    (tE:Xt=Yt) =X,Y contin.(tQ:Xt=Yt)=1-(tQ{XtYt})
    1-tQ(XtYt)=0.
Exercise 3 (Hölder Continuity).

Prove the following statements

  1. (i)

    If f is locally γ-Hölder continuous, then f is also locally β-Hölder continuous for all βγ. Why is this wrong for global Hölder continuity?

    Solution.

    Let Ux be the neighborhood of x such that for all yUx we have the γ-Hölder continuity. Then for all βγ we get

    f(x)-f(y)Kxx-yγ=exp(γlog(x-y)<0(if x-y1))Kxx-yβ.

    So using the neighborhood UxB1(x) we have local β-Hölder continuity. Because we can not intersect the neighborhood with a radius one ball in the global case, this is where the proof breaks. And f(y)=|y|γ is already a counterexample of the statement as for x=0 we have

    |f(x)-f(y)|=|x-y|γ>K|x-y|β|y|γ/β>K|y|Kβ/γ,

    so we just have to select y large enough. ∎

  2. (ii)

    If f is continuously differentiable, then f is locally 1-Hölder continuous (Lipschitz continuous).

    Solution.

    Let ϵ>0, then for all yBϵ(x) by the mean value theorem, there exists ξBϵ(x) such that

    |f(x)-f(y)| =|f(ξ)|x-ysupzBϵ(x)|f(z)|=:Kxx-y.
  3. (iii)

    If f is Hölder continuous with index γ>1, then f is constant.

    Hint.

    Show f is differentiable using the definition of differentiable.

    Solution.

    We have for every x, f(x)=0 because

    limyxf(y)-f(x)-f(x)(x-y)x-ylimyxKxx-yγ-1=0.

    But f0 implies f is constant. ∎

  4. (iv)

    If g is (locally) γ-Hölder continuous and f is (locally) β-Hölder continuous, then gf is (locally) γβ-Hölder continuous.

    Solution.

    Using the respective definitions we get

    gf(x)-gf(y)Kgf(x)-f(y)γKg(Kfx-yβ)γ=KgKfγ=:Kx-yγβ.

    For the local version we need to ensure that f(y) is in an for g appropriate neighborhood of f(x). But due to Hölder continuity of f we can ensure

    f(x)-f(y)ϵ

    by selecting x-y(ϵKf)1/β. ∎

  5. (v)

    For β<1, f(x)=xβ is Hölder continuous with index β.

    Hint.

    Show that g:+xβ is β-Hölder continuous and use (iv). Note that zβz for all z[0,1]. Deduce for all a,b0

    (aa+b)β+(ba+b)β1aβ+bβ(a+b)β

    which is kind of a triangle inequality. Now you just need to recall how you show Lipschitz continuity for norms.

    Solution.

    We use f=g with g:+xβ. The norm is 1-Hölder continuous because of

    xx-y+yx-yx-y (1)

    since by symmetry we get Lipschitz continuity

    |x-y|x-y.

    So if g is β-Hölder continuous, we are done by (iv). For β<1 we have zβz for all z[0,1]. Using this fact, we get for all a,b0

    (aa+b)βaa+b+(ba+b)βba+b1aβ+bβ(a+b)β.

    This is a type of triangle inequality so we can essentially do (1) again, except we need to keep a,b0. Assuming x,y+ and without loss of generality xy, we define b=x-y and a=y to get

    xβ=(a+b)βyβ+(x-y)β

    and with xy and monotonicity of g we have

    |g(x)-g(y)|=xβ-yβ(x-y)β=|x-y|β.

    Therefore g is β-Hölder continuous. ∎

Exercise 4 (Fractional Gaussian is Hölder).
  1. (i)

    Prove that there exists a centred Gaussian process (Xt)t with Var(Xt-Xs)=|t-s|2H and X0=0 for all H[0,1]. You can use that

    k(s,t)=12(|t|2H+|s|2H-|t-s|2H)

    is positive semi-definite without proof. Prove that the law of this process is uniquely determined. (This process is called fractional Brownian motion and the BM is a special case with H=12).

    Solution.

    By Theorem 8.1.18 there exists a centred Gaussian process Xt with covariance k. And we have

    Var(Xt-Xs) =𝔼[(Xt-Xs)2]=𝔼[Xt2]-2𝔼[XtXs]+𝔼[Xs2]
    =k(t,t)=|t|2H-2k(t,s)+k(s,s)=|s|2H
    =|t-s|2H

    As the covariance function is uniquely determined because of

    Cov(Xt,Xs)=12(𝔼[Xt2]=Var(Xt-X0)-Var(Xt-Xs)+𝔼[Xs2]).

    The law is uniquely determined by Proposition 8.1.14. ∎

  2. (ii)

    Prove that for all γ<H, the fractional Brownian motion has a modification which is γ-Hölder continuous.

    Hint.

    For X𝒩(0,σ2) we have

    𝔼[Xn]={0n oddσn(n-1)!!n even,

    where n!!=n(n-2)(n-4)31 for odd n.

    Solution.

    Because we have for all n

    𝔼[|Xt-Xs|2n]=(2n-1)!!|t-s|2nH

    We get a γ-Hölder continuous modification for all

    γ<2nH-12n=H-12n (2)

    by the Kolmogorov-Chentsov Theorem. But as n was arbitrary, we can find an n for all γ<H such that Equation (2) is still satisfied. ∎