Chapter 8

The PDE connection

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Problem 8.1

Let ff be the initial value in the problem considered in Lemma 8.1 and write u(t,x):=Ptf(x)=Ef(Bt+x)u(t, x): = P_{t} f(x) = \mathbb {E} f\left(B_{t}+x\right) where (Bt)t⩾0\left(B_{t}\right)_{t \geqslant 0} is a BM d{ }^{d}.

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(a)

Assume that f∈C∞(Rd)f \in \mathcal{C}_{\infty }\left(\mathbb {R}^{d}\right). Show that ∂tu(t,x),∂ju(t,x)\partial_{t} u(t, x), \partial_{j} u(t, x) and ∂j∂ku(t,x)\partial_{j} \partial_{k} u(t, x) exist and are functions in C((0,∞)×Rd)\mathcal{C}\left((0, \infty ) \times \mathbb {R}^{d}\right).

(b)

Assume that f:Rd→Rf: \mathbb {R}^{d} \rightarrow \mathbb {R} is measurable and exponentially bounded, i.e. ∣f(x)∣⩽CeC∣x∣\left|f(x)\right| \leqslant C e^{C\left|x\right|} for all x∈Rdx \in \mathbb {R}^{d} and some constant CC. Show that ∂tu(t,x),∂ju(t,x)\partial_{t} u(t, x), \partial_{j} u(t, x) and ∂j∂ku(t,x),j,k=1,…,d\partial_{j} \partial_{k} u(t, x), j, k = 1, \ldots , d, exist and are exponentially bounded functions in C((0,∞)×Rd)\mathcal{C}\left((0, \infty ) \times \mathbb {R}^{d}\right).

(c)

What happens, if we assume in Part b) that f(x)⩽CeC∣x∣2f(x) \leqslant C e^{C\left|x\right|^{2}} ?

Problem 8.2

Assume that in Lemma 8.1 the initial datum satisfies f∈C∞(Rd)f \in \mathcal{C}_{\infty }\left(\mathbb {R}^{d}\right) but not necessarily f∈D(A)f \in \mathfrak {D}(A). Consider (8.3) with PϵfP_{\epsilon } f instead of ff. Discuss the limit ϵ→0\epsilon \rightarrow 0.

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Problem 8.3

Let (Bt)t⩾0\left(B_{t}\right)_{t \geqslant 0} be a BMd,f:Rd→R\mathrm{BM}^{d}, f: \mathbb {R}^{d} \rightarrow \mathbb {R} be a continuous function such that ∫0tf(Bs)ds=0\int_{0}^{t} f\left(B_{s}\right) d s = 0 for all t>0t > 0. Show that f(Bs)=0f\left(B_{s}\right) = 0 for all s>0s > 0, and conclude that f≡0f \equiv 0.

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Problem 8.4

Complete the approximation argument for Lévy's arc - sine law from §8.9\S 8.9 :

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(a)

Show, by a direct calculation, that vn,λ(x)v_{n, \lambda }(x) converges as n→∞n \rightarrow \infty. Conclude from (8.16) that vn,λ′′v_{n, \lambda }^{\prime \prime } converges.

(b)

Integrate the ODE (8.16) to see that vn,λ(x)−vn,λ′(0)v_{n, \lambda }(x) - v_{n, \lambda }^{\prime }(0) has a limit. Integrating once again shows that vn,λ′(0)v_{n, \lambda }^{\prime }(0) converges, too.

(c)

Identify the limits of vn,λ,vn,λ′v_{n, \lambda }, v_{n, \lambda }^{\prime } and vn,λ′′v_{n, \lambda }^{\prime \prime }.

Problem 8.5

Show Theorem 8.5 with semigroup methods.

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Problem 8.6

Find the solution to the Dirichlet problem in dimension d=1:u′′(x)=0d = 1: u^{\prime \prime }(x) = 0 for all x∈(0,1),u(0)=a,u(1)=bx \in (0,1), u(0) = a, u(1) = b and uu is continuous in [0,1]. Compare your findings with Wald's identities, cf. Theorem 5.10 and Corollary 5.11.

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Problem 8.7

Use Lemma 7.33 and give an alternative derivation of the result of Lemma 8.10.

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Problem 8.8

Show that Lemma 8.10 remains true for any dd - dimensional Feller process XtX_{t} with continuous paths and generator L=∑j,k=1dajk(x)∂j∂k+∑j=1dbj(x)∂jL = \sum_{j, k = 1}^{d} a_{j k}(x) \partial_{j} \partial_{k}+\sum_{j = 1}^{d} b_{j}(x) \partial_{j} such that a11(x)⩾a0>0a_{11}(x) \geqslant a_{0} > 0 and ∣b1(x)∣⩽b0<∞\left|b_{1}(x)\right| \leqslant b_{0} < \infty.

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Problem 8.9

Table 8.1 No . 2 records the solution to the initial value problem (8.6). Explain how this result follows from our considerations regarding (8.3) and (8.7).

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Problem 8.10

Let g:[0,∞)×Rd→Rg:[0, \infty ) \times \mathbb {R}^{d} \rightarrow \mathbb {R} be a bounded continuous function such that g(t,⋅)g(t, \cdot ) is κ\kappa - Hölder continuous with a Hölder constant which does not depend on tt or xx. Mimic the proof of Lemma 8.7 to prove that v(t,x):=Ex(∫0tg(t−s,Bs)ds)v(t, x): = \mathbb {E}^{x}\left(\int_{0}^{t} g\left(t - s, B_{s}\right) d s\right) is in C1,2((0,∞)×Rd)∩Cb([0,∞)×Rd)\mathcal{C}^{1,2}\left((0, \infty ) \times \mathbb {R}^{d}\right) \cap \mathcal{C}_{b}\left([0, \infty ) \times \mathbb {R}^{d}\right) and satisfies (8.1). Explain why this proves, under suitable assumptions on g(t,x)g(t, x), No. 3. in Table 8.1.

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Problem 8.11

Use the LIL (Corollary 12.2) to give an alternative proof for the fact that a one - dimensional Brownian motion oscillates in every time interval [0,ϵ][0, \epsilon ] infinitely often around its starting point.

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Problem 8.12

Let d⩾2d \geqslant 2. A flat cone in Rd\mathbb {R}^{d} is a cone in Rd−1\mathbb {R}^{d - 1}. Adapt the argument of Example 8.18.e) to show the following useful regularity criterion for a BMd\mathrm{BM}^{d} : The boundary point x0x_{0} is regular for DcD^{c} if there is a truncated flat cone with vertex at x0x_{0} and lying entirely in DcD^{c}.

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Problem 8.13

Let (b,β)(b, \beta ) be a BM2\mathrm{BM}^{2} and σn=inf⁡{t>1/n:b(t)=0}\sigma_{n} = \inf \left\{ t > 1 / n: b(t) = 0\right\}. Show that the random variable β(σn)\beta \left(\sigma_{n}\right) has a probability density.

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