Chapter 4

Markov properties of Brownian motion

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Problem 4.1

If WW is a Brownian motion, let St=sup⁡s≤tWsS_{t}=\sup_{s \leq t} W_{s}. Find the density for StS_{t}.

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Problem 4.2

With WW and SS as in Exercise 4.1, find the joint density of (St,Wt)\left(S_{t}, W_{t}\right).

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Problem 4.3

Let WW be a Brownian motion started at a>0a>0 and let T0T_{0} be the first time WW hits 00. Find the law of sup⁡t≤T0Wt\sup_{t \leq T_{0}} W_{t}.

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Problem 4.4

Use the reflection principle to prove that if WW is a Brownian motion and T=inf⁡{t>0:Wt∈T=\inf \left\{ t>0: W_{t} \in \right. (0,∞)}(0, \infty )\}, then

P(T=0)=1 \mathbb {P}\left(T=0\right)=1

In other words, Brownian motion enters the interval (0,∞)(0, \infty ) immediately. By symmetry it enters the interval (−∞,0)(-\infty , 0) immediately. Conclude that Brownian motion hits 0 infinitely often in every time interval [0,t][0, t].

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Problem 4.5

Let WtW_{t} be a Brownian motion and {Ft}\left\{ \mathcal{F}_{t}\right\} be the minimal augmented filtration generated by WW. Let

T=inf⁡{t>0:Wt=sup⁡0≤s≤1Ws} T=\inf \left\{ t>0: W_{t}=\sup _{0 \leq s \leq 1} W_{s}\right\}

Show that TT is not a stopping time with respect to {Ft}\left\{ \mathcal{F}_{t}\right\}.

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Problem 4.6

Let WW and SS be as in Exercise 4.1.

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(1)

Let 0<s<t<u0<s<t<u and let a<ba<b with b−a≤1b-a \leq 1. Show that there exists a constant cc, depending on s,ts, t, and uu, but not aa or bb, such that

P(Ss∈[a,b],sup⁡t≤r≤uWr∈[a,b])≤c(b−a)2 \mathbb {P}\left(S_{s} \in [a, b], \sup _{t \leq r \leq u} W_{r} \in [a, b]\right) \leq c(b-a)^{2}
(2)

Show that the path of a Brownian motion does not take on the same value as a local maximum twice. That is, if SS and TT are times when WW has a local maximum, then WS≠WTW_{S} \neq W_{T}, a.s.

Problem 4.7

Let VtV_{t} be the number of upcrossings of [0,1][0,1] by a Brownian motion WW up to time tt. This means we let S1=0,Ti=inf⁡{t>Si:Wt≥1}S_{1}=0, T_{i}=\inf \left\{ t>S_{i}: W_{t} \geq 1\right\}, and Si+1=inf⁡{T>Ti:Wt≤0}S_{i+1}=\inf \left\{ T>T_{i}: W_{t} \leq 0\right\} for i=1,2,…i=1,2, \ldots, and we set Vt=sup⁡{k:Tk≤t}V_{t}=\sup \left\{ k: T_{k} \leq t\right\}. Show that Vt→∞V_{t} \rightarrow \infty, a.s., as t→∞t \rightarrow \infty.

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Problem 4.8

Let WW be a Brownian motion. The zero set of Brownian motion is the random set

Z(ω)={t∈[0,1]:Wt(ω)=0} Z(\omega )=\left\{ t \in [0,1]: W_{t}(\omega )=0\right\}
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(1)

Show that Z(ω)Z(\omega ) is a closed set for each ω\omega.

(2)

Show that with probability one, every point of Z(ω)Z(\omega ) is a limit point of Z(ω)Z(\omega ). Conclude that Z(ω)Z(\omega ) is an uncountable set.

Problem 4.9

Let WW be a one-dimensional Brownian motion and δ>0\delta >0.

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(1)

Prove that there exists γ\gamma such that if t≤γt \leq \gamma, then

P(0≤Wt≤δ/2)≥1/4 and P(−δ/2≤Wt≤0)≥1/4 \mathbb {P}\left(0 \leq W_{t} \leq \delta / 2\right) \geq 1 / 4 \quad \text{ and } \quad \mathbb {P}\left(-\delta / 2 \leq W_{t} \leq 0\right) \geq 1 / 4
(2)

Prove there exists γ\gamma such that

P(sup⁡s≤γ∣Ws∣>δ/2)≤1/8 \mathbb {P}\left(\sup _{s \leq \gamma }\left|W_{s}\right|>\delta / 2\right) \leq 1 / 8
(3)

Prove that if m≥1m \geq 1, then

P(sup⁡mγ≤s≤(m+1)γ∣Ws−Wmγ∣≤δ/2,Wmγ∈[0,δ/2],∣W(m+1)γ∣≤δ/2∣Fmγ)≥18P(sup⁡mγ≤s≤(m+1)γ∣Ws−Wmγ∣≤δ/2,Wmγ∈[0,δ/2]) \begin{aligned} & \mathbb {P}\left( \sup _{m \gamma \leq s \leq (m+1) \gamma }\left|W_{s}-W_{m \gamma }\right| \leq \delta / 2, W_{m \gamma } \in [0, \delta / 2],\left|W_{(m+1) \gamma }\right| \leq \delta / 2 \mid \mathcal{F}_{m \gamma } \right) \\ & \geq \frac{1}{8} \mathbb {P}\left(\sup _{m \gamma \leq s \leq (m+1) \gamma }\left|W_{s}-W_{m \gamma }\right| \leq \delta / 2, W_{m \gamma } \in [0, \delta / 2]\right) \end{aligned}

and the same with Wmγ∈[−δ/2,0]W_{m \gamma } \in [-\delta / 2,0] in place of Wmγ∈[0,δ/2]W_{m \gamma } \in [0, \delta / 2]. Conclude that

P(sup⁡mγ≤s≤(m+1)γ∣Ws−Wmγ∣≤δ/2,∣Wmγ∣≤δ/2,∣W(m+1)γ∣≤δ/2∣Fmγ)≥18P(sup⁡mγ≤s≤(m+1)γ∣Ws−Wmγ∣≤δ/2,∣Wmγ∣≤δ/2) \begin{aligned} & \mathbb {P}\left( \sup _{m \gamma \leq s \leq (m+1) \gamma }\left|W_{s}-W_{m \gamma }\right| \leq \delta / 2,\left|W_{m \gamma }\right| \leq \delta / 2,\left|W_{(m+1) \gamma }\right| \leq \delta / 2 \mid \mathcal{F}_{m \gamma } \right) \\ & \geq \frac{1}{8} \mathbb {P}\left(\sup _{m \gamma \leq s \leq (m+1) \gamma }\left|W_{s}-W_{m \gamma }\right| \leq \delta / 2,\left|W_{m \gamma }\right| \leq \delta / 2\right) \end{aligned}
(4)

Use induction to prove that if t0>0t_{0}>0, there exists c1>0c_{1}>0 such that

P(sup⁡s≤t0∣Ws∣≤δ)>c1 \mathbb {P}\left(\sup _{s \leq t_{0}}\left|W_{s}\right| \leq \delta \right)>c_{1}
(5)

Prove that if WW is a dd-dimensional Brownian motion, t0>0t_{0}>0, and δ>0\delta >0, there exists c2c_{2} such that

P(sup⁡s≤t0∣Ws∣≤δ)>c2. \mathbb {P}\left(\sup _{s \leq t_{0}}\left|W_{s}\right| \leq \delta \right)>c_{2} .
Problem 4.10

The pp-variation of a function ff on the interval [0,1][0,1] is defined by

Vp(f)=sup⁡{∑i=0n−1∣f(ti+1)−f(ti)∣p:n≥1,0=t0<t1,⋯<tn=1} V^{p}(f)=\sup \left\{ \sum _{i=0}^{n-1}\left|f\left(t_{i+1}\right)-f\left(t_{i}\right)\right|^{p}: n \geq 1,0=t_{0}<t_{1}, \cdots <t_{n}=1\right\}

the supremum is over all partitions PP of [0,1][0,1]. In this exercise we will prove that if p<2p<2 and WW is a Brownian motion, then Vp(W)=∞V^{p}(W)=\infty, a.s.

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(1)

Let XiX_{i} be an i.i.d. sequence of random variables with finite mean. Use the strong law of large numbers to prove that if K>E[X1]K>\mathbb {E}\left[X_{1}\right], then

P(∑i=1nXi>Kn)→0 \mathbb {P}\left(\sum _{i=1}^{n} X_{i}>K n\right) \rightarrow 0

as n→∞n \rightarrow \infty.

(2)

If p<2p<2, take r∈(p,2)r \in (p, 2), and let εn=n−1/r\varepsilon_{n}=n^{-1 / r}. Let S0=0S_{0}=0 and for i≥0i \geq 0, set Si+1=inf⁡{t>Si:∣Wt−WSi∣>εn}S_{i+1}=\inf \left\{ t>S_{i}:\left|W_{t}-W_{S_{i}}\right|>\varepsilon_{n}\right\}. Set Xi=εn−2(Si−Si−1)X_{i}=\varepsilon_{n}^{-2}\left(S_{i}-S_{i-1}\right). Prove that the XiX_{i} are i.i.d. with finite mean.

(3)

Use (1) to show that

P(Sn>1)=P(∑i=1nXi>εn−2)→0 \mathbb {P}\left(S_{n}>1\right)=\mathbb {P}\left(\sum _{i=1}^{n} X_{i}>\varepsilon _{n}^{-2}\right) \rightarrow 0

as n→∞n \rightarrow \infty.

(4)

Using the partition {S0,S1,…,Sn}\left\{ S_{0}, S_{1}, \ldots , S_{n}\right\}, show that Vp(W)≥nεnpV^{p}(W) \geq n \varepsilon_{n}^{p} on the event (Sn≤1)\left(S_{n} \leq 1\right).

(5)

Conclude Vp(W)=∞V^{p}(W)=\infty, a.s.