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布朗运动与随机微积分

Brownian Motion and Stochastic Calculus

专题
Finance / 金融
难度
L4

题目详情

  • (A) 什么是布朗运动?列举一些性质。
  • (B) 对标准布朗运动 BtB_tE[Bt]\mathbb{E}[B_t]E[Bt2]\mathbb{E}[B_t^2] 分别是什么?Cov(Bt,Bt2)\operatorname{Cov}(B_t,B_t^2) 呢?
  • (C) 若标准布朗运动满足 B1>0B_1>0B2<0B_2<0,该事件的概率是多少?
  • (停时) 对标准布朗运动 BtB_t,令 T=min{t:Bt=+1 或 Bt=1}.T=\min\{t: B_t=+1\text{ 或 }B_t=-1\}.E[T]\mathbb{E}[T]。更一般地,若首次命中 +α+\alphaβ-\beta,如何求 E[T]\mathbb{E}[T]
  • (Ito 引理) 举例说明。
  • (A) What is Brownian motion? Name some properties.
  • (B) For standard Brownian motion BtB_t, how are E[Bt]\mathbb{E}[B_t] and E[Bt2]\mathbb{E}[B_t^2]? What about Cov(Bt,Bt2)\operatorname{Cov}(B_t,B_t^2)?
  • (C) If B1>0B_1>0 and B2<0B_2<0 (standard Brownian motion), what is the probability of this event?
  • (Stopping Times): For a standard Brownian motion BtB_t, let T=min{t:Bt=+1 or Bt=1}.T = \min\{\,t:B_t=+1 \text{ or } B_t=-1\}. What is E[T]\mathbb{E}[T]? More generally, if you hit +α\alpha or -β\beta, how do you find E[T]\mathbb{E}[T]?
  • (Ito’s Lemma) examples.
解析

5.4.1 布朗运动

  1. 定义:过程 {W(t),t0}\{W(t),t\ge 0\} 是标准布朗运动若
  • W(0)=0W(0)=0
  • 增量独立;
  • 增量 W(ti+1)W(ti)N(0,ti+1ti)W(t_{i+1})-W(t_i)\sim N(0,t_{i+1}-t_i)
  • 样本路径连续(无跳跃)。
  1. 性质
  • W(t)N(0,t)W(t)\sim N(0,t),因此 E[W(t)]=0\mathbb{E}[W(t)]=0Var(W(t))=t\mathrm{Var}(W(t))=t
  • 鞅性质:E[W(t+s)W(t)]=W(t)\mathbb{E}[W(t+s)\mid W(t)]=W(t)
  • Markov 性。
  • cov(W(s),W(t))=min(s,t)\operatorname{cov}(W(s),W(t))=\min(s,t)
  1. 相关鞅:
  • Y(t)=W(t)2tY(t)=W(t)^2-t 是鞅。
  • 指数鞅:
Z(t)=exp{λW(t)12λ2t}.Z(t)=\exp\{\lambda W(t)-\tfrac12\lambda^2 t\}.
  1. Cov(Bt,Bt2)=0\operatorname{Cov}(B_t,B_t^2)=0:因为 BtN(0,t)B_t\sim N(0,t),有 E[Bt3]=0\mathbb{E}[B_t^3]=0,于是
Cov(Bt,Bt2)=E[Bt3]E[Bt]E[Bt2]=0.\operatorname{Cov}(B_t,B_t^2)=\mathbb{E}[B_t^3]-\mathbb{E}[B_t]\mathbb{E}[B_t^2]=0.
  1. P(B1>0,B2<0)P(B_1>0,B_2<0):由对称性(或反射原理)可得该概率为 1/81/8

5.4.2 停时 / 首次穿越时间

  • 命中 ±1\pm 1:令 T=min{tBt=1 或 1}T=\min\{t\mid B_t=1\text{ 或 }-1\}。对鞅 M(t)=Bt2tM(t)=B_t^2-t 用可选停时定理:
E[BT2T]=E[B02]=0.\mathbb{E}[B_T^2-T]=\mathbb{E}[B_0^2]=0.

BT2=1B_T^2=1,因此 E[T]=1\mathbb{E}[T]=1

  • 一般命中 +α+\alphaβ-\betaα,β>0\alpha,\beta>0)时:E[T]=αβ\mathbb{E}[T]=\alpha\beta

5.4.3 Ito 引理

dXt=β(t,Xt)dt+γ(t,Xt)dWt,dX_t=\beta(t,X_t)\,dt+\gamma(t,X_t)\,dW_t,

f(t,x)f(t,x) 足够光滑,则

df(t,Xt)=(tf+βxf+12γ2xxf)dt+γxfdWt.df(t,X_t)=\Bigl(\partial_t f+\beta\,\partial_x f+\tfrac12\gamma^2\,\partial_{xx} f\Bigr)dt+\gamma\,\partial_x f\,dW_t.

Original Explanation

5.4.1 Brownian Motion

  1. Definition: A process {W(t),t0}\{W(t),t\ge 0\} is a standard Brownian motion if:

    • W(0)=0W(0)=0,
    • It has independent increments,
    • Each increment W(ti+1)W(ti)W(t_{i+1})-W(t_i) is normally distributed with mean 0, variance ti+1tit_{i+1}-t_i,
    • It has continuous paths (no jumps).
  2. Properties:

    • W(t)N(0,t)W(t)\sim N(0,t), hence E[W(t)]=0\mathbb{E}[W(t)]=0, Var(W(t))=t\mathrm{Var}(W(t))=t.
    • Martingale: E[W(t+s)W(t)]=W(t)\mathbb{E}[W(t+s)\mid W(t)] = W(t).
    • Markov property.
    • cov(W(s),W(t))=min(s,t)\operatorname{cov}(W(s),W(t))=\min(s,t).
  3. Martingales related to BM:

    • Y(t)=W(t)2tY(t)=W(t)^2 - t is a martingale.
    • The exponential martingale: Z(t)=exp{λW(t)12λ2t}.Z(t) = \exp\bigl\{\lambda\,W(t) - \tfrac12\,\lambda^2\,t\bigr\}.
  4. Cov(Bt,Bt2)=0\operatorname{Cov}(B_t,B_t^2)=0. Since BtN(0,t)B_t\sim N(0,t), E[Bt3]=0\mathbb{E}[B_t^3]=0. Then Cov(Bt,Bt2)=E[Bt3]E[Bt]E[Bt2]=00t=0.\operatorname{Cov}(B_t,B_t^2) = \mathbb{E}[B_t^3] - \mathbb{E}[B_t]\mathbb{E}[B_t^2] = 0 - 0\cdot t = 0.

  5. Probability {B1>0,B2<0}\{B_1>0,B_2<0\} is 1/81/8. By symmetry (or reflection principle arguments), the chance that B1>0B_1>0 and later B2<0B_2<0 ends up being 1/81/8.


5.4.2 Stopping Time / First Passage Time

  • For Brownian motion hitting ±1\pm 1 for the first time:

    • Let T=min{tBt=1 or Bt=1}T = \min\{\,t\mid B_t=1 \text{ or } B_t=-1\}. Using the martingale M(t)=Bt2tM(t)=B_t^2 - t, we get E[BT2T]=E[B02]=0\mathbb{E}[B_T^2 - T]=\mathbb{E}[B_0^2]=0. But BT2=1B_T^2=1. Thus E[T]=1\mathbb{E}[T]=1.
  • In general, to hit +α\alpha or -β\beta (α,β>0\alpha,\beta>0), E[T]=αβ\mathbb{E}[T] = \alpha\,\beta.

  • With drift mm, dXt=mdt+dWtdX_t = m\,dt + dW_t, one solves via ODE or exponential martingale. For example, from 0 to +3 or -5: p+3=e10m1e10me6m.p_{\,+3} = \frac{e^{10\,m}-1}{\,e^{10\,m}-e^{-6\,m}\,}. If m=0m=0, it becomes 58\tfrac58.


5.4.3 Ito’s Lemma

Ito’s lemma says for dXt=β(t,Xt)dt+γ(t,Xt)dWt,dX_t = \beta(t,X_t)\,dt + \gamma(t,X_t)\,dW_t, and f(t,x)f(t,x) sufficiently smooth, df=[tf+βxf+12γ2xxf]dt+γxf  dWt.df = \bigl[\partial_t f + \beta\,\partial_x f + \tfrac12\,\gamma^2\,\partial_{xx} f\bigr]\,dt + \gamma\,\partial_x f\;dW_t.

  • Example: Zt=tBtZ_t = \sqrt{t}\,B_t. By Ito’s lemma, it has a drift term 12t1/2Bt\tfrac12\,t^{-1/2}\,B_t, so it is not a martingale.

  • Example: Bt3B_t^3. The drift term is 3Btdt3\,B_t\,dt, so Bt3B_t^3 is not a martingale.