Problem 18.7 Easy Free 3 variations

Log-Price Dynamics of GBM

A price process satisfies dSt=3St dt+4St dWtdS_t = 3S_t\,dt + 4S_t\,dW_t for a standard Brownian motion WtW_t. Writing the dynamics of Xt=ln⁡StX_t=\ln S_t as dXt=a dt+b dWtdX_t = a\,dt + b\,dW_t, find a2+b2a^2+b^2.

Work it out, then compare with the answer.

SolutionShow the worked solution

Key idea. Apply Itô’s lemma to f(x)=ln⁡xf(x)=\ln x. Because f′′<0f''<0, the second-order term lowers the drift by 12σ2\tfrac12\sigma^2.

We have f′(x)=1/xf'(x)=1/x and f′′(x)=−1/x2f''(x)=-1/x^2. The quadratic variation of SS is d[S,S]t=16St2 dtd[S,S]_t=16S_t^2\,dt. Itô’s lemma gives

dXt=1St dSt−12⋅1St2 d[S,S]t.dX_t=\frac{1}{S_t}\,dS_t-\frac12\cdot\frac{1}{S_t^2}\,d[S,S]_t .

Substituting dStdS_t and d[S,S]td[S,S]_t:

dXt=(3 dt+4 dWt)−8 dt=−5 dt+4 dWt.dX_t=(3\,dt+4\,dW_t)-8\,dt=-5\,dt+4\,dW_t .

Hence a=3−12⋅42=−5a=3-\tfrac12\cdot 4^2=-5 and b=4b=4, so

a2+b2=25+16=41.a^2+b^2=25+16=41.
41\boxed{41}

Variations

The same idea with a twist. Each solution gives only the changed step.

Variation 18.7a

Consider the process MtM_t solving dMt=σMt dWtdM_t = \sigma M_t\,dW_t. Two attempts below compute dln⁡(Mt2)d\ln(M_t^2) and reach different answers, so exactly one contains an error. Let a=1a=1 if Method 1 is the flawed one and a=2a=2 if Method 2 is; let ll be the index of the first incorrect displayed line in that method’s derivation (lines numbered from 11 within each method). Find 100a+l100a+l.

Method 1

dM2=(M2)′ dM+12(M2)′′ d[M,M]dM2=2M dM+d[M,M]dM2=2σM2 dWt+σ2M2 dtdM2M2=2σ dWt+σ2 dtdln⁡M2=2σ dWt+σ2 dt\begin{align*} dM^2 &= (M^2)'\,dM + \tfrac12 (M^2)''\,d[M,M] \\ dM^2 &= 2M\,dM + d[M,M] \\ dM^2 &= 2\sigma M^2\,dW_t + \sigma^2 M^2\,dt \\ \frac{dM^2}{M^2} &= 2\sigma\,dW_t + \sigma^2\,dt \\ d\ln M^2 &= 2\sigma\,dW_t + \sigma^2\,dt \end{align*}

Method 2

dln⁡M2=(ln⁡M2)′ dM+12(ln⁡M2)′′ d[M,M]dln⁡M2=2MM2 dM+12(2MM2)′ d[M,M]dln⁡M2=2M dM+12(2M)′ d[M,M]dln⁡M2=2M dM−12⋅2M2 d[M,M]dln⁡M2=2M dM−1M2 d[M,M]dln⁡M2=2σ dWt−σ2 dt\begin{align*} d\ln M^2 &= (\ln M^2)'\,dM + \tfrac12(\ln M^2)''\,d[M,M] \\ d\ln M^2 &= \frac{2M}{M^2}\,dM + \tfrac12\left(\frac{2M}{M^2}\right)'\,d[M,M] \\ d\ln M^2 &= \frac{2}{M}\,dM + \tfrac12\left(\frac{2}{M}\right)'\,d[M,M] \\ d\ln M^2 &= \frac{2}{M}\,dM - \frac12\cdot\frac{2}{M^2}\,d[M,M] \\ d\ln M^2 &= \frac{2}{M}\,dM - \frac{1}{M^2}\,d[M,M] \\ d\ln M^2 &= 2\sigma\,dW_t - \sigma^2\,dt \end{align*}

Work it out, then compare with the answer.

Solution

First find the correct dynamics. Since ln⁡M2=2ln⁡M\ln M^2=2\ln M, and Itô’s lemma gives dln⁡M=σ dWt−12σ2 dtd\ln M=\sigma\,dW_t-\tfrac12\sigma^2\,dt, we get

dln⁡M2=2σ dWt−σ2 dt.d\ln M^2=2\sigma\,dW_t-\sigma^2\,dt .

Method 2 is correct. Take f(M)=ln⁡M2f(M)=\ln M^2, so f′=2/Mf'=2/M and f′′=−2/M2f''=-2/M^2. Every line follows from the one before. With d[M,M]=σ2M2 dtd[M,M]=\sigma^2M^2\,dt, the last line is 2σ dWt−σ2 dt2\sigma\,dW_t-\sigma^2\,dt, which matches.

Method 1 is flawed. Lines 1 to 4 are valid: Itô for x2x^2, then division by M2M^2. Line 5 sets dln⁡M2=dM2/M2d\ln M^2=dM^2/M^2, which is false. The correct relation is

dln⁡Y=dYY−d[Y,Y]2Y2.d\ln Y=\frac{dY}{Y}-\frac{d[Y,Y]}{2Y^2}.

Here Y=M2Y=M^2, so the omitted term is −12(2σ)2 dt=−2σ2 dt-\tfrac12(2\sigma)^2\,dt=-2\sigma^2\,dt. Adding it to line 4 recovers 2σ dWt−σ2 dt2\sigma\,dW_t-\sigma^2\,dt.

So a=1a=1 and l=5l=5, giving 100a+l=105100a+l=105.

105\boxed{105}
Variation 18.7b

Let WtW_t be a standard Brownian motion and let XtX_t be a process such that Yt=1/XtY_t = 1/X_t satisfies dYt=Yt(2 dt−dWt)dY_t = Y_t(2\,dt - dW_t). Writing the resulting dynamics of XtX_t as dXt=Xt(a dt+b dWt)dX_t = X_t(a\,dt + b\,dW_t) for integers a,ba,b, find abab.

Work it out, then compare with the answer.

Solution

Take X=f(Y)=1/YX=f(Y)=1/Y, so f′(y)=−1/y2f'(y)=-1/y^2 and f′′(y)=2/y3f''(y)=2/y^3. The quadratic variation is d[Y,Y]t=Yt2 dtd[Y,Y]_t=Y_t^2\,dt. Itô’s lemma gives

dXt=−1Yt2 Yt(2 dt−dWt)+1Yt3 Yt2 dt=1Yt(−dt+dWt)=Xt(−dt+dWt).dX_t=-\frac{1}{Y_t^2}\,Y_t(2\,dt-dW_t)+\frac{1}{Y_t^3}\,Y_t^2\,dt =\frac{1}{Y_t}(-dt+dW_t)=X_t(-dt+dW_t).

So a=−1a=-1 and b=1b=1, giving ab=−1ab=-1.

−1\boxed{-1}
Variation 18.7c

Let StS_t be a geometric Brownian motion with both drift and volatility parameters equal to 11, and S0=1S_0=1. Then E[S22]=ek\mathbb{E}[S_2^2] = e^k for some constant kk. Find kk.

Work it out, then compare with the answer.

Solution

The process satisfies dSt=St(dt+dWt)dS_t=S_t(dt+dW_t), so d[S,S]t=St2 dtd[S,S]_t=S_t^2\,dt. Itô’s lemma for x2x^2 gives

dSt2=2St dSt+d[S,S]t=St2(3 dt+2 dWt).dS_t^2=2S_t\,dS_t+d[S,S]_t=S_t^2(3\,dt+2\,dW_t).

So St2S_t^2 is a geometric Brownian motion with drift 33 and initial value 11. Hence E[St2]=e3t\mathbb{E}[S_t^2]=e^{3t}.

Check: St=et/2+WtS_t=e^{t/2+W_t}, so St2=et+2WtS_t^2=e^{t+2W_t}. Then E[St2]=et+2t=e3t\mathbb{E}[S_t^2]=e^{t+2t}=e^{3t}.

At t=2t=2 this is e6e^6, so k=6k=6.

6\boxed{6}