Unit 5, lesson 40

Girsanov theorem and risk neutral dynamics

Girsanov's theorem with its density hypotheses and sign convention, how a measure change shifts a diffusion drift, the market price of risk, risk-neutral stock dynamics, measure equivalence and Lévy's characterization.

  • Video 40
  • Measure changes and Girsanov's theorem

In a constructed model a stock has expected growth rate 0.080.08 per year and volatility 0.20.2 per square-root year under the physical measure, while cash earns 0.030.03 per year. A pricing measure for the cash numeraire must make the discounted stock a martingale, so under it the drift has to be 0.030.03. Which change of probability does this, and why can it move the drift while the volatility stays at 0.20.2? This lesson states Girsanov’s theorem with its hypotheses and an explicit sign convention, derives how a measure change shifts the drift of a diffusion, and finds the market price of risk that produces risk-neutral stock dynamics.

Key terms

Girsanov’s theorem

Definition Fix a finite horizon TT, a filtration (Ft)0≤t≤T(\mathcal{F}_t)_{0 \le t \le T} satisfying the usual conditions and a standard Brownian motion WW under P\mathbb{P} with respect to it. Let λ\lambda be predictable with ∫0Tλs2 ds<∞\int_0^T \lambda_s^2 \, ds < \infty almost surely, let Z=E(−∫λ dW)Z = \mathcal{E}(-\int \lambda \, dW) be its stochastic exponential from Exponential martingales and measure changes, and assume that ZZ is a true martingale on [0,T][0, T], that is EP[ZT]=1\mathbb{E}^{\mathbb{P}}[Z_T] = 1, for example because the Novikov condition holds. Define Q\mathbb{Q} on FT\mathcal{F}_T by

dQdP∣FT=ZT.\left.\frac{d\mathbb{Q}}{d\mathbb{P}}\right|_{\mathcal{F}_T} = Z_T .

Girsanov’s theorem says that Q\mathbb{Q} is equivalent to P\mathbb{P} on FT\mathcal{F}_T and that the process

WtQ=Wt+∫0tλs dsW^{\mathbb{Q}}_t = W_t + \int_0^t \lambda_s \, ds

for 0≤t≤T0 \le t \le T is a standard Brownian motion under Q\mathbb{Q} with respect to the same filtration. The signs belong together. A density with −∫λ dW-\int \lambda \, dW in its exponent adds ∫λ ds\int \lambda \, ds to WW, while a density written as E(∫θ dW)\mathcal{E}(\int \theta \, dW) makes Wt−∫0tθs dsW_t - \int_0^t \theta_s \, ds the Q\mathbb{Q}-Brownian motion. In dd dimensions, with WW a dd-dimensional Brownian motion and λ\lambda predictable with values in Rd\mathbb{R}^d, the density exponent is −∫λ⊤dW−12∫∣λ∣2 ds-\int \lambda^{\top} dW - \tfrac12 \int \lvert \lambda \rvert^2 \, ds and W+∫λ dsW + \int \lambda \, ds is a dd-dimensional Q\mathbb{Q}-Brownian motion. The proof has the following structure. The added integral has finite variation, so [WQ]t=[W]t=t[W^{\mathbb{Q}}]_t = [W]_t = t, and because Q≪P\mathbb{Q} \ll \mathbb{P}, sums of squared increments that converge in P\mathbb{P}-probability converge in Q\mathbb{Q}-probability to the same limit. In the product rule for ZWQZ W^{\mathbb{Q}} the term Zt dWtQZ_t \, dW^{\mathbb{Q}}_t contains Ztλt dtZ_t \lambda_t \, dt, and the covariation d[Z,WQ]t=−Ztλt dtd[Z, W^{\mathbb{Q}}]_t = -Z_t \lambda_t \, dt cancels it, leaving

d(ZtWtQ)=Zt (1−λtWtQ) dWt.\begin{aligned} &d(Z_t W^{\mathbb{Q}}_t) \\[0.4em] &\quad = Z_t \, (1 - \lambda_t W^{\mathbb{Q}}_t) \, dW_t . \end{aligned}

So ZWQZ W^{\mathbb{Q}} is a P\mathbb{P}-local martingale, the conditional Bayes formula applied after localization makes WQW^{\mathbb{Q}} a continuous Q\mathbb{Q}-local martingale, and Lévy’s characterization identifies it as a Q\mathbb{Q}-Brownian motion. The localization details and the general semimartingale version of the theorem are further study.

In plain words Reweighting by the exponential density moves no path, but it makes paths that drift at the rate −λt-\lambda_t typical. Under the new weights the old Brownian motion WW has the drift −λt-\lambda_t, and WW plus its integrated tilt behaves exactly like a Brownian motion.

Example For the constant λ=0.25\lambda = 0.25 per square-root year and T=1T = 1, the previous lesson gives W1∼N(−0.25,1)W_1 \sim N(-0.25, 1) under Q\mathbb{Q}, so W1Q=W1+0.25W^{\mathbb{Q}}_1 = W_1 + 0.25 is N(0,1)N(0, 1), as the theorem requires. The density gives the same mean directly, since EP[W1eaW1]=aea2/2\mathbb{E}^{\mathbb{P}}[W_1 e^{a W_1}] = a e^{a^2/2} with a=−0.25a = -0.25 and

EQ[W1]=e−0.03125 (−0.25) e0.03125=−0.25.\begin{aligned} &\mathbb{E}^{\mathbb{Q}}[W_1] \\[0.4em] &\quad = e^{-0.03125} \, (-0.25) \, e^{0.03125} \\[0.4em] &\quad = -0.25 . \end{aligned}

The theorem says more than the terminal law. Under Q\mathbb{Q} the increments W0.5QW^{\mathbb{Q}}_{0.5} and W1Q−W0.5QW^{\mathbb{Q}}_1 - W^{\mathbb{Q}}_{0.5} are independent with variance 0.50.5 each, so for instance Cov⁡Q(W0.5Q,W1Q)=0.5\operatorname{Cov}^{\mathbb{Q}}(W^{\mathbb{Q}}_{0.5}, W^{\mathbb{Q}}_1) = 0.5.

Lévy’s characterization

Definition Lévy’s characterization, stated here without proof, says the following. Let MM be a continuous process adapted to (Ft)(\mathcal{F}_t) with M0=0M_0 = 0 that is a local martingale under a probability measure Q\mathbb{Q}, and suppose that [M]t=t[M]_t = t for 0≤t≤T0 \le t \le T. Then MM is a standard Brownian motion under Q\mathbb{Q} with respect to (Ft)(\mathcal{F}_t), so for s<ts < t the increment Mt−MsM_t - M_s is N(0,t−s)N(0, t - s) and independent of Fs\mathcal{F}_s. For a continuous local martingale the condition [M]t=t[M]_t = t is equivalent to Mt2−tM_t^2 - t being a local martingale. In dd dimensions the condition is [Mi,Mj]t=δij t[M^i, M^j]_t = \delta_{ij} \, t, where δij\delta_{ij} is 11 for i=ji = j and 00 otherwise. Each hypothesis matters. Quadratic variation is the same under equivalent measures, but the local martingale property depends on the measure, and the conclusion fails for processes with jumps.

In plain words A continuous martingale whose squared fluctuations accumulate at rate one per unit of time is automatically a Brownian motion. Normal increments and independence from the past follow without computing any distribution.

Example Let W1W^1 and W2W^2 be independent Brownian motions for the same filtration and measure, and set B=0.6 W1+0.8 W2B = 0.6 \, W^1 + 0.8 \, W^2. It is a continuous martingale with [B]t=(0.36+0.64) t=t[B]_t = (0.36 + 0.64) \, t = t, so BB is a Brownian motion, and [B,W1]t=0.6 t[B, W^1]_t = 0.6 \, t gives it correlation 0.60.6 with W1W^1. This is how correlated Brownian factors are built. Two other cases show the hypotheses at work. The compensated Poisson process Nt−tN_t - t with unit intensity has mean 00 and variance tt, and both Nt−tN_t - t and (Nt−t)2−t(N_t - t)^2 - t are martingales, but its paths jump, so it is not a Brownian motion. Under the Girsanov measure with a constant λ≠0\lambda \ne 0, the old process WW is continuous with [W]t=t[W]_t = t but is not a Q\mathbb{Q}-local martingale, since Wt=WtQ−λtW_t = W^{\mathbb{Q}}_t - \lambda t, so it is not a Q\mathbb{Q}-Brownian motion.

Measure equivalence

Definition Two probability measures on FT\mathcal{F}_T are equivalent when they have the same null events. The Girsanov measure is equivalent to P\mathbb{P} on FT\mathcal{F}_T, because its density ZTZ_T is an exponential and hence strictly positive, and its P\mathbb{P}-mean is 11 by hypothesis. Equivalence makes every almost sure statement the same under both measures. Paths remain continuous, and for an Itô process dXt=bt dt+σt dWtdX_t = b_t \, dt + \sigma_t \, dW_t the quadratic variation [X]T=∫0Tσt2 dt[X]_T = \int_0^T \sigma_t^2 \, dt, a limit in probability of sums of squared increments, is the same under both. A payoff that is nonnegative almost surely and positive with positive probability under P\mathbb{P} has the same two properties under Q\mathbb{Q}. This is why a pricing measure must be equivalent. If the discounted value of a self-financing strategy starts at 00 and is a Q\mathbb{Q}-martingale, its terminal value has Q\mathbb{Q}-mean 00, so it cannot be nonnegative almost surely and positive with positive probability, and the strategy is not an arbitrage. Distributions, drifts and expectations do change. Equivalence is also a finite horizon statement. For a constant λ≠0\lambda \ne 0 the strong law of large numbers gives Wt/t→0W_t/t \to 0 almost surely under P\mathbb{P}, while under any measure that makes Wt+λtW_t + \lambda t a Brownian motion for all t≥0t \ge 0 it gives Wt/t→−λW_t/t \to -\lambda almost surely, so no such measure on the whole infinite horizon is equivalent to P\mathbb{P}.

In plain words Equivalent measures agree on what can happen and on everything that a single path reveals, such as how rough it is and how much it varies. They differ only in how likely the possible outcomes are, which shows up in drifts, distributions and expectations.

Example With the constant λ=0.25\lambda = 0.25 and T=1T = 1, the event {W1>3}\{W_1 > 3\} has P\mathbb{P}-probability 1−Φ(3)≈0.001351 - \Phi(3) \approx 0.00135 and Q\mathbb{Q}-probability 1−Φ(3.25)≈0.000581 - \Phi(3.25) \approx 0.00058, two different numbers that are both positive. For a stock with dSt=μSt dt+0.2 St dWtdS_t = \mu S_t \, dt + 0.2 \, S_t \, dW_t, the quadratic variation of ln⁡S\ln S over one year is 0.22=0.040.2^2 = 0.04 under both measures, so no equivalent change of measure can turn a volatility of 0.20.2 into 0.30.3. In the degenerate case without noise, the path St=S0eμtS_t = S_0 e^{\mu t} is the same with probability one under every equivalent measure, so its drift cannot be changed at all.

Drift transformation

Definition Let the hypotheses of Girsanov’s theorem hold with the density exponent −∫λ dW-\int \lambda \, dW, and let XX be an Itô process with

dXt=bt dt+σt dWtdX_t = b_t \, dt + \sigma_t \, dW_t

under P\mathbb{P}, where bb and σ\sigma are adapted and measurable with ∫0T∣bt∣ dt<∞\int_0^T \lvert b_t \rvert \, dt < \infty and ∫0Tσt2 dt<∞\int_0^T \sigma_t^2 \, dt < \infty almost surely. Substituting dWt=dWtQ−λt dtdW_t = dW^{\mathbb{Q}}_t - \lambda_t \, dt gives

dXt=(bt−σtλt) dt+σt dWtQ.\begin{aligned} dX_t &= (b_t - \sigma_t \lambda_t) \, dt \\[0.4em] &\quad + \sigma_t \, dW^{\mathbb{Q}}_t . \end{aligned}

The drift changes by −σtλt-\sigma_t \lambda_t, while the diffusion coefficient and the quadratic variation stay the same. The new drift is integrable, since ∫0T∣σtλt∣ dt≤(∫0Tσt2 dt)1/2(∫0Tλt2 dt)1/2\int_0^T \lvert \sigma_t \lambda_t \rvert \, dt \le (\int_0^T \sigma_t^2 \, dt)^{1/2} (\int_0^T \lambda_t^2 \, dt)^{1/2} by the Cauchy-Schwarz inequality. With this construction a prescribed Q\mathbb{Q}-drift b~t\tilde b_t is reached only through a λ\lambda with σtλt=bt−b~t\sigma_t \lambda_t = b_t - \tilde b_t, which needs σt≠0\sigma_t \ne 0 wherever the two drifts differ, and that λ\lambda must still give a true martingale density. Writing a new drift into an equation does not by itself construct a measure.

In plain words Under the new measure the same noise is split differently into a predictable part and a fresh Brownian part. The volatility converts the tilt into a change of drift, so where there is no volatility there is nothing to tilt.

Example A constructed mean-reverting factor follows dXt=0.5 (0.04−Xt) dt+0.01 dWtdX_t = 0.5\,(0.04 - X_t) \, dt + 0.01 \, dW_t under P\mathbb{P}, with time in years. A constant λ=0.2\lambda = 0.2 per square-root year satisfies the Novikov condition, and σλ=0.01⋅0.2=0.002\sigma \lambda = 0.01 \cdot 0.2 = 0.002, so the drift becomes 0.5 (0.04−Xt)−0.002=0.5 (0.036−Xt)0.5\,(0.04 - X_t) - 0.002 = 0.5\,(0.036 - X_t) and

dXt=0.5 (0.036−Xt) dt+0.01 dWtQ.\begin{aligned} dX_t &= 0.5\,(0.036 - X_t) \, dt \\[0.4em] &\quad + 0.01 \, dW^{\mathbb{Q}}_t . \end{aligned}

The speed of mean reversion 0.50.5 per year and the volatility 0.010.01 per square-root year are unchanged, and only the long-run level moves from 0.040.04 to 0.0360.036.

Market price of risk

Definition Consider a dividend-free stock with dSt=μtSt dt+σtSt dWtdS_t = \mu_t S_t \, dt + \sigma_t S_t \, dW_t under P\mathbb{P}, where σt>0\sigma_t > 0, and a money-market account Bt=exp⁡(∫0trs ds)B_t = \exp(\int_0^t r_s \, ds) in a frictionless market. Under a Girsanov measure the discounted price satisfies

d(St/Bt)St/Bt=(μt−rt−σtλt) dt+σt dWtQ,\begin{aligned} &\frac{d(S_t/B_t)}{S_t/B_t} \\[0.4em] &\quad = (\mu_t - r_t - \sigma_t \lambda_t) \, dt \\[0.4em] &\qquad + \sigma_t \, dW^{\mathbb{Q}}_t , \end{aligned}

so it can be a Q\mathbb{Q}-local martingale only if its drift vanishes, which forces

λt=μt−rtσt.\lambda_t = \frac{\mu_t - r_t}{\sigma_t} .

This is the market price of risk of WW, the expected return in excess of the cash rate per unit of volatility, measured per square-root year. For nn dividend-free assets driven by a dd-dimensional Brownian motion, with dSti=Sti(μti dt+∑jΣtij dWtj)dS^i_t = S^i_t \bigl(\mu^i_t \, dt + \sum_j \Sigma^{ij}_t \, dW^j_t\bigr) and an n×dn \times d loading matrix Σt\Sigma_t whose rows are assets and whose columns are risk factors, the condition becomes

Σtλt=μt−rt1.\Sigma_t \lambda_t = \mu_t - r_t \mathbf{1} .

If it has no solution, no measure of this Girsanov form makes every discounted price a local martingale. With constant coefficients there is then a vector ww with w⊤Σ=0w^{\top} \Sigma = 0 and w⊤(μ−r1)>0w^{\top}(\mu - r \mathbf{1}) > 0, and holding the currency amounts ww in the assets, with the balance in cash, gives a riskless portfolio that grows faster than cash, an arbitrage. If it has several solutions, some directions of λ\lambda are not fixed by the traded assets. A solution must still give a true martingale density, and when the coefficients are random the discounted prices must also be checked to be true Q\mathbb{Q}-martingales.

In plain words The market price of risk is the extra expected return per unit of Brownian risk that the physical model pays above cash. The pricing measure removes exactly that compensation from the drift, and traded assets pin it down only for the risks they carry.

Example For the constructed stock with μ=0.08\mu = 0.08 and r=0.03r = 0.03 per year and σ=0.2\sigma = 0.2 per square-root year,

λ=0.08−0.030.2=0.25\lambda = \frac{0.08 - 0.03}{0.2} = 0.25

per square-root year, and the Q\mathbb{Q}-drift is 0.08−0.2⋅0.25=0.030.08 - 0.2 \cdot 0.25 = 0.03. With the physical drift 0.120.12 instead, λ=0.09/0.2=0.45\lambda = 0.09/0.2 = 0.45 and the Q\mathbb{Q}-drift is again 0.12−0.2⋅0.45=0.030.12 - 0.2 \cdot 0.45 = 0.03, because the physical forecast and the drift change move together. In a stochastic volatility model where the stock loads only on W1W^1 and its variance also loads on an independent W2W^2, the loading row of the stock is (σt,0)(\sigma_t, 0). The stock then fixes λt1=(μt−rt)/σt\lambda^1_t = (\mu_t - r_t)/\sigma_t and leaves λ2\lambda^2 free, subject to the density conditions.

Risk-neutral dynamics

Definition With the money-market account as numeraire, risk-neutral dynamics are the dynamics of a model under an equivalent measure Q\mathbb{Q} for which the discounted price of every traded asset is a Q\mathbb{Q}-martingale, or for an asset that pays dividends, its discounted gains with the dividends reinvested. For the dividend-free stock with σt>0\sigma_t > 0, Girsanov’s theorem with λt=(μt−rt)/σt\lambda_t = (\mu_t - r_t)/\sigma_t gives

dSt=rtSt dt+σtSt dWtQ,dS_t = r_t S_t \, dt + \sigma_t S_t \, dW^{\mathbb{Q}}_t ,

with the same volatility as under P\mathbb{P}. With constant rr and σ\sigma on [0,T][0, T],

ST=S0exp⁡((r−12σ2) T+σWTQ),\begin{aligned} S_T = S_0 \exp\bigl(&(r - \tfrac12 \sigma^2) \, T \\[0.4em] &+ \sigma W^{\mathbb{Q}}_T\bigr), \end{aligned}

and the discounted price e−rtSt=S0exp⁡(σWtQ−12σ2t)e^{-rt} S_t = S_0 \exp(\sigma W^{\mathbb{Q}}_t - \tfrac12 \sigma^2 t) is a true Q\mathbb{Q}-martingale. For a stock with a continuous dividend yield qq and ex-dividend P\mathbb{P}-drift μ\mu, the total return has drift μ+q\mu + q, the market price of risk is (μ+q−r)/σ(\mu + q - r)/\sigma, and the ex-dividend price has Q\mathbb{Q}-drift r−qr - q. The physical drift disappears from the Q\mathbb{Q}-dynamics, which is why it does not enter option prices in the complete constant-coefficient model of the next unit. That the Girsanov measure is the only equivalent martingale measure when the filtration is generated by WW rests on the martingale representation theorem, which is further study.

In plain words Under the pricing measure every traded asset grows on average at the cash rate, while each path keeps the volatility it had. The physical drift has been absorbed into the change of measure, and the risk-neutral dynamics describe prices, not forecasts.

Example For the constructed stock with S0=100S_0 = 100, μ=0.08\mu = 0.08, r=0.03r = 0.03, σ=0.2\sigma = 0.2 and T=1T = 1 year,

EQ[S1]=100 e0.03≈103.0455,e−0.03 EQ[S1]=100,\begin{gathered} \mathbb{E}^{\mathbb{Q}}[S_1] = 100 \, e^{0.03} \approx 103.0455, \\[0.4em] e^{-0.03} \, \mathbb{E}^{\mathbb{Q}}[S_1] = 100, \end{gathered}

while EP[S1]=100 e0.08≈108.3287\mathbb{E}^{\mathbb{P}}[S_1] = 100 \, e^{0.08} \approx 108.3287. The medians are 100 e0.01≈101.005100 \, e^{0.01} \approx 101.005 under Q\mathbb{Q} and 100 e0.06≈106.184100 \, e^{0.06} \approx 106.184 under P\mathbb{P}, and the probabilities of ending above 100100 are Q(S1>100)=Φ(0.05)≈0.5199\mathbb{Q}(S_1 > 100) = \Phi(0.05) \approx 0.5199 and P(S1>100)=Φ(0.3)≈0.6179\mathbb{P}(S_1 > 100) = \Phi(0.3) \approx 0.6179. The paths are the same under both measures. The number 0.51990.5199 is a pricing weight for the event, not a forecast of how often it happens.

Check yourself

  1. A constructed dividend-free stock has dSt=0.10 St dt+0.25 St dWtdS_t = 0.10 \, S_t \, dt + 0.25 \, S_t \, dW_t under P\mathbb{P}, with S0=50S_0 = 50 and a constant cash rate r=0.04r = 0.04, continuously compounded. Find the market price of risk, check that it gives a valid density on [0,2][0, 2], write the risk-neutral dynamics, and compute EQ[S2]\mathbb{E}^{\mathbb{Q}}[S_2], its discounted value and EP[S2]\mathbb{E}^{\mathbb{P}}[S_2].
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The market price of risk is

λ=0.10−0.040.25=0.24\lambda = \frac{0.10 - 0.04}{0.25} = 0.24

per square-root year. It is constant, so the Novikov expectation is the number e12⋅0.242⋅2=e0.0576≈1.0593e^{\frac12 \cdot 0.24^2 \cdot 2} = e^{0.0576} \approx 1.0593, which is finite, and the stochastic exponential defines Q\mathbb{Q} equivalent to P\mathbb{P} on F2\mathcal{F}_2. With WtQ=Wt+0.24 tW^{\mathbb{Q}}_t = W_t + 0.24 \, t the risk-neutral dynamics are dSt=0.04 St dt+0.25 St dWtQdS_t = 0.04 \, S_t \, dt + 0.25 \, S_t \, dW^{\mathbb{Q}}_t, with the same volatility 0.250.25. Then

EQ[S2]=50 e0.08≈54.1644,e−0.08 EQ[S2]=50,\begin{gathered} \mathbb{E}^{\mathbb{Q}}[S_2] = 50 \, e^{0.08} \approx 54.1644, \\[0.4em] e^{-0.08} \, \mathbb{E}^{\mathbb{Q}}[S_2] = 50, \end{gathered}

while EP[S2]=50 e0.2≈61.0701\mathbb{E}^{\mathbb{P}}[S_2] = 50 \, e^{0.2} \approx 61.0701.

  1. A classmate uses the stock of this lesson, with μ=0.08\mu = 0.08, r=0.03r = 0.03, σ=0.2\sigma = 0.2 and S0=100S_0 = 100, and the density exp⁡(0.25 W1−0.03125)\exp(0.25 \, W_1 - 0.03125) on [0,1][0, 1]. They then write dSt=0.03 St dt+0.2 St dWtQdS_t = 0.03 \, S_t \, dt + 0.2 \, S_t \, dW^{\mathbb{Q}}_t with WtQ=Wt+0.25 tW^{\mathbb{Q}}_t = W_t + 0.25 \, t. Find the error, the actual Q\mathbb{Q}-drift of the stock under this density, and the discounted Q\mathbb{Q}-expectation of S1S_1.
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The density is a valid exponential martingale, but its sign is the opposite of the course’s convention. Written as E(−∫θ dW)\mathcal{E}(-\int \theta \, dW) it has θ=−0.25\theta = -0.25, so Girsanov’s theorem makes Wt−0.25 tW_t - 0.25 \, t the Q\mathbb{Q}-Brownian motion, not Wt+0.25 tW_t + 0.25 \, t. Completing the square confirms that W1W_1 is N(0.25,1)N(0.25, 1) under this measure. Substituting dWt=dWtQ+0.25 dtdW_t = dW^{\mathbb{Q}}_t + 0.25 \, dt gives

dSt=(0.08+0.2⋅0.25) St dt+0.2 St dWtQ,\begin{aligned} dS_t &= (0.08 + 0.2 \cdot 0.25) \, S_t \, dt \\[0.4em] &\quad + 0.2 \, S_t \, dW^{\mathbb{Q}}_t , \end{aligned}

a drift of 0.130.13, and e−0.03 EQ[S1]=100 e0.10≈110.517e^{-0.03} \, \mathbb{E}^{\mathbb{Q}}[S_1] = 100 \, e^{0.10} \approx 110.517, not 100100. The discounted stock is not a Q\mathbb{Q}-martingale, so this measure is not risk-neutral. The density exp⁡(−0.25 W1−0.03125)\exp(-0.25 \, W_1 - 0.03125) gives the drift 0.030.03.

  1. Two dividend-free stocks are driven by the same Brownian motion, with dSt1=St1(0.08 dt+0.2 dWt)dS^1_t = S^1_t (0.08 \, dt + 0.2 \, dW_t) and dSt2=St2(0.11 dt+0.3 dWt)dS^2_t = S^2_t (0.11 \, dt + 0.3 \, dW_t), and the cash rate is r=0.03r = 0.03. Is there a market price of risk that makes both discounted prices local martingales under a Girsanov measure? If not, build a zero-cost portfolio that shows why, assuming frictionless continuous trading.
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The condition Σλ=μ−r1\Sigma \lambda = \mu - r \mathbf{1} has the single column Σ=(0.2,0.3)⊤\Sigma = (0.2, 0.3)^{\top}, so it needs 0.2λ=0.050.2 \lambda = 0.05 and 0.3λ=0.080.3 \lambda = 0.08. The first gives λ=0.25\lambda = 0.25 and the second λ≈0.2667\lambda \approx 0.2667, so there is no solution and no such measure. The vector w=(−150,100)w = (-150, 100) has w⊤Σ=−30+30=0w^{\top} \Sigma = -30 + 30 = 0 and w⊤(μ−r1)=−7.5+8=0.5w^{\top}(\mu - r \mathbf{1}) = -7.5 + 8 = 0.5. Hold −150-150 currency units in the first stock and 100100 in the second at all times, and keep the balance Vt+50V_t + 50 in cash, so the portfolio costs V0=0V_0 = 0. Its value changes by

dVt=−150 (0.08 dt+0.2 dWt)+100 (0.11 dt+0.3 dWt)+0.03 (Vt+50) dt=(0.03 Vt+0.5) dt,\begin{aligned} dV_t &= -150 \, (0.08 \, dt + 0.2 \, dW_t) \\[0.4em] &\quad + 100 \, (0.11 \, dt + 0.3 \, dW_t) \\[0.4em] &\quad + 0.03 \, (V_t + 50) \, dt \\[0.4em] &= (0.03 \, V_t + 0.5) \, dt , \end{aligned}

so Vt=0.50.03(e0.03t−1)V_t = \tfrac{0.5}{0.03}(e^{0.03 t} - 1), for example V1≈0.5076V_1 \approx 0.5076. The portfolio costs nothing and is worth a positive amount at every later date with probability one, which is an arbitrage. This matches the absence of a measure, since under any equivalent measure making both discounted prices martingales the discounted value of this portfolio would be a martingale starting at 00 with a positive terminal value.

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