Exchange Option - Pricing
What is an exchange option? How do you price it?
An exchange option is an option written on two assets \( S_{1} \& S_{2}\) with their difference \( S_{1} - S_{2} \) as payoff when \( S_{1} > S_{2} \). Put another way, the asset price \( S_{2} \) acts as the strike price for the option, and the option allows you to exchange \( S_{2} \) for \( S_{1} \) when it expires in the money, hence the name exchange option. Mathematically, the payoff function for exchange option can be written as
\[ V(S_{1,T}, S_{2,T}, T) = max(S_{1} - S_{2}, 0) \]
A more general form for the exchange option payoff where you exchange \( n_{2} \) units of \( S_{2} \) for \( n_{1} \) units of \( S_{1} \) would be
\[ V(S_{1,T}, S_{2,T}, T) = max(n_{1}S_{1,T} - n_{2}S_{2,T}, 0) \]
The corresponding PDE as can be derived using the equation for Multi-Asset options is
\[ \frac{\partial V}{\partial t} + (r - D_{1})S_{1,t}\frac{\partial V}{\partial S_{1,t}} + (r - D_{2})S_{2,t}\frac{\partial V}{\partial S_{2,t}} + \frac{1}{2}\sigma_{1}^2S_{1}^2\frac{\partial^2V}{\partial S_{1,t}^2} + \frac{1}{2}\sigma_{2}^2S_{2,t}^2\frac{\partial^2V}{\partial S_{2,t}^2} + \rho\sigma_{1}\sigma_{2}S_{1,t}S_{2,t}\frac{\partial^2V}{\partial S_{1,t}\partial S_{2,t}} - rV= 0 \]
This equation can be simplified by considering a similarity reduction for the option price \( V(S_{1,t}, S_{2,t}, t) \) as
\[ V(S_{1,t}, S_{2,t}, t) = n_{1}S_{2}H(\xi_{t}, t) \]
\[ \xi_{t} = \frac{S_{1,t}}{S_{2,t}} \]
The boundary condition for \( H(\xi, t) \) becomes
\[ H(\xi_{T}, T) = max(\xi_{T} - \frac{n_{2}}{n_{2}}, 0) \]
We can now substitute for \( V(S_{1,t}, S_{2,t}, t) \) in the equation after evaluating each of the partial derivatives
\[ \frac{\partial V}{\partial t} = \frac{\partial(n_{1}S_{2,t}H)}{\partial t} = n_{1}S_{2,t}\frac{\partial H}{\partial t} \]
\[ \frac{\partial V}{\partial S_{1,t}} = \frac{\partial(n_{1}S_{2,t}H)}{\partial S_{1,t}} = n_{1}S_{2,t}\frac{\partial H}{\partial S_{1,t}} \]
\[ \frac{\partial V}{\partial S_{2,t}} = \frac{\partial(n_{1}S_{2,t}H)}{\partial S_{2,t}} = n_{1}S_{2,t}\frac{\partial H}{\partial S_{2,t}} + n_{1}H \]
\[ \frac{\partial^2V}{\partial S_{1,t}^2} = \frac{\partial}{\partial S_{1,t}}(\frac{\partial V}{\partial S_{1,t}}) = \frac{\partial }{\partial S_{1,t}}(n_{1}S_{2,t}\frac{\partial H}{\partial S_{1,t}}) = n_{1}S_{2,t}\frac{\partial^2H}{\partial S_{1,t}^2} \]
\[ \frac{\partial^2V}{\partial S_{2,t}^2} = \frac{\partial}{\partial S_{2,t}}(\frac{\partial V}{\partial S_{2,t}}) = \frac{\partial }{\partial S_{2,t}}(n_{1}S_{2,t}\frac{\partial H}{\partial S_{2,t}} + n_{1}H) = n_{1}S_{2,t}\frac{\partial^2H}{\partial S_{2,t}^2} + 2n_{1}\frac{\partial H}{\partial S_{2,t}} \]
\[ \frac{\partial^2V}{\partial S_{1,t}\partial S_{2,t}} = \frac{\partial}{\partial S_{1,t}}(\frac{\partial V}{\partial S_{2,t}}) = \frac{\partial }{\partial S_{1,t}}(n_{1}S_{2,t}\frac{\partial H}{\partial S_{2,t}} + n_{1}H) = n_{1}S_{2,t}\frac{\partial^2H}{\partial S_{1,t}\partial S_{2,t}} + n_{1}\frac{\partial H}{\partial S_{1,t}} \]
Substituting for the derivatives in the equation and removing the common factor \( n_{1}S_{2,t} \), we get
\[ \frac{\partial H}{\partial t} + (r - D_{1})S_{1,t}\frac{\partial H}{\partial S_{1,t}} + (r - D_{2})S_{2,t}\frac{\partial H}{\partial S_{2,t}} + (r - D_{2})H + \frac{1}{2}\sigma_{1}^2S_{1,t}^2\frac{\partial^2H}{\partial S_{1,t}^2} + \frac{1}{2}\sigma_{2}^2S_{2,t}^2\frac{\partial^2H}{\partial S_{2,t}^2} + \sigma_{2}^2S_{2,t}\frac{\partial H}{\partial S_{2,t}} + \rho\sigma_{1}\sigma_{2}S_{1,t}S_{2,t}\frac{\partial^2H}{\partial S_{1,t}\partial S_{2,t}} + \rho\sigma_{1}\sigma_{2}S_{1,t}\frac{\partial H}{\partial S_{1,t}} - rH= 0 \]
\[ \frac{\partial H}{\partial t} + (r - D_{1} + \rho\sigma_{1}\sigma_{2})S_{1,t}\frac{\partial H}{\partial S_{1,t}} + (r - D_{2} + \sigma_{2}^2)S_{2,t}\frac{\partial H}{\partial S_{2,t}} + \frac{1}{2}\sigma_{1}^2S_{1,t}^2\frac{\partial^2H}{\partial S_{1,t}^2} + \frac{1}{2}\sigma_{2}^2S_{2,t}^2\frac{\partial^2H}{\partial S_{2,t}^2} + \rho\sigma_{1}\sigma_{2}S_{1,t}S_{2,t}\frac{\partial^2H}{\partial S_{1,t}\partial S_{2,t}} - D_{2}H= 0 \]
Moving from \( S_{1,t} \& S_{2,t} \) to \( \xi_{t} \)
\[ \frac{\partial H}{\partial S_{1,t}} = \frac{\partial \xi_{t}}{\partial S_{1,t}}\frac{\partial H}{\partial \xi_{t}} = \frac{1}{S_{2,t}}\frac{\partial H}{\partial \xi_{t}} \]
\[ \frac{\partial H}{\partial S_{2,t}} = \frac{\partial \xi_{t}}{\partial S_{2,t}}\frac{\partial H}{\partial \xi_{t}} = -\frac{\xi_{t}}{S_{2,t}}\frac{\partial H}{\partial \xi_{t}} \]
\[ \frac{\partial^2H}{\partial S_{1,t}^2} = \frac{\partial}{\partial S_{1,t}}(\frac{1}{S_{2,t}}\frac{\partial H}{\partial \xi_{t}}) = \frac{1}{S_{2,t}^2}\frac{\partial^2H}{\partial \xi_{t}^2} \]
\[ \frac{\partial^2H}{\partial S_{2,t}^2} = \frac{\partial}{\partial S_{2,t}}(-\frac{S_{1,t}}{S_{2,t}^2}\frac{\partial H}{\partial \xi_{t}}) = \frac{\xi_{t}^2}{S_{2,t}^2}\frac{\partial^2H}{\partial \xi_{t}^2} + \frac{2\xi_{t}}{S_{2,t}^2}\frac{\partial H}{\partial \xi_{t}} \]
\[ \frac{\partial^2H}{\partial S_{1,t}\partial S_{2,t}} = \frac{\partial}{\partial S_{2,t}}(\frac{1}{S_{2,t}}\frac{\partial H}{\partial \xi_{t}}) = -\frac{\xi_{t}}{S_{2,t}^2}\frac{\partial^2H}{\partial \xi_{t}^2} - \frac{1}{S_{2,t}^2}\frac{\partial H}{\partial \xi_{t}} \]
Substituting in the equation, we have
\[ \frac{\partial H}{\partial t} + (r - D_{1} + \rho\sigma_{1}\sigma_{2})\xi_{t}\frac{\partial H}{\partial \xi_{t}} - (r - D_{2} + \sigma_{2}^2)\xi_{t}\frac{\partial H}{\partial \xi_{t}} + \frac{1}{2}\sigma_{1}^2\xi_{t}^2\frac{\partial^2H}{\partial \xi_{t}^2} + \frac{1}{2}\sigma_{2}^2\xi_{t}^2\frac{\partial^2H}{\partial \xi_{t}^2} + \sigma_{2}^{2}\xi_{t}\frac{\partial H}{\partial \xi_{t}} - \rho\sigma_{1}\sigma_{2}\xi_{t}^2\frac{\partial^2H}{\partial \xi_{t}^2} -\rho\sigma_{2}\sigma_{2}\xi_{t}\frac{\partial H}{\partial \xi_{t}} - D_{2}H= 0 \]
\[ \implies \frac{\partial H}{\partial t} + (D_{2} - D_{1})\xi_{t}\frac{\partial H}{\partial \xi_{t}} + \frac{1}{2}(\sigma_{1}^2 + \sigma_{2}^2 - 2\rho\sigma_{1}\sigma_{2})\xi_{t}^2\frac{\partial^2H}{\partial \xi_{t}^2} - D_{2}H= 0 \]
This equation now has the same structure as the Black-Scholes PDE and the boundary conditions similar to a vanilla call option. So the price of the Exchange option would be
\[ V(S_{1,t}, S_{2,t}, t) = n_{1}S_{1,t}e^{-D_{1}(T-t)}\Phi(d_{1}) - n_{2}S_{2,t}e^{-D_{2}(T-t)}\Phi(d_{2}) \]
\[ d_{1} = \frac{ln\frac{n_{1}S_{1}}{n_{2}S_{2}} + (D_{2} - D_{1} + \frac{\sigma^2}{2})(T-t)}{\sigma\sqrt{T-t}} \& d_{2} = d_{1} - \sigma\sqrt{T-t} \]
\[ \sigma = \sqrt{\sigma_{1}^2 - 2\rho\sigma_{1}\sigma_{2} + \sigma_{2}^2} \]