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Option Hedging with a Stochastic Portfolio Diffusion

Article Quant Q&A · Author: Étienne Bézout

Summary

The document explores how a Black–Scholes-style option equation changes when the hedged portfolio is assumed to have its own stochastic diffusion. Starting with geometric Brownian motion for the underlying, it applies Itô’s lemma to the option value and matches the resulting portfolio dynamics to an assumed drift and volatility. This produces an implicit equation for the hedge ratio. When the added portfolio volatility depends only on time, the author derives an explicit hedge and a modified pricing equation.

For volatility that also depends on portfolio value, the proposed approach requires inverting a nonlinear function of that value. The example of a quadratic mapping illustrates that inversion may fail to be unique, leaving the hedge and resulting equation ambiguous under the stated setup. The document poses this as an open question rather than establishing a general pricing result. Its derivation relies on the chosen diffusion assumptions and does not address whether the setup is economically consistent or arbitrage-free.

Key ideas

  • Applying Itô’s lemma yields portfolio dynamics that can be matched against an assumed stochastic portfolio process.
  • A time-only portfolio volatility permits an explicit hedge ratio in the proposed setup.
  • Value-dependent portfolio volatility requires solving an implicit relation for the hedge.
  • If that relation is not invertible, the hedge may not be uniquely determined.
  • The document leaves the general pricing equation unresolved.

Tags

Full text
# Black and Scholes equation for portfolio **with** arbitrage


# Black and Scholes equation for portfolio **with** arbitrage












I am well aware of how the ordinary Black and Scholes equation is derived, under the assumption of an arbitrage free portfolio, $V=G-hS$. Here $S$ is the price of the underlying and $G$ is the option price. Suppose now that the portfolio is stochastic, and follows the process $$(1): dV=rVdt+f(V,t)VdW,$$ where $r$ is a constant parameter. The change of the portfolio also satisfies $dV=dG-h \cdot dS$. In the standard Black and Scholes, we have $h = \partial G/\partial S$. Assuming that the underlying follows a GBM, we have $$dS = \mu S dt + \sigma SdW,$$ where $\mu$ and $\sigma$ are constant parameters. Itô's lemma then provides $$dG = \left(\frac{\partial G}{\partial t}+\mu S\frac{\partial G}{\partial S}+\frac{1}{2}\sigma^2S^2\frac{\partial G^2}{\partial S^2} \right)dt + \sigma S\frac{\partial G}{\partial S}dW,$$ so that $$(2): dV=dG-hdS = \left(\frac{\partial G}{\partial t}+\mu S\left(\frac{\partial G}{\partial S}-h\right)+\frac{1}{2}\sigma^2S^2\frac{\partial G^2}{\partial S^2} \right)dt + \sigma S\left(\frac{\partial G}{\partial S}-h\right)dW $$

Matching 1) and 2), we see that we must have the following implicit relation for $h$ $$(3): f(G-hS,t)(G-hS)=\sigma S \left(\frac{\partial G}{\partial S}-h\right). $$ In the standard Black and Scholes we would have $f=0$, thus recovering $h = \frac{\partial G}{\partial S}$. If $f$ only depends on its second argument ($t$), then 3) can also easily be solved for $h$, yielding $$(5):h =\frac{Gf(t)-\sigma S \frac{\partial G}{\partial S}}{S(f(t)-\sigma)}, \ f \ \mathrm{independent \ of} \ V$$

Combining 1) and 2) would then give the Black and Scholes like equation $$(6):\frac{\partial G}{\partial t}+\mu S\frac{\partial G}{\partial S}+\frac{1}{2}\sigma^2S^2\frac{\partial G^2}{\partial S^2}+(r-\mu)\frac{Gf(t)-\sigma S \frac{\partial G}{\partial S}}{f(t)-\sigma}-rG=0, \ f \ \mathrm{independent \ of} \ V $$

EDIT

The above model is considered in the following paper by Contreras et al.. They write the stochastic portfolio 1) as $$(1'): dV=rVdt+f(t,S(t))VdW. $$ Then $h$ can again be determine as in equation 5), yielding the Black and Scholes like equation 6). See section 2 of the cited paper.

However, I would like to know what could we do if $f$ is not independent of $V$, i.e. if we retain the formulation in 1).

EDIT

I edit the question to clarify what I mean. Suppose we retain the dependence of $V$ in $f$. With $V=G-hS$, we can write equation 3) as $$(7):f(V,t)-\sigma V = \sigma S \frac{\partial G}{\partial S} - \sigma G.$$ Suppose the function $V \mapsto f(V,t)V-\sigma V$ is invertible for each $t$ and $\sigma$, and call the inverse $\phi$, so that $\phi(x,t) = (V \mapsto f(V,t)V-\sigma V)^{-1}(x)$. We can then solve for $h$ to get $$(8):h=\frac{G-\phi(\sigma S \frac{\partial G}{\partial S} - \sigma G,t)}{S},$$ from which we get the modified Black and Scholes equation $$(9): \frac{\partial G}{\partial t}+\mu S\frac{\partial G}{\partial S}+\frac{1}{2}\sigma^2S^2\frac{\partial G^2}{\partial S^2}+(r-\mu)\left[G-\phi(\sigma S \frac{\partial G}{\partial S} - \sigma G,t) \right]-rG=0.$$ If $f$ is independent of $V$ then $\phi(x,t) = x/(f(t)-\sigma)$, so we recover the previous equation 6).

However, for a general function $f$ the map $V \mapsto f(V,t)V-\sigma V$ is not invertible. Consider, for example, $f(V,t)=V$, for which $V \mapsto f(V,t)V-\sigma V = V^2 - \sigma V$ is not invertible. Then we cannot uniquely determine $h$. Can we say anything about the equation for $G$ in this case?

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This summary was written by Stratmill's research agent from the original; it is not a copy of the source.