[Math] How to solve this differential equation? (Steady State Solution of Forward Kolmogorov Equation)

partial differential equationsstochastic-calculus

Here's the full question and my attempt at answering it by solving the differential equation.

Consider the following SDE
$$
d\sigma = a(\sigma,t)dt + b(\sigma,t)dW
$$
The Forward Equation (FKE) is given by
$$
\frac{\partial p}{\partial t} = \frac{1}{2}\frac{\partial^2}{\partial\sigma^2}(b^2p) – \frac{\partial}{\partial\sigma}(ap)
$$

The steady state solution is given by setting $\frac{\partial p}{\partial t}=0$. Considering the boundary conditions that as $\sigma\rightarrow\infty$, $p\rightarrow 0$ and $\frac{\partial p}{\partial \sigma}\rightarrow 0$, show that the steady state solution is given by

$$
p(\sigma) = \frac{A}{b^2}e^{\int^\sigma\frac{2a}{b^2}d\sigma '}
$$

Essentially, this is a differential equation problem. Thing is, I'm stuck on how to solve it.

This is what I've got so far:

So, as per the question, the steady state solution is:
$$
\frac{1}{2}\frac{d^2}{d\sigma^2}(b^2p) – \frac{d}{d\sigma}(ap) = 0
$$

Integrating to convert to a first order differential equation?:

$$
\frac{1}{2}\frac{d}{d\sigma}(b^2p) – ap = A
$$

Given the boundary conditions in the question, $A = 0$??

$$
\frac{1}{2}\frac{d}{d\sigma}(b^2p) = ap
$$

Re-arranging we have a variable separable D.E

$$
\frac{1}{p} dp = \frac{2a}{b^2} d\sigma
$$

Integrating:

$$
\log p = \int \frac{2a}{b^2} d\sigma + D
$$

$$
p = e^{\int \frac{2a}{b^2} d\sigma + D}
$$

….and this is where I'm stuck. It looks a little like the expected solution but I don't know where the extra $\frac{A}{b^2}$ coefficient comes from and why there is a $d\sigma '$ in the expected solution.

Where have I gone wrong?

Best Answer

From $$\frac{1}{2} \frac{d}{d\sigma} (b^2 \cdot p) = a \cdot p$$ you concluded $$\frac{1}{p} \, dp = \frac{2a}{b^2} \, d\sigma$$

But this is not correct: Note that $b$ does depend on $\sigma$. You have to apply the chain rule:

$$\begin{align} \frac{1}{2} \frac{d}{d\sigma} (b^2 \cdot p) &= a \cdot p \\ \Rightarrow b \cdot \frac{d b}{d \sigma} \cdot p + \frac{1}{2} b^2 \cdot \frac{dp}{d \sigma} &= a \cdot p \\ \Rightarrow \frac{1}{p} \, dp &= 2 \frac{ \left(a- b \cdot \frac{db}{d\sigma}\right) }{b^2} \, d\sigma = \frac{2a}{b^2} \, d\sigma - 2 \frac{1}{b} \cdot \frac{db}{d\sigma} \, d\sigma \end{align}$$

From the second term on the righthand-side you obtain the factor $\frac{1}{b^2}$ in the given solution.

Concerning $d\sigma'$: Since $p=p(\sigma)$ you shouldn't use $\sigma$ as variable of integration at the same time. That's why they called it $\sigma'$ instead (has nothing to do with the derivative!).

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