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Higher Moments of a Time-Varying Mean-Reverting Jump Diffusion

Article Quant Q&A · Author: Mark Viola

Summary

The document sets up a mean-reverting jump-diffusion with deterministic, time-varying mean-reversion, level, volatility, and jump-arrival parameters. It gives an integral representation of the process and derives expressions for its conditional mean and second moment using the independence of the Brownian and jump components.

It then asks how to extend direct expectation calculations to the third and fourth moments by evaluating products of stochastic integrals. The text provides no derivation or answer for those higher moments; it only points to the characteristic function as an alternative that the questioner does not want to use. Consequently, it is a useful framing of a stochastic-process calculation problem, but readers seeking formulas or a worked method will need another source. Its setup assumes independent driving processes and deterministic smooth coefficients, so conclusions drawn from a solution would depend on those modeling assumptions.

Key ideas

  • The process combines mean reversion, Brownian diffusion, and random jumps with time-varying parameters.
  • Its conditional mean includes the expected jump contribution weighted by the mean-reversion kernel.
  • The second moment is expressed as the squared mean plus integrated diffusion and jump variance contributions.
  • The document asks for direct third- and fourth-moment calculations but does not provide their solution.

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Full text
# How can one calculate third and fourth moments of a jump-diffusion process with time-varying parameters?


# How can one calculate third and fourth moments of a jump-diffusion process with time-varying parameters?












Suppose that $x_t$ is a random process that satisfies the mean-reversion jump-diffusion process governed by the stochastic differential equation

$$dx_t=\alpha(t)(\beta(t)-x_t)\,dt+\sigma(t)\,dW_t+J_t\,d\pi_t\tag1$$

where $\alpha$, $\beta$, and $\sigma$ are deterministic smooth functions of $t$, $J_t$ is a random process, $W_t$ is a Wiener process, and $\pi_t$ is a Poisson process with time-varying deterministic arrival frequency $h(t)$. It is assumed herein that $W_t$, $J_t$, and $\pi_t$ are independent random processes.

Solution to $(1)$ can be written

$$x_T=A(t,T)+\int_t^T e^{-\int_{t'}^T \alpha(t'')\,dt''}[\sigma(t')dW_{t'}+J_{t'}d\pi_{t'}] \tag2$$

where $A(t,T)=\beta(T)+e^{-\int_t^T\alpha(t')\,dt'}(x_t-\beta(t))-\int_t^T e^{\int_{t'}^T\alpha(t'')\,dt''}\beta'(t')\,dt'$ is purely determinisitic.

Now, suppose we wish to calculate the expected value, $\mathbb{E_t}\{x_T\}$, of $x_T$ as given by $(2)$. Inasmuch as $\mathbb{E_t}\{dW_t\}=0$ and $J_t$ and $\pi_t$ are independent, we find that

$$\begin{align} \mathbb{E_t}\{x_T\}&=A(t,T)+\int_t^T e^{-\int_{t'}^T \alpha(t'')\,dt''}\mathbb{E_t}\{\sigma(t')dW_{t'}+J_{t'}d\pi_{t'}\}\\\\ &=A(t,T)+\int_t^T e^{-\int_{t'}^T \alpha(t'')\,dt''} h(t')\mathbb{E_t}\{J_{t'}\}\,dt'\tag3 \end{align}$$

Similarly, we can evaluate the second moment, $\mathbb{E_t}\{x^2_T\}$, of $x_T$. Proceeding and exploiting the independence of the random processes along with knowledge of the mean and variance of both $dW_t$ and $d\pi_t$, we find that

$$\mathbb{E_t}\{x^2_T\}=\left(\mathbb{E_t}\{x_T\}\right)^2+\int_t^T e^{-2\int_{t'}^T \alpha(t'')}\left[\sigma^2(t')+h(t')\mathbb{E_t}\{J^2_{t'}\}\right]\,dt'$$

To evaluate higher order moments, one would need to evaluate the expectation of the stochastic multiple integrals given by

$$ \prod_{i=1}^N \int_t^T e^{-\int_{t_i}^T \alpha(\tau)\,d\tau}\left[\sigma(t_i)dW_{t_i}+J_{t_i}\,d\pi_{t_i}\right]\,dt_i\tag4$$

for $N>2$.

How can one evaluate $(4)$ for $N=3$ and $N=4$, respectively, by direct computation of the expectations?

I realize that one may use the characteristic function of the MRJD process to compute moments. Instead, I am asking how to take expectations of powers of $x_T$ directly using the stochastic multiple integrals.

Shown in full with attribution under the source's licence. Licence: CC BY-SA 4.0 (Stack Exchange)

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