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Strong Taylor Schemes for Stochastic Volatility

Introduction

Ito and Stratonovich Stochastic Calculus

Ito-Stratonovich drift conversion

Strong Numerical Schemes for SDE

Milstein scheme for commutative noise

Approximations of Volatility Models

General 2D Milstein scheme for stochastic volatility models

Approximations of the Double Integral

Subdivision (Kloeden - IC = 0)

Fourier Lévy formulae

Exact Fourier Lévy formulae

Real Variance formulae

Simulation of the Double Integral

Conclusions and Observations

Ornstein-Uhlenbeck Process

Formulae derivation for Heston Volatility

The fundamental solution

Derivation of the 2D Milstein Scheme

Numerical Data of the Double Integral

References

Books Related

Strong Taylor Schemes for Stochastic Volatility

Approximations of Volatility Models

We begin by writing down the usual Geometric Brownian Motion SDE where the volatility σ is written as the square root of a variance ν and is assumed to follow its own SDE:

(15)

where (r − D) is the deterministic instantaneous drift of stock price returns, κ is the mean-reverting speed, θ is the long-run mean, λ is the market price of risk function, ξ is the volatility of volatility, and dW1 and dW2 are two Wiener processes (Brownian motion) with correlation coefficient ρ. We use γ to generalize {15}. The six parameters κ, θ, λ, ξ, γ and ρ are assumed to be constant.

If one wishes to use a Monte Carlo scheme to calculate risk-neutral expectations, we need to find an approximation or discretization of {15}.

Euler and Milstein Scheme for 1D

Using the definition in {9} and {10}, the strong stochastic Taylor approximation of order 0.5 for the {SDE-15}, usually called the 1D Euler scheme (or simply Euler scheme), has the following form:

(16)

and the strong stochastic Taylor approximation of order 1.0 for the {SDE- 15}, called the 1D Milstein scheme, is:

(17)

where: {(∆W1,t)2 − ∆t} is called the Milstein correction.

Euler and Milstein Scheme for 2D

Using X1 = S, and X2 = ν, the {SDE-15} can be transformed to a vector with independent noise sources:

(18)

where:

The strong stochastic approximation of order 0.5 for the 2D vector {SDE- 18}, called 2D Euler scheme, remains the same as the Euler scheme for one dimension {SDE-16}. However, after some calculations shown in Appendix 2, the strong stochastic Taylor approximation of order 1.0 for the 2D vector {SDE-18}, called 2D Milstein scheme, is:

(19)

or for Heston model (γ = 1/2):

(20)

where:

(21)

The derivation of the {SDE-19} is explained in more detail in Appendix 2 and, in the next section, is explained how we can approximate the double integral {21}. Simulations, comparisons and conclusions are also given in the end of the chapter.

Prof. Klaus Schmitz

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