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Variance gamma process

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Through Stochastic process, Diffusion and Skewness

There are several representations of the VG process that relate it to other processes. It can for example be written as a Brownian motion W(t) with drift θt subjected to a random time change which follows a gamma process Γ(t;1,ν) (equivalently one finds in literature the notation Γ(t;γ=1/ν,λ=1/ν)):

XVG(t;σ,ν,θ):=θΓ(t;1,ν)+σW(Γ(t;1,ν)).

An alternative way of stating this is that the variance gamma process is a Brownian motion subordinated to a gamma subordinator.

Since the VG process is of finite variation it can be written as the difference of two independent gamma processes:

XVG(t;σ,ν,θ):=Γ(t;μp,μp2ν)−Γ(t;μq,μq2ν)

where

μp:=12θ2+2σ2ν+θ2andμq:=12θ2+2σ2ν−θ2.

Alternatively it can be approximated by a compound Poisson process that leads to a representation with explicitly given (independent) jumps and their locations. This last characterization gives an understanding of the structure of the sample path with location and sizes of jumps.

On the early history of the variance-gamma process see Seneta (2000).

Moments

The mean of a variance gamma process is independent of σ and ν and is given by

E⁡[X(t)]=θt

The variance is given as

Var⁡[X(t)]=(θ2ν+σ2)t

The 3rd central moment is

E⁡[(X(t)−E⁡[X(t)])3]=(2θ3ν2+3σ2θν)t

The 4th central moment is

E⁡[(X(t)−E⁡[X(t)])4]=(3σ4ν+12σ2θ2ν2+6θ4ν3)t+(3σ4+6σ2θ2ν+3θ4ν2)t2

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