Lévy's stochastic area

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In probability theory, Lévy's stochastic area is a stochastic process that describes the enclosed area of a trajectory of a two-dimensional Brownian motion and its chord. The process was introduced by Paul Lévy in 1940,[1] and in 1950[2] he computed the characteristic function and conditional characteristic function.

The process has many unexpected connections to other objects in mathematics such as the soliton solutions of the Korteweg–De Vries equation[3] and the Riemann zeta function.[4] In the Malliavin calculus, the process can be used to construct a process that is smooth in the sense of Malliavin but that has no continuous modification with respect to the Banach norm.[5]

Lévy's stochastic area

Let W=(Ws(1),Ws(2))s0 be a two-dimensional Brownian motion in 2 then Lévy's stochastic area is the process

S(t,W)=120t(Ws(1)dWs(2)Ws(2)dWs(1)),

where the Itō integral is used.[2]

Define the 1-Form ϑ=12(x1dx2x2dx1) then S(t,W) is the stochastic integral of ϑ along the curve φ:[0,t]2,s(Ws(1),Ws(2))

S(t,W)=W[0,t]ϑ.[6]

Area formula

Let x=(x1,x2)2, a, b=at/2 and St=S(t,W) then Lévy computed

𝔼[exp(iaSt)]=1cosh(b)

and

𝔼[exp(iaSt)Wt=x]=bsinh(b)exp(x22t(1bcoth(b))),

where x2 is the Euclidean norm.[2]Template:Rp

Further topics

  • In 1980 Yor found a short probabilistic proof.[7]
  • In 1983 Helmes and Schwane found a higher-dimensional formula.[8]

References