Skorokhod integral explained

In mathematics, the Skorokhod integral, also named Hitsuda–Skorokhod integral, often denoted

\delta

, is an operator of great importance in the theory of stochastic processes. It is named after the Ukrainian mathematician Anatoliy Skorokhod and Japanese mathematician Masuyuki Hitsuda. Part of its importance is that it unifies several concepts:

\delta

is an extension of the Itô integral to non-adapted processes;

\delta

is the adjoint of the Malliavin derivative, which is fundamental to the stochastic calculus of variations (Malliavin calculus);

\delta

is an infinite-dimensional generalization of the divergence operator from classical vector calculus.

The integral was introduced by Hitsuda in 1972[1] and by Skorokhod in 1975.[2]

Definition

Preliminaries: the Malliavin derivative

(\Omega,\Sigma,P)

and a Hilbert space

H

;

E

denotes expectation with respect to

P

\mathbf [X] := \int_\Omega X(\omega) \, \mathrm \mathbf(\omega).

Intuitively speaking, the Malliavin derivative of a random variable

F

in

Lp(\Omega)

is defined by expanding it in terms of Gaussian random variables that are parametrized by the elements of

H

and differentiating the expansion formally; the Skorokhod integral is the adjoint operation to the Malliavin derivative.

Consider a family of

R

-valued random variables

W(h)

, indexed by the elements

h

of the Hilbert space

H

. Assume further that each

W(h)

is a Gaussian (normal) random variable, that the map taking

h

to

W(h)

is a linear map, and that the mean and covariance structure is given by

\mathbf [W(h)] = 0,\mathbf [W(g) W(h)] = \langle g, h \rangle_H,

for all

g

and

h

in

H

. It can be shown that, given

H

, there always exists a probability space

(\Omega,\Sigma,P)

and a family of random variables with the above properties. The Malliavin derivative is essentially defined by formally setting the derivative of the random variable

W(h)

to be

h

, and then extending this definition to "smooth enough" random variables. For a random variable

F

of the form

F = f(W(h_1), \ldots, W(h_n)),

where

f:Rn\toR

is smooth, the Malliavin derivative is defined using the earlier "formal definition" and the chain rule:

\mathrm F := \sum_^n \frac (W(h_1), \ldots, W(h_n)) h_i.

In other words, whereas

F

was a real-valued random variable, its derivative

DF

is an

H

-valued random variable, an element of the space

Lp(\Omega;H)

. Of course, this procedure only defines

DF

for "smooth" random variables, but an approximation procedure can be employed to define

DF

for

F

in a large subspace of

Lp(\Omega)

; the domain of

D

is the closure of the smooth random variables in the seminorm :

\| F \|_ := \big(\mathbf[|F|^p] + \mathbf[\| \mathrm{D}F \|_H^p] \big)^.

This space is denoted by

D1,

and is called the Watanabe–Sobolev space.

The Skorokhod integral

For simplicity, consider now just the case

p=2

. The Skorokhod integral

\delta

is defined to be the

L2

-adjoint of the Malliavin derivative

D

. Just as

D

was not defined on the whole of

L2(\Omega)

,

\delta

is not defined on the whole of

L2(\Omega;H)

: the domain of

\delta

consists of those processes

u

in

L2(\Omega;H)

for which there exists a constant

C(u)

such that, for all

F

in

D1,

,

\big| \mathbf [\langle \mathrm{D} F, u \rangle_{H} ] \big| \leq C(u) \| F \|_.

The Skorokhod integral of a process

u

in

L2(\Omega;H)

is a real-valued random variable

\deltau

in

L2(\Omega)

; if

u

lies in the domain of

\delta

, then

\deltau

is defined by the relation that, for all

F\inD1,

,

\mathbf [F \, \delta u] = \mathbf [\langle \mathrm{D}F, u \rangle_{H} ].

Just as the Malliavin derivative

D

was first defined on simple, smooth random variables, the Skorokhod integral has a simple expression for "simple processes": if

u

is given by

u = \sum_^ F_ h_

with

Fj

smooth and

hj

in

H

, then

\delta u = \sum_^ \left(F_ W(h_) - \langle \mathrm F_, h_ \rangle_ \right).

Properties

u

in

D1,

that lies in the domain of

\delta

, \mathbf \big[(\delta u)^{2} \big] = \mathbf \int | u_t |^ dt + \mathbf \int D_s u_t\, D_t u_s\,ds\, dt. If

u

is an adapted process, then

Dsut=0

for

s>t

, so the second term on the right-hand side vanishes. The Skorokhod and Itô integrals coincide in that case, and the above equation becomes the Itô isometry.

DhX

stands for

(DX)(h)

, the random variable that is the value of the process

DX

at "time"

h

in

H

.

F

in

D1,

and a process

u

in

\operatorname{dom}(\delta)

is given by the formula \delta (F u) = F \, \delta u - \langle \mathrm F, u \rangle_.

Alternatives

An alternative to the Skorokhod integral is the Ogawa integral.

References

Notes and References

  1. Masuyuki. Hitsuda. Formula for Brownian partial derivatives. Second Japan-USSR Symp. Probab. Th.2.. 1972. 111–114.
  2. Kuo. Hui-Hsiung. 2014. The Itô calculus and white noise theory: a brief survey toward general stochastic integration. Communications on Stochastic Analysis. 8. 1. 10.31390/cosa.8.1.07. free.