Difference between revisions of "Wiener chaos decomposition"
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− | + | Let | |
+ | be a dense subspace of a separable Hilbert space H . | ||
+ | The triplet U \subset H \subset U ^ {*} | ||
+ | given by the injection $ i : U \rightarrow H $ | ||
+ | is obtained by identifying H | ||
+ | with its dual, taking the dual of i , | ||
+ | and endowing U ^ {*} , | ||
+ | the algebraic dual of U , | ||
+ | with the weak topology. For any real \lambda , | ||
+ | let \lambda H | ||
+ | be the Hilbert space obtained from H | ||
+ | by multiplying the norm on H | ||
+ | by \lambda . | ||
− | + | The dual of the symmetric k - | |
+ | fold tensor product S _ {k} ( U) | ||
+ | is the space \mathop{\rm Pol} _ {k} ( U) | ||
+ | of all homogeneous polynomials of degree k | ||
+ | on U . | ||
+ | The value of F _ {k} \in \mathop{\rm Pol} _ {k} ( U) | ||
+ | at u \in U | ||
+ | is $ F _ {k} ( u ) = \langle F _ {k} , u ^ {\otimes k } \rangle _ {k! } $. | ||
+ | Thus, for each k | ||
+ | there is a triplet | ||
− | + | $$ \tag{a1 } | |
+ | S _ {k} ( U) \subset \sqrt k! S _ {k} ( H) \subset \mathop{\rm Pol} _ {k} ( U) . | ||
+ | $$ | ||
+ | |||
+ | Taking the direct sum of the internal space $ S _ {k} ( U) $ | ||
+ | and the Hilbert sum of the central spaces there results a triplet | ||
+ | |||
+ | $$ \tag{a2 } | ||
+ | S( U) \subset \mathop{\rm Fock} ( H) \subset \mathop\widehat{ {\rm Pol}} ( U), | ||
+ | $$ | ||
called dressed Fock space. The middle term is the usual [[Fock space|Fock space]] | called dressed Fock space. The middle term is the usual [[Fock space|Fock space]] | ||
− | + | $$ \tag{a3 } | |
+ | \mathop{\rm Fock} ( H) = \oplus \sqrt k! S _ {k} ( H) . | ||
+ | $$ | ||
− | The external space is the space | + | The external space is the space \prod _ {k} \mathop{\rm Pol} _ {k} ( U) |
+ | of all formal power series on U . | ||
+ | The value F( u ) | ||
+ | at u \in U | ||
+ | of such an F \in \mathop\widehat{ {\rm Pol}} ( U) | ||
+ | is defined as $ \lim\limits _ \rightarrow \sum _ {k=} 1 ^ {N} F _ {k} ( u ) $, | ||
+ | if this limit exists. For example, for any $ F = \sum F _ {k} \in \mathop{\rm Fock} ( H) $ | ||
+ | one has | ||
− | + | $$ \tag{a4 } | |
+ | F( u ) = \langle F, e ^ {u} \rangle , | ||
+ | $$ | ||
− | where | + | where $ e ^ {u} = \sum ( k!) ^ {-} 1 u ^ {\otimes k } $. |
A probabilized vector space is a structure | A probabilized vector space is a structure | ||
− | + | $$ \tag{a5 } | |
+ | ( U \dots X \supset \Omega , {\mathsf P} ) | ||
+ | $$ | ||
− | where | + | where U |
+ | and X | ||
+ | are two spaces in duality and $ X = \mathop{\rm span} ( \Omega ) $ | ||
+ | is linearly generated by the subset \Omega | ||
+ | of X . | ||
+ | This subset is endowed with a Polish (or Suslin) topology such that any u \in U | ||
+ | defines a Borel function $ u( \omega ) = \langle u , \omega \rangle $ | ||
+ | on \Omega . | ||
+ | The space U | ||
+ | contains a countable subset separating the points of \Omega ( | ||
+ | so that the Borel \sigma - | ||
+ | field is generated by U ). | ||
+ | Finally, {\mathsf P} | ||
+ | is a probability measure on this \sigma - | ||
+ | field. | ||
− | Assume, moreover, that the space of cylindrical polynomials | + | Assume, moreover, that the space of cylindrical polynomials $ P( \Omega ) = \mathop{\rm span} ( u ( \omega ) ^ {k} : u \in U, k = 0, 1, 2 , . . . ) $ |
+ | is dense in L _ {2} ( \Omega ) . | ||
+ | Assume that the following bilinear form on U | ||
+ | is a scalar product: | ||
− | + | $$ \tag{a6 } | |
+ | b( u , v) = {\mathsf E} ( [ u ( \omega )- {\mathsf E} ( u ( \omega ))] | ||
+ | [ v( \omega ) - {\mathsf E} ( v( \omega ))]) , | ||
+ | $$ | ||
− | and let | + | and let H |
+ | be the completion of U . | ||
+ | For any $ k > 0 $, | ||
+ | let \pi _ {k} | ||
+ | denote the orthogonal projection of L _ {2} ( \Omega ) | ||
+ | with range $ \overline{ {P _ {<} k ( \Omega ) }}\; $, | ||
+ | the closure of $ \mathop{\rm span} ( u ( \omega ) ^ {j} : u \in U, j< k ) $. | ||
+ | Let KO _ {k} | ||
+ | be the orthogonal complement of $ \overline{ {P _ {<} k ( \Omega ) }}\; $ | ||
+ | in \overline{ {P _ \leq k ( \Omega ) }}\; . | ||
+ | This space is called the k - | ||
+ | th homogeneous chaos. The space L _ {2} ( \Omega ) | ||
+ | is the Hilbert direct sum of the KO _ {k} . | ||
+ | One says that L _ {2} ( \Omega ) | ||
+ | admits a decomposition in chaos if for any k | ||
+ | the following mapping is isometric: | ||
− | + | $$ | |
+ | \sqrt k! S _ {k} ( H) \supset S _ {k} ( U) \ni \ | ||
+ | Q \mapsto ^ { {I _ k} } Q - \pi _ {k} ( Q) \in \ | ||
+ | KO _ {k} \subset L _ {2} ( \Omega ) . | ||
+ | $$ | ||
− | The collection of these isometries for | + | The collection of these isometries for $ k = 0, 1 \dots $ |
+ | is an isometry I | ||
+ | whose inverse | ||
− | + | $$ \tag{a7 } | |
+ | L _ {2} ( \Omega ) \rightarrow ^ { {I ^ {-}} 1 } \mathop{\rm Fock} ( H) ,\ \ | ||
+ | f \rightarrow \widehat{f} , | ||
+ | $$ | ||
− | extended to distributions on | + | extended to distributions on \Omega , |
+ | is the starting point of distribution calculus on \Omega . | ||
+ | Because of (a4), \widehat{f} | ||
+ | is explicitly given by | ||
− | + | $$ \tag{a8 } | |
+ | \widehat{f} ( u ) = \langle \widehat{f} , e ^ {u} \rangle = {\mathsf E} [ f \epsilon ^ {u} ] , | ||
+ | $$ | ||
− | where | + | where $ \epsilon ^ {u} = I ^ {-} 1 ( e ^ {u} ) $. |
− | Decomposition in chaos was discovered by N. Wiener (in the case | + | Decomposition in chaos was discovered by N. Wiener (in the case \Omega |
+ | is Wiener space), [[#References|[a1]]]. Further contributions are due to Th.A. Dwyer and I. Segal ([[#References|[a2]]], [[#References|[a3]]]) and these have been important for constructive quantum field theory. K. Itô obtained a decomposition into chaos for Poisson probability spaces and interpreted I _ {k} ( f ) | ||
+ | as iterated stochastic integrals. For formula (a8), extended to distributions for Gaussian probability spaces, cf. [[#References|[a5]]], [[#References|[a6]]], [[#References|[a7]]], [[#References|[a9]]], [[#References|[a10]]]. There are links with Malliavin calculus, [[#References|[a8]]]. | ||
For more material cf. e.g. also [[#References|[a11]]], [[#References|[a12]]]; [[Wick product|Wick product]] and [[White noise analysis|White noise analysis]], and the references therein. | For more material cf. e.g. also [[#References|[a11]]], [[#References|[a12]]]; [[Wick product|Wick product]] and [[White noise analysis|White noise analysis]], and the references therein. |
Revision as of 08:29, 6 June 2020
Let U
be a dense subspace of a separable Hilbert space H .
The triplet U \subset H \subset U ^ {*}
given by the injection i : U \rightarrow H
is obtained by identifying H
with its dual, taking the dual of i ,
and endowing U ^ {*} ,
the algebraic dual of U ,
with the weak topology. For any real \lambda ,
let \lambda H
be the Hilbert space obtained from H
by multiplying the norm on H
by \lambda .
The dual of the symmetric k - fold tensor product S _ {k} ( U) is the space \mathop{\rm Pol} _ {k} ( U) of all homogeneous polynomials of degree k on U . The value of F _ {k} \in \mathop{\rm Pol} _ {k} ( U) at u \in U is F _ {k} ( u ) = \langle F _ {k} , u ^ {\otimes k } \rangle _ {k! } . Thus, for each k there is a triplet
\tag{a1 } S _ {k} ( U) \subset \sqrt k! S _ {k} ( H) \subset \mathop{\rm Pol} _ {k} ( U) .
Taking the direct sum of the internal space S _ {k} ( U) and the Hilbert sum of the central spaces there results a triplet
\tag{a2 } S( U) \subset \mathop{\rm Fock} ( H) \subset \mathop\widehat{ {\rm Pol}} ( U),
called dressed Fock space. The middle term is the usual Fock space
\tag{a3 } \mathop{\rm Fock} ( H) = \oplus \sqrt k! S _ {k} ( H) .
The external space is the space \prod _ {k} \mathop{\rm Pol} _ {k} ( U) of all formal power series on U . The value F( u ) at u \in U of such an F \in \mathop\widehat{ {\rm Pol}} ( U) is defined as \lim\limits _ \rightarrow \sum _ {k=} 1 ^ {N} F _ {k} ( u ) , if this limit exists. For example, for any F = \sum F _ {k} \in \mathop{\rm Fock} ( H) one has
\tag{a4 } F( u ) = \langle F, e ^ {u} \rangle ,
where e ^ {u} = \sum ( k!) ^ {-} 1 u ^ {\otimes k } .
A probabilized vector space is a structure
\tag{a5 } ( U \dots X \supset \Omega , {\mathsf P} )
where U and X are two spaces in duality and X = \mathop{\rm span} ( \Omega ) is linearly generated by the subset \Omega of X . This subset is endowed with a Polish (or Suslin) topology such that any u \in U defines a Borel function u( \omega ) = \langle u , \omega \rangle on \Omega . The space U contains a countable subset separating the points of \Omega ( so that the Borel \sigma - field is generated by U ). Finally, {\mathsf P} is a probability measure on this \sigma - field.
Assume, moreover, that the space of cylindrical polynomials P( \Omega ) = \mathop{\rm span} ( u ( \omega ) ^ {k} : u \in U, k = 0, 1, 2 , . . . ) is dense in L _ {2} ( \Omega ) . Assume that the following bilinear form on U is a scalar product:
\tag{a6 } b( u , v) = {\mathsf E} ( [ u ( \omega )- {\mathsf E} ( u ( \omega ))] [ v( \omega ) - {\mathsf E} ( v( \omega ))]) ,
and let H be the completion of U . For any k > 0 , let \pi _ {k} denote the orthogonal projection of L _ {2} ( \Omega ) with range \overline{ {P _ {<} k ( \Omega ) }}\; , the closure of \mathop{\rm span} ( u ( \omega ) ^ {j} : u \in U, j< k ) . Let KO _ {k} be the orthogonal complement of \overline{ {P _ {<} k ( \Omega ) }}\; in \overline{ {P _ \leq k ( \Omega ) }}\; . This space is called the k - th homogeneous chaos. The space L _ {2} ( \Omega ) is the Hilbert direct sum of the KO _ {k} . One says that L _ {2} ( \Omega ) admits a decomposition in chaos if for any k the following mapping is isometric:
\sqrt k! S _ {k} ( H) \supset S _ {k} ( U) \ni \ Q \mapsto ^ { {I _ k} } Q - \pi _ {k} ( Q) \in \ KO _ {k} \subset L _ {2} ( \Omega ) .
The collection of these isometries for k = 0, 1 \dots is an isometry I whose inverse
\tag{a7 } L _ {2} ( \Omega ) \rightarrow ^ { {I ^ {-}} 1 } \mathop{\rm Fock} ( H) ,\ \ f \rightarrow \widehat{f} ,
extended to distributions on \Omega , is the starting point of distribution calculus on \Omega . Because of (a4), \widehat{f} is explicitly given by
\tag{a8 } \widehat{f} ( u ) = \langle \widehat{f} , e ^ {u} \rangle = {\mathsf E} [ f \epsilon ^ {u} ] ,
where \epsilon ^ {u} = I ^ {-} 1 ( e ^ {u} ) .
Decomposition in chaos was discovered by N. Wiener (in the case \Omega is Wiener space), [a1]. Further contributions are due to Th.A. Dwyer and I. Segal ([a2], [a3]) and these have been important for constructive quantum field theory. K. Itô obtained a decomposition into chaos for Poisson probability spaces and interpreted I _ {k} ( f ) as iterated stochastic integrals. For formula (a8), extended to distributions for Gaussian probability spaces, cf. [a5], [a6], [a7], [a9], [a10]. There are links with Malliavin calculus, [a8].
For more material cf. e.g. also [a11], [a12]; Wick product and White noise analysis, and the references therein.
References
[a1] | N. Wiener, "The homogeneous chaos" Amer. J. Math. , 60 (1938) pp. 897–936 |
[a2] | Th.A., III Dwyer, "Partial differential equations in Fischer–Fock spaces for the Hilbert–Schmidt holomorphy type" Bull. Amer. Math. Soc. , 77 (1971) pp. 725–730 |
[a3] | I. Segal, "Tensor algebras over Hilbert spaces, I" Trans. Amer. Math. Soc. , 81 (1956) pp. 106–134 |
[a4] | K. Itô, "Multiple Wiener integral" J. Math. Soc. Japan (1951) pp. 157–169 |
[a5] | P. Krée, "Solutions faibles d'equations aux dérivées fonctionelles II" , Sem. P. Lelong 1973/1974 , Lect. notes in math. , 474 , Springer (1974) pp. 16–47 |
[a6] | P. Krée, R. Raczka, "Kernels and symbols of operators in quantum field theory" Ann. Inst. H. Poincaré (1978) |
[a7] | B. Lascar, "Propriétés locales des espaces de type Sobolev en dimension infinie" Comm. Partial Diff. Eq. , 1 : 6 (1976) pp. 561–584 |
[a8] | D. Ocone, "Malliavin calculus and stochastic integral representation of functionals of diffusion processes" Stochastics , 12 (1984) pp. 161–185 |
[a9] | M. Krée, "Propriété de trace en dimension infinie d'espaces du type Sobolev" C.R Acad. Sci. Paris , 279 (1974) pp. 157–160 |
[a10] | M. Krée, "Propriété de trace en dimension infinie d'espaces de type Sobolev" Bull. Soc. Math. de France , 105 (1977) pp. 141–163 |
[a11] | G. Kallianpur, "The role of reproducing kernel Hilbert spaces in the study of Gaussian processes" P. Ney (ed.) , Advances in probability and related topics , 2 , M. Dekker (1970) pp. 49–84 |
[a12] | J. Neveu, "Processus aléatoires Gaussiens" , Univ. Montréal (1968) |
Wiener chaos decomposition. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Wiener_chaos_decomposition&oldid=14192