Difference between revisions of "Wiener space, abstract"
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− | The [[Probability distribution|probability distribution]] of a [[Brownian motion|Brownian motion]] | + | <!-- |
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+ | The [[Probability distribution|probability distribution]] of a [[Brownian motion|Brownian motion]] $ \{ {B ( t ) } : {t \geq 0 } \} $ | ||
+ | is a Gaussian measure (cf. also [[Constructive quantum field theory|Constructive quantum field theory]]) that can be supported by the space $ C = C [ 0, \infty ) $ | ||
+ | of continuous functions. For this reason, $ C $ | ||
+ | is also called the classical Wiener space. This notion can be generalized to a [[Banach space|Banach space]] on which a Gaussian measure can be introduced. | ||
Advanced stochastic analysis can be carried out on a Wiener space. The analysis was initiated by P. Lévy and N. Wiener, and a systematic development was made by R.H. Cameron and W.T. Martin, I.E. Segal, L. Gross, K. Itô, and others. | Advanced stochastic analysis can be carried out on a Wiener space. The analysis was initiated by P. Lévy and N. Wiener, and a systematic development was made by R.H. Cameron and W.T. Martin, I.E. Segal, L. Gross, K. Itô, and others. | ||
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Following [[#References|[a2]]], one can introduce the notion of an abstract Wiener space, which is a generalization of the classical Wiener space. | Following [[#References|[a2]]], one can introduce the notion of an abstract Wiener space, which is a generalization of the classical Wiener space. | ||
− | Let | + | Let $ H $ |
+ | be a real separable [[Hilbert space|Hilbert space]] with norm $ \| \cdot \| $. | ||
+ | On $ H $ | ||
+ | one introduces the weak Gaussian distribution $ \nu $ | ||
+ | in such a way that on any finite-, say $ n $-, | ||
+ | dimensional subspace $ K $ | ||
+ | of $ H $ | ||
+ | the restriction of $ \nu $ | ||
+ | to $ K $ | ||
+ | is the $ n $- | ||
+ | dimensional standard Gaussian distribution. In fact, $ \nu $ | ||
+ | may be called the weak white noise measure. A semi-norm (or norm) $ \| \cdot \| _ {1} $ | ||
+ | on $ H $ | ||
+ | is called a measurable norm if for any positive $ \epsilon $ | ||
+ | there exists a finite-dimensional projection operator $ P _ {0} $ | ||
+ | such that for any finite-dimensional projection operator $ P $ | ||
+ | orthogonal to $ P _ {0} $ | ||
+ | the inequality $ \nu \{ x : {\| {Px } \| _ {1} > \epsilon } \} < \epsilon $ | ||
+ | holds. | ||
− | Now, let | + | Now, let $ \| x \| _ {1} $ |
+ | be a measurable norm on $ H $ | ||
+ | and let $ B $ | ||
+ | be the completion of $ H $ | ||
+ | with respect to this norm (cf. [[Complete space|Complete space]]). Then $ B $ | ||
+ | is a Banach space. Let $ {\mathcal R} $ | ||
+ | be the $ \sigma $- | ||
+ | ring generated by the cylinder subsets of $ B $( | ||
+ | cf. [[Cylinder set|Cylinder set]]). For a cylinder set measure $ \mu $ | ||
+ | on $ {\mathcal R} $ | ||
+ | induced by the Gaussian distribution on $ H $, | ||
+ | the measure $ \mu $ | ||
+ | is countably additive on $ {\mathcal R} $. | ||
+ | Therefore, taking the $ \sigma $- | ||
+ | field $ {\mathcal B} $ | ||
+ | generated by $ {\mathcal R} $, | ||
+ | a [[Measure space|measure space]] $ ( H, {\mathcal B}, \mu ) $ | ||
+ | is obtained. | ||
− | The classical definition of an abstract Wiener space is given as follows. First, take a Hilbert space | + | The classical definition of an abstract Wiener space is given as follows. First, take a Hilbert space $ H $ |
+ | with norm $ \| \cdot \| $ | ||
+ | and take a measurable norm $ \| \cdot \| _ {1} $, | ||
+ | to obtain a Banach space $ B $. | ||
+ | The injection mapping from $ H $ | ||
+ | into $ B $ | ||
+ | is denoted by $ i $. | ||
+ | Then the triple $ ( i,H,B ) $ | ||
+ | is called an abstract Wiener space. This means that a weak measure on $ H $ | ||
+ | can be extended to a completely additive measure supported by $ B $. | ||
+ | A stochastic analysis can be developed for this latter measure (see [[#References|[a4]]]). | ||
− | One of the developments of the notion of an abstract Wiener space is that of a [[Rigged Hilbert space|rigged Hilbert space]], due to I.M. Gel'fand and N.Ya. Vilenkin (see [[#References|[a1]]]). Let | + | One of the developments of the notion of an abstract Wiener space is that of a [[Rigged Hilbert space|rigged Hilbert space]], due to I.M. Gel'fand and N.Ya. Vilenkin (see [[#References|[a1]]]). Let $ H $ |
+ | be a real Hilbert space and let $ \Phi $ | ||
+ | be a countably Hilbert [[Nuclear space|nuclear space]] that is continuously imbedded in $ H $. | ||
+ | The dual space $ \Phi ^ {*} $ | ||
+ | of $ \Phi $ | ||
+ | gives rise to the rigged Hilbert space | ||
− | + | $$ | |
+ | \Phi \subset H \subset \Phi ^ {*} . | ||
+ | $$ | ||
− | Given a characteristic functional | + | Given a characteristic functional $ C ( \xi ) $, |
+ | $ \xi \in \Phi $, | ||
+ | that is, $ C ( \xi ) $ | ||
+ | is continuous in $ \xi $, | ||
+ | positive definite and $ C ( 0 ) = 1 $, | ||
+ | there exists a countably additive probability measure $ \mu $ | ||
+ | in $ \Phi ^ {*} $ | ||
+ | such that | ||
− | + | $$ | |
+ | C ( \xi ) = \int\limits _ {\Phi ^ {*} } { { \mathop{\rm exp} } [ i \left \langle {x, \xi } \right \rangle ] } {d \mu ( x ) } . | ||
+ | $$ | ||
− | A typical example of a rigged Hilbert space is the triple consisting of the Hilbert space | + | A typical example of a rigged Hilbert space is the triple consisting of the Hilbert space $ L _ {2} ( \mathbf R ) $, |
+ | the Schwartz space $ S $ | ||
+ | and the space $ S ^ {*} $ | ||
+ | of tempered distributions (cf. [[Generalized function|Generalized function]]). [[White noise|White noise]] is also an important example of $ \mu $ | ||
+ | on $ S ^ {*} $; | ||
+ | it has characteristic functional $ C ( \xi ) = { \mathop{\rm exp} } [ - { {\| \xi \| ^ {2} } / 2 } ] $. | ||
+ | The analysis on the function space with the white noise measure is well developed (see [[#References|[a3]]]). | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> I.M. Gel'fand, N.Ya. Vilenkin, "Generalized functions 4: applications of harmonic analysis" , Acad. Press (1964) (In Russian)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> L. Gross, "Abstract Wiener spaces" , ''Proc. 5th Berkeley Symp. Math. Stat. Probab.'' , '''2''' (1965) pp. 31–42</TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> T. Hida, H.H. Kuo, J. Potthoff, L. Streit, "White noise. An infinite dimensional calculus" , Kluwer Acad. Publ. (1993)</TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> H.H. Kuo, "Gaussian measures in Banach spaces" , ''Lecture Notes in Mathematics'' , '''463''' , Springer (1975)</TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> I.M. Gel'fand, N.Ya. Vilenkin, "Generalized functions 4: applications of harmonic analysis" , Acad. Press (1964) (In Russian)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> L. Gross, "Abstract Wiener spaces" , ''Proc. 5th Berkeley Symp. Math. Stat. Probab.'' , '''2''' (1965) pp. 31–42</TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> T. Hida, H.H. Kuo, J. Potthoff, L. Streit, "White noise. An infinite dimensional calculus" , Kluwer Acad. Publ. (1993)</TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> H.H. Kuo, "Gaussian measures in Banach spaces" , ''Lecture Notes in Mathematics'' , '''463''' , Springer (1975)</TD></TR></table> |
Latest revision as of 08:29, 6 June 2020
The probability distribution of a Brownian motion $ \{ {B ( t ) } : {t \geq 0 } \} $
is a Gaussian measure (cf. also Constructive quantum field theory) that can be supported by the space $ C = C [ 0, \infty ) $
of continuous functions. For this reason, $ C $
is also called the classical Wiener space. This notion can be generalized to a Banach space on which a Gaussian measure can be introduced.
Advanced stochastic analysis can be carried out on a Wiener space. The analysis was initiated by P. Lévy and N. Wiener, and a systematic development was made by R.H. Cameron and W.T. Martin, I.E. Segal, L. Gross, K. Itô, and others.
Following [a2], one can introduce the notion of an abstract Wiener space, which is a generalization of the classical Wiener space.
Let $ H $ be a real separable Hilbert space with norm $ \| \cdot \| $. On $ H $ one introduces the weak Gaussian distribution $ \nu $ in such a way that on any finite-, say $ n $-, dimensional subspace $ K $ of $ H $ the restriction of $ \nu $ to $ K $ is the $ n $- dimensional standard Gaussian distribution. In fact, $ \nu $ may be called the weak white noise measure. A semi-norm (or norm) $ \| \cdot \| _ {1} $ on $ H $ is called a measurable norm if for any positive $ \epsilon $ there exists a finite-dimensional projection operator $ P _ {0} $ such that for any finite-dimensional projection operator $ P $ orthogonal to $ P _ {0} $ the inequality $ \nu \{ x : {\| {Px } \| _ {1} > \epsilon } \} < \epsilon $ holds.
Now, let $ \| x \| _ {1} $ be a measurable norm on $ H $ and let $ B $ be the completion of $ H $ with respect to this norm (cf. Complete space). Then $ B $ is a Banach space. Let $ {\mathcal R} $ be the $ \sigma $- ring generated by the cylinder subsets of $ B $( cf. Cylinder set). For a cylinder set measure $ \mu $ on $ {\mathcal R} $ induced by the Gaussian distribution on $ H $, the measure $ \mu $ is countably additive on $ {\mathcal R} $. Therefore, taking the $ \sigma $- field $ {\mathcal B} $ generated by $ {\mathcal R} $, a measure space $ ( H, {\mathcal B}, \mu ) $ is obtained.
The classical definition of an abstract Wiener space is given as follows. First, take a Hilbert space $ H $ with norm $ \| \cdot \| $ and take a measurable norm $ \| \cdot \| _ {1} $, to obtain a Banach space $ B $. The injection mapping from $ H $ into $ B $ is denoted by $ i $. Then the triple $ ( i,H,B ) $ is called an abstract Wiener space. This means that a weak measure on $ H $ can be extended to a completely additive measure supported by $ B $. A stochastic analysis can be developed for this latter measure (see [a4]).
One of the developments of the notion of an abstract Wiener space is that of a rigged Hilbert space, due to I.M. Gel'fand and N.Ya. Vilenkin (see [a1]). Let $ H $ be a real Hilbert space and let $ \Phi $ be a countably Hilbert nuclear space that is continuously imbedded in $ H $. The dual space $ \Phi ^ {*} $ of $ \Phi $ gives rise to the rigged Hilbert space
$$ \Phi \subset H \subset \Phi ^ {*} . $$
Given a characteristic functional $ C ( \xi ) $, $ \xi \in \Phi $, that is, $ C ( \xi ) $ is continuous in $ \xi $, positive definite and $ C ( 0 ) = 1 $, there exists a countably additive probability measure $ \mu $ in $ \Phi ^ {*} $ such that
$$ C ( \xi ) = \int\limits _ {\Phi ^ {*} } { { \mathop{\rm exp} } [ i \left \langle {x, \xi } \right \rangle ] } {d \mu ( x ) } . $$
A typical example of a rigged Hilbert space is the triple consisting of the Hilbert space $ L _ {2} ( \mathbf R ) $, the Schwartz space $ S $ and the space $ S ^ {*} $ of tempered distributions (cf. Generalized function). White noise is also an important example of $ \mu $ on $ S ^ {*} $; it has characteristic functional $ C ( \xi ) = { \mathop{\rm exp} } [ - { {\| \xi \| ^ {2} } / 2 } ] $. The analysis on the function space with the white noise measure is well developed (see [a3]).
References
[a1] | I.M. Gel'fand, N.Ya. Vilenkin, "Generalized functions 4: applications of harmonic analysis" , Acad. Press (1964) (In Russian) |
[a2] | L. Gross, "Abstract Wiener spaces" , Proc. 5th Berkeley Symp. Math. Stat. Probab. , 2 (1965) pp. 31–42 |
[a3] | T. Hida, H.H. Kuo, J. Potthoff, L. Streit, "White noise. An infinite dimensional calculus" , Kluwer Acad. Publ. (1993) |
[a4] | H.H. Kuo, "Gaussian measures in Banach spaces" , Lecture Notes in Mathematics , 463 , Springer (1975) |
Wiener space, abstract. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Wiener_space,_abstract&oldid=49223