Cylinder set measure

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In mathematics, cylinder set measure (sometimes abbreviated as CSM) is a kind of prototype for a measure on an infinite-dimensional vector space. An example is the Gaussian cylinder set measure on Hilbert space. Cylinder set measures are in general not measures (and in particular need not be countably additive), but can be used to define measures, such as classical Wiener measure on the set of continuous paths starting at the origin in Euclidean space.

1 Definition
2 Remarks
3 Cylinder set measures versus true measures
4 Cylinder set measures on Hilbert spaces
5 Nuclear spaces and cylinder set measures
6 References

[edit] Definition

Let $E$ be a separable real topological vector space. Let $\mathcal{A} (E)$ denote the collection of all continuous linear maps $T$ defined on $E$ whose image is some finite-dimensional real vector space $F T$ :

$\mathcal{A} (E) := \{ T \in \mathrm{Lin} (E; F_{T}) | T \mbox{ surjective and } \dim_{\mathbb{R}} F_{T} < + \infty \}.$

A cylinder set measure on $E$ is a collection of probability measures

$\{ \mu_{T} | T \in \mathcal{A} (E) \}.$

where $μ T$ is a probability measure on $F T$ . These measures are required to satisfy the following consistency condition: if $\pi_{ST} : F_{S} \to F_{T}$ is a surjective projection, then the measures push forward as follows:

$\mu_{T} = \left( \pi_{ST} \right)_{*} (\mu_{S}).$

[edit] Remarks

The consistency condition $\mu_{T} = \left( \pi_{ST} \right)_{*} (\mu_{S})$ is modelled on the way that true measures push forward (see the section cylinder set measures versus true measures). However, it is important to understand that in the case of cylinder set measures, this is a requirement that is part of the definition, not a result.

A cylinder set measure can be intuitively understood as defining a finitely additive function on the cylinder sets of the topological vector space $E$ . The cylinder sets are the pre-images in $E$ of measurable sets in $F T$ : if $\mathcal{B}_{T}$ denotes the σ-algebra on $F T$ on which $μ T$ is defined, then

$\mathrm{Cyl} (E) := \{ T^{-1} (B) | B \in \mathcal{B}_{T}, T \in \mathcal{A} (E) \}.$

In practice, one often takes $\mathcal{B}_{T}$ to be the Borel algebra $\mathcal{B} (F_{T})$ . In this case, one can show that when $E$ is a separable Banach space, the σ-algebra generated by the cylinder sets is precisely the Borel σ-algebra of $E$ :

$\mathcal{B} (E) = \sigma \left( \mathrm{Cyl} (E) \right)$ .

[edit] Cylinder set measures versus true measures

A cylinder set measure on $E$ is not actually a measure on $E$ : it is a collection of measures defined on all finite-dimensional images of $E$ . If $E$ has a probability measure $μ$ already defined on it, then $μ$ gives rise to a cylinder set measure on $E$ using the push forward: set $μ T : = T * (μ)$ on $F T$ .

When there is a measure $μ$ on $E$ such that $μ T : = T * (μ)$ in this way, we abuse notation slightly and say that the cylinder set measure $\{ \mu_{T} | T \in \mathcal{A} (E) \}$ "is" the measure $μ$ .

[edit] Cylinder set measures on Hilbert spaces

When the Banach space $E$ is actually a Hilbert space $H$ , there is a canonical Gaussian cylinder set measure $γ H$ arising from the inner product structure on $H$ . Specifically, if $\langle - , - \rangle$ denotes the inner product on $H$ , let $\langle - , -\rangle_{T}$ denote the quotient inner product on $F T$ . The measure $\gamma_{T}^{H}$ on $F T$ is then defined to be the canonical Gaussian measure on $F T$ :

$\gamma_{T}^{H} := i_{*} \left( \gamma^{\dim F_{T}} \right),$

where $i : \mathbb{R}^{\dim F_{T}} \to F_{T}$ is an isometry taking the Euclidean inner product on $\mathbb{R}^{\dim F_{T}}$ to the inner product $\langle - , -\rangle_{T}$ on $F T$ , and $γ n$ is Gaussian measure on $\mathbb{R}^{n}$ .

The canonical Gaussian cylinder set measure on an infinite-dimensional separable Hilbert space $H$ does not correspond to a true measure on $H$ . The proof is quite simple: the ball of radius r (and center 0) has measure at most equal to that of the ball of radius r in an n-dimensional Hilbert space, and this tends to 0 as n tends to infinity. So the ball of radius r has measure 0; as the Hilbert space is a countable union of such balls it also has measure 0, which is a contradiction.

An alternative proof that the Gaussian cylinder set measure is not a measure uses the Cameron-Martin theorem and a result on the quasi-invariance of measures. If $γ H = γ$ really were a measure, then the identity function on $H$ would radonify that measure, thus making $\mathrm{id} : H \to H$ into an abstract Wiener space. By the Cameron-Martin theorem, $γ$ would then be quasi-invariant under translation by any element of $H$ , which implies that either $H$ is finite-dimensional or that $γ$ is the zero measure. In either case, we have a contradiction.

[edit] Nuclear spaces and cylinder set measures

A cylinder set measure on the dual of a nuclear Frechet space automatically extends to a measure.

Example: Let S be the space of Schwartz functions on a finite dimensional vector space; it is nuclear. It is contained in the Hilbert space H of L² functions, which is in turn contained in the space of tempered distributions S′, the dual of the nuclear Frechet space S:

$S \subseteq H \subseteq S'.$

The Gaussian cylinder set measure on H gives a cylinder set measure on the space of tempered distributions, which extends to a measure on the space of tempered distributions, S′.

The Hilbert space H has measure 0 in S′, by the first argument used above to show that the canonical Gaussian cylinder set measure on H does not extend to a measure on H.

[edit] References

I.M. Gel'fand, N.Ya. Vilenkin, Generalized functions. Applications of harmonic analysis , Vol 4 , Acad. Press (1968)
R.A. Minlos, "cylindrical measure" SpringerLink Encyclopaedia of Mathematics (2001)
R.A. Minlos, "cylinder set" SpringerLink Encyclopaedia of Mathematics (2001)
L. Schwartz, Radon measures.