Classical Wiener space In mathematics , classical Wiener space is the collection of all continuous functions on a given domain , taking values in a metric space . Classical Wiener space is useful in the study of stochastic processes whose sample paths are continuous functions. It is named after the American mathematician Norbert Wiener .Definition Consider E ⊆ R n and a metric space. The classical Wiener space C is the space of all continuous functions f : E → M . I.e. for every fixed t in E , In almost all applications, one takes E = or 0, +∞) and M = R n for some n in N . For brevity, write C for C ; this is a [vector space . Write C 0 for the linear subspace consisting only of those functions that take the value zero at the infimum of the set E . Many authors refer to C 0 as "classical Wiener space".Properties of classical Wiener space The vector space C can be equipped with the uniform norm turning it into a normed vector space . This norm induces a metric on C in the usual way:. The topology generated by the open sets in this metric is the topology of uniform convergence on , or the uniform topology . Thinking of the domain as "time" and the range R n as "space", an intuitive view of the uniform topology is that two functions are "close" if we can "wiggle space a bit" and get the graph of f to lie on top of the graph of g , while leaving time fixed. Contrast this with the Skorokhod topology , which allows us to "wiggle" both space and time .Separability and completeness With respect to the uniform metric , C is both a separable and a complete space: Since it is both separable and complete, C is a Polish space .Tightness in classical Wiener space Recall that the modulus of continuity for a function f : → R n is defined by This definition makes sense even if f is not continuous, and it can be shown that f is continuous if and only if its modulus of continuity tends to zero as δ → 0: By an application of the Arzelà-Ascoli theorem , one can show that a sequence of probability measures on classical Wiener space C is tight if and only if both the following conditions are met:There is a "standard" measure on C 0 , known as classical Wiener measure . Wiener measure has two equivalent characterizations: If one defines Brownian motion to be a Markov stochastic process B : × Ω → R n , starting at the origin, with almost surely continuous paths and independent increments then classical Wiener measure γ is the law of the process B . Alternatively, one may use the abstract Wiener space construction, in which classical Wiener measure γ is the radonification of the canonical Gaussian cylinder set measure on the Cameron-Martin Hilbert space corresponding to C 0 . Classical Wiener measure is a Gaussian measure: in particular, it is a strictly positive probability measure . Given classical Wiener measure γ on C 0 , the product measure γn × γ is a probability measure on C , where γn denotes the standard Gaussian measure on R n .
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