In mathematics, classical Wiener space is the collection of all continuous functions on a given domain (usually a subinterval of the real line), taking values in a metric space (usually n-dimensional Euclidean 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.
Consider E ⊆ Rn and a metric space (M, d). The classical Wiener space C(E; M) is the space of all continuous functions f : E → M. I.e. for every fixed t in E,
d(f(s),f(t))\to0
|s-t|\to0.
In almost all applications, one takes E = [0, ''T'' ] or [0, +∞) and ''M'' = '''R'''<sup>''n''</sup> for some ''n'' in '''N'''. For brevity, write ''C'' for ''C''([0, ''T'' ]; Rn); this is a vector space. Write C0 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 C0 as "classical Wiener space".
For a stochastic process
\{Xt,t\inT\}:(\Omega,l{F},P)\to(E,l{B})
l{F}(T,E)
T
E
\varphi:\Omega\tol{F}(T,E)\congET
T\to | |
Y | |
t:E |
E
Yt(\omega)=\omega(t)
\{Yt,t\inT\}
C0(\R+,\R)
The vector space C can be equipped with the uniform norm
\|f\|:=\supt|f(t)|
turning it into a normed vector space (in fact a Banach space). This norm induces a metric on C in the usual way:
d(f,g):=\|f-g\|
Thinking of the domain [0, ''T'' ] as "time" and the range Rn as "space", an intuitive view of the uniform topology is that two functions are "close" if we can "wiggle space slightly" 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.
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.
Recall that the modulus of continuity for a function f : [0, ''T'' ] → Rn is defined by
\omegaf(\delta):=\sup\left\{|f(s)-f(t)|:s,t\in[0,T],|s-t|\leq\delta\right\}.
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:
f\inC\iff\omegaf(\delta)\to0as\delta\to0
By an application of the Arzelà-Ascoli theorem, one can show that a sequence
(\mun
infty | |
) | |
n=1 |
\lima\limsupn\mun\{f\inC\mid|f(0)|\geqa\}=0,
\lim\delta\limsupn\mun\{f\inC\mid\omegaf(\delta)\geq\varepsilon\}=0
There is a "standard" measure on C0, known as classical Wiener measure (or simply Wiener measure). Wiener measure has (at least) two equivalent characterizations:
If one defines Brownian motion to be a Markov stochastic process B : [0, ''T'' ] × Ω → Rn, starting at the origin, with almost surely continuous paths and independent increments
Bt-Bs\simNormal\left(0,|t-s|\right),
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 C0.
Classical Wiener measure is a Gaussian measure: in particular, it is a strictly positive probability measure.
Given classical Wiener measure γ on C0, the product measure γ n × γ is a probability measure on C, where γ n denotes the standard Gaussian measure on Rn.