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Natural filtration

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In the theory of stochastic processes in mathematics and statistics, the generated filtration or natural filtration associated to a stochastic process is a filtration associated to the process which records its "past behaviour" at each time. It is in a sense the simplest filtration available for studying the given process: all information concerning the process, and only that information, is available in the natural filtration.

Formal definition

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Let

Then the natural filtration of 𝒜 with respect to X is defined to be the filtration 𝔽X=ℱ∙X=(ℱiX)i∈I given by

ℱiX=σ{Xj−1(B)|j∈I,j≤i,B∈Σ},

i.e., the smallest σ-algebra on Ω that contains all pre-images of Σ-measurable subsets of S for "times" j up to i.

Any stochastic process X is an adapted process with respect to its natural filtration.

Examples

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Two examples are given below, the Bernoulli process and the Wiener process. The simpler example, the Bernoullii process, is treated somewhat awkwardly and verbosely, belabored, but using a notation that allows more direct contact with the Wiener process.

Bernoulli process

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The Bernoulli process is the process X of coin-flips. The sample space is Ω={0,1}ℕ=2ℕ, the set of all infinitely-long sequences of binary strings. A single point ω∈Ω then specifies a single, specific infinitely long sequence. The index set I=ℕ is the natural numbers. The state space is the set of symbols S={H,T} indicating heads or tails. Fixing ω to a specific sequence, X(i,ω) then indicates the i'th outcome of the coin-flip, heads or tails. The conventional notation for this process is Xi=X(i,−), indicating that all possibilities should be considered at time i.

The sigma algebra on the state space contains four elements: Σ={∅,{H},{T},S}. The set Xj−1(B) for some B∈Σ is then a cylinder set, consisting of all strings having an element of B at location j:

Xj−1(B)={ω∈Ω:X(j,ω)=b and b∈B}

The filtration is then the sigma algebra generated by these cylinder sets; it is exactly as above:

ℱi=σ{Xj−1(B):j≤i,B∈Σ},

The sub-sigma-algebra ℱi can be understood as the sigma algebra for which the first i symbols of the process have been fixed, and all the remaining symbols are left indeterminate.

This can also be looked at from a "sideways" direction. The set

C(i,ω)={α∈Ω:X(j,α)=X(j,ω) for j≤i}

is a cylinder set, for which all points α∈C(i,ω) match exactly X(−,ω) for the first i coin-flips. Clearly, one has that C(k,ω)⊂C(i,ω) whenever k>i. That is, as more and more of the initial sequence is fixed, the corresponding cylinder sets become finer.

Let A∈𝒜 be one of the sets in the sigma algebra 𝒜. Cylinder sets can be defined in a corresponding manner:

C(i,A)={α∈Ω:X(j,α)=X(j,ω) for j≤i and ω∈A}

Again, one has that C(k,A)⊂C(i,A) whenever k>i.

The filtration can be understood to be

ℱi={C(i,A)|A∈𝒜}

consisting of all sets for which the first i outcomes have been fixed. As time progresses, the filtrations become finer, so that ℱi⊂ℱk for i<k.

Wiener process

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The Wiener process X can be taken to be set in the classical Wiener space Ω=C0([0,T]) consisting of all continuous functions on the interval I=[0,T]. The state space S can be taken to be Euclidean space: S=ℝn and Σ=ℬ(ℝn) the standard Borel algebra on ℝn. The Wiener process is then X:I×Ω→S.

The interpretation is that fixing a single point ω∈Ω fixes a single continuous path X(⋅,ω):I→S. Unlike the Bernoulli process, however, it is not possible to construct the filtration out of the components

Xt−1(B)={ω∈Ω:X(t,ω)=x and x∈B}

for some B∈ℬ(ℝn). The primary issue is that I is uncountable, and so one cannot perform a naive union of such sets, while also preserving continuity. However, the approach of fixing the initial portion of the path does follow through. By analogy, define

C(t,ω)={α∈Ω:X(s,α)=X(s,ω) for s≤t}

This consists of all continuous functions, that is, elements of Ω for which the initial segment s≤t exactly matches a selected sample function X(⋅,ω). As before, one has that C(u,ω)⊂C(t,ω) whenever t<u, that is, the set becomes strictly finer as time increases.

Presuming that one has defined a sigma algebra 𝒜 on the (classical) Wiener space, then for a given A∈𝒜, the corresponding cylinder can be defined as

C(t,A)={α∈Ω:X(s,α)=X(s,ω) for s≤t and ω∈A}

which also becomes finer for increasing time: C(u,A)⊂C(t,A) whenever t<u.

The desired filtration is then

ℱt={C(t,A)|A∈𝒜}.

As before, it becomes strictly finer with increasing time: ℱt⊂ℱu whenever t<u.

References

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  • Delia Coculescu; Ashkan Nikeghbali (2010), "Filtrations", Encyclopedia of Quantitative Finance

See also

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