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Brownian motion has a jointly measurable continuous version

Statement

Let B be a standard Brownian motion Brownian motion on a probability space (Ω,F,P). Then there is a process B^=(B^t)t0 with the following properties.

  1. B^ is indistinguishable from B, and B^0=0 on all of Ω.
  2. Every path tB^t(ω) is continuous on [0,), so ωB^(ω) is a map into the path space C([0,),R) of Uniform-on-compacts metric on continuous path space.
  3. That map is Borel measurable for the uniform-on-compacts Borel σ-algebra, and (t,ω)B^t(ω) is measurable for B([0,))F.

The version is obtained by keeping the original process on one probability-one event and replacing the whole path by the zero path outside it; no distribution of B is altered and no path is selected by any choice principle.

Facts & Assumptions

Given: AC and a standard Brownian motion B on (Ω,F,P).

[F1]

There is a measurable event A with P(A)=1 on which every path tBt(ω) is continuous, and B0=0 almost surely. Brownian motion

[F2]

On C([0,),R) the uniform-on-compacts metric induces the topology of uniform convergence on compact subsets of [0,). Uniform-on-compacts metric on continuous path space

[F3]

The Borel σ-algebra of C([0,),R) is generated by the coordinate maps πt(f)=f(t), t0. Borel sigma-algebra of continuous path space is generated by coordinates

[F4]

The evaluation map e(f,t):=f(t) on C([0,),R)×[0,) is defined for every pair, and it is continuous when the path space carries the uniform-on-compacts topology. The evaluation map e:C(X,Y)×XY, e(f,x)=f(x)

[F5]

AC is the ambient assumption of the Brownian interfaces. The Axiom of Choice

Proof

technique · direct
1.1

Put A:=A{B0=0}, a measurable event with P(A)=1 by [F1], and define B^t(ω):=Bt(ω) for ωA and B^t(ω):=0 for ωA; then B^ is indistinguishable from B because it differs from B only on the null set (A)c, and B^0(ω)=0 for every ω.

givenF1
1.2

The evaluation map of [F4] is continuous: if fmf in the metric of [F2] and tmt in [0,), choose N with tmN for all m and f(s)f(t)<ε/2 for st<η, which is possible because the continuous f is continuous at t; convergence in the metric of [F2] gives sup0sNfm(s)f(s)<ε/2 for all large m, and then fm(tm)f(t)sup0sNfm(s)f(s)+f(tm)f(t)<ε for all large m.

F2F4
2.1

Every path of B^ is continuous: for ωA it is the Brownian path, continuous by [F1], and for ωA it is the zero path.

step 1.1F1
2.2

Each time coordinate of B^ is measurable: B^t=1ABt is the product of a measurable indicator with the measurable function Bt.

step 1.1
3.1

The map ωB^(ω) is a random element of C([0,),R) with its Borel σ-algebra: by [F3] that σ-algebra is σ(πt:t0), and for every t and every Borel ER one has {ω:πt(B^(ω))E}={B^tE}, measurable by [step 2.2]; the family of Borel sets with measurable preimage is a σ-algebra containing the generating sets πt1(E), hence all of B(C).

step 2.1step 2.2F3
4.1

The pair map (t,ω)(B^(ω),t) is measurable from B([0,))F into the product of the Borel σ-algebras, because its first component is measurable by [step 3.1] and its second is a coordinate projection; composing with the continuous, hence Borel measurable, evaluation map of [step 1.2] shows that (t,ω)B^t(ω) is B([0,))F-measurable.

step 3.1step 1.2
5.1

The boundary cases are covered: the normalization changes the process only on the null set (A)c, so indistinguishability and every almost-sure statement are preserved; the initial value is 0 on all outcomes as required; the case t=0 enters the measurability statements through the coordinate B^0, which is identically zero; and AC enters only through [F5] as the ambient assumption of the Brownian definition.

step 1.1step 2.1step 4.1F5given

Source notes

Durrett, Section 7.1, fixes a continuous version of Brownian motion as part of the definition of the process; Sousi's Chapter 6 treats Brownian motion as a random continuous path. The lemma records the two measurability consequences used later on the page: the path map is a random element of the continuous path space, and the evaluation map makes the process jointly measurable, which is what the Tonelli and Fubini arguments for the zero set and the occupation time need.

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Sources