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Space-time harmonic functions yield Brownian local martingales up to exit lifetime

Statement

Assume the Axiom of Choice. Let d1, let U[0,)×Rd be open in the relative topology, and let fC1,2(U) satisfy the space-time harmonicity equation tf+12Δf=0on U, where Δ=k=1dxk2 is the spatial Laplacian. Let B be a standard d-dimensional Brownian motion adapted to a filtration satisfying the usual conditions, and assume explicitly that BtBs is independent of Fs for every 0s<t, with (0,0)U. Use its everywhere-continuous adapted representative obtained by setting B to zero off the measurable full event on which it is continuous and B0=0; the usual conditions put that event in F0. This preserves all vector Brownian laws and the vector increment-independence hypothesis. All exit times and integrands below use this representative. For a compact KU put τK:=inf{t0:(t,Bt)intK}, where the interior is relative to [0,)×Rd.

  1. For every compact KU with (0,0)intK, up to indistinguishability f(tτK,BtτK)=f(0,0)+k=1d0t1[0,τK](s)xkf(s,Bs)dBsk, and the right-hand integral is a continuous square-integrable martingale; thus each stopped piece is a true martingale. In this display the stopped gradient is the predictable bounded extension supplied by [F3], equal to f(s,Bs) through τK and zero afterwards; it does not evaluate f outside U.
  2. If τU:=inf{t0:(t,Bt)U} and E0tf2(s,Bs)1[0,τU)(s)ds< for a given t0, then the process Nr:=k=1d0r1[0,τU)(s)xkf(s,Bs)dBsk,0rt, is a square-integrable martingale, and for every 0rt one has f(r,Br)f(0,0)=Nron the event {r<τU}. No value of f at the exit point (τU,BτU)U is asserted.
  3. On the stochastic interval [0,τU) the process tf(t,Bt), read through continuous versions, is a continuous local martingale up to lifetime τU: for any time-capped compact exhaustion satisfying KnintKn+1 and nKn=U, after discarding finitely many initial sets so that (0,0)intK1, its stopped pieces at τKn are true martingales and τKnτU almost surely. This is not a claim that f(t,Bt) is defined after the lifetime or that these times tend to infinity.

Facts & Assumptions

Given: AC, an open U[0,)×Rd, a function fC1,2(U) with tf+12Δf=0 on U, a standard d-dimensional Brownian motion B adapted to a usual filtration with each vector increment independent of the past filtration, its F0-normalized everywhere-continuous representative, and compact sets KU.

[F1]

B is a continuous Brownian Ito process. The vector filtration hypothesis implies the scalar standing hypothesis (H) for every coordinate. The normalized B is therefore a continuous Brownian Ito process with drift 0 and dispersion δik. The one-block elementary process 1(0,T] represents the constant integrand class and has integral BtiB0i=Bti; its localized integral is Bi up to indistinguishability. Continuous Brownian Ito processes d-dimensional Brownian motion Brownian motion Elementary predictable Brownian integrands Ito integral of an elementary predictable process Localized Ito integral

[F2]

Multidimensional Ito formula. For a C1,2 function g and a continuous Brownian Ito process X, dg(t,Xt)=(tg+ibiig+12i,j(σσT)ijijg)(t,Xt)dt+i,kig(t,Xt)σtikdBtk up to indistinguishability. Multidimensional Ito formula for Brownian-driven processes

[F3]

Cutoffs on compact subsets and local boundedness. Because U is relatively open, the formula f~(t,x)=3f(t,x)2f(2t,x) for small t<0 gives a C1,2 extension across t=0 on a Euclidean-open neighbourhood of each compact KU: value and time derivative match because 32=1 and 3+4=1, and the spatial derivatives match by the same value identity. Choose compact neighbourhoods KintK there. The cutoff lemma gives a continuous compactly supported cutoff equal to 1 on K; convolving it with a sufficiently small compactly supported mollifier gives χCc equal to 1 near K and supported in the extension domain. Then g:=χf~, extended by zero, is a global C1,2 function and agrees with f and its displayed derivatives near K. In particular f is bounded there. The spaces Cc(Rn) and Cc(Rn) The mollifier family generated by a unit-mass smooth bump Convolution with a mollifier is smooth, and derivatives pass under the integral sign A compact set inside a bounded open set admits an explicit compactly supported continuous cutoff Heine-Cantor: a continuous map from a compact metric space to any metric space is uniformly continuous Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line Continuity of f:AR at a point of A and on A: the ε-δ condition, its agreement with limxcf(x)=f(c) at a limit point, and continuity at an isolated point

[F4]

Localized-integral interfaces. For a bounded predictable integrand H on [0,T]: the integral HdBk is a continuous square-integrable martingale with E(0THdBk)2=E0TH2ds, the stopping identity identifies stopped integrals with integrals of H1[0,τ], and a bounded integrand has finite energy. Localized Ito integral Stopping an Ito integral The Ito integral process has a continuous martingale version Ito isometry and linearity in predictable L2 Locally square-integrable predictable Brownian integrands Progressively measurable and predictable processes

[F5]

Stopping times and exhaustion. Put S=[0,)×Rd. For a relatively open VS with nonempty complement C=SV, the distance q(y)=d(y,C) is continuous and zero exactly on C. The Lipschitz estimate is supplied by d(x,A)d(y,A)d(x,y), so the distance to a fixed nonempty set is 1-Lipschitz; positivity outside C follows from an open ball disjoint from this closed set. For Ys=(s,Bs), continuity and compactness of Y([0,t]) give {τVt}={infs([0,t]Q){t}q(Ys)=0}. Indeed the continuous distance attains its minimum on the compact path image, and a zero minimum is a hit by time t; approximation by rational times gives the same infimum, including t=0. The displayed event is Ft-measurable. If V=S, its exit time is infinity directly. For exhaustion, set a(y)=min(1,d(y,SU)) when the complement is nonempty, and a=1 when U=S. Let Ln={(s,x)S:sn, xn, a(s,x)1/n}. These sets are closed and bounded, hence compact, contained in U, satisfy LnintSLn+1, and cover U. Discard finitely many initial sets so that the origin belongs to the first interior, and denote the tail by Kn. The time caps remain finite. For any such nested exhaustion, every compact path segment before τU is covered by finitely many interiors, hence lies in one. Thus τKnτU. Moreover τKn<τU: the finite exit point from intKn lies in KnU, and continuity gives a positive interval still in U after this time. Consequently [0,τU)=n[0,τKn], so its indicator is predictable by the stopping-indicator generators. Continuous-time stopping times and stopped sigma-algebras Progressively measurable and predictable processes Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line The image of a compact metric space under a continuous map is compact, and so is the image of any compact subset Heine-Cantor: a continuous map from a compact metric space to any metric space is uniformly continuous

[F7]

Finite-energy approximation. Dominated convergence applies on the product of Lebesgue measure on a finite interval and probability when the squared integrand error has the stated integrable majorant. Dominated convergence

[F6]

AC bookkeeping. Choice is declared for the conditional-expectation and completeness interfaces, and any countable selection of compact cutoffs. The distance exhaustion is explicit. The Axiom of Choice

Proof

technique · direct
1.1

Local reduction to a global test function: fix a compact KU with (0,0)intK and a cutoff χ and global function g=χf~ as in [F3]. Applying the multidimensional Ito formula [F2] to g along the class process X=B of [F1], whose drift is 0 and whose dispersion is the identity, gives g(t,Bt)=g(0,0)+0t(tg+12Δg)(s,Bs)ds+k0txkg(s,Bs)dBsk up to indistinguishability.

F1F2F3
2.1

Cancellation on the stopped region: the compact set K has bounded time projection, so τK<. Continuity of s(s,Bs) and the definition through the relative interior give (s,Bs)K for 0sτK. On a neighbourhood of K one has g=f, so tg+12Δg=0 and xkg=xkf there. Apply the stopping identity to the formula of step 1.1: its drift vanishes through τK, and its left side becomes f(tτK,BtτK).

F3step 1.1
3.1

The stopped identity: the stopping identity of [F4] changes the stochastic term of step 1.1 into k0t1[0,τK](s)xkg(s,Bs)dBsk. This predictable integrand is bounded, and through τK it equals xkf(s,Bs); after τK it is declared zero. Substituting step 2.1 gives clause 1. The finite-energy integral is a continuous square-integrable martingale, so the stopped process is a true martingale.

F3F4step 2.1
4.1

Clause 2: fix t0 and assume the displayed energy is finite. Define H(s,ω)=f(s,Bs(ω)) when (s,Bs(ω))U and H=0 otherwise. The zero extension of f from the relatively open set U is a Borel function on S. The map (s,ω)(s,Bs(ω)) is predictable by the everywhere-continuous adapted representative and the predictable generators, so this composition H is predictable. By [F5] the strict-lifetime indicator is predictable too, and 1[0,τU)H has finite energy by assumption. For an exhaustion from [F5], the bounded stopped extensions H(n):=1[0,τKn]gn(,B) of clause 1 converge to 1[0,τU)H in L2([0,t]×Ω); indeed [F5] gives H(n)=1[0,τKn]H and these indicators increase pointwise to 1[0,τU). The squared difference is bounded by H21[0,τU), integrable on [0,t]×Ω by assumption, so dominated convergence applies. This uses the zero-extension convention also in the energy hypothesis. The isometry gives Nr(n)Nr in L2 for every rt, and N is a square-integrable martingale. Put En={r<τKn} and E={r<τU}. Then EnE, and on En clause 1 gives Nr(n)=f(r,Br)f(0,0). Hence for every ε>0, P(E{Nr(f(r,Br)f(0,0))>ε})P(EEn)+P(NrNr(n)>ε), which tends to zero. This proves the asserted equality without evaluating f at the exit point.

F4F5F7step 3.1
5.1

Clause 3 and boundary cases: clause 1 exhibits each stopped piece for a time-capped exhaustion as a martingale, and [F5] gives τKnτU almost surely; this is exactly the lifetime-local assertion of clause 3. If U is all of relative space-time, one may choose the usual expanding time-space cylinders and the lifetime is infinity. If f is constant the gradient vanishes; if d=1 there is one stochastic integral; and the growth of f outside the localized compact sets is irrelevant. AC enters only through [F6].

F5F6step 3.1step 4.1

Source notes

Lawler, Section 3.7, records that space-time harmonic functions of Brownian motion produce local martingales via the Ito formula, with bounded-domain stopping making the integrals square-integrable. The cutoff reduction of step 1.1 is included because the Ito formula is stated for globally defined C1,2 functions, while the equation is only assumed on the open set U.

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