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The Ito Integral with Respect to Brownian Motion

1 · Prerequisites

2 · Summary

This page constructs the Ito integral with respect to Brownian motion along the standard route: continuous-time vocabulary Continuous-time adapted processes and martingales Progressively measurable and predictable processes, predictability of continuous adapted processes Adapted continuous processes are progressively measurable, the elementary integral on step integrands Elementary predictable Brownian integrands Ito integral of an elementary predictable process, and its representation independence Elementary Ito integrals do not depend on step representation. The elementary isometry Ito isometry for elementary integrands and its polarized form Cross Ito isometry control the L2 extension, whose density input is Density of elementary predictable processes in predictable L2; the extension itself is defined in Ito integral for square-integrable predictable processes and shown to be independent of the approximating sequence in The general Ito integral is well defined. The isometric linearity of the extension Ito isometry and linearity in predictable L2, the continuous martingale version The Ito integral process has a continuous martingale version and the Doob maximal bound Doob maximal bound for the Ito integral carry the construction to integrands that are only locally square-integrable Locally square-integrable predictable Brownian integrands, and localization Localized Ito integral, the stopping identity Stopping an Ito integral and the quadratic variation Quadratic variation of an Ito integral complete the Brownian-calculus interface. Deterministic integrands give Gaussian integrals with the L2 inner product as covariance Deterministic Ito integrals are Gaussian.

Only Brownian integrators are treated: general semimartingales, jump compensators, change of measure and stochastic differential equations are outside this page, and the companion examples page records the boundary cases of the construction.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Continuous-time adapted processes and martingales

Definition

Assume the Axiom of Choice The Axiom of Choice. Fix a probability space (Ω,F,P) with a continuous-time filtration (Ft)t0 in the sense of Continuous-time filtrations and all-pairs martingales. All processes in this definition are real-valued and indexed by [0,); the filtration is neither assumed complete nor right-continuous. The Axiom of Choice is declared because the conditional-expectation classes used in clause 3 are supplied by the Radon--Nikodym interface of Conditional expectation as an ae class, which assumes it; the countable-choice obligations inherited from that interface are declared as dependencies of this item.

  1. Adapted. X=(Xt)t0 is adapted to (Ft) when Xt is Ft-measurable for every t0. This is exactly the notion of Continuous-time filtrations and all-pairs martingales.

  2. Stopped process. For a stopping time τ for (Ft) Continuous-time stopping times and stopped sigma-algebras the stopped process is Xtτ(ω):=Xtτ(ω)(ω),t0, with the convention t:=t, so no value X is ever required and X0τ=X0 identically. This formula defines a pathwise family; adaptedness of X alone does not assert measurability or adaptedness of its stopped values. If in addition τc for a deterministic constant c, then Xtτ=Xtτ, and only the values of X on [0,c] enter. Stopping at a stopping time is not the same as replacing a process by a modification; it is a pathwise operation.

  3. Martingale. M=(Mt)t0 is a martingale (an all-pairs continuous-time martingale) relative to (Ft) when it is adapted, EMt< for every t0, and for all 0st E[MtFs]=Msalmost surely. The equality is an equality of the almost-everywhere classes of Conditional expectation as an ae class; equivalently, every version of the conditional expectation on the left equals Ms off one null set. At s=t the identity reduces to the known-variable case. The word "continuous-time" refers to the index set only and does not assert path continuity.

  4. Local martingale. X=(Xt)t0 is a local martingale relative to (Ft) when it is adapted, EX0<, and there exist stopping times (τn)n0 with τ0τ1 and τn almost surely such that for every n0 the stopped process XτnX0=(XtτnX0)t0 is a martingale in the sense of clause 3. The sequence (τn) is called a localizing sequence. Equivalently, every Xτn is a martingale: adaptedness makes the integrable variable X0 measurable with respect to every Ft, so the constant process with value X0 is a martingale and may be added to, or subtracted from, each stopped process. The centering merely makes every localized process start at 0; apart from the required integrability of X0, no claim is made that X is integrable at a positive deterministic time, and no claim is made that X has continuous paths.

  5. Path and integrability attributes. A process has continuous paths when tXt(ω) is continuous on [0,) for every ω in an event of probability one; the usual almost-sure path conventions of Process law, modification, and indistinguishability apply. A martingale M is square-integrable when EMt2< for every t0, and L2-bounded when supt0EMt2<. These are properties of the single process under consideration, not of its versions: a modification of a martingale need not be adapted, so every later statement names the adapted versions it uses.

The following remarks specify what follows directly from this vocabulary.

  1. A martingale is a local martingale. If M is a martingale, the constant sequence τn:=n, n0, localizes it: the stopped process MnM0 is again a martingale by the martingale identity applied at the deterministic times sntn. The converse fails; a local martingale need not be a martingale, and no such implication is used in this development.
  2. Localization after a separately justified stopping operation. Suppose (τn) localizes X, σ is a stopping time, Xσ is adapted, and each (XτnX0)σ is a martingale. Then (τn) localizes Xσ. Indeed it still increases to infinity, (Xσ)0=X0, and the pathwise identity (Xσ)τn(Xσ)0=XστnX0=(XτnX0)σ verifies exactly clause 4. The stopped-piece martingale assertion and adaptedness are hypotheses here, not consequences of the unrestricted all-pairs definition. They must be established in each application. The sequence (στn) is not a substitute for (τn): its almost-sure limit is σ, which need not be infinity.

No path continuity, no right continuity of the filtration, and no completeness of the underlying probability space is imposed by this definition. Choice enters only through the conditional-expectation interface named above, whose countable-choice obligations are declared as dependencies of this item.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Progressively measurable and predictable processes

Definition

Assume the Axiom of Choice The Axiom of Choice. Let (Ω,F,P) be a probability space with a continuous-time filtration (Ft)t0 Continuous-time filtrations and all-pairs martingales. All processes here are real-valued and indexed by [0,). AC is inherited from the cited continuous-time-filtration interface, whose separate martingale clause uses conditional expectation. Once the filtered probability space and stopping times are given, the progressive and predictable constructions below make no additional choice: they use only generated sigma-algebras and product rectangles.

  1. Progressively measurable. A process X=(Xt)t0 is progressively measurable relative to (Ft) when for every t0 the restricted map [0,t]×ΩR, (s,ω)Xs(ω), is measurable for the product sigma-algebra B([0,t])Ft The product sigma-algebra and its finite iterates.

  2. Time-zero and interval generators. On the product space [0,)×Ω, let P be the sigma-algebra generated by the family G:={(s,u]×A: 0s<u<, AFs}  {{0}×A: AF0}. The interval generators with s=0 are included, so (0,u]×A with AF0 is a generator. The sigma-algebra P exists by Nonempty intersections of sigma-algebras are sigma-algebras, so the generated sigma-algebra exists and is minimal and is called the predictable sigma-algebra. A process H=(Ht)t0 is predictable when the map (s,ω)Hs(ω) is P-measurable. For a finite horizon T>0 we write PT for the sigma-algebra on [0,T]×Ω generated by the same family restricted to uT together with the time-zero generators; this is the trace of P on [0,T]×Ω. Indeed, the trace of an interval generator is empty when sT, and otherwise is (s,min(u,T)]×A, while time-zero generators are unchanged. Conversely every listed finite-horizon generator is such a trace.

  3. Sections, adaptedness, and null sets. Two structural conventions are used repeatedly and are part of the definition. (a) Every generator is a measurable rectangle of B([0,))F, hence PB([0,))F; the time-zero generator {0}×A has dtP-measure zero for every A. A set in P has its section at each fixed time s in Fs: sets with that section property form a sigma-algebra, and each generator has the property by the increasing-filtration condition. Its section at each fixed ω is Borel in time, by the same sigma-algebra argument. (b) If a process is predictable then it is progressively measurable: for st the section ωHs(ω) is Fs-measurable Ft-measurable, and the progressive-measurability claim is the restriction of the joint map to [0,t]×Ω; the restriction of a P-measurable map to [0,t]×Ω is measurable for B([0,t])Ft because every generator with ut lies in that product sigma-algebra and the generators with u>t have intersection with [0,t]×Ω of the form (s,t]×A with s<t and AFs, or the empty set when st. The time-zero generators also lie in B([0,t])Ft.

The family G need not itself contain the whole space, but a finite intersection of generators is empty or again a generator, or a time-zero generator, because (s,u](s,u]=(ss,uu] and AAFss whenever AFs, AFs, while {0}×A is disjoint from every interval generator, including (0,u]×A. Two time-zero generators intersect in {0}×(AA) with AAF0. Thus the family consisting of the whole space together with finite intersections of generators is a pi-system generating P; this is the structural fact used by the density theorem below.

Because predictability is a measurability requirement for the joint map, it is preserved by pointwise limits, products and linear combinations of predictable processes. A deterministic function h of time defines a predictable process exactly when h is Borel measurable: the sets C for which C×ΩP form a sigma-algebra containing the intervals (s,u] and {0}, hence all Borel sets. Conversely, take any fixed ωΩ (a probability space is nonempty) and use the Borel time-section property from 3(a) on every inverse image of an open set. This single choice uses no choice axiom. In particular the indicators 1[0,u] and 1(0,u] are predictable for every deterministic u0, and the process s1sτ(ω) for a stopping time τ Continuous-time stopping times and stopped sigma-algebras is predictable, since {(s,ω):s>τ(ω)}=qQ>0(q,)×{τ<q}=qQ>0n>q(q,n]×{τ<q} is a countable union of generators: for rational q>0 one has {τ<q}=q<q, qQ{τq}Fq. The complement of that set inside [0,)×Ω is the event of the indicator, so 1[0,τ] is predictable; its left-continuity in the time variable is the visual form of the same computation.

No completeness of the filtration and no right continuity of (Ft) is used or assumed. Apart from the inherited ambient assumption just recorded, the constructions in this definition are choice-free.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Adapted continuous processes are progressively measurable

Statement

Let (Ω,F,P) be a probability space with a continuous-time filtration (Ft)t0, and let X=(Xt)t0 be a real process that satisfies Xt:ΩR is Ft-measurable for every t0, and has continuous paths, in the strong sense that sXs(ω) is continuous on [0,) for every ωΩ. Then X is progressively measurable and predictable relative to (Ft) in the sense of Progressively measurable and predictable processes, including at time zero under the generator convention {0}×A, AF0. No choice principle is used. Here a filtration means an increasing family of sub-sigma-algebras of F. The fixed-time measurability hypothesis is the adaptedness terminology of clause 1 of Continuous-time adapted processes and martingales; only that clause is used, not its conditional-expectation or martingale interface and its Choice assumption.

If instead the paths are continuous only on an event AF with P(A)=1, the conclusion holds for the modification that is set equal to 0 off A provided AF0; without such a measurability assumption on the continuity event no predictability claim is made, because predictability is a property of the given joint map.

Facts & Assumptions

Given: a probability space with a filtration (Ft)t0, a real adapted process X with continuous paths everywhere, a horizon T>0, and for n1 the dyadic grid tk=kT/2n, 0k2n.

[F1]

X is adapted: Xu is Fu-measurable for every u0; in particular Xu is FT-measurable for uT. Continuous-time adapted processes and martingales

[F2]

Each rectangle C×A, where CB([0,T]) and AFu for some uT, belongs to B([0,T])FT, since FuFT. Finite unions of these rectangles also belong to that sigma-algebra. Progressively measurable and predictable processes

[F3]

A pointwise limit of measurable functions into R is measurable; the same theorem applied coordinatewise gives measurability of limits of jointly measurable maps. Sequential suprema, infima, limsup, liminf, and pointwise limits of measurable functions are measurable

[F4]

The generators of the predictable sigma-algebra are the sets (s,u]×A with AFs and the time-zero sets {0}×A with AF0. The set [0,T]×Ω is predictable, being the union of the generator (0,T]×Ω and the time-zero generator {0}×Ω. Progressively measurable and predictable processes

Proof

technique · direct
1.1

Fix n1 and define, for (s,ω)[0,T]×Ω, Hsn(ω):=k=02n1Xtk(ω)1(tk,tk+1](s)+X0(ω)1{0}(s). For a Borel set BR the preimage is {HnB}=({0}×{X0B})k=02n1((tk,tk+1]×{XtkB}), a finite union of measurable rectangles of B([0,T])FT, since Xtk is Ftk-measurable and FtkFT.

F1F2given
2.1

Each Hn is measurable for B([0,T])FT, and for every (s,ω) the identity Hsn(ω)Xs(ω) holds: at s=0 both sides equal X0(ω), and for s(0,T] the left endpoints tk of the dyadic intervals containing s tend to s, so path continuity gives Xtk(ω)Xs(ω).

step 1.1given
2.2

Each Hn is predictable: the preimage formula of step 1.1 exhibits each Borel inverse image as a finite union of generators of the predictable sigma-algebra, since Xtk is Ftk-measurable and each interval (tk,tk+1] is a generator interval, while the time-zero term is {0}×{X0B} with {X0B}F0.

F1F4step 1.1
3.1

By [F3] the pointwise limit X restricted to [0,T]×Ω is B([0,T])FT-measurable; T>0 was arbitrary, so X is progressively measurable.

F3step 2.1
3.2

For each fixed T the restriction of X to [0,T]×Ω is a pointwise limit of the predictable processes Hn restricted to [0,T], hence is predictable on that horizon by [F3]; and the horizon-T pieces assemble to a globally predictable process because [0,T]×ΩP and a set is predictable as soon as all its intersections with the countably many sets [0,m]×Ω, m1, are.

F3F4step 2.2
4.1

Collecting steps 3.1 and 3.2, an adapted process with everywhere continuous paths is progressively measurable and predictable. The time-zero case is included: H0n=X0 at every stage and the generator {0}×A, AF0, was used in step 2.2. For the final statement about AF0, the map Yt=Xt1A is Ft-measurable (its Borel inverse images are (A{XtB})(Ac if 0B)), has continuous paths everywhere, and agrees with X on A. Apply the conclusion to Y. No grid point, approximant or limit in the argument is chosen: the dyadic grids and the left endpoints are fixed functions of n, and pointwise limits are unique.

step 3.1step 3.2given

Source notes

The approximation is the standard dyadic-step argument of van der Vaart, Section 5.1; continuous adapted processes generate the predictable sigma-algebra, and the left-continuous staircase approximants are predictable by construction. The time-zero section uses exactly the generators {0}×A, AF0. The proof explicitly supplies the fixed-time measurable maps and does not invoke any conditional-expectation existence theorem.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Elementary predictable Brownian integrands

Definition

Assume the Axiom of Choice The Axiom of Choice, and fix a probability space (Ω,F,P) with a continuous-time filtration (Ft)t0 Continuous-time filtrations and all-pairs martingales and a standard Brownian motion B Brownian motion on it. Standing hypothesis (H). B is adapted to (Ft) and for all 0s<t the increment BtBs is independent of Fs and has law N(0,ts). The raw natural filtration and the usual augmented natural filtration Natural and usual augmented Brownian filtrations both satisfy (H) for a standard Brownian motion, by Future-path Markov property; for a general filtration, (H) is part of the data and is not automatic. Every statement in this development names (H) when it is used.

Throughout, fix a finite horizon T>0. An elementary predictable Brownian integrand on [0,T] is a process of the form Hs(ω)=k=0m1ξk(ω)1(tk,tk+1](s),s[0,T], where 0=t0<t1<<tm=T is a finite partition of [0,T], each ξk is a bounded real Ftk-measurable random variable, and the values at the partition points are irrelevant because the intervals are left-open and right-closed. The mesh of the representation is maxk(tk+1tk), and the supremum norm of the representation is maxkξk. The integrand itself is the process H; a second list of the same name with different coefficients is the same elementary integrand only if the two processes coincide in the almost-everywhere sense made precise below.

The following properties are part of the definition and are used at once.

  1. Predictability. H is predictable Progressively measurable and predictable processes. Indeed, for a Borel set ΓR, {HΓ}=ZΓk=0m1((tk,tk+1]×{ξkΓ}),ZΓ:={{0}×Ω,0Γ,,0Γ, a finite union of generators of the predictable sigma-algebra because {ξkΓ}Ftk and {0}×Ω is a time-zero generator. Consequently H is progressively measurable and measurable for the product sigma-algebra B([0,T])F, and H belongs to L2([0,T]×Ω,dtP): with c:=maxkξk< one has E0THs2dsc2T<.

  2. Endpoint and null-set conventions. Replacing the intervals by (tk,tk+1] makes the value at s=0 zero for every elementary integrand. More generally, if two elementary integrands agree for all s[0,T] except at finitely many deterministic times, then they agree (dtP)-almost everywhere, since a finite set of times is Lebesgue-null and Tonelli computes dtP({u}×Ω)=0. All integrands and all integrals below are therefore elements of the quotient spaces of L2(dtP) and L2(P); a claim about a process is a claim about its almost-everywhere class unless a representative is explicitly named, and path statements name the continuous representative.

  3. Deterministic coefficients. If every ξk is a deterministic real number, H is a deterministic step function on [0,T], so the elementary integrands include all step functions with deterministic coefficients. These are the integrands for which the integral is a Gaussian variable below.

The Axiom of Choice is declared because the Brownian construction and the conditional-expectation interface used in items 6, 7 and 13 assume it; the definition itself, including the predictability computation of clause 1, uses no choice. The countable-choice obligations inherited from that interface are declared as dependencies of this item.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Ito integral of an elementary predictable process

Definition

Assume the Axiom of Choice and work under the standing hypothesis (H) of Elementary predictable Brownian integrands: a filtered probability space with a standard Brownian motion B adapted to the filtration, with increments BtBs independent of Fs of law N(0,ts). Fix T>0 and an elementary predictable integrand Hs=k=0m1ξk1(tk,tk+1](s),0=t0<<tm=T, with bounded Ftk-measurable coefficients ξk. The Ito integral of H against B is the process It(H):=k=0m1ξk(Bttk+1Bttk),0tT, also written 0tHsdBs or (HB)t. The sum is finite and is evaluated with the Brownian path of the given representative; on the event where tBt is continuous it is continuous in t, and I0(H)=0 because 0tk=0 for every k.

Three conventions are part of the definition.

  1. Adaptedness and continuity. For fixed t, each summand ξk(Bttk+1Bttk) is Ft-measurable: if t<tk, the Brownian difference and hence the summand are zero; if ttk, then FtkFt, while Btu is Ft-measurable for every u because tut. Thus I(H) is adapted. For each fixed ω the map tBttk+1(ω)Bttk(ω) is continuous outside the single exceptional null set of (H) on which the Brownian path is discontinuous; the finite sum is therefore continuous on the same event.

  2. Linearity on a common refinement. If H and K are elementary integrands and a partition refines both representations, then the defining sums of H, K, H+K and aH are taken over that common partition, and the finite sums give It(H+K)=It(H)+It(K) and It(aH)=aIt(H) for real a identically. In particular It(H)It(K)=It(HK) for the elementary integrand HK represented on that refinement. This is a rearrangement of finitely many terms, not a limiting statement.

  3. Dependence on the representation is temporary. The definition attaches It(H) to a chosen elementary representation. Elementary Ito integrals do not depend on step representation proves that two representations that agree (dtP)-almost everywhere produce the same random variables almost surely at each fixed time, so that It(H) is a function of the (dtP)-class of H alone. Until then, every statement about an elementary integrand names the representation it uses.

The Axiom of Choice is declared because the standing hypothesis (H) is part of the Brownian interface of Elementary predictable Brownian integrands, which assumes it; the definition of the finite sum uses no choice. The countable-choice obligations inherited from that interface are declared as dependencies of this item.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Elementary Ito integrals do not depend on step representation

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let H and H be two elementary predictable integrands on [0,T] whose values agree (dtP)-almost everywhere, and let It(H), It(H) be their defining sums Ito integral of an elementary predictable process for the chosen representations. Then IT(H)=IT(H) almost surely, and in fact It(H)=It(H) almost surely for every deterministic t[0,T]. In particular, replacing a representation by a deterministic refinement of its partition, or by any other elementary representation of the same (dtP)-class, does not change the sums; the elementary integral is a function of that class.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a horizon T>0, elementary representations Hs=k=0m1ξk1(tk,tk+1](s) and Hs=l=0m1ξl1(ul,ul+1](s) with bounded coefficients measurable at the left endpoints, agreeing (dtP)-almost everywhere, and their defining sums.

[F1]

A (dtP)-almost-everywhere equality of two elementary processes, each predictable and hence product measurable, may be integrated by Tonelli: 0TΩHHdPdt=0. Tonelli's theorem for nonnegative measurable functions on a sigma-finite product Elementary predictable Brownian integrands

[F2]

For 0s<t the increment BtBs is independent of Fs, has law N(0,ts), mean 0 and second moment ts. Elementary predictable Brownian integrands Brownian covariance is equivalent to independent stationary normal increments Gaussian even moments for Brownian increments

[F3]

If YL1(P) is independent of a sub-sigma-algebra G, then E[YG]=EY almost surely: the constant EY is G-measurable, and for AG the factorization of expectations for the independent pair (Y,1A) gives E[Y1A]=EYP(A). Independent sigma-algebras and independent events Expectations factor over finite products of independent random variables Conditional expectation is unique almost surely

[F4]

For integrable Z and HG, E[E[ZG]H]=E[ZH] almost surely. If WL1, Z is G-measurable, and both ZW and ZE[WG] are integrable, then E[ZWG]=ZE[WG]. Tower property of conditional expectation Taking out what is known

[F5]

The defining sums are linear under a common refinement and I0(H)=0; adaptedness and path continuity are part of the definition. Ito integral of an elementary predictable process

[F6]

AC is declared for the conditional-expectation interface. The Axiom of Choice

Proof

technique · direct
1.1

Let 0=w0<w1<<wJ=T be the common refinement of the two partitions, and write Hs=j=0J1ηj1(wj,wj+1](s) and Hs=j=0J1ηj1(wj,wj+1](s), where ηj is the coefficient ξk of the block containing (wj,wj+1] and similarly for ηj; then ηj and ηj are bounded and Fwj-measurable, because FtkFwj whenever tkwj.

F5given
1.2

On each time interval the difference is the constant random variable ηjηj: HH=j(ηjηj)1(wj,wj+1] identically on [0,T], so Tonelli gives 0=0T ⁣ ⁣ΩHHdPdt=j=0J1(wj+1wj)Eηjηj. Every summand is nonnegative, wj+1wj>0, and therefore Eηjηj=0, that is, ηj=ηj almost surely for each j.

F1given
2.1

On the common refinement the elementary sum of item 5 can be taken over the refined partition: within each original block the increments telescope, j:(wj,wj+1](tk,tk+1]ξk(Bwj+1Bwj)=ξk(Btk+1Btk), a finite rearrangement of the defining sum. Applying this to H and to H, the difference of the two terminal sums is D:=IT(H)IT(H)=j=0J1(ηjηj)(Bwj+1Bwj) identically.

F5step 1.1
3.1

Write ζj:=ηjηj and Δj:=Bwj+1Bwj for each j. By [F2] the increment Δj is independent of Fwj and has law N(0,wj+1wj). Hence [F3] gives E[ΔjFwj]=0 and E[Δj2Fwj]=wj+1wj almost surely, because these conditional expectations of a variable independent of Fwj equal its unconditional mean. Since ζj is bounded and Fwj-measurable, [F4] yields E[ζjΔjFwj]=ζjE[ΔjFwj]=0 and E[ζj2Δj2Fwj]=ζj2(wj+1wj) almost surely.

F2F3F4step 2.1
4.1

Expanding the square, ED2=j,j=0J1E[ζjζjΔjΔj]. If j<j, then ζjΔjζj is Fwj-measurable and integrable, so the tower property and step 3.1 give E[ζjζjΔjE[ΔjFwj]]=0; by symmetry every off-diagonal term vanishes. The diagonal terms satisfy E[ζj2Δj2]=E[E[ζj2Δj2Fwj]]=E[ζj2](wj+1wj) by step 3.1.

F4step 3.1
5.1

Combining steps 4.1 and 1.2, ED2=j=0J1E[ζj2](wj+1wj)maxjζjj=0J1(wj+1wj)Eζj=0, where the last identity is the Tonelli computation of step 1.2. Since D is square-integrable, ED2=0 forces D=0 almost surely.

step 1.2step 4.1
6.1

The same computation at a deterministic time t[0,T] uses the truncated common partition {wjt}: its nonempty blocks are (wj,wj+1t] with wj<t, whose left endpoints are wj and whose coefficients ζj are Fwj-measurable, so the truncated sum is elementary; the difference of the truncated sums is jζj(Bwj+1tBwjt), each increment is independent of Fwj with second moment (wj+1t)(wjt), and the off-diagonal terms vanish by the same tower argument. The diagonal sum is jE[ζj2]((wj+1t)(wjt))maxjζjjEζj((wj+1t)(wjt)), and this is 0 by the Tonelli identity of step 1.2 restricted to [0,t]. Hence It(H)=It(H) almost surely for every t. A deterministic refinement of one partition is the special case in which the two representations are identically equal, and then the shared coefficients cancel in ζj, recovering that refinement changes nothing. AC enters only through the conditional-expectation facts [F3] and [F4]; the grid, the coefficients and the limits in the argument are all determined by the given representations.

step 5.1F2F4F6given

Source notes

Van der Vaart, Definition 5.20 and Lemma 5.22, first defines the integral on step processes and then checks that the definition does not depend on the representation; the isometry computation for the difference is the same conditional-centering expansion used here. The nearly-sure statement at every fixed time is what makes the notation 0tHdB well defined before the completion step of item 10.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Ito isometry for elementary integrands

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let H be an elementary predictable integrand on [0,T] with representation Hs=k=0m1ξk1(tk,tk+1](s) and defining sums It(H) Ito integral of an elementary predictable process. Extend those sums to [0,) by setting It(H):=IT(H) for tT. Then tIt(H) is a continuous square-integrable martingale relative to (Ft) Continuous-time adapted processes and martingales, and for every t[0,T] E[It(H)2]=E0tHs2ds=k=0m1E[ξk2](ttk+1ttk). By the representation independence of Elementary Ito integrals do not depend on step representation both sides depend only on the (dtP)-class of H.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a horizon T>0, an elementary representation Hs=k=0m1ξk1(tk,tk+1](s) with bounded Ftk-measurable ξk, its defining sums It(H), and 0stT.

[F1]

For 0u<v, the increment BvBu is independent of Fu and has law N(0,vu), hence mean 0 and second moment vu; for bounded Fu-measurable Z, E[Z(BvBu)Fu]=0 and E[Z(BvBu)2Fu]=Z(vu) almost surely. Elementary predictable Brownian integrands Brownian covariance is equivalent to independent stationary normal increments Gaussian even moments for Brownian increments Taking out what is known

[F2]

If YL1(P) is independent of a sub-sigma-algebra G then E[YG]=EY almost surely; here Y=BvBu and G=Fu qualify by [F1]. Independent sigma-algebras and independent events Expectations factor over finite products of independent random variables Conditional expectation is unique almost surely

[F3]

I(H) is adapted, I0(H)=0, and each It(H) is a finite sum of products of bounded coefficients with Gaussian increments, so EIt(H)< and EIt(H)2<; path continuity holds on the Brownian continuity event. Ito integral of an elementary predictable process

[F4]

For HG and integrable Z, E[E[ZG]H]=E[ZH], and E[ZWG]=ZE[WG] whenever WL1(P), Z is finite real and G-measurable, and both ZW and ZE[WG] are integrable. Tower property of conditional expectation Taking out what is known

[F5]

A martingale is exactly an adapted process with EMt< and E[MtFr]=Mr almost surely for all rt. Continuous-time adapted processes and martingales

[F6]

AC is declared for the conditional-expectation interface. The Axiom of Choice

Proof

technique · direct
1.1

Refining the partition of H if necessary so that s is a partition point, write the increments of the defining sum between the deterministic times st as It(H)Is(H)=kξk(Btuk+1Btuk)kξk(Bsuk+1Bsuk) over the refined partition 0=u0<<un=T; this is a finite rearrangement and does not change the values by the definition of the sums. Term by term, a block with uk+1s contributes 0, a block with ukt contributes 0, and every remaining block contributes ξk(BakBbk) with bk=max(s,uk) and ak=tuk+1, so that sbkakT and ξk is Fuk-measurable with FukFbk.

F3given
1.2

For each such block, BakBbk is independent of Fbk with mean 0 and second moment akbk by (H): E[BakBbkFbk]=0 and E[(BakBbk)2Fbk]=akbk almost surely.

F1F2given
2.1

For every remaining block, E[ξk(BakBbk)Fs]=E[ξkE[BakBbkFbk]Fs]=0 almost surely, because FsFbk, ξk is bounded and Fbk-measurable, and the inner conditional expectation vanishes by step 1.2; summing the finitely many blocks gives E[It(H)Is(H)Fs]=0, so E[It(H)Fs]=Is(H) almost surely by linearity of conditional expectation and the Fs-measurability of Is(H).

F4step 1.1step 1.2
2.2

For the variance, write Δkt:=Bttk+1Bttk for the blocks of the original partition, so that It(H)=kξkΔkt. For k<l the random variable Δkt is Ftl-measurable, because ttk+1tk+1tl, and ξk,ξlFtl; Each increment is in L2, and 2aba2+b2 shows that a product of two increments is integrable; bounded coefficients preserve these bounds. In the off-diagonal use of [F4], take W=Δlt and Z=ξkΔktξl; WL1, ZWL1, and ZE[WFtl]=0 is integrable. In the diagonal use, W=(Δkt)2L1 and Z=ξk2 is bounded. By (H) applied to the increment over the interval (tl,ttl+1] (which is empty, hence contributes 0, when ttl), E[ΔltFtl]=0 almost surely, so the tower property and taking out what is known give E[ξkΔktξlΔlt]=E[ξkΔktξlE[ΔltFtl]]=0. For the diagonal terms, the same identity gives E[ξk2(Δkt)2]=E[ξk2E[(Δkt)2Ftk]]=E[ξk2](ttk+1ttk), where the block contributes 0 when ttk.

F1F4step 1.2
3.1

Summing the diagonal terms of step 2.2 and using Hs2=kξk21(tk,tk+1](s) gives EIt(H)2=k=0m1E[ξk2](ttk+1ttk)=E0tHs2ds, finite because there are finitely many bounded coefficients.

step 2.2F3
4.1

Steps 2.1, 3.1 and [F3] show the martingale and isometry assertions on [0,T]. The constant extension from the statement is adapted and continuous; if s<T<t, the already proved identity gives E[It(H)Fs]=E[IT(H)Fs]=Is(H), while for Tst both sides equal IT(H). Thus [F5] makes the extended process a continuous square-integrable martingale on [0,). Independence of the representation is the content of item 6. AC is used only through the conditional-expectation facts [F2], [F4] and the Brownian interface (H); the partition, the blocks and the sums are fixed by the representation.

step 2.1step 3.1F3F5F6given

Source notes

Lawler, Proposition 3.2.1, proves precisely this package for simple processes: the integral is a martingale, and its variance is the integral of the square of the integrand (Proposition 3.2.1(iii)). The proof here separates the conditional-centering identity from the variance expansion; both use only independence and mean zero of future increments, not their full Gaussian law beyond the second moment.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Cross Ito isometry

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. For elementary predictable integrands H,K on [0,T] and every t[0,T], E[It(H)It(K)]=E0tHsKsds, where the sums It() are the elementary integrals of the chosen representations Ito integral of an elementary predictable process. Both sides depend only on the (dtP)-classes of H and K and are finite.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a horizon T>0, elementary representations of H,K on some partitions, their common refinement, and t[0,T].

[F1]

On the common refinement, H+K, HK and their scalar multiples are again elementary predictable integrands with bounded coefficients measurable at the left endpoints of that refinement; the defining sums are linear there, so It(H±K)=It(H)±It(K) identically. Ito integral of an elementary predictable process Elementary predictable Brownian integrands

[F2]

For every elementary predictable G, E[It(G)2]=E0tGs2ds is finite and tIt(G) is a continuous square-integrable martingale. Ito isometry for elementary integrands

[F3]

The pointwise identity (H+K)2(HK)2=4HK holds on [0,T]×Ω, and the same expansion applies to the random variables It(H)±It(K). Elementary predictable Brownian integrands

[F4]

AC is inherited from the elementary isometry and representation-independence interfaces. In particular, the proof of the elementary isometry uses conditional expectations, but its exported interface here is only the martingale and squared-isometry statement [F2]. The Axiom of Choice

Proof

technique · direct
1.1

Pass to the common refinement of the two partitions and keep the notation H,K for the refined representations; by [F1] both H+K and HK are elementary predictable integrands on that refinement, and It(H+K)=It(H)+It(K), It(HK)=It(H)It(K) identically, with all quantities square-integrable.

F1F2given
1.2

Applying the elementary isometry [F2] to H+K and to HK gives the two finite identities E[It(H+K)2]=E0t(H+K)2ds and E[It(HK)2]=E0t(HK)2ds.

F2given
2.1

Subtracting the second identity of step 1.2 from the first and expanding with [F3] gives E[(It(H)+It(K))2]E[(It(H)It(K))2]=E0t((H+K)2(HK)2)ds=4E0tHsKsds, where the right-hand side is finite because HK12(H2+K2) and both elementary integrands have finite energy.

F2F3step 1.2
3.1

The left-hand side of step 2.1 equals 4E[It(H)It(K)] by the algebraic expansion [F3], and 4 is invertible in R, so E[It(H)It(K)]=E0tHsKsds. Representation independence follows from Elementary Ito integrals do not depend on step representation applied to H and to K; the AC bookkeeping is exactly the inherited use recorded in [F4], not an additional conditional-expectation interface asserted by this lemma.

step 2.1F3F4given

Source notes

Van der Vaart, Lemma 5.22, records the bilinear form of the isometry as the polarized version of the squared identity. No additional source of randomness or integrability beyond the elementary isometry is used.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Density of elementary predictable processes in predictable L2

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix T>0 and let PT be the predictable sigma-algebra on [0,T]×Ω Progressively measurable and predictable processes, with the finite measure dtP. Then the classes of bounded elementary predictable integrands Elementary predictable Brownian integrands are dense in L2([0,T]×Ω,PT,dtP): for every PT-measurable H with 0T ⁣ ⁣ΩH2dPdt< and every ε>0 there is a bounded elementary predictable integrand G with (0T ⁣ ⁣Ω(HG)2dPdt)1/2<ε. Equalities are equalities of (dtP)-classes, so two elementary integrands whose difference vanishes almost everywhere represent the same approximant.

Facts & Assumptions

Given: AC, T>0, the predictable sigma-algebra PT generated by the sets (s,u]×C with 0s<uT, CFs, and {0}×C with CF0, the finite measure μ:=dtP on it, and the class E of (dtP)-classes of bounded elementary predictable integrands.

[F1]

E is a real vector space: on a common refinement of two elementary representations the coefficients of a sum, difference or scalar multiple are bounded and measurable at the left endpoints of the refinement, and the representation of H on a refinement is elementary. The constant L2(dtP) class belongs to E, represented by the elementary process 1(0,T] (and its scalar multiples); the literal constant process is not elementary because elementary processes vanish at time zero. Every element of E is bounded, say by G. Elementary predictable Brownian integrands Ito integral of an elementary predictable process

[F2]

The L2 norm on the quotient space of almost-everywhere classes is well defined and satisfies the norm axioms, including the triangle inequality; distances are computed by UV2=((UV)2dμ)1/2. The Lp norm descends to the quotient and makes Lp a normed space for 1p

[F3]

A finite intersection of generators of PT is empty, or a generator (s,u]×C, or a time-zero generator {0}×C; the family of finite unions of disjoint generators is an algebra generating PT. Progressively measurable and predictable processes

[F4]

If PD is a pi-system of sets and D is a lambda-system, then σ(P)D. Dynkin's pi-lambda theorem

[F5]

Every H0 that is PT-measurable admits nonnegative simple PT-measurable snH pointwise; each sn is a finite nonnegative linear combination of indicators of PT-sets and is bounded, its values being finitely many. Every nonnegative measurable function is the increasing limit of simple measurable functions

[F6]

If measurable functions satisfy fng for a single integrable g and fnf pointwise, then fnf2dμ0 whenever the domination is square-integrable: here 0snH with HL2, and Hsn0 pointwise. Dominated convergence

[F7]

μ({0}×C)=0 for every C: the section at ω is the singleton {0}, which is Lebesgue-null, so Tonelli gives μ({0}×C)=C ⁣ ⁣1{0}(s)dsdP=0. Tonelli's theorem for nonnegative measurable functions on a sigma-finite product

[F8]

AC is declared for uniformity with the ambient probability interfaces; the density argument itself is choice-free, and the implication bridge records the inherited obligations. The Axiom of Choice

Proof

technique · direct
1.1

Put D:={APT:1AE}, where the closure is taken in the L2(μ) metric of [F2]. By [F1] the set E contains every constant L2(μ) class (represented elementarily by its value on (0,T] and by 0 at time 0) and is closed under finite linear combinations of its elements: if U1,,UkE and a1,,akR, choose GiE with UiGi2<δ and use the triangle inequality to bound iaiUiiaiGi2 by δiai.

F1F2
1.2

Every generator of PT lies in D, and D contains and [0,T]×Ω. Indeed, for (s,u]×C with s>0 the process 1C1(s,u] is elementary on the partition 0<s<u<T when u<T, with coefficients 0,1C,0, and on the partition 0<s<u=T when u=T, with coefficients 0,1C; all coefficients are measurable at the left endpoints since 1CFs and constants are F0-measurable. For a generator (0,u]×C with CF0, use coefficients 1C,0 on 0<u<T when u<T, and the single coefficient 1C when u=T. For {0}×C the zero process is elementary with 1{0}×C022=μ({0}×C)=0 by [F7]. The one-block elementary process 1(0,T] represents 1[0,T]×Ω in L2(μ) because the omitted time-zero slice is null, so the whole space belongs to D; the zero elementary process represents 1, so D.

F1F7given
2.1

D is closed under complements: if 1A is approximated by bounded elementary Gn, then the bounded elementary processes 1(0,T]Gn represent the classes 1Gn and converge to 11A=1Ac in L2(μ) by the linearity of [F1] and the norm axioms of [F2].

F1F2step 1.1
2.2

D is closed under countable unions of pairwise disjoint sets: let A1,A2,D be pairwise disjoint with union A. Given ε>0, choose m so large that (j>mμ(Aj))1/2<ε/2, which is possible because the disjoint additivity of the finite measure μ gives jμ(Aj)=μ(A)T<; since each Aj lies in D, choose for jm a bounded elementary Gj with 1AjGj2<ε/(2m); the finite sum S:=jmGj is bounded and elementary on a common refinement by [F1]; the complement of jmAj inside A is j>mAj, so [F2] and the triangle inequality give 1AS2(μ(j>mAj))1/2+j=1m1AjGj2<ε/2+ε/2=ε, hence AD.

F1F2step 1.1
2.3

The family of finite intersections of generators of PT is the pi-system generated by the generators, and it is contained in D: by [F3] a finite intersection is empty, a generator, or a time-zero generator, and D contains and every generator by step 1.2.

F3step 1.2
3.1

The family D contains , the whole space [0,T]×Ω and is closed under complements (step 2.1) and under countable disjoint unions (step 2.2), so it is a lambda-system; step 2.3 shows that it contains the pi-system of finite intersections of generators, whose generated sigma-algebra is PT by [F3].

step 2.1step 2.2step 2.3
4.1

By Dynkin's pi-lambda theorem [F4], PT=σ(generators)D. Hence the indicator of every predictable set is an L2(μ) limit of bounded elementary processes.

F4step 3.1
5.1

Consequently every bounded PT-measurable simple function i=1kai1Ai is in E: approximate each indicator 1Ai by bounded elementary processes and combine the finitely many approximants with the coefficients ai using the closure under finite linear combinations from step 1.1.

step 1.1step 4.1
6.1

Let H0 be PT-measurable with HL2(μ). By [F5] choose nonnegative simple PT-measurable snH pointwise; each sn is bounded and lies in E by step 5.1. Since 0snH and HL2(μ), [F6] gives Hsn20, and for ε>0 one takes n with Hsn2<ε/2 and then a bounded elementary G with snG2<ε/2, so that HG2<ε by the triangle inequality.

F5F6step 5.1
7.1

For a general real HL2(μ), decompose H=H+H; both parts are nonnegative and PT-measurable with H±H, so both lie in L2(μ) and each is approximated to within ε/2 by a bounded elementary process by step 6.1; their difference is bounded and elementary on a common refinement by [F1] and is within ε of H by the triangle inequality.

F1step 6.1
8.1

Steps 6.1 and 7.1 prove the density statement for nonnegative and for general predictable L2 classes, with all approximants bounded and elementary; equalities of processes are equalities of (dtP)-classes throughout, which is exactly the qualification "modulo product-almost-everywhere equality". For each fixed m, step 2.2 selects only the finite list G1,,Gm, so the density argument itself uses no choice principle; the declared AC is inherited from the standing hypothesis (H) and ambient probability interfaces as recorded in [F8].

step 2.2step 6.1step 7.1F8given

Source notes

Van der Vaart, Lemmas 5.21--5.23, obtains density by a monotone-class argument on the predictable rectangles followed by simple approximation. The version here separates the two steps: the lambda-system argument produces indicator approximants for every predictable set, and the increasing simple approximation plus dominated convergence produces the general L2 approximant. No completeness of L2 is used at this stage; the completion step is item 10.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Ito integral for square-integrable predictable processes

Definition

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix a horizon T>0 and let PT be the predictable sigma-algebra on [0,T]×Ω Progressively measurable and predictable processes. Let H be a predictable process with E0THs2ds=[0,T]×ΩH2d(dtP)<, so that H is an element of the quotient space L2(dtP) over PT; its class is what is integrated. The Ito integral 0THsdBs, also written HB or IT(H), is defined as follows.

  1. Construction. By the density theorem Density of elementary predictable processes in predictable L2 there is a sequence (Hn) of bounded elementary predictable integrands Elementary predictable Brownian integrands with HnHL2(dtP)0. For such a sequence the elementary integrals IT(Hn) Ito integral of an elementary predictable process form a Cauchy sequence in L2(P): by the elementary isometry Ito isometry for elementary integrands and the well-definedness of the elementary integral, E(IT(Hn)IT(Hm))2=E0T(HnHm)2ds=HnHmL2(dtP)2, and the right-hand side tends to 0. Since L2(P) is complete Riesz-Fischer completeness of Lp for 1p, the classes IT(Hn) converge in L2(P); the limit is a class in L2(P), and 0THsdBs:=limnIT(Hn)in L2(P). The limit is a random variable only up to almost-sure equality; statements about it are statements about that class. The limit does not depend on the chosen sequence: if another elementary sequence KnH is used, then the elementary isometry and linearity give IT(Hn)IT(Kn)L2(P)=HnKnL2(dtP)HnH2+KnH20, so the two L2(P) limits agree.

  2. Integrals at a time. For t[0,T] put 0tHsdBs:=0THs1[0,t](s)dBs, the construction of clause 1 applied to the truncated process H1[0,t]. That process is predictable: H is PT-measurable and 1[0,t] is a deterministic predictable indicator, so the product is PT-measurable; and it is square-integrable because H1[0,t]H pointwise. The same construction applied to H itself gives t=T. The family (0tHdB)t[0,T] is a family of L2(P)-classes indexed by t; its continuous version is supplied by item 13, and no path property is asserted by this definition.

  3. Consistency with elementary integrands. If H is itself elementary, then the constant sequence Hn:=H is admissible in clause 1, so 0THdB is the limit of the constant sequence of elementary sums, namely the elementary sum IT(H) of Ito integral of an elementary predictable process. The same argument with H1[0,t] in place of H, and the finite telescoping of the elementary sum over a refinement containing t, gives 0tHdB=It(H) for every t[0,T]. In particular the general definition extends, rather than replaces, the elementary definition.

  4. Linearity in the integrand is not asserted here. Clause 1 defines each integral separately from an arbitrary approximating sequence; the linear and isometric properties of the extension are item 12. Until item 12 is proved, linearity may be used only for elementary integrands, where it is part of Ito integral of an elementary predictable process.

  5. Comparison with deterministic Riemann integration. The integral is a stochastic integral: the integrand is paired with the Brownian path through left-endpoint sums and an L2(P) limit. This definition does not assert convergence of arbitrary tagged Riemann--Stieltjes sums for a general predictable integrand. Particular integrands can have a pathwise interpretation: for H1 every tagged sum telescopes to BTB0, which is also its Ito integral by clause 3 (the value at time zero is irrelevant to its product-measure class). The notation 0THdB here always refers to the L2(P)-class defined above.

The Axiom of Choice is declared because the construction selects an approximating sequence and uses the completeness and conditional-expectation interfaces that assume it; the inherited obligations are declared as dependencies of this item. An alternative construction that avoids selecting the sequence is not needed, because clause 1 shows every sequence gives the same class.

LemmaStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

The general Ito integral is well defined

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let H be a predictable process on [0,T] with E0TH2ds<, and let (Hn) and (Kn) be two sequences of bounded elementary predictable integrands converging to H in L2(dtP). Then limnIT(Hn)=limnIT(Kn)in L2(P), so the integral 0THdB of Ito integral for square-integrable predictable processes does not depend on the approximating sequence. If H is any predictable process with H=H (dtP)-almost everywhere and finite energy, then 0THdB=0THdB almost surely; the integral is a function of the (dtP)-class alone.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a finite-energy predictable H, two elementary approximating sequences HnH and KnH in L2(dtP), and a predictable H with H=H almost everywhere and finite energy.

[F1]

For elementary predictable G,G on a common refinement, IT(G)IT(G)=IT(GG) identically and E(IT(G)IT(G))2=E0T(GG)2ds=GGL2(dtP)2. Ito isometry for elementary integrands Ito integral of an elementary predictable process

[F2]

Each of the sequences IT(Hn) and IT(Kn) is Cauchy in the complete space L2(P) and therefore has an L2(P) limit. The construction designates the limit obtained from one admissible approximating sequence as 0THdB; equality with the limit from every other sequence is what is proved below. Ito integral for square-integrable predictable processes

[F3]

The L2 triangle inequality and the identities UV2=0    U=V almost surely hold on the quotient space. The Lp norm descends to the quotient and makes Lp a normed space for 1p

[F4]

The elementary integral of the difference is the difference of the elementary integrals on a common refinement, and the class of a bounded elementary integrand depends only on its (dtP)-class. Ito integral of an elementary predictable process Elementary Ito integrals do not depend on step representation

[F5]

AC is declared for the ambient interfaces; the argument below only uses the two given sequences and the metric algebra of L2. The Axiom of Choice

Proof

technique · direct
1.1

Pass to a common refinement of the two elementary representations at each index and use [F1]: IT(Hn)IT(Kn)22=HnKnL2(dtP)2, a finite quantity depending only on the two indices.

F1given
1.2

The triangle inequality gives HnKn2HnH2+HKn20 as n, because both approximating sequences converge to H.

F3given
1.3

If H=H almost everywhere, then every approximating sequence for H is an approximating sequence for H: HnH2HnH2+HH2=HnH20, and likewise in the other direction.

F3given
2.1

By step 1.1 and step 1.2 the difference of the two sequences of elementary integrals converges to 0 in L2(P), while by [F2] each sequence converges; two convergent sequences with difference tending to 0 have the same limit, and by [F3] the limits agree as L2(P)-classes, that is, almost surely.

F2F3step 1.1step 1.2
3.1

Consequently the class 0THdB is independent of the approximating sequence; and by step 1.3, replacing H by an almost-everywhere equal H keeps the same admissible sequences and hence the same limit, so 0THdB=0THdB almost surely. Only the two given sequences are used, and AC enters only as the declared ambient interface [F5].

F4F5step 1.3step 2.1

Source notes

Van der Vaart, Definition 5.25 and Theorem 5.26, performs the same two descents: independence of the approximating sequence for a fixed integrand, and invariance under changing the integrand on a product-null set. Both are isometry statements for elementary differences, so no pathwise argument is involved.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Ito isometry and linearity in predictable L2

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix T>0. For predictable H,K with finite energy E0TH2ds,E0TK2ds< the integrals 0THdB of Ito integral for square-integrable predictable processes satisfy 0T(H+K)dB=0THdB+0TKdB,0T(aH)dB=a0THdB(aR), and the identities are equalities of L2(P)-classes (almost sure equalities). Moreover the map H0THdB is an isometry, E(0THdB)2=E0TH2ds=HL2(dtP)2, it takes values in the mean-zero subspace of L2(P), and the bilinear cross identity E[(0THdB)(0TKdB)]=E0THsKsds holds for all such H,K. In particular the image of the map is a closed subspace of L2(P) isometric to the predictable L2 space of H's, and H0THdB is injective up to the (dtP)-class.

Facts & Assumptions

Given: AC, the standing hypothesis (H), T>0, finite-energy predictable H,K, elementary sequences HnH and KnK in L2(dtP), and aR.

[F1]

Hn+Kn(H+K)2HnH2+KnK20 and aHnaH2=aHnH20, so Hn+Kn and aHn are admissible approximating sequences for H+K and aH. The Lp norm descends to the quotient and makes Lp a normed space for 1p

[F2]

For elementary G one has IT(G)= the elementary sum, EIT(G)2=E0TG2, EIT(G)=0, and for elementary G,G on a common refinement E[IT(G)IT(G)]=E0TGG. Ito integral of an elementary predictable process Ito isometry for elementary integrands Cross Ito isometry Continuous-time adapted processes and martingales

[F3]

Each integral 0TGdB is the L2(P)-limit of IT(Gn) for any admissible elementary sequence, and the limit is independent of the sequence. Ito integral for square-integrable predictable processes The general Ito integral is well defined

[F4]

On the quotient space L2(P), L2-convergence implies convergence of norms and of expectations: Xn2X2XnX2 and EXnEXXnX2; and the predictable L2 space, like every L2 space, is complete. The Lp norm descends to the quotient and makes Lp a normed space for 1p Basic algebra and order properties of conditional expectation Riesz-Fischer completeness of Lp for 1p

[F5]

The algebraic identities (X+Y)2(XY)2=4XY and X2Y2=(XY)(X+Y) hold for real random variables, and L2(P) is a real vector space of classes. Conditional expectation as an ae class

[F6]

AC is declared for the ambient interfaces. The Axiom of Choice

Proof

technique · direct
1.1

For each n the elementary integrals are linear on a common refinement, IT(Hn+Kn)=IT(Hn)+IT(Kn) and IT(aHn)=aIT(Hn) identically; by [F2] the isometry EIT(G)2=E0TG2, the mean identity EIT(G)=0 for elementary G, and the cross identity hold at every index.

F2given
1.2

By [F1] the sequences Hn+Kn and aHn are admissible for H+K and aH, so [F3] gives IT(Hn+Kn)0T(H+K)dB and IT(aHn)0T(aH)dB in L2(P), as well as IT(Hn)0THdB and IT(Kn)0TKdB.

F1F3given
2.1

Letting n in the linear identities of step 1.1 and using uniqueness of L2(P)-limits, 0T(H+K)dB=0THdB+0TKdB and 0T(aH)dB=a0THdB almost surely.

F3step 1.1step 1.2
2.2

Taking the limit in the elementary isometry of step 1.1 gives E(0THdB)2=limnEIT(Hn)2=limnE0T(Hn)2=HL2(dtP)2 by [F4] applied to the L2(P)-limits and to the L2(dtP)-convergence HnH. Likewise E0THdB=limnEIT(Hn)=0, and the triangle inequality gives E0THdB0THdB2<. So the image is mean-zero and isometric.

F4step 1.1step 1.2
3.1

For the cross identity use 4XY=(X+Y)2(XY)2 with X=0THdB and Y=0TKdB: by step 2.1, 4E[XY]=E(0T(H+K)dB)2E(0T(HK)dB)2=H+K22HK22=4E0THKds by step 2.2. All terms are finite by step 2.2.

F5step 2.1step 2.2
4.1

Steps 2.1--3.1 are exactly the linearity, isometry, mean-zero and cross-identity claims; injectivity follows because 0T(HK)dB2=HKL2(dtP), and closedness of the image follows because the image of a complete space under an isometry onto it is complete, hence closed, with the target metric restricted: the domain of classes is complete by [F4], and the isometry carries its Cauchy sequences to Cauchy sequences whose limits are the images of the domain limits. AC enters only through the declared ambient interfaces [F6]; the approximating sequences are the given ones and the limits are unique.

step 2.1step 3.1F4F6given

Source notes

Lawler, Sections 3.2.2--3.2.3, proves linearity and the variance rule for the extended integral by approximation. The presentation here keeps the two descents separate: item 11 supplies well-definedness of the limit, and the elementary isometry and cross isometry of items 7 and 8 are passed to the limit through the continuity of the L2 norm and of the expectation.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

The Ito integral process has a continuous martingale version

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let H be a predictable process with E0THs2ds< for every finite T. Then there is an adapted process M=(Mt)t0 with continuous paths such that Mt=0tHsdBs almost surely for every t0 Ito integral for square-integrable predictable processes, and M is a square-integrable martingale relative to (Ft) Continuous-time adapted processes and martingales: EMt2=E0tHs2ds< for every t. Any two such continuous versions agree at every time on one measurable event of probability one; in particular the continuous version is unique in this common-full-measure-event sense, and it is the only continuous square-integrable martingale whose value at each deterministic t is the integral class.

This conclusion is deliberately distinguished from the exact definition of indistinguishability in Process law, modification, and indistinguishability. On a noncomplete probability space the full equality set, although it contains the measurable probability-one event constructed below, need not itself be measurable. On a complete probability space the two notions coincide, because the complement of the equality set is then a measurable subset of a null set.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a finite-energy predictable H with E0TH2ds< for all finite T, and a horizon T>0.

[F1]

For every δ>0 there is a bounded elementary predictable G with HGL2(dtP)<δ. Density asserts existence, not an enumeration of all elementary integrands. Density of elementary predictable processes in predictable L2

[F2]

For elementary J the process I(J) is a continuous square-integrable martingale with E(It(J)Is(J))2=EstJ2du for st, and EIT(J)2=E0TJ2du. Ito integral of an elementary predictable process Ito isometry for elementary integrands

[F3]

Doob's L2 maximal inequality: for a discrete martingale Y0,,YN with YNL2, EmaxkNYk24EYN2; the sampled family (IkT/2m(J))k is a discrete martingale for the filtration (FkT/2m)k, by the tower property. Doob Lp maximal inequality Tower property of conditional expectation

[F4]

If a sequence 0ZnZ of nonnegative random variables increases pointwise, then EZnEZ; the dyadic grids Dm:={kT/2m:0k2m} are nested with union a countable dense subset D of [0,T], so supqDIq(J)=limmmaxqDmIq(J). Monotone convergence for the integral

[F5]

The rationals are dense in R, and each rational is a limit of dyadic rationals k/2n; a continuous function on [0,T] therefore satisfies supt[0,T]f(t)=supqDf(q). The rationals embed densely in the reals

[F6]

For every t the class 0tHdB is the L2(P)-limit of It(Hn) for every admissible elementary sequence HnH, and 0tHdB22=E0tH2ds; the integration map is linear and isometric in the predictable L2 variable. Ito integral for square-integrable predictable processes The general Ito integral is well defined Ito isometry and linearity in predictable L2

[F7]

If XnX in L2(P) then EXnXXnX20, and conditional expectations are L1-contractive: E[XnG]E[XG]1EXnX. Cauchy-Schwarz for random variables Basic algebra and order properties of conditional expectation

[F8]

AC supplies a selection from each nonempty set of elementary representations satisfying a prescribed error tolerance, simultaneously over countably many tolerances and integer horizons. The Axiom of Choice AC supplies countable selections and prescribed serial paths

Proof

technique · direct
1.1

Fix T>0 and choose, using [F8] on the nonempty sets supplied by [F1] with tolerance 22n, bounded elementary predictable Hn with HnHL2(dtP)22n; write Xtn:=It(Hn) for the continuous elementary process of [F2].

F1F2F8given
1.2

For every elementary predictable J and every S>0, writing the path supremum as its measurable version on the scaled dyadic grid, EsuptSIt(J)24E0SJ2du: on the full-measure event where I(J) is continuous, [F5] identifies the supremum over [0,S] with the supremum over the scaled dyadic grid, [F4] writes the latter as the increasing limit of the finite maxima over the nested grids Dm, [F3] bounds EmaxqDmIq(J)24EIS(J)2=4E0SJ2du for every m, and monotone convergence passes the bound to the limit.

F2F3F4F5
2.1

For each n, Hn+1Hn is elementary on a common refinement and Hn+1HnL2(dtP)22(n+1)+22n212n; applying step 1.2 to J=Hn+1Hn gives Ean24(212n)2=244n for the measurable random variable an:=suptDXtn+1Xtn, which equals the full supremum on the common event of continuity.

F2step 1.1step 1.2
3.1

Consequently En12nan2=n12nEan2n1243n< by monotone convergence for the nonnegative series [F4], so n2nan2< almost surely; the Cauchy--Schwarz inequality nan=n(2n/2an)2n/2(n2nan2)1/2(n2n)1/2 then gives nan< almost surely, on a measurable event AT of probability one, intersected with the common continuity event of the elementary processes.

F4step 2.1
4.1

On AT the sequence Xn converges uniformly on [0,T] to a limit; put Lt:=lim supnXtn and define Mt(T):=Lt when Lt is finite, and Mt(T):=0 otherwise. This is real-valued and Ft-measurable: Lt is an extended-real measurable limit superior and its finite-value event belongs to Ft. The resulting variable satisfies Mt(T)=limnXtn almost surely for every t; on AT the paths of M(T) are continuous, being uniform limits of continuous paths.

F2step 3.1
5.1

For every t[0,T] the sequence Xtn=It(Hn) converges to 0tHdB in L2(P) by [F6] applied to the truncations Hn1[0,t]H1[0,t]; combined with step 4.1 and the almost-sure uniqueness of limits, Mt(T)=0tHdB almost surely for every t[0,T].

F6step 4.1
5.2

For every t[0,T], E(Mt(T))2=limnE(Xtn)2=limnE0t(Hn)2ds=E0tH2ds<, using [F6] and the L2-norm continuity of the elementary integrals; hence M(T) is square-integrable.

F6step 2.1step 4.1
6.1

For 0stT and n, E[XtnFs]=Xsn by [F2], and step 5.1 and [F7] give XtnMt(T) and XsnMs(T) in L1(P) as well, so [F7] lets the conditional expectations pass to the limit: E[Mt(T)Fs]=Ms(T) almost surely.

F2F7step 5.1
7.1

Steps 4.1, 5.1, 6.1 and 5.2 show that M(T) is an adapted continuous square-integrable martingale version on [0,T]. If N is another continuous version on [0,T], then Mq(T)=Nq almost surely for each rational q[0,T]; intersecting the countably many measurable full-measure events and the two continuity events, and then invoking continuity, gives Mt(T)=Nt for every t[0,T] on one measurable event of probability one.

F5step 4.1step 5.1step 6.1step 5.2
8.1

Apply the construction on the horizons T=m, m=1,2,; two versions on adjacent horizons agree on the smaller one by the uniqueness of step 7.1 applied there, since the restriction of the larger-horizon version is a continuous version on the smaller horizon. For t0 put m(t):=max(1,t) and define Mt:=Mt(m(t)). This is well typed and Ft-measurable. On the intersection of the countably many overlap-agreement and continuity events, it coincides at every time with the compatible local versions, so its path is continuous. At each deterministic time it is a version of 0tHdB; hence the local martingale identities show that M is a square-integrable martingale with EMt2=E0tH2ds. Uniqueness on one measurable full-measure event over [0,) follows from the same rationals-and-continuity argument. AC supplies the approximants of step 1.1 simultaneously for all integer horizons, and is also inherited through the declared ambient interfaces.

step 7.1F8given

Source notes

Van der Vaart, Theorem 5.26(i)--(iii), proves the martingale and continuity conclusions using maximal estimates and an almost-sure uniformly convergent subsequence. Lawler, Proposition 3.2.4, gives a related summable-error uniform-convergence criterion for the integrands treated there. The proof here follows the summable-error route, which is why no almost-sure-subsequence theorem is needed: the weighted series n2nan2 is summable in expectation, and Cauchy--Schwarz converts it into almost-sure summability of the sup norms.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Doob maximal bound for the Ito integral

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let H be a predictable process on [0,T], where T0, with E0THs2ds<. Extend H by zero after T when applying the global continuous-version theorem, and let Mt=0tHsdBs be the continuous version of The Ito integral process has a continuous martingale version. Then Esup0tTMt24E0THs2ds. The left-hand side is finite and does not depend on the chosen version, since any two continuous versions are indistinguishable. Every continuous version of the integral process satisfies the same bound. The path supremum in this expectation means its measurable version SD=supqDMq on the countable scaled dyadic grid D (including both endpoints). Continuity identifies it with the path supremum on a measurable event of probability one. Indistinguishability here uses that full-event convention, as in the cited continuous-version theorem, without assuming completeness of the filtration.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a finite-energy predictable H on [0,T], and the continuous version M with Mt=0tHdB a.s. and EMt2=E0tH2ds.

[F1]

M is an adapted continuous square-integrable martingale with EMt2=E0tH2ds for every tT, and MT is the integral class at T. The Ito integral process has a continuous martingale version Ito isometry and linearity in predictable L2

[F2]

For each m1 the sampled family Yk:=MkT/2m, 0k2m, is a discrete martingale for the filtration (FkT/2m)k, by the tower property; hence Doob's L2 inequality gives Emaxk2mYk24EY2m2. Tower property of conditional expectation Doob Lp maximal inequality

[F3]

By the continuous-version theorem there is an event of probability one on which the path of M is continuous on [0,T]. On that event its supremum equals the supremum over the dyadic grid union D:=m{kT/2m}, which in turn is the increasing limit limmmaxk2mMkT/2m because the grids are nested. The rationals embed densely in the reals The Ito integral process has a continuous martingale version

[F4]

For 0ZmZ, EZmEZ, so the expectation of the supremum is the limit of the expectations of the finite-grid maxima. Monotone convergence for the integral

[F5]

Two continuous versions of the same integral process are indistinguishable, so their path suprema agree almost surely. The Ito integral process has a continuous martingale version Process law, modification, and indistinguishability

[F6]

AC is declared for the ambient interfaces. The Axiom of Choice

Proof

technique · direct
1.1

If T=0, M0=0 almost surely and both sides vanish. For T>0 and fixed m1 the finite-grid quantity maxk2mMkT/2m2 is integrable, and [F2] gives Emaxk2mMkT/2m24EMT2=4E0TH2ds.

F1F2
1.2

As m increases the grids {kT/2m:0k2m} are nested, so the unsquared maxima increase pointwise to the measurable random variable SD:=supqDMq. By [F3], SD=supt[0,T]Mt almost surely.

F3
2.1

Monotone convergence [F4] applies pointwise to Zm:=maxk2mMkT/2m2SD2. Hence, using the almost-sure equality in step 1.2, EsuptTMt2=ESD2=limmEZm4E0TH2ds, and the bound is finite because the right-hand side is finite.

F1F4step 1.1step 1.2
3.1

For any other continuous version N, intersect the fixed-time equality events {Nq=Mq} over the countable grid D and the two measurable continuity events. On the resulting measurable probability-one event the paths agree at every time by continuity, and their grid suprema agree. Thus the measurable supremum for N has the same expectation and satisfies the bound, even if N is not adapted. AC enters through the declared ambient interfaces [F6].

F5F6step 2.1

Source notes

Lawler, Proposition 3.2.4, uses discrete maximal estimates on refining grids to prove a uniform-convergence criterion. The expectation bound here follows directly from the library discrete Doob inequality with p=2 and monotone convergence; no fourth moment is assumed.

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-09-22Open item page →

Locally square-integrable predictable Brownian integrands

Definition

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. For this localization interface, assume in addition that (Ft)t0 satisfies the usual conditions: F0 contains every subset of every P-null event in F, and Ft=u>tFu for every t0. The earlier finite-energy construction does not require these additional conditions. Let H=(Hs)s0 be a predictable process Progressively measurable and predictable processes. Its energy process is At(ω):=0tHs(ω)2ds,t0, the integral of the nonnegative function sHs(ω)2; it may be +. The process H is locally square-integrable when At< almost surely for every finite t0. No uniform bound over t and no bound on EAt is imposed; the localization below converts almost-sure local finiteness into finite energy.

The following properties are part of the definition and are used in items 16 to 18.

  1. Measurability and adaptation of the energy. A is well defined and adapted: for each t the map (s,ω)Hs(ω)21[0,t](s) is product measurable, so Tonelli Tonelli's theorem for nonnegative measurable functions on a sigma-finite product expresses At=0Hs21[0,t](s)ds as an integral of measurable sections and, for tt, the section computation over [0,t] shows that At is Ft-measurable (the integral of a nonnegative measurable function is measurable in the parameter). Thus every level or sublevel event of At belongs to Ft. On the event G:=m1{Am<}, which has probability one, the maps tAt(ω) are nondecreasing, finite-valued and continuous on [0,): on each [0,m] the nonnegative integrand H(ω)2 has finite integral, and dominated convergence on that finite interval gives continuity. Moreover Gc is a null event in F, so completeness gives GcF0 and every subset of Gc belongs to every Ft.

  2. Canonical localization times. For n1 put σn:=inf{t0:Atn},inf:=+,τn:=σnn. Then τnn everywhere, the sequence (τn) is nondecreasing and τn almost surely: on G, for fixed m, one has σn>m and n>m for every sufficiently large integer n>Am, hence τn>m eventually. Each τn is a stopping time for (Ft) Continuous-time stopping times and stopped sigma-algebras. For tn the event {τnt} is Ω. For t<n, continuity and monotonicity give {τnt}G={Atn}G. Thus the symmetric difference of {τnt} and the Ft-event {Atn} is a subset of Gc and belongs to F0Ft by completeness. Hence {τnt}Ft.

  3. The localization localizes the energy. For every n and every t0, Atτnnalmost surely, because on G the process A is nondecreasing, tτnτnn, and Aτnn: if σn<n then continuity gives Aσn=n and τn=σn, while if σnn then τn=n and Ann by the definition of σn as an infimum. Consequently E0tHs21(0,τn](s)ds=EAtτnn<, so H1(0,τn] is a predictable integrand of finite energy and its L2 integral exists by Ito integral for square-integrable predictable processes. The same holds for H1[0,τn], which differs from H1(0,τn] only at s=0, a null set for dtP.

  4. Predictability of the truncations. The process 1[0,τn] is predictable for every stopping time τn, by the generator computation recorded in Progressively measurable and predictable processes, and the products H1(0,τn] and H1[0,τn] are therefore predictable, being products of predictable functions.

These conventions are the only sense in which the definition localizes: the times τn are canonical functions of the energy process, so no auxiliary sequence of stopping times is selected, and the constants n are the natural numbers. Completeness is what makes exceptional-path discrepancies measurable; right-continuity is retained as part of the standard usual-conditions convention used by the localization sources and downstream stopping theory. AC is declared because the ambient L2 integral interface assumes it; the definition of the energy process and of the times τn uses no choice beyond that interface.

Source notes

Van der Vaart, Definition 5.32 and Theorem 5.36, defines stochastic integration from an actual localizing sequence of stopping times and works throughout with filtrations satisfying the usual conditions. Eberle, Remark on the usual conditions and Lemma 5.11, likewise obtains the energy hitting times on the completed right-continuous filtration. The present page therefore keeps its finite-energy construction on raw filtrations but adopts the usual conditions at the point where almost-sure local energy, continuous versions and stopping must interact.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Localized Ito integral

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let H be a locally square-integrable predictable process with energy process A and canonical localization times (indexed by n1) τn=inf{t:Atn}n Locally square-integrable predictable Brownian integrands, and let M(n) denote the continuous version of the finite-energy integral H1(0,τn]dB The Ito integral process has a continuous martingale version. The filtration is assumed to satisfy the usual conditions, as required by the cited local-integrability definition. Choose the progressively measurable versions constructed in step 1.1 for these integrals and for the finite-energy integrals below. Continuity means continuity on a measurable probability-one event, and indistinguishability means equality at all times on such an event, as in that continuous-version theorem. Local square integrability and the canonical energy bounds are almost-sure assertions.

  1. Existence. There is an adapted process M=(Mt)t0 with continuous paths, called the localized Ito integral HB, such that for every n the stopped process Mτn is indistinguishable from M(n). Consequently M is a continuous local martingale relative to (Ft) with localizing sequence (τn), and for every n and t EMtτn2=EAtτnn.

  2. Characterization. If N is an adapted process with continuous paths and N0=0 such that Nτn is indistinguishable from M(n) for every n, then N is indistinguishable from M. In particular M is the unique continuous local martingale, up to indistinguishability, whose stopped finite-energy integrals are the M(n).

  3. Independence of the localizing sequence. Let (ρk) be a nondecreasing sequence of stopping times with ρk almost surely and E0tHs21(0,ρk](s)ds< for all k and all finite t, and let N be an adapted process with continuous paths and N0=0 such that Nρk is indistinguishable from the finite-energy integral of H1(0,ρk] for every k. Then N is indistinguishable from M.

  4. Stopping identity for finite-energy integrands. If G is a predictable process with E0TG2ds< and GB denotes its continuous version The Ito integral process has a continuous martingale version, with the same progressive version convention (extending G by zero after T), then for every stopping time σ and every 0tT (GB)tσ=0tGs1(0,σ](s)dBsalmost surely, and the two sides are continuous processes on [0,T], hence indistinguishable there. A global identity follows by applying this clause on each finite horizon when G has finite energy on every finite horizon. This clause is the finite-energy stopping identity used by item 17.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a locally square-integrable predictable H with energy A and canonical times τn, finite-energy predictable integrands G,Gk, stopping times σ,ρk, and the continuous versions GB and M(n) of items 13 and 15.

[F1]

H1(0,τn] is predictable and has finite energy EAtτnn, so its integral has a continuous version M(n) with E(Mt(n))2=EAtτn; the times (τn) are nondecreasing stopping times with τn a.s. Locally square-integrable predictable Brownian integrands The Ito integral process has a continuous martingale version

[F2]

For a finite-energy predictable G the continuous version GB satisfies GB=0tGdB at every deterministic t, and EsuptT(GB)t24E0TG2ds; hence (GB)tσ and the integrals of approximating integrands are controlled by the L2(dtP) distance. The Ito integral process has a continuous martingale version Doob maximal bound for the Ito integral

[F3]

For elementary predictable G the defining sum is a continuous process and the general integral of G1[0,t] equals that sum at every deterministic t; elementary integrals are linear on a common refinement, and G1[0,t] for elementary G is elementary on the refinement containing t. Ito integral of an elementary predictable process Ito integral for square-integrable predictable processes

[F4]

Every finite-energy predictable G is the L2(dtP)-limit of bounded elementary integrands, and the integral map is an isometry: 0T(GJ)dB2=GJL2(dtP). Density of elementary predictable processes in predictable L2 Ito isometry and linearity in predictable L2

[F5]

For a stopping time σ the indicator 1[0,σ] is predictable and every truncation 1[0,t] is predictable; products of predictable processes are predictable. Progressively measurable and predictable processes

[F6]

Finite pointwise limits of measurable functions, set to zero where no finite limit exists, are measurable. Almost-sure convergence dominated by an Lp random variable gives Lp convergence. Sequential suprema, infima, limsup, liminf, and pointwise limits of measurable functions are measurable Dominated convergence in Lp

[F7]

AC supplies countable selections of versions and approximating sequences; the localization times themselves are canonical. The Axiom of Choice AC supplies countable selections and prescribed serial paths

Proof

technique · direct
1.1

Measurable versions and stopping: for an adapted process X with almost-sure continuous paths and X0=0 almost surely, define X0j=0 and Xsj=Xk2j on (k2j,(k+1)2j], k0. For each finite horizon these step processes are progressive by [F5]'s predictable generators and predictable-to-progressive inclusion: the coefficient is measurable at the left endpoint, so its inverse images give the required rectangles. Put X^s=limjXsj where this limit exists finitely, and zero otherwise. By [F6] on each product sigma-algebra, X^ is progressive. It equals X at every time on the measurable full event of continuity and zero start. Thus it preserves every deterministic-time integral class and martingale identity. A progressive Y has adapted stopped values: for fixed t, r=tσ is Ft-measurable, and the map ω(r(ω),ω) into [0,t]×Ω is measurable into B([0,t])Ft by rectangle inverse images. Composition with the progressive restriction of Y gives YtσFt. Choose this construction for every finite-energy integral used below; [F7] permits the countably many required choices. All sequences indexed by positive integers are reindexed by n=j+1 when applying an interface indexed from zero.

F2F5F6F7given
2.1

Clause 4 for elementary G and finite-valued σ: refine the partition of G so that it contains the finitely many values of σ and the point t; on each block (tk,tk+1] the indicator 1sσ is constant in s with value 1σtk+1, and {σ<tk+1}={σtk}Ftk because σ takes only partition values, so G1[0,σ]1[0,t] is elementary with coefficients ξk1σtk+1; its defining sum is kξk1σtk+1(Btk+1tBtkt), which term-by-term equals kξk(B(tσ)tk+1B(tσ)tk)=(GB)tσ on the measurable full event where the progressive version agrees with the elementary sum at all times, by step 1.1.

F3F5givenstep 1.1
3.1

Clause 4 for elementary G and arbitrary σ: let σm:=2m2m(σm) be the dyadic ceiling of the bounded stopping time σm, a finite-valued stopping time with σmσm and σmσ; by step 2.1 and [F3], (GB)tσm=IT(G1[0,σm]1[0,t]) for every m.

F3step 2.1
4.1

As m: (GB)tσm(GB)tσ in L2(P) by continuity of the path and the maximal bound [F2] with [F6] (the measurable grid supremum of [F2] supplies the dominating random variable); and IT(G1[0,σm]1[0,t])IT(G1[0,σ]1[0,t]) in L2(P) because their indicators converge for Lebesgue-almost every time (the possible boundary s=σ is irrelevant), and they are dominated by G1[0,t]L2, and the integral is an isometry [F4]. Hence (GB)tσ=0tG1(0,σ]dB almost surely for elementary G and every stopping time σ.

F2F4F6step 1.1step 3.1
5.1

Clause 4 for general finite-energy G: approximate G by bounded elementary Gj in L2(dtP) [F4]; then (GjB)tσ(GB)tσ in L2(P) by the maximal bound [F2], and 0tGj1(0,σ]dB0tG1(0,σ]dB by the isometry and Gj1(0,σ]G1(0,σ]GjG; passing to the limit in the identities of step 4.1 gives clause 4 in general, and since both sides are continuous in t and agree at every deterministic t almost surely, they are indistinguishable.

F2F4step 4.1
6.1

Agreement of stopped finite-energy integrals (clause 1, first assertion): for mn apply clause 4 to G:=H1(0,τm], which has finite energy EAtτmm by [F1], and to the stopping time τn: (M(m))tτn=(GB)tτn=0tG1(0,τn]dB=0tH1(0,τn]dB=Mt(n) almost surely for every t, using 1[0,τn]1(0,τm]=1(0,τn] because τnτm. Both sides are continuous, so (M(m))τn and M(n) are indistinguishable.

F1step 5.1
7.1

Construction of M: put Mt:=limnMt(n) where the limit exists finitely, and zero otherwise. This is progressive by [F6] applied on every finite-horizon product sigma-algebra, since each M(n) was chosen progressive in step 1.1. In particular M0=0 everywhere and its stopped values are adapted by step 1.1. On the event A where all the agreements of step 6.1 hold, every M(n) is continuous and τn, fix ω and t; choose n with τn(ω)t; then for every mn, Mt(m)=Mtτn(m)=Mt(n) by step 6.1, so the sequence is eventually constant and Mt(ω)=Mt(n)(ω). Hence on A the process M agrees on [0,τn(ω)] with the continuous path of M(n), so M has continuous paths on the full-measure event A.

F1F6step 1.1step 6.1
8.1

M is a local martingale with localizing sequence (τn): by step 6.1 and the definition of M on A, Mτn is indistinguishable from M(n), and M(n) is a martingale. Since Mτn is adapted by step 1.1 and has the same deterministic-time values almost surely, it is itself a martingale; moreover EMtτn2=E(Mt(n))2=EAtτnn by [F1].

F1step 6.1step 7.1
9.1

Clauses 2 and 3: if N is continuous with N0=0 and Nτn=M(n) for all n, then for each t and each n with τnt one has Nt=Ntτn=Mt(n)=Mt almost surely, and letting n along the full-measure event where τn gives Nt=Mt almost surely for every t; continuity and the rationals argument make N indistinguishable from M. For clause 3, apply clause 4 twice: for each k,n, (Nρk)τn=(GkB)τn=0tGk1(0,τn]dB and (M(n))ρk=(GnB)ρk=0tGn1(0,ρk]dB with Gk=H1(0,ρk], Gn=H1(0,τn], and both integrands equal H1(0,ρkτn]; hence N(ρkτn) and M(ρkτn) are indistinguishable, and for each t on the full-measure event where ρkτnt eventually, Nt=Mt almost surely; continuity gives indistinguishability. The countable intersections of full events give the simultaneous identities; AC supplies the choices of versions and approximations through [F7].

F5F7step 5.1step 6.1step 8.1

Source notes

Van der Vaart proves the finite-energy stopping lemma (Lemma 5.28), the agreement of stopped integrals on overlaps (Lemma 5.33) and the existence of the localized continuous version (Theorem 5.36) in this order. Clause 4 is the stopping lemma in the form needed here; clauses 1--3 are Theorem 5.36 with the canonical energy times of Definition 5.32, and the agreement of stopped integrals is derived by applying the stopping lemma at the pairwise minimum of the two localization times.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Stopping an Ito integral

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let H be a locally square-integrable predictable process Locally square-integrable predictable Brownian integrands with localized integral HB in the progressively measurable version of Localized Ito integral, with its measurable-full-event convention for indistinguishability. The filtration satisfies the usual conditions and local energy is finite almost surely on every finite horizon, as required by the local-integrability definition. Let τ be a stopping time Continuous-time stopping times and stopped sigma-algebras. Then the process s(HB)sτ and the localized integral of the process 1[0,τ]H are indistinguishable: (HB)tτ=0t1[0,τ](s)HsdBsfor every t0, up to indistinguishability. In particular, for H of finite energy this reduces to the stopping identity of Localized Ito integral, and for τ it is the definition of the localized integral.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a locally square-integrable predictable H with energy A and canonical stopping times τn, n1, its localized integral HB, and a stopping time τ.

[F1]

1[0,τ] is predictable for every stopping time, and 1[0,τ]H is predictable and locally square-integrable with energy 0t1[0,τ]H2dsAt< almost surely for every finite t; its localized integral exists and is a continuous local martingale. Progressively measurable and predictable processes Localized Ito integral

[F2]

The canonical times τn satisfy τnn, τn a.s., 1(0,τn]H has finite energy EAtτnn, and (HB)τn is the finite-energy integral of H1(0,τn]; the finite-energy stopping identity gives (GB)tσ=0tG1(0,σ]dB for finite-energy G and any stopping time σ. Locally square-integrable predictable Brownian integrands Localized Ito integral

[F3]

If (ρk) is a nondecreasing sequence of stopping times with ρk a.s., each H1(0,ρk] has finite energy, and a continuous adapted N with N0=0 has Nρk indistinguishable from the finite-energy integral of H1(0,ρk] for every k, then N is indistinguishable from the localized integral of H. Localized Ito integral

[F4]

The chosen localized integral is progressive. The measurable stopped-evaluation argument of Localized Ito integral, proof step 1.1, shows that its stopped values are adapted; stopping also preserves continuity on the same full event. Thus N:=(HB)τ is an adapted continuous process with N0=0. The proof below uses the original sequence (τn) to localize N; the bounded sequence (ττn) is not asserted to be a localizing sequence. Continuous-time adapted processes and martingales Localized Ito integral

[F5]

AC is declared for the ambient interfaces. The Axiom of Choice

Proof

technique · direct
1.1

Put G:=1[0,τ]H and N:=(HB)τ, so that N is adapted with continuous paths and N0=(HB)0=0 by [F4]; by [F1] the localized integral GB exists and is a continuous local martingale. No local-martingale property of N is assumed at this stage.

F1F4given
1.2

For every k the stopped integral (HB)τk is the finite-energy integral of H1(0,τk] by [F2], and the finite-energy stopping identity applied with the stopping time τ gives (HB)ττk=(H1(0,τk]B)τ=0tH1(0,τk]1(0,τ]dB.

F2given
2.1

The integrand identity H1(0,τk]1(0,τ]=G1(0,ττk]=G1(0,τk] holds for every (s,ω) with s>0, the three expressions differing at most at s=0, a (dtP)-null set; hence 0tH1(0,τk]1(0,τ]dB equals the finite-energy integral of G1(0,τk], and the canonical sequence ρk:=τk consists of stopping times, is nondecreasing with ρk almost surely, (indexed by k1, or reindexed by k=j+1 when required), while G1(0,ρk] has finite energy E0tGs21(0,ρk]dsEAtρkk.

F2step 1.2
3.1

Steps 1.1, 1.2 and 2.1 verify the hypotheses of [F3] for the process N=(HB)τ and the localizing sequence (ρk): N is adapted and continuous with N0=0, and Nρk=(HB)ττk is indistinguishable from the finite-energy integral of G1(0,ρk] for every k. Therefore N is indistinguishable from the localized integral GB, which is exactly the identity (HB)tτ=0t1[0,τ]HdB up to indistinguishability.

F3step 1.1step 1.2step 2.1
4.1

The special cases are consistent: for τ one has 1[0,τ]1 and the identity is the definition of the localized integral; for finite-energy H it is the finite-energy stopping identity [F2] used in the proof; and for a deterministic τt0 it recovers the convention 0tH1[0,t0]dB=(HB)tt0. AC enters only through the declared ambient interfaces [F5], and the localizing sequence (τn) is canonical.

F2F5step 3.1given

Source notes

Van der Vaart, Lemma 5.28, proves the finite-energy stopping identity, and Theorem 5.36 plus Lemma 5.33 extends it to the localized integral. The proof here packages the extension as an application of the characterization clause of the localized integral, with the canonical localizing sequence ρk=τk of H: the stopping identity for each τk is step 1.2, and the a.e. integrand identity of step 2.1 expresses Nτk as the integral of G1(0,τk], so clause 3 of Localized Ito integral applies with ρk.

TheoremStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Quadratic variation of an Ito integral

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix T>0, let H be a locally square-integrable predictable process Locally square-integrable predictable Brownian integrands with localized integral M=HB in the progressive version of Localized Ito integral, under the usual conditions and almost-sure local-energy convention of the cited local-integrability definition, and let (πn) be a deterministic partition sequence of [0,T] with mesh tending to 0 Quadratic variation along a partition sequence. Write Qn(t) for the step-convention partial sum j:sj+1(n)t(Msj+1(n)Msj(n))2. Then sup0tTQn(t)0tHs2ds0in probability, and the partial-increment convention of Quadratic variation along a partition sequence has the same limit. Thus along every deterministic vanishing-mesh partition sequence the quadratic variation of the path of M is the random function t0tHs2ds, uniformly in probability. All full-path suprema use measurable versions: replace each process by zero outside a common measurable event of continuity before taking such a supremum. In all energy expressions, use the continuous representative equal to 0tHs2ds on G=r1{0rHs2ds<} and zero on Gc. The local-integrability definition proves that Gc is an F0-measurable null event. This normalization preserves all almost-sure identities and makes the energy finite and continuous everywhere. The step sums minus this energy are right-continuous, so their supremum equals that over a countable dense set including T.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a locally square-integrable predictable H with energy At=0tH2ds, its canonical times τm, m1 and localized integral M, a horizon T>0, and a deterministic partition sequence πn of [0,T] with mesh δn0.

[F1]

For every 0u<v the increment of the localized integral is the localized Ito integral of the predictable restriction, MvMu=(1(u,v]H)B evaluated after time v. If H has finite energy on the horizon under consideration, this localized integral is the finite-energy integral 0T1(u,v]HdB, and the isometry gives E(MvMu)2=EuvH2ds. Ito integral for square-integrable predictable processes Ito isometry and linearity in predictable L2 Localized Ito integral

[F2]

On a deterministic partition 0=s0<<sJ=T, put Yk=(Bsk+1Bsk)2(sk+1sk) for 0k<J and Nj=0k<jYk for 0jJ, so N0=0. The independent Gaussian increments have second and fourth moments h and 3h2, so EYk=0 and EYk2=2(sk+1sk)2. Relative to the finite-grid filtration Nj is a martingale by (H); cross terms have zero expectation by conditioning. Extend it constantly after J to apply discrete Doob with p=2. For nonnegative Z, the elementary inequality ε1{Z>ε}Z gives P(Z>ε)EZ/ε; applied to Z2 this also converts an L2 bound to a probability bound. Gaussian even moments for Brownian increments Brownian motion Doob Lp maximal inequality Tower property of conditional expectation

[F4]

For a finite-energy predictable G and a stopping time ρ, (GB)ρ is the finite-energy integral of G1(0,ρ]; for the canonical times of H, Mτm is the finite-energy integral of H1(0,τm] and Atτm=0tH21(0,τm]ds. Localized Ito integral Stopping an Ito integral Locally square-integrable predictable Brownian integrands

[F5]

For finite-energy G the maximal bound EsuptT(GB)t24E0TG2ds holds, and for elementary G the defining sums reduce to the explicit finite combinations of Brownian increments. Doob maximal bound for the Ito integral Ito integral of an elementary predictable process Elementary predictable Brownian integrands

[F6]

The two quadratic-sum conventions differ by the last partial increment squared. Probability continuity for increasing events follows by monotone convergence of indicators; decreasing continuity follows by complements. In particular almost-sure convergence of nonnegative random errors implies convergence in probability, by applying decreasing continuity to the tail-supremum events. Quadratic variation along a partition sequence Monotone convergence for the integral

[F7]

AC supplies the declared ambient interfaces and the countably chosen elementary approximations and versions; partition and localization times are given or canonical. The Axiom of Choice AC supplies countable selections and prescribed serial paths

[F8]

For real numbers and for random variables one has jajbj(jaj2)1/2(jbj2)1/2 and E[XY]X2Y2; these Cauchy--Schwarz inequalities control the polarization of the squared-increment sums and the expected products of the block sums. Cauchy-Schwarz for random variables

[F9]

Every predictable integrand of finite expected energy on [0,T] admits bounded elementary predictable approximations in L2(dtP). Density of elementary predictable processes in predictable L2

Proof

technique · direct
1.1

Brownian estimate: for a deterministic partition π of [0,T] with mesh δ and Nj as in [F2], independence of the Brownian increments gives ENJ2=k2(sk+1sk)22δT, and Doob's L2 inequality gives EmaxjNj28δT; since [B]tπ,stept=Nk(t)+sk(t)t where k(t)=max{j:0jJ, sjt} and sk(t)tδ, one has EsuptT[B]tπ,stept216δT+2δ2, which tends to 0; [F2]'s elementary probability bound turns this into uniform convergence in probability.

F2
1.2

For elementary H with partition 0=t0<<tm=T and a sub-interval (u,v], the increment MvMu=0T1(u,v]HdB is the elementary sum of the elementary integrand 1(u,v]H, whose coefficients are ξk on (utk,vtk+1], measurable at the left endpoints utktk; consequently MvMu=kξk(Bvtk+1Butk) over the at most two blocks meeting (u,v] when vu<mink(tk+1tk), and equals ξk(BvBu) when (u,v] is contained in a single block (tk,tk+1].

F1F5
2.1

Elementary refinement: fix a bounded elementary H with blocks (tk,tk+1], 0k<m, and a deterministic bound K for its coefficients on a common probability-one event. For sufficiently large n, δn<mink(tk+1tk), so each interval of πn crosses at most one elementary boundary. Refine by all these boundaries, and write Rk for the induced partition of [tk,tk+1]. Let Sk(n)(t) be the Brownian step sum on Rk, extended by zero before tk and its terminal value after tk+1. The refined integral sum is kξk2Sk(n)(t). Away from crossing intervals it equals Qn(t). On a crossing interval, the original increment has absolute value at most 2KωB(δn), while each of the at most two refined increments has absolute value at most KωB(δn), where ωB(δ)=supuvδ,u,v[0,T]BuBv on the continuous representative. This also bounds the discrepancy when the refined sum has included the boundary but the original interval is not yet complete. Adding the original squared contribution and the two subtracted refined squared contributions bounds the absolute discrepancy uniformly in t by 6mK2ωB(δn)2, which tends to zero almost surely by [F3].

F3F5step 1.2
3.1

Apply step 1.1 on each deterministic interval [tk,tk+1] to its translated Brownian increments and the induced mesh Rk, whose mesh is at most δn. Thus supt[tk,tk+1]Sk(n)(t)(ttk)0 in probability. Since At=kξk2(ttk+1ttk), the refined-sum error is bounded by K2 times the finite sum of these block errors. A finite union bound and step 2.1, with [F6] for its almost-sure vanishing error, give suptQn(t)At0 in probability for each bounded elementary H. No independence of ξk from these error suprema is needed, because the deterministic bound K is used.

F3F6step 1.1step 2.1
4.1

Finite-energy case: use [F9] and [F7] to choose HlH in L2(dtP) with Hl bounded elementary and set Nl:=HHl; by Cauchy--Schwarz in each partial sum, suptQn(H)(t)Qn(Hl)(t)Qn(Nl)(T)+2Qn(Nl)(T)1/2Qn(Hl)(T)1/2, and [F1] gives EQn(Nl)(T)=E0T(Nl)2ds0 and EQn(Hl)(T)=E0T(Hl)2dsC uniformly in n, so EsuptQn(H)Qn(Hl)0 as l uniformly in n; combined with step 3.1 for Hl and EsuptAHl(t)AH(t)HlH2Hl+H20, the finite-energy case follows by a two-parameter argument: for error threshold ε, split the total error into the quadratic-sum approximation, the elementary convergence error and the energy approximation, each at threshold ε/3. Their probabilities are bounded by 3/ε times the two expected approximation errors, plus the elementary error probability. The latter vanishes as n at fixed l, and the former vanish as l, uniformly in n.

F1F2F7F8F9step 3.1
5.1

Localized case: on the event {τmT} the processes M and Mτm agree on [0,T] and At(m)=At for tT by [F4], so the squared-increment sums of M coincide with those of the finite-energy integral Mτm there; consequently, for every ε>0, P(suptQn(M)A>ε)P(τm<T)+P(suptQn(Mτm)A(m)>ε), and the second term tends to 0 by step 4.1 while the first tends to 0 as m because τm almost surely.

F4step 4.1
6.1

Steps 3.1 and 5.1 establish uniform convergence in probability for the step convention; the partial-increment convention differs from the step value by at most the squared maximal oscillation of the continuous path of M over the partition intervals, which tends to 0 by [F3] and continuity of M, so both conventions have the same limit. The dyadic partitions are included; no almost-sure dyadic conclusion is asserted for general H. AC covers the declared interfaces and the countable approximating choices in [F7].

F3F6F7step 3.1step 5.1

Source notes

Van der Vaart, Lemma 5.77, uses elementary approximation and localization for covariation with a locally bounded predictable integrand. Lawler, Theorem 3.2.6, treats continuous or piecewise-continuous integrands and regular meshes. Neither is invoked as the full arbitrary-predictable, arbitrary-partition claim: the Brownian estimate, refinement error, finite-energy approximation and localization needed here are proved explicitly.

CorollaryStatement: Literature-sourcedProof: AI-adaptedaudited 2026-09-22Open item page →

Deterministic Ito integrals are Gaussian

Statement

Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix T>0 and let hL2[0,T] be deterministic, choose a Borel representative of its Lebesgue-equivalence class, and set h(s,ω):=h(s). This process is predictable with finite energy. Then the Ito integral 0ThsdBs Ito integral for square-integrable predictable processes is centered normal with variance 0Th2ds: its law is N(0,0Th2ds) in the convention of Standard normal and normal laws, where N(0,0) is the Dirac law at 0. More generally, for deterministic h1,,hdL2[0,T] the vector of integrals is jointly Gaussian in the sense of Multivariate normal law, including singular covariance: its law is Nd(0,Σ) with Σjk=0Thj(s)hk(s)ds. In particular the covariance of the pair is Cov(hjdB,hkdB)=hjhk, the integrals are uncorrelated exactly when hjhk=0, and integrals of deterministic integrands with disjoint supports are independent.

Facts & Assumptions

Given: AC, the standing hypothesis (H), a horizon T>0, deterministic h,h1,,hdL2[0,T] represented by Borel functions, and real coefficients c1,,cd.

[F1]

A deterministic step function is an elementary predictable integrand with deterministic coefficients, and its Ito integral is the finite sum kakm(Btk+1mBtkm); the Brownian increments over disjoint intervals are independent with laws N(0,Δk) and mean 0. Elementary predictable Brownian integrands Ito integral of an elementary predictable process Brownian motion

[F2]

A finite linear combination of independent centered normal variables is centered normal, and a N(0,σ2) variable has characteristic function teσ2t2/2, including σ=0; a Borel probability law on R is determined by its characteristic function. Characteristic functions under affine maps and independent sums Characteristic function of a normal law Uniqueness of a law from its characteristic function

[F3]

Convergence in L2(P) implies convergence in probability, which implies weak convergence of the laws. Weak convergence tests bounded continuous real functions; applying it separately to xcos(tx) and xsin(tx) and then combining the two real limits gives convergence of the complex characteristic functions. Convergence in probability Convergence in probability implies convergence in distribution Weak convergence of borel probability measures

[F4]

The integration map on predictable L2 is linear and isometric, and the integral of h is the L2(P)-limit of the elementary integrals of any admissible elementary approximation; the approximation hm is admissible because hmh in L2(dtP) equals the deterministic L2[0,T] distance. Ito isometry and linearity in predictable L2 The general Ito integral is well defined Ito integral for square-integrable predictable processes

[F5]

If hmh in L2[0,T], the reverse triangle inequality in the stated normed space gives hm2h2hmh20. Hence 0T(hm)2ds=hm22h22=0Th2ds. The Lp norm descends to the quotient and makes Lp a normed space for 1p

[F6]

A Borel probability law on Rd is Nd(0,Σ) exactly when every projection uX has law N(0,uTΣu); such a vector has mean 0 and covariance Σ. Multivariate normal law, including singular covariance

[F7]

Under AC, hence Countable Choice, finite linear combinations of box indicators are dense in L2(R). Extend h by zero outside [0,T] and approximate that extension by such a box-step function. Its restriction to [0,T] agrees almost everywhere with a function kak1(tk,tk+1] after adjoining the finitely many box endpoints and 0,T to one partition. Thus deterministic step functions of the required elementary form are dense in L2[0,T]. Finite linear combinations of box indicators are dense in Lp(Rn) for 1p< AC supplies countable selections and prescribed serial paths The Axiom of Choice

Proof

technique · direct
1.1

For a deterministic step function hm as in [F1], the integral kakm(Btk+1mBtkm) is a finite sum of independent centered normal variables with variances (akm)2Δkm, so by [F2] its law is N(0,σm2) with σm2=k(akm)2Δkm=0T(hm)2ds; in particular its characteristic function is φm(t)=eσm2t2/2, and its mean is 0.

F1F2
2.1

For general deterministic hL2[0,T], choose by [F7] step functions hmh in L2[0,T]; by [F4] the elementary integrals converge to 0ThdB in L2(P), hence in probability and weakly by [F3]. Apply the real-valued weak-convergence test separately to cos(tx) and sin(tx) and combine the limits to obtain pointwise convergence of characteristic functions: φ(t)=limmφm(t)=limmeσm2t2/2=eσ2t2/2 with σ2=0Th2ds, using [F5] for the convergence of variances and continuity of the exponential.

F3F4F5F7step 1.1
3.1

By [F2] the function teσ2t2/2 is the characteristic function of N(0,σ2) and determines a unique Borel law, so the law of 0ThdB is N(0,σ2); consequently it is centered with variance 0Th2ds, and the case σ=0 (that is, h=0 in L2) gives the Dirac law at 0.

F2step 2.1
4.1

For a finite family, linearity [F4] gives jcj0ThjdB=0T(jcjhj)dB in L2(P), and step 3.1 applied to the deterministic integrand jcjhj shows that this projection is N(0,0T(jcjhj)2ds)=N(0,cTΣc) with Σjk=0Thjhkds; by [F6] the vector of the d integrals therefore has law Nd(0,Σ), hence is jointly Gaussian with mean 0 and covariance Σ.

F4F6step 3.1
5.1

The covariance identity is the jk entry of Σ; the zero-covariance case is uncorrelatedness, which for the jointly Gaussian pair means independence, and disjoint supports make every mixed integral hjhk vanish, so the corresponding integrals are independent. Deterministic integrands are the only class treated here. AC supplies the inherited ambient interfaces and the Countable Choice hypothesis of the deterministic density theorem recorded in [F7]; no further approximation premise is assumed.

F6F7step 4.1given

Source notes

Lawler, Exercise 3.8, states that deterministic integrands produce Gaussian integrals with variance equal to the squared L2 norm, and Section 3.2 built the step-function case from independent Gaussian increments. The corollary here identifies the limit law by characteristic functions rather than by citing a weak-convergence theorem for Gaussian parameter families, so that every supplier lies on an earlier page of this track; the multivariate clause is the defining projection property of the multivariate normal law.

5 · Examples, counterexamples and false statements

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