How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
The Ito Integral with Respect to Brownian Motion
1 · Prerequisites
- Absolute and Conditional Convergence; Rearrangement; Products
- Algebraic Closure, Embeddings, and Separability
- Algebraic Extensions, Extension Degree, and Finite Fields
- Areas of Elementary Plane Figures
- Binary Operations, Monoids, Groups and Subgroups
- Brownian Motion Construction and Continuity
- Brownian Motion, Markov Properties and Hitting Times
- Brownian Path Properties
- Central Limit Theorems
- Characteristic Functions Inversion and Continuity
- Compactness
- Compactness in Metric Spaces
- Complete Metrizability, Čech-Completeness, and Baire Category
- Completeness, Completion, and Uniform Continuity
- Complex Lp Spaces and Test-Function Conventions
- Composition Series, the Jordan–Hölder Theorem and Solvable Groups
- Conditional Distributions and Regular Conditional Probability
- Conditional Expectation
- Congruences, the Integers Modulo n and the Chinese Remainder Theorem
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Convexity
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Countability Axioms and Cardinal Functions
- Cyclic Groups and Direct Products
- Darboux, L'Hôpital, and Taylor's Theorem
- Density Separability and Convolution in Lᵖ
- Determinants of Matrices over a Commutative Ring
- Diagonalisation and the Minimal Polynomial
- Discrete Time Martingales
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Divisibility, Greatest Common Divisors and Bézout's Identity
- Dual Spaces, Bilinear and Quadratic Forms, and Sylvester's Law of Inertia
- Eigenvalues, Eigenvectors and the Characteristic Polynomial
- Filters and Ultrafilters
- Finite Counting, Factorials and Binomial Coefficients
- Finite Probability and the Probabilistic Method
- Foundations of the Real Numbers for Analysis
- Fourier Transform Convolution and Approximate Identities
- Fubini and Change of Variables
- Function Space Topologies and the Exponential Law
- Fundamental Trigonometric Identities
- Gaussian Elimination, Elementary Matrices and Reduced Row Echelon Form
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Group Homomorphisms and the Isomorphism Theorems
- Hausdorff via the Diagonal
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Improper and Parameter-Dependent Multiple Integrals
- Improper Integrals
- Independence Borel Cantelli and Zero One Laws
- Infinite Product Measures and Kolmogorov Extension
- Inner Product Spaces, Gram-Schmidt, Projections and Adjoints
- Lebesgue Measure on Euclidean Space
- Lebesgue-Stieltjes Measures and Distribution Functions
- Limits of Real Functions
- limsup, liminf, and Subsequential Limits
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Martingale Inequalities and Convergence
- Matrices, the Matrix of a Linear Map, and Change of Basis
- Measurable Functions and Simple Approximation
- Measures and Their Basic Properties
- Metric Spaces
- Mixed Partials, Taylor Formulae, and Extrema
- Modes of Convergence Egorov and Lusin
- Modes of Convergence for Random Variables
- Monotone Functions, Discontinuities, and Continuity Sets
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Normal Subgroups and Quotient Groups
- Order, Zorn's Lemma, and the Axiom of Choice
- Outer Measure and the Caratheodory Extension Theorem
- Partitions of Unity and Paracompactness
- Polynomial Rings, the Division Algorithm and Roots
- Power Series and Real-Analytic Functions
- Primes, Euclid's Lemma and the Fundamental Theorem of Arithmetic
- Probability Spaces Random Variables and Expectation
- Product Measures and the Fubini Tonelli Theorems
- Properties of the Integral and the Working FTC
- Radon Measures and the Riesz Markov Kakutani Theorem
- Relations, Functions, and Quotients
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Roots, Rational Powers, and Classical Inequalities
- Separation Axioms: the Hierarchy
- Sequences and Limits
- Sequences and Series of Functions; Uniform Convergence
- Series: Convergence and the Nonnegative Tests
- Sigma Algebras and Borel Sets
- Signed and Complex Measures Hahn and Jordan
- Simple Field Extensions and the Construction of the Complex Numbers
- Sine, Cosine, and the Definition of Pi
- Splitting Fields
- Subspaces, Products, and Quotients
- Suprema and Infima
- Sylow's Theorems, p-Groups and Nilpotent Groups
- Symmetric Groups, Cycle Decomposition and the Sign Homomorphism
- The Cantor Set, Baire Category, and Measure Zero in ℝ
- The Complex Exponential and Euler's Formula
- The Derivative and the Mean Value Theorems
- The Determinant of a Linear Operator, Cofactors and Cramer's Rule
- The Exponential Function
- The Fundamental Theorem of Algebra
- The Fundamental Theorem of Finite Abelian Groups
- The Galois Correspondence
- The Inverse and Implicit Function Theorems
- The Lebesgue and Riemann Integrals Compared
- The Lebesgue Integral and the Convergence Theorems
- The Logarithm and General Powers
- The Lᵖ Spaces Holder Minkowski and Riesz Fischer
- The Maximal Function and Lebesgue Differentiation
- The Radon Nikodym Theorem and Lebesgue Decomposition
- The Riemann Integral in Rᵐ and Jordan Content
- The Riemann Integral: Definition and Integrability
- The Spectral Theorem, Positive Operators and Singular Value Decomposition
- The Topology of Euclidean Space
- The Total Derivative in ℝᵐ → ℝⁿ
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topology of ℝ
- Triangularisation, Generalised Eigenspaces and Jordan Canonical Form
- Urysohn's Lemma and the Tietze Extension Theorem
- Vector Spaces, Linear Subspaces, Span and Direct Sums
- Weak Convergence Tightness and Representation
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 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 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
Continuous-time adapted processes and martingales
Definition
Assume the Axiom of Choice The Axiom of Choice. Fix a probability space with a continuous-time filtration in the sense of Continuous-time filtrations and all-pairs martingales. All processes in this definition are real-valued and indexed by ; 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.
-
Adapted. is adapted to when is -measurable for every . This is exactly the notion of Continuous-time filtrations and all-pairs martingales.
-
Stopped process. For a stopping time for Continuous-time stopping times and stopped sigma-algebras the stopped process is with the convention , so no value is ever required and identically. This formula defines a pathwise family; adaptedness of alone does not assert measurability or adaptedness of its stopped values. If in addition for a deterministic constant , then , and only the values of on enter. Stopping at a stopping time is not the same as replacing a process by a modification; it is a pathwise operation.
-
Martingale. is a martingale (an all-pairs continuous-time martingale) relative to when it is adapted, for every , and for all 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 off one null set. At the identity reduces to the known-variable case. The word "continuous-time" refers to the index set only and does not assert path continuity.
-
Local martingale. is a local martingale relative to when it is adapted, , and there exist stopping times with and almost surely such that for every the stopped process is a martingale in the sense of clause 3. The sequence is called a localizing sequence. Equivalently, every is a martingale: adaptedness makes the integrable variable measurable with respect to every , so the constant process with value is a martingale and may be added to, or subtracted from, each stopped process. The centering merely makes every localized process start at ; apart from the required integrability of , no claim is made that is integrable at a positive deterministic time, and no claim is made that has continuous paths.
-
Path and integrability attributes. A process has continuous paths when is continuous on for every in an event of probability one; the usual almost-sure path conventions of Process law, modification, and indistinguishability apply. A martingale is square-integrable when for every , and -bounded when . 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.
- A martingale is a local martingale. If is a martingale, the constant sequence , , localizes it: the stopped process is again a martingale by the martingale identity applied at the deterministic times . The converse fails; a local martingale need not be a martingale, and no such implication is used in this development.
- Localization after a separately justified stopping operation. Suppose localizes , is a stopping time, is adapted, and each is a martingale. Then localizes . Indeed it still increases to infinity, , and the pathwise identity 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 is not a substitute for : its almost-sure limit is , 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.
Progressively measurable and predictable processes
Definition
Assume the Axiom of Choice The Axiom of Choice. Let be a probability space with a continuous-time filtration Continuous-time filtrations and all-pairs martingales. All processes here are real-valued and indexed by . 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.
-
Progressively measurable. A process is progressively measurable relative to when for every the restricted map , , is measurable for the product sigma-algebra The product sigma-algebra and its finite iterates.
-
Time-zero and interval generators. On the product space , let be the sigma-algebra generated by the family The interval generators with are included, so with is a generator. The sigma-algebra 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 is predictable when the map is -measurable. For a finite horizon we write for the sigma-algebra on generated by the same family restricted to together with the time-zero generators; this is the trace of on . Indeed, the trace of an interval generator is empty when , and otherwise is , while time-zero generators are unchanged. Conversely every listed finite-horizon generator is such a trace.
-
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 , hence ; the time-zero generator has -measure zero for every . A set in has its section at each fixed time in : 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 is Borel in time, by the same sigma-algebra argument. (b) If a process is predictable then it is progressively measurable: for the section is -measurable -measurable, and the progressive-measurability claim is the restriction of the joint map to ; the restriction of a -measurable map to is measurable for because every generator with lies in that product sigma-algebra and the generators with have intersection with of the form with and , or the empty set when . The time-zero generators also lie in .
The family 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 and whenever , , while is disjoint from every interval generator, including . Two time-zero generators intersect in with . Thus the family consisting of the whole space together with finite intersections of generators is a pi-system generating ; 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 of time defines a predictable process exactly when is Borel measurable: the sets for which form a sigma-algebra containing the intervals and , hence all Borel sets. Conversely, take any fixed (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 and are predictable for every deterministic , and the process for a stopping time Continuous-time stopping times and stopped sigma-algebras is predictable, since is a countable union of generators: for rational one has . The complement of that set inside is the event of the indicator, so 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 is used or assumed. Apart from the inherited ambient assumption just recorded, the constructions in this definition are choice-free.
Adapted continuous processes are progressively measurable
Statement
Let be a probability space with a continuous-time filtration , and let be a real process that satisfies is -measurable for every , and has continuous paths, in the strong sense that is continuous on for every . Then is progressively measurable and predictable relative to in the sense of Progressively measurable and predictable processes, including at time zero under the generator convention , . No choice principle is used. Here a filtration means an increasing family of sub-sigma-algebras of . 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 with , the conclusion holds for the modification that is set equal to off provided ; 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 , a real adapted process with continuous paths everywhere, a horizon , and for the dyadic grid , .
is adapted: is -measurable for every ; in particular is -measurable for . Continuous-time adapted processes and martingales
Each rectangle , where and for some , belongs to , since . Finite unions of these rectangles also belong to that sigma-algebra. Progressively measurable and predictable processes
A pointwise limit of measurable functions into 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
The generators of the predictable sigma-algebra are the sets with and the time-zero sets with . The set is predictable, being the union of the generator and the time-zero generator . Progressively measurable and predictable processes
Proof
Fix and define, for , For a Borel set the preimage is , a finite union of measurable rectangles of , since is -measurable and .
Each is measurable for , and for every the identity holds: at both sides equal , and for the left endpoints of the dyadic intervals containing tend to , so path continuity gives .
Each 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 is -measurable and each interval is a generator interval, while the time-zero term is with .
By [F3] the pointwise limit restricted to is -measurable; was arbitrary, so is progressively measurable.
For each fixed the restriction of to is a pointwise limit of the predictable processes restricted to , hence is predictable on that horizon by [F3]; and the horizon- pieces assemble to a globally predictable process because and a set is predictable as soon as all its intersections with the countably many sets , , are.
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: at every stage and the generator , , was used in step 2.2. For the final statement about , the map is -measurable (its Borel inverse images are ), has continuous paths everywhere, and agrees with on . Apply the conclusion to . No grid point, approximant or limit in the argument is chosen: the dyadic grids and the left endpoints are fixed functions of , and pointwise limits are unique.
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 , . The proof explicitly supplies the fixed-time measurable maps and does not invoke any conditional-expectation existence theorem.
Elementary predictable Brownian integrands
Definition
Assume the Axiom of Choice The Axiom of Choice, and fix a probability space with a continuous-time filtration Continuous-time filtrations and all-pairs martingales and a standard Brownian motion Brownian motion on it. Standing hypothesis (H). is adapted to and for all the increment is independent of and has law . 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 . An elementary predictable Brownian integrand on is a process of the form where is a finite partition of , each is a bounded real -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 , and the supremum norm of the representation is . The integrand itself is the process ; 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.
-
Predictability. is predictable Progressively measurable and predictable processes. Indeed, for a Borel set , a finite union of generators of the predictable sigma-algebra because and is a time-zero generator. Consequently is progressively measurable and measurable for the product sigma-algebra , and belongs to : with one has .
-
Endpoint and null-set conventions. Replacing the intervals by makes the value at zero for every elementary integrand. More generally, if two elementary integrands agree for all except at finitely many deterministic times, then they agree -almost everywhere, since a finite set of times is Lebesgue-null and Tonelli computes . All integrands and all integrals below are therefore elements of the quotient spaces of and ; 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.
-
Deterministic coefficients. If every is a deterministic real number, is a deterministic step function on , 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.
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 adapted to the filtration, with increments independent of of law . Fix and an elementary predictable integrand with bounded -measurable coefficients . The Ito integral of against is the process also written or . The sum is finite and is evaluated with the Brownian path of the given representative; on the event where is continuous it is continuous in , and because for every .
Three conventions are part of the definition.
-
Adaptedness and continuity. For fixed , each summand is -measurable: if , the Brownian difference and hence the summand are zero; if , then , while is -measurable for every because . Thus is adapted. For each fixed the map 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.
-
Linearity on a common refinement. If and are elementary integrands and a partition refines both representations, then the defining sums of , , and are taken over that common partition, and the finite sums give and for real identically. In particular for the elementary integrand represented on that refinement. This is a rearrangement of finitely many terms, not a limiting statement.
-
Dependence on the representation is temporary. The definition attaches to a chosen elementary representation. Elementary Ito integrals do not depend on step representation ↗ proves that two representations that agree -almost everywhere produce the same random variables almost surely at each fixed time, so that is a function of the -class of 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.
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 and be two elementary predictable integrands on whose values agree -almost everywhere, and let , be their defining sums Ito integral of an elementary predictable process for the chosen representations. Then almost surely, and in fact almost surely for every deterministic . In particular, replacing a representation by a deterministic refinement of its partition, or by any other elementary representation of the same -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 , elementary representations and with bounded coefficients measurable at the left endpoints, agreeing -almost everywhere, and their defining sums.
A -almost-everywhere equality of two elementary processes, each predictable and hence product measurable, may be integrated by Tonelli: . Tonelli's theorem for nonnegative measurable functions on a sigma-finite product Elementary predictable Brownian integrands
For the increment is independent of , has law , mean and second moment . Elementary predictable Brownian integrands Brownian covariance is equivalent to independent stationary normal increments Gaussian even moments for Brownian increments
If is independent of a sub-sigma-algebra , then almost surely: the constant is -measurable, and for the factorization of expectations for the independent pair gives . Independent sigma-algebras and independent events Expectations factor over finite products of independent random variables Conditional expectation is unique almost surely
For integrable and , almost surely. If , is -measurable, and both and are integrable, then . Tower property of conditional expectation Taking out what is known
The defining sums are linear under a common refinement and ; adaptedness and path continuity are part of the definition. Ito integral of an elementary predictable process
AC is declared for the conditional-expectation interface. The Axiom of Choice
Proof
Let be the common refinement of the two partitions, and write and , where is the coefficient of the block containing and similarly for ; then and are bounded and -measurable, because whenever .
On each time interval the difference is the constant random variable : identically on , so Tonelli gives . Every summand is nonnegative, , and therefore , that is, almost surely for each .
On the common refinement the elementary sum of item 5 can be taken over the refined partition: within each original block the increments telescope, , a finite rearrangement of the defining sum. Applying this to and to , the difference of the two terminal sums is identically.
Write and for each . By [F2] the increment is independent of and has law . Hence [F3] gives and almost surely, because these conditional expectations of a variable independent of equal its unconditional mean. Since is bounded and -measurable, [F4] yields and almost surely.
Expanding the square, . If , then is -measurable and integrable, so the tower property and step 3.1 give ; by symmetry every off-diagonal term vanishes. The diagonal terms satisfy by step 3.1.
Combining steps 4.1 and 1.2, , where the last identity is the Tonelli computation of step 1.2. Since is square-integrable, forces almost surely.
The same computation at a deterministic time uses the truncated common partition : its nonempty blocks are with , whose left endpoints are and whose coefficients are -measurable, so the truncated sum is elementary; the difference of the truncated sums is , each increment is independent of with second moment , and the off-diagonal terms vanish by the same tower argument. The diagonal sum is , and this is by the Tonelli identity of step 1.2 restricted to . Hence almost surely for every . 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 , 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.
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 well defined before the completion step of item 10.
Ito isometry for elementary integrands
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let be an elementary predictable integrand on with representation and defining sums Ito integral of an elementary predictable process. Extend those sums to by setting for . Then is a continuous square-integrable martingale relative to Continuous-time adapted processes and martingales, and for every By the representation independence of Elementary Ito integrals do not depend on step representation both sides depend only on the -class of .
Facts & Assumptions
Given: AC, the standing hypothesis (H), a horizon , an elementary representation with bounded -measurable , its defining sums , and .
For , the increment is independent of and has law , hence mean and second moment ; for bounded -measurable , and 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
If is independent of a sub-sigma-algebra then almost surely; here and qualify by [F1]. Independent sigma-algebras and independent events Expectations factor over finite products of independent random variables Conditional expectation is unique almost surely
is adapted, , and each is a finite sum of products of bounded coefficients with Gaussian increments, so and ; path continuity holds on the Brownian continuity event. Ito integral of an elementary predictable process
For and integrable , , and whenever , is finite real and -measurable, and both and are integrable. Tower property of conditional expectation Taking out what is known
A martingale is exactly an adapted process with and almost surely for all . Continuous-time adapted processes and martingales
AC is declared for the conditional-expectation interface. The Axiom of Choice
Proof
Refining the partition of if necessary so that is a partition point, write the increments of the defining sum between the deterministic times as over the refined partition ; this is a finite rearrangement and does not change the values by the definition of the sums. Term by term, a block with contributes , a block with contributes , and every remaining block contributes with and , so that and is -measurable with .
For each such block, is independent of with mean and second moment by (H): and almost surely.
For every remaining block, almost surely, because , is bounded and -measurable, and the inner conditional expectation vanishes by step 1.2; summing the finitely many blocks gives , so almost surely by linearity of conditional expectation and the -measurability of .
For the variance, write for the blocks of the original partition, so that . For the random variable is -measurable, because , and ; Each increment is in , and shows that a product of two increments is integrable; bounded coefficients preserve these bounds. In the off-diagonal use of [F4], take and ; , , and is integrable. In the diagonal use, and is bounded. By (H) applied to the increment over the interval (which is empty, hence contributes , when ), almost surely, so the tower property and taking out what is known give . For the diagonal terms, the same identity gives , where the block contributes when .
Summing the diagonal terms of step 2.2 and using gives , finite because there are finitely many bounded coefficients.
Steps 2.1, 3.1 and [F3] show the martingale and isometry assertions on . The constant extension from the statement is adapted and continuous; if , the already proved identity gives , while for both sides equal . Thus [F5] makes the extended process a continuous square-integrable martingale on . 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.
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.
Cross Ito isometry
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. For elementary predictable integrands on and every , where the sums are the elementary integrals of the chosen representations Ito integral of an elementary predictable process. Both sides depend only on the -classes of and and are finite.
Facts & Assumptions
Given: AC, the standing hypothesis (H), a horizon , elementary representations of on some partitions, their common refinement, and .
On the common refinement, , 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 identically. Ito integral of an elementary predictable process Elementary predictable Brownian integrands
For every elementary predictable , is finite and is a continuous square-integrable martingale. Ito isometry for elementary integrands
The pointwise identity holds on , and the same expansion applies to the random variables . Elementary predictable Brownian integrands
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
Pass to the common refinement of the two partitions and keep the notation for the refined representations; by [F1] both and are elementary predictable integrands on that refinement, and , identically, with all quantities square-integrable.
Applying the elementary isometry [F2] to and to gives the two finite identities and .
Subtracting the second identity of step 1.2 from the first and expanding with [F3] gives , where the right-hand side is finite because and both elementary integrands have finite energy.
The left-hand side of step 2.1 equals by the algebraic expansion [F3], and is invertible in , so . Representation independence follows from Elementary Ito integrals do not depend on step representation applied to and to ; the AC bookkeeping is exactly the inherited use recorded in [F4], not an additional conditional-expectation interface asserted by this lemma.
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.
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 and let be the predictable sigma-algebra on Progressively measurable and predictable processes, with the finite measure . Then the classes of bounded elementary predictable integrands Elementary predictable Brownian integrands are dense in : for every -measurable with and every there is a bounded elementary predictable integrand with Equalities are equalities of -classes, so two elementary integrands whose difference vanishes almost everywhere represent the same approximant.
Facts & Assumptions
Given: AC, , the predictable sigma-algebra generated by the sets with , , and with , the finite measure on it, and the class of -classes of bounded elementary predictable integrands.
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 on a refinement is elementary. The constant class belongs to , represented by the elementary process (and its scalar multiples); the literal constant process is not elementary because elementary processes vanish at time zero. Every element of is bounded, say by . Elementary predictable Brownian integrands Ito integral of an elementary predictable process
The 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 . The norm descends to the quotient and makes a normed space for
A finite intersection of generators of is empty, or a generator , or a time-zero generator ; the family of finite unions of disjoint generators is an algebra generating . Progressively measurable and predictable processes
If is a pi-system of sets and is a lambda-system, then . Dynkin's pi-lambda theorem
Every that is -measurable admits nonnegative simple -measurable pointwise; each is a finite nonnegative linear combination of indicators of -sets and is bounded, its values being finitely many. Every nonnegative measurable function is the increasing limit of simple measurable functions
If measurable functions satisfy for a single integrable and pointwise, then whenever the domination is square-integrable: here with , and pointwise. Dominated convergence
for every : the section at is the singleton , which is Lebesgue-null, so Tonelli gives . Tonelli's theorem for nonnegative measurable functions on a sigma-finite product
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
Put , where the closure is taken in the metric of [F2]. By [F1] the set contains every constant class (represented elementarily by its value on and by at time ) and is closed under finite linear combinations of its elements: if and , choose with and use the triangle inequality to bound by .
Every generator of lies in , and contains and . Indeed, for with the process is elementary on the partition when , with coefficients , and on the partition when , with coefficients ; all coefficients are measurable at the left endpoints since and constants are -measurable. For a generator with , use coefficients on when , and the single coefficient when . For the zero process is elementary with by [F7]. The one-block elementary process represents in because the omitted time-zero slice is null, so the whole space belongs to ; the zero elementary process represents , so .
is closed under complements: if is approximated by bounded elementary , then the bounded elementary processes represent the classes and converge to in by the linearity of [F1] and the norm axioms of [F2].
is closed under countable unions of pairwise disjoint sets: let be pairwise disjoint with union . Given , choose so large that which is possible because the disjoint additivity of the finite measure gives ; since each lies in , choose for a bounded elementary with ; the finite sum is bounded and elementary on a common refinement by [F1]; the complement of inside is , so [F2] and the triangle inequality give , hence .
The family of finite intersections of generators of is the pi-system generated by the generators, and it is contained in : by [F3] a finite intersection is empty, a generator, or a time-zero generator, and contains and every generator by step 1.2.
The family contains , the whole space 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 by [F3].
By Dynkin's pi-lambda theorem [F4], . Hence the indicator of every predictable set is an limit of bounded elementary processes.
Consequently every bounded -measurable simple function is in : approximate each indicator by bounded elementary processes and combine the finitely many approximants with the coefficients using the closure under finite linear combinations from step 1.1.
Let be -measurable with . By [F5] choose nonnegative simple -measurable pointwise; each is bounded and lies in by step 5.1. Since and , [F6] gives , and for one takes with and then a bounded elementary with , so that by the triangle inequality.
For a general real , decompose ; both parts are nonnegative and -measurable with , so both lie in and each is approximated to within by a bounded elementary process by step 6.1; their difference is bounded and elementary on a common refinement by [F1] and is within of by the triangle inequality.
Steps 6.1 and 7.1 prove the density statement for nonnegative and for general predictable classes, with all approximants bounded and elementary; equalities of processes are equalities of -classes throughout, which is exactly the qualification "modulo product-almost-everywhere equality". For each fixed , step 2.2 selects only the finite list , 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].
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 approximant. No completeness of is used at this stage; the completion step is item 10.
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 and let be the predictable sigma-algebra on Progressively measurable and predictable processes. Let be a predictable process with so that is an element of the quotient space over ; its class is what is integrated. The Ito integral , also written or , is defined as follows.
-
Construction. By the density theorem Density of elementary predictable processes in predictable L2 there is a sequence of bounded elementary predictable integrands Elementary predictable Brownian integrands with . For such a sequence the elementary integrals Ito integral of an elementary predictable process form a Cauchy sequence in : by the elementary isometry Ito isometry for elementary integrands and the well-definedness of the elementary integral, and the right-hand side tends to . Since is complete Riesz-Fischer completeness of for , the classes converge in ; the limit is a class in , and 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 is used, then the elementary isometry and linearity give so the two limits agree.
-
Integrals at a time. For put , the construction of clause 1 applied to the truncated process . That process is predictable: is -measurable and is a deterministic predictable indicator, so the product is -measurable; and it is square-integrable because pointwise. The same construction applied to itself gives . The family is a family of -classes indexed by ; its continuous version is supplied by item 13, and no path property is asserted by this definition.
-
Consistency with elementary integrands. If is itself elementary, then the constant sequence is admissible in clause 1, so is the limit of the constant sequence of elementary sums, namely the elementary sum of Ito integral of an elementary predictable process. The same argument with in place of , and the finite telescoping of the elementary sum over a refinement containing , gives for every . In particular the general definition extends, rather than replaces, the elementary definition.
-
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.
-
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 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 every tagged sum telescopes to , which is also its Ito integral by clause 3 (the value at time zero is irrelevant to its product-measure class). The notation here always refers to the -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.
The general Ito integral is well defined
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let be a predictable process on with , and let and be two sequences of bounded elementary predictable integrands converging to in . Then so the integral of Ito integral for square-integrable predictable processes does not depend on the approximating sequence. If is any predictable process with -almost everywhere and finite energy, then almost surely; the integral is a function of the -class alone.
Facts & Assumptions
Given: AC, the standing hypothesis (H), a finite-energy predictable , two elementary approximating sequences and in , and a predictable with almost everywhere and finite energy.
For elementary predictable on a common refinement, identically and . Ito isometry for elementary integrands Ito integral of an elementary predictable process
Each of the sequences and is Cauchy in the complete space and therefore has an limit. The construction designates the limit obtained from one admissible approximating sequence as ; equality with the limit from every other sequence is what is proved below. Ito integral for square-integrable predictable processes
The triangle inequality and the identities almost surely hold on the quotient space. The norm descends to the quotient and makes a normed space for
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 -class. Ito integral of an elementary predictable process Elementary Ito integrals do not depend on step representation
AC is declared for the ambient interfaces; the argument below only uses the two given sequences and the metric algebra of . The Axiom of Choice
Proof
Pass to a common refinement of the two elementary representations at each index and use [F1]: , a finite quantity depending only on the two indices.
The triangle inequality gives as , because both approximating sequences converge to .
If almost everywhere, then every approximating sequence for is an approximating sequence for : , and likewise in the other direction.
By step 1.1 and step 1.2 the difference of the two sequences of elementary integrals converges to in , while by [F2] each sequence converges; two convergent sequences with difference tending to have the same limit, and by [F3] the limits agree as -classes, that is, almost surely.
Consequently the class is independent of the approximating sequence; and by step 1.3, replacing by an almost-everywhere equal keeps the same admissible sequences and hence the same limit, so almost surely. Only the two given sequences are used, and AC enters only as the declared ambient interface [F5].
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.
Ito isometry and linearity in predictable L2
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix . For predictable with finite energy the integrals of Ito integral for square-integrable predictable processes satisfy and the identities are equalities of -classes (almost sure equalities). Moreover the map is an isometry, it takes values in the mean-zero subspace of , and the bilinear cross identity holds for all such . In particular the image of the map is a closed subspace of isometric to the predictable space of 's, and is injective up to the -class.
Facts & Assumptions
Given: AC, the standing hypothesis (H), , finite-energy predictable , elementary sequences and in , and .
and , so and are admissible approximating sequences for and . The norm descends to the quotient and makes a normed space for
For elementary one has the elementary sum, , , and for elementary on a common refinement . Ito integral of an elementary predictable process Ito isometry for elementary integrands Cross Ito isometry Continuous-time adapted processes and martingales
Each integral is the -limit of 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
On the quotient space , -convergence implies convergence of norms and of expectations: and ; and the predictable space, like every space, is complete. The norm descends to the quotient and makes a normed space for Basic algebra and order properties of conditional expectation Riesz-Fischer completeness of for
The algebraic identities and hold for real random variables, and is a real vector space of classes. Conditional expectation as an ae class
AC is declared for the ambient interfaces. The Axiom of Choice
Proof
For each the elementary integrals are linear on a common refinement, and identically; by [F2] the isometry , the mean identity for elementary , and the cross identity hold at every index.
By [F1] the sequences and are admissible for and , so [F3] gives and in , as well as and .
Letting in the linear identities of step 1.1 and using uniqueness of -limits, and almost surely.
Taking the limit in the elementary isometry of step 1.1 gives by [F4] applied to the -limits and to the -convergence . Likewise , and the triangle inequality gives . So the image is mean-zero and isometric.
For the cross identity use with and : by step 2.1, by step 2.2. All terms are finite by step 2.2.
Steps 2.1--3.1 are exactly the linearity, isometry, mean-zero and cross-identity claims; injectivity follows because , 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.
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 norm and of the expectation.
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 be a predictable process with for every finite . Then there is an adapted process with continuous paths such that almost surely for every Ito integral for square-integrable predictable processes, and is a square-integrable martingale relative to Continuous-time adapted processes and martingales: for every . 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 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 with for all finite , and a horizon .
For every there is a bounded elementary predictable with . Density asserts existence, not an enumeration of all elementary integrands. Density of elementary predictable processes in predictable L2
For elementary the process is a continuous square-integrable martingale with for , and . Ito integral of an elementary predictable process Ito isometry for elementary integrands
Doob's maximal inequality: for a discrete martingale with , ; the sampled family is a discrete martingale for the filtration , by the tower property. Doob Lp maximal inequality Tower property of conditional expectation
If a sequence of nonnegative random variables increases pointwise, then ; the dyadic grids are nested with union a countable dense subset of , so . Monotone convergence for the integral
The rationals are dense in , and each rational is a limit of dyadic rationals ; a continuous function on therefore satisfies . The rationals embed densely in the reals
For every the class is the -limit of for every admissible elementary sequence , and ; the integration map is linear and isometric in the predictable variable. Ito integral for square-integrable predictable processes The general Ito integral is well defined Ito isometry and linearity in predictable L2
If in then , and conditional expectations are -contractive: . Cauchy-Schwarz for random variables Basic algebra and order properties of conditional expectation
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
Fix and choose, using [F8] on the nonempty sets supplied by [F1] with tolerance , bounded elementary predictable with ; write for the continuous elementary process of [F2].
For every elementary predictable and every , writing the path supremum as its measurable version on the scaled dyadic grid, : on the full-measure event where is continuous, [F5] identifies the supremum over with the supremum over the scaled dyadic grid, [F4] writes the latter as the increasing limit of the finite maxima over the nested grids , [F3] bounds for every , and monotone convergence passes the bound to the limit.
For each , is elementary on a common refinement and ; applying step 1.2 to gives for the measurable random variable , which equals the full supremum on the common event of continuity.
Consequently by monotone convergence for the nonnegative series [F4], so almost surely; the Cauchy--Schwarz inequality then gives almost surely, on a measurable event of probability one, intersected with the common continuity event of the elementary processes.
On the sequence converges uniformly on to a limit; put and define when is finite, and otherwise. This is real-valued and -measurable: is an extended-real measurable limit superior and its finite-value event belongs to . The resulting variable satisfies almost surely for every ; on the paths of are continuous, being uniform limits of continuous paths.
For every the sequence converges to in by [F6] applied to the truncations ; combined with step 4.1 and the almost-sure uniqueness of limits, almost surely for every .
For every , , using [F6] and the -norm continuity of the elementary integrals; hence is square-integrable.
For and , by [F2], and step 5.1 and [F7] give and in as well, so [F7] lets the conditional expectations pass to the limit: almost surely.
Steps 4.1, 5.1, 6.1 and 5.2 show that is an adapted continuous square-integrable martingale version on . If is another continuous version on , then almost surely for each rational ; intersecting the countably many measurable full-measure events and the two continuity events, and then invoking continuity, gives for every on one measurable event of probability one.
Apply the construction on the horizons , ; 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 put and define . This is well typed and -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 ; hence the local martingale identities show that is a square-integrable martingale with . Uniqueness on one measurable full-measure event over 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.
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 is summable in expectation, and Cauchy--Schwarz converts it into almost-sure summability of the sup norms.
Doob maximal bound for the Ito integral
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let be a predictable process on , where , with . Extend by zero after when applying the global continuous-version theorem, and let be the continuous version of The Ito integral process has a continuous martingale version. Then 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 on the countable scaled dyadic grid (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 on , and the continuous version with a.s. and .
is an adapted continuous square-integrable martingale with for every , and is the integral class at . The Ito integral process has a continuous martingale version Ito isometry and linearity in predictable L2
For each the sampled family , , is a discrete martingale for the filtration , by the tower property; hence Doob's inequality gives . Tower property of conditional expectation Doob Lp maximal inequality
By the continuous-version theorem there is an event of probability one on which the path of is continuous on . On that event its supremum equals the supremum over the dyadic grid union , which in turn is the increasing limit because the grids are nested. The rationals embed densely in the reals The Ito integral process has a continuous martingale version
For , , so the expectation of the supremum is the limit of the expectations of the finite-grid maxima. Monotone convergence for the integral
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
AC is declared for the ambient interfaces. The Axiom of Choice
Proof
If , almost surely and both sides vanish. For and fixed the finite-grid quantity is integrable, and [F2] gives .
As increases the grids are nested, so the unsquared maxima increase pointwise to the measurable random variable . By [F3], almost surely.
Monotone convergence [F4] applies pointwise to . Hence, using the almost-sure equality in step 1.2, , and the bound is finite because the right-hand side is finite.
For any other continuous version , intersect the fixed-time equality events over the countable grid 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 has the same expectation and satisfies the bound, even if is not adapted. AC enters through the declared ambient interfaces [F6].
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.
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 satisfies the usual conditions: contains every subset of every -null event in , and for every . The earlier finite-energy construction does not require these additional conditions. Let be a predictable process Progressively measurable and predictable processes. Its energy process is the integral of the nonnegative function ; it may be . The process is locally square-integrable when No uniform bound over and no bound on 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.
-
Measurability and adaptation of the energy. is well defined and adapted: for each the map is product measurable, so Tonelli Tonelli's theorem for nonnegative measurable functions on a sigma-finite product expresses as an integral of measurable sections and, for , the section computation over shows that is -measurable (the integral of a nonnegative measurable function is measurable in the parameter). Thus every level or sublevel event of belongs to . On the event which has probability one, the maps are nondecreasing, finite-valued and continuous on : on each the nonnegative integrand has finite integral, and dominated convergence on that finite interval gives continuity. Moreover is a null event in , so completeness gives and every subset of belongs to every .
-
Canonical localization times. For put Then everywhere, the sequence is nondecreasing and almost surely: on , for fixed , one has and for every sufficiently large integer , hence eventually. Each is a stopping time for Continuous-time stopping times and stopped sigma-algebras. For the event is . For , continuity and monotonicity give Thus the symmetric difference of and the -event is a subset of and belongs to by completeness. Hence .
-
The localization localizes the energy. For every and every , because on the process is nondecreasing, , and : if then continuity gives and , while if then and by the definition of as an infimum. Consequently so is a predictable integrand of finite energy and its integral exists by Ito integral for square-integrable predictable processes. The same holds for , which differs from only at , a null set for .
-
Predictability of the truncations. The process is predictable for every stopping time , by the generator computation recorded in Progressively measurable and predictable processes, and the products and are therefore predictable, being products of predictable functions.
These conventions are the only sense in which the definition localizes: the times are canonical functions of the energy process, so no auxiliary sequence of stopping times is selected, and the constants 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 integral interface assumes it; the definition of the energy process and of the times 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.
Localized Ito integral
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let be a locally square-integrable predictable process with energy process and canonical localization times (indexed by ) Locally square-integrable predictable Brownian integrands, and let denote the continuous version of the finite-energy integral 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.
-
Existence. There is an adapted process with continuous paths, called the localized Ito integral , such that for every the stopped process is indistinguishable from . Consequently is a continuous local martingale relative to with localizing sequence , and for every and
-
Characterization. If is an adapted process with continuous paths and such that is indistinguishable from for every , then is indistinguishable from . In particular is the unique continuous local martingale, up to indistinguishability, whose stopped finite-energy integrals are the .
-
Independence of the localizing sequence. Let be a nondecreasing sequence of stopping times with almost surely and for all and all finite , and let be an adapted process with continuous paths and such that is indistinguishable from the finite-energy integral of for every . Then is indistinguishable from .
-
Stopping identity for finite-energy integrands. If is a predictable process with and denotes its continuous version The Ito integral process has a continuous martingale version, with the same progressive version convention (extending by zero after ), then for every stopping time and every and the two sides are continuous processes on , hence indistinguishable there. A global identity follows by applying this clause on each finite horizon when 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 with energy and canonical times , finite-energy predictable integrands , stopping times , and the continuous versions and of items 13 and 15.
is predictable and has finite energy , so its integral has a continuous version with ; the times are nondecreasing stopping times with a.s. Locally square-integrable predictable Brownian integrands The Ito integral process has a continuous martingale version
For a finite-energy predictable the continuous version satisfies at every deterministic , and ; hence and the integrals of approximating integrands are controlled by the distance. The Ito integral process has a continuous martingale version Doob maximal bound for the Ito integral
For elementary predictable the defining sum is a continuous process and the general integral of equals that sum at every deterministic ; elementary integrals are linear on a common refinement, and for elementary is elementary on the refinement containing . Ito integral of an elementary predictable process Ito integral for square-integrable predictable processes
Every finite-energy predictable is the -limit of bounded elementary integrands, and the integral map is an isometry: . Density of elementary predictable processes in predictable L2 Ito isometry and linearity in predictable L2
For a stopping time the indicator is predictable and every truncation is predictable; products of predictable processes are predictable. Progressively measurable and predictable processes
Finite pointwise limits of measurable functions, set to zero where no finite limit exists, are measurable. Almost-sure convergence dominated by an random variable gives convergence. Sequential suprema, infima, limsup, liminf, and pointwise limits of measurable functions are measurable Dominated convergence in
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
Measurable versions and stopping: for an adapted process with almost-sure continuous paths and almost surely, define and on , . 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 where this limit exists finitely, and zero otherwise. By [F6] on each product sigma-algebra, is progressive. It equals 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 has adapted stopped values: for fixed , is -measurable, and the map into is measurable into by rectangle inverse images. Composition with the progressive restriction of gives . 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 when applying an interface indexed from zero.
Clause 4 for elementary and finite-valued : refine the partition of so that it contains the finitely many values of and the point ; on each block the indicator is constant in with value , and because takes only partition values, so is elementary with coefficients ; its defining sum is , which term-by-term equals on the measurable full event where the progressive version agrees with the elementary sum at all times, by step 1.1.
Clause 4 for elementary and arbitrary : let be the dyadic ceiling of the bounded stopping time , a finite-valued stopping time with and ; by step 2.1 and [F3], for every .
As : in by continuity of the path and the maximal bound [F2] with [F6] (the measurable grid supremum of [F2] supplies the dominating random variable); and in because their indicators converge for Lebesgue-almost every time (the possible boundary is irrelevant), and they are dominated by , and the integral is an isometry [F4]. Hence almost surely for elementary and every stopping time .
Clause 4 for general finite-energy : approximate by bounded elementary in [F4]; then in by the maximal bound [F2], and by the isometry and ; passing to the limit in the identities of step 4.1 gives clause 4 in general, and since both sides are continuous in and agree at every deterministic almost surely, they are indistinguishable.
Agreement of stopped finite-energy integrals (clause 1, first assertion): for apply clause 4 to , which has finite energy by [F1], and to the stopping time : almost surely for every , using because . Both sides are continuous, so and are indistinguishable.
Construction of : put where the limit exists finitely, and zero otherwise. This is progressive by [F6] applied on every finite-horizon product sigma-algebra, since each was chosen progressive in step 1.1. In particular everywhere and its stopped values are adapted by step 1.1. On the event where all the agreements of step 6.1 hold, every is continuous and , fix and ; choose with ; then for every , by step 6.1, so the sequence is eventually constant and . Hence on the process agrees on with the continuous path of , so has continuous paths on the full-measure event .
is a local martingale with localizing sequence : by step 6.1 and the definition of on , is indistinguishable from , and is a martingale. Since is adapted by step 1.1 and has the same deterministic-time values almost surely, it is itself a martingale; moreover by [F1].
Clauses 2 and 3: if is continuous with and for all , then for each and each with one has almost surely, and letting along the full-measure event where gives almost surely for every ; continuity and the rationals argument make indistinguishable from . For clause 3, apply clause 4 twice: for each , and with , , and both integrands equal ; hence and are indistinguishable, and for each on the full-measure event where eventually, 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].
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.
Stopping an Ito integral
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Let be a locally square-integrable predictable process Locally square-integrable predictable Brownian integrands with localized integral 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 be a stopping time Continuous-time stopping times and stopped sigma-algebras. Then the process and the localized integral of the process are indistinguishable: In particular, for of finite energy this reduces to the stopping identity of Localized Ito integral, and for it is the definition of the localized integral.
Facts & Assumptions
Given: AC, the standing hypothesis (H), a locally square-integrable predictable with energy and canonical stopping times , , its localized integral , and a stopping time .
is predictable for every stopping time, and is predictable and locally square-integrable with energy almost surely for every finite ; its localized integral exists and is a continuous local martingale. Progressively measurable and predictable processes Localized Ito integral
The canonical times satisfy , a.s., has finite energy , and is the finite-energy integral of ; the finite-energy stopping identity gives for finite-energy and any stopping time . Locally square-integrable predictable Brownian integrands Localized Ito integral
If is a nondecreasing sequence of stopping times with a.s., each has finite energy, and a continuous adapted with has indistinguishable from the finite-energy integral of for every , then is indistinguishable from the localized integral of . Localized Ito integral
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 is an adapted continuous process with . The proof below uses the original sequence to localize ; the bounded sequence is not asserted to be a localizing sequence. Continuous-time adapted processes and martingales Localized Ito integral
AC is declared for the ambient interfaces. The Axiom of Choice
Proof
Put and , so that is adapted with continuous paths and by [F4]; by [F1] the localized integral exists and is a continuous local martingale. No local-martingale property of is assumed at this stage.
For every the stopped integral is the finite-energy integral of by [F2], and the finite-energy stopping identity applied with the stopping time gives .
The integrand identity holds for every with , the three expressions differing at most at , a -null set; hence equals the finite-energy integral of , and the canonical sequence consists of stopping times, is nondecreasing with almost surely, (indexed by , or reindexed by when required), while has finite energy .
Steps 1.1, 1.2 and 2.1 verify the hypotheses of [F3] for the process and the localizing sequence : is adapted and continuous with , and is indistinguishable from the finite-energy integral of for every . Therefore is indistinguishable from the localized integral , which is exactly the identity up to indistinguishability.
The special cases are consistent: for one has and the identity is the definition of the localized integral; for finite-energy it is the finite-energy stopping identity [F2] used in the proof; and for a deterministic it recovers the convention . AC enters only through the declared ambient interfaces [F5], and the localizing sequence is canonical.
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 of : the stopping identity for each is step 1.2, and the a.e. integrand identity of step 2.1 expresses as the integral of , so clause 3 of Localized Ito integral applies with .
Quadratic variation of an Ito integral
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix , let be a locally square-integrable predictable process Locally square-integrable predictable Brownian integrands with localized integral 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 be a deterministic partition sequence of with mesh tending to Quadratic variation along a partition sequence. Write for the step-convention partial sum . Then 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 is the random function , 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 on and zero on . The local-integrability definition proves that is an -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 .
Facts & Assumptions
Given: AC, the standing hypothesis (H), a locally square-integrable predictable with energy , its canonical times , and localized integral , a horizon , and a deterministic partition sequence of with mesh .
For every the increment of the localized integral is the localized Ito integral of the predictable restriction, evaluated after time . If has finite energy on the horizon under consideration, this localized integral is the finite-energy integral , and the isometry gives . Ito integral for square-integrable predictable processes Ito isometry and linearity in predictable L2 Localized Ito integral
On a deterministic partition , put for and for , so . The independent Gaussian increments have second and fourth moments and , so and . Relative to the finite-grid filtration is a martingale by (H); cross terms have zero expectation by conditioning. Extend it constantly after to apply discrete Doob with . For nonnegative , the elementary inequality gives ; applied to this also converts an bound to a probability bound. Gaussian even moments for Brownian increments Brownian motion Doob Lp maximal inequality Tower property of conditional expectation
A continuous real function on the compact interval is uniformly continuous, so for a fixed continuous path and mesh tending to the maximal oscillation over the partition intervals tends to . Heine-Cantor in : a continuous real function on a compact subset of is uniformly continuous, proved -natively from sequential compactness Partition of as a finite strictly increasing list , its subintervals and their lengths, its mesh, refinement, and the common refinement of two partitions
For a finite-energy predictable and a stopping time , is the finite-energy integral of ; for the canonical times of , is the finite-energy integral of and . Localized Ito integral Stopping an Ito integral Locally square-integrable predictable Brownian integrands
For finite-energy the maximal bound holds, and for elementary 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
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
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
For real numbers and for random variables one has and ; 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
Every predictable integrand of finite expected energy on admits bounded elementary predictable approximations in . Density of elementary predictable processes in predictable L2
Proof
Brownian estimate: for a deterministic partition of with mesh and as in [F2], independence of the Brownian increments gives , and Doob's inequality gives ; since where and , one has , which tends to ; [F2]'s elementary probability bound turns this into uniform convergence in probability.
For elementary with partition and a sub-interval , the increment is the elementary sum of the elementary integrand , whose coefficients are on , measurable at the left endpoints ; consequently over the at most two blocks meeting when , and equals when is contained in a single block .
Elementary refinement: fix a bounded elementary with blocks , , and a deterministic bound for its coefficients on a common probability-one event. For sufficiently large , , so each interval of crosses at most one elementary boundary. Refine by all these boundaries, and write for the induced partition of . Let be the Brownian step sum on , extended by zero before and its terminal value after . The refined integral sum is . Away from crossing intervals it equals . On a crossing interval, the original increment has absolute value at most , while each of the at most two refined increments has absolute value at most , where 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 by , which tends to zero almost surely by [F3].
Apply step 1.1 on each deterministic interval to its translated Brownian increments and the induced mesh , whose mesh is at most . Thus in probability. Since , the refined-sum error is bounded by 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 in probability for each bounded elementary . No independence of from these error suprema is needed, because the deterministic bound is used.
Finite-energy case: use [F9] and [F7] to choose in with bounded elementary and set ; by Cauchy--Schwarz in each partial sum, , and [F1] gives and uniformly in , so as uniformly in ; combined with step 3.1 for and , the finite-energy case follows by a two-parameter argument: for error threshold , split the total error into the quadratic-sum approximation, the elementary convergence error and the energy approximation, each at threshold . Their probabilities are bounded by times the two expected approximation errors, plus the elementary error probability. The latter vanishes as at fixed , and the former vanish as , uniformly in .
Localized case: on the event the processes and agree on and for by [F4], so the squared-increment sums of coincide with those of the finite-energy integral there; consequently, for every , , and the second term tends to by step 4.1 while the first tends to as because almost surely.
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 over the partition intervals, which tends to by [F3] and continuity of , so both conventions have the same limit. The dyadic partitions are included; no almost-sure dyadic conclusion is asserted for general . AC covers the declared interfaces and the countable approximating choices in [F7].
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.
Deterministic Ito integrals are Gaussian
Statement
Assume the Axiom of Choice and the standing hypothesis (H) of Elementary predictable Brownian integrands. Fix and let be deterministic, choose a Borel representative of its Lebesgue-equivalence class, and set . This process is predictable with finite energy. Then the Ito integral Ito integral for square-integrable predictable processes is centered normal with variance : its law is in the convention of Standard normal and normal laws, where is the Dirac law at . More generally, for deterministic the vector of integrals is jointly Gaussian in the sense of Multivariate normal law, including singular covariance: its law is with In particular the covariance of the pair is , the integrals are uncorrelated exactly when , and integrals of deterministic integrands with disjoint supports are independent.
Facts & Assumptions
Given: AC, the standing hypothesis (H), a horizon , deterministic represented by Borel functions, and real coefficients .
A deterministic step function is an elementary predictable integrand with deterministic coefficients, and its Ito integral is the finite sum ; the Brownian increments over disjoint intervals are independent with laws and mean . Elementary predictable Brownian integrands Ito integral of an elementary predictable process Brownian motion
A finite linear combination of independent centered normal variables is centered normal, and a variable has characteristic function , including ; a Borel probability law on 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
Convergence in implies convergence in probability, which implies weak convergence of the laws. Weak convergence tests bounded continuous real functions; applying it separately to and 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
The integration map on predictable is linear and isometric, and the integral of is the -limit of the elementary integrals of any admissible elementary approximation; the approximation is admissible because in equals the deterministic distance. Ito isometry and linearity in predictable L2 The general Ito integral is well defined Ito integral for square-integrable predictable processes
If in , the reverse triangle inequality in the stated normed space gives Hence . The norm descends to the quotient and makes a normed space for
A Borel probability law on is exactly when every projection has law ; such a vector has mean and covariance . Multivariate normal law, including singular covariance
Under AC, hence Countable Choice, finite linear combinations of box indicators are dense in . Extend by zero outside and approximate that extension by such a box-step function. Its restriction to agrees almost everywhere with a function after adjoining the finitely many box endpoints and to one partition. Thus deterministic step functions of the required elementary form are dense in . Finite linear combinations of box indicators are dense in for AC supplies countable selections and prescribed serial paths The Axiom of Choice
Proof
For a deterministic step function as in [F1], the integral is a finite sum of independent centered normal variables with variances , so by [F2] its law is with ; in particular its characteristic function is , and its mean is .
For general deterministic , choose by [F7] step functions in ; by [F4] the elementary integrals converge to in , hence in probability and weakly by [F3]. Apply the real-valued weak-convergence test separately to and and combine the limits to obtain pointwise convergence of characteristic functions: with , using [F5] for the convergence of variances and continuity of the exponential.
By [F2] the function is the characteristic function of and determines a unique Borel law, so the law of is ; consequently it is centered with variance , and the case (that is, in ) gives the Dirac law at .
For a finite family, linearity [F4] gives in , and step 3.1 applied to the deterministic integrand shows that this projection is with ; by [F6] the vector of the integrals therefore has law , hence is jointly Gaussian with mean and covariance .
The covariance identity is the entry of ; the zero-covariance case is uncorrelatedness, which for the jointly Gaussian pair means independence, and disjoint supports make every mixed integral 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.
Source notes
Lawler, Exercise 3.8, states that deterministic integrands produce Gaussian integrals with variance equal to the squared 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
None yet.
Sources
- Aad van der Vaart, Martingales, Diffusions and Financial Mathematics (preliminary notes), Sections 4.1 and 5.4
- Aad van der Vaart, Stochastic Integration and Differential Equations, Section 5.1
- Gregory F. Lawler, Stochastic Calculus: An Introduction with Applications, Section 3.2.2
- Aad van der Vaart, Stochastic Integration and Differential Equations, Definition 5.20 and Lemma 5.22
- Gregory F. Lawler, Stochastic Calculus: An Introduction with Applications, Proposition 3.2.1
- Aad van der Vaart, Stochastic Integration and Differential Equations, Lemma 5.22
- Aad van der Vaart, Stochastic Integration and Differential Equations, Lemmas 5.21-5.23
- Aad van der Vaart, Stochastic Integration and Differential Equations, Definition 5.25
- Aad van der Vaart, Stochastic Integration and Differential Equations, Definition 5.25 and Theorem 5.26
- Gregory F. Lawler, Stochastic Calculus: An Introduction with Applications, Sections 3.2.2-3.2.3
- Aad van der Vaart, Stochastic Integration and Differential Equations, Theorem 5.26
- Gregory F. Lawler, Stochastic Calculus: An Introduction with Applications, Proposition 3.2.4
- Aad van der Vaart, Stochastic Integration and Differential Equations, Sections 5.4-5.5
- Andreas Eberle, Stochastic Analysis, Sections 3.1 and 5.3
- Aad van der Vaart, Martingales, Diffusions and Financial Mathematics, Lemma 5.28, Lemma 5.33 and Theorem 5.36
- Aad van der Vaart, Martingales, Diffusions and Financial Mathematics, Lemma 5.28 and Theorem 5.36
- Aad van der Vaart, Stochastic Integration and Differential Equations, Section 5.8 and Lemma 5.77
- Gregory F. Lawler, Stochastic Calculus: An Introduction with Applications, Theorem 3.2.6
- Gregory F. Lawler, Stochastic Calculus: An Introduction with Applications, Section 3.2 and Exercise 3.8