Itô's Formula (Itô's Lemma)

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Core Idea

Itô's formula is the chain rule of stochastic calculus: for a C² function f and a process X(t) = X(0) + ∫μ ds + ∫σ dW, we have df(X) = f'(X)dX + (1/2)f''(X)σ²dt. The extra second-order term (1/2)f''σ²dt arises because (dW)² = dt — the non-zero quadratic variation of Brownian motion prevents the second-order Taylor term from vanishing as it does in classical calculus. This formula is the single most used tool in stochastic calculus.

Explainer

Itô's formula is to stochastic calculus what the chain rule is to ordinary calculus — it tells you how to compute df(X) when X is a stochastic process. But unlike the classical chain rule, the stochastic version has an extra term. If X(t) satisfies dX = μ(t)dt + σ(t)dW and f is C², then df(X) = f'(X)μ dt + f'(X)σ dW + (1/2)f''(X)σ² dt. The third term, (1/2)f''σ²dt, is the Itô correction — it is absent from classical calculus and arises entirely from the non-zero quadratic variation of Brownian motion.

The derivation follows from a second-order Taylor expansion: f(X + dX) ≈ f(X) + f'(X)dX + (1/2)f''(X)(dX)². In classical calculus, (dX)² is second-order infinitesimal and vanishes. But for stochastic processes, (dX)² = (μ dt + σ dW)² = σ²(dW)² + 2μσ(dt)(dW) + μ²(dt)². Using the multiplication rules dt·dt = 0, dt·dW = 0, and dW·dW = dt (the quadratic variation), only the σ²dt term survives. This is a rigorous consequence of the quadratic variation computation you studied in the previous topic: Σ(ΔWᵢ)² → T in L², so squared Brownian increments behave like dt at the infinitesimal level.

The formula's power lies in its ability to transform one stochastic differential equation into another. To analyze a complicated process Y(t) = f(X(t)), apply Itô's formula to find the SDE for Y directly. For example, if S follows geometric Brownian motion dS = μS dt + σS dW, then applying Itô's formula to f(S) = ln(S) gives d(ln S) = (μ - σ²/2)dt + σ dW. The logarithm converts the multiplicative SDE into an additive one with constant coefficients — immediately showing that ln S(T) is normally distributed and S(T) is lognormally distributed. This single computation underlies the Black-Scholes option pricing model.

The multidimensional version handles functions of several Itô processes simultaneously. If X₁, ..., Xₙ are Itô processes driven by possibly correlated Brownian motions, then for f(X₁, ..., Xₙ) the formula includes all partial derivatives ∂f/∂xᵢ (first order), all cross terms (1/2)∂²f/∂xᵢ∂xⱼ times the quadratic covariation d[Xᵢ, Xⱼ] (second order), and the time derivative ∂f/∂t if f depends explicitly on t. The structure is always the same: classical chain rule plus second-order corrections from quadratic (co)variation. Mastering this formula is the single most important skill in stochastic calculus.

Practice Questions 4 questions

Prerequisite Chain

Counting to 10Counting to 20Understanding ZeroThe Number ZeroCounting to FiveOne-to-One CorrespondenceCombining Small Groups Within 5Addition Within 10Addition Within 20Two-Digit Addition Without RegroupingTwo-Digit Addition with RegroupingAddition Within 100Repeated Addition as MultiplicationMultiplication Facts Within 100Division as Equal SharingDivision as Grouping (Measurement Division)Division: Grouping (Repeated Subtraction) ModelDivision: Fair Sharing ModelDivision as Equal SharingDivision as GroupingBasic Division FactsDivision Facts Within 100Two-Digit by One-Digit DivisionDivision with RemaindersRemainders and Quotients in DivisionDivision Word ProblemsIntroduction to Long DivisionFactors and MultiplesPrime and Composite NumbersEquivalent FractionsRelating Fractions and DecimalsDecimal Place ValueReading and Writing DecimalsComparing and Ordering DecimalsAdding and Subtracting DecimalsMultiplying DecimalsDividing DecimalsDividing FractionsMixed Number ArithmeticOrder of OperationsInteger Order of OperationsVariable ExpressionsCombining Like TermsOne-Step EquationsTwo-Step EquationsSolving Multi-Step EquationsEquations with Variables on Both SidesAngle Pairs: Complementary, Supplementary, and VerticalParallel Lines and TransversalsCorresponding AnglesAlternate Interior AnglesTriangle Angle Sum TheoremExterior Angle TheoremTriangle Inequality TheoremSimilar Triangles: AA SimilaritySimilar Triangles: SSS and SAS SimilarityProportions in Similar TrianglesRight Triangle Trigonometry IntroductionTrigonometric Ratios ReviewRadian MeasureConverting Between Degrees and RadiansThe Unit CircleGraphing Sine and CosineGraphing Tangent and Reciprocal Trigonometric FunctionsDerivatives of Trigonometric FunctionsAntiderivativesIterated Integrals and Fubini's TheoremDouble Integrals in Cartesian CoordinatesDouble Integrals over Rectangular RegionsDouble Integrals in Polar CoordinatesDouble Integrals: Definition and SetupIterated Integrals and Fubini's TheoremDouble Integrals over Rectangular RegionsDouble Integrals over General RegionsApplications of Double Integrals: Area, Mass, and MomentsCenter of MassConservation of Linear MomentumElastic CollisionsInelastic CollisionsCoefficient of RestitutionCollision Analysis and Real-World ApplicationsTwo-Body Collisions in the Center-of-Mass FrameReduced Mass and Two-Body ProblemsKinematics in Two DimensionsProjectile MotionCircular Motion: KinematicsRotational KinematicsTorqueMoment of InertiaRotational Kinetic EnergyThe Work-Energy TheoremConservation of Mechanical EnergyFirst Law of ThermodynamicsThermodynamic Processes and the PV DiagramIsobaric and Isochoric ProcessesHeat EnginesThermal Efficiency of Heat EnginesRefrigerators and Heat PumpsSecond Law of ThermodynamicsEntropyMicrostates and MacrostatesEnsemble Theory FundamentalsCanonical Ensemble (NVT)Partition Function: Definition and PropertiesThe Canonical Partition Function and Thermodynamic DerivationMaxwell-Boltzmann Distribution and Classical LimitBrownian MotionProperties of Brownian MotionThe Itô IntegralItô's Formula (Itô's Lemma)

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