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Ito's Formula for Brownian Motion · Tutorial 150 of 600

Polynomial Tests of the Ito Correction

See how the Ito correction changes the square and cube identities for Brownian motion, and check those identities using moments and conditional expectations.

Advanced 9 min read

What You'll Learn

  • Apply Ito’s formula to the square and cube functions with their derivatives shown explicitly.
  • Identify the second-order correction in each polynomial identity.
  • Verify the integrability needed for the stochastic integrals that appear.
  • Check the square identity using expectations and variances.
  • Derive a conditional cubic-moment formula from the Ito identity.
  • Recognize why the ordinary chain rule omits a nonzero Brownian correction.

Two Polynomial Tests of Ito’s Formula

For a differentiable path \(x(t)\), the ordinary chain rule gives \(d(x^2)=2x\,dx\) and \(d(x^3)=3x^2\,dx\). Brownian paths are not differentiable, and their nonzero quadratic variation contributes an additional term. The square and cube functions make the correction visible with minimal algebra: the square receives a constant time term, while the cube receives a term proportional to Brownian motion.

Work on a filtered probability space \((\Omega,\mathcal{F},(\mathcal{F}_t)_{t\ge0},\mathbb{P})\) carrying a standard Brownian motion \(B_t\) relative to \((\mathcal{F}_t)\). In particular, \(B_t-B_s\) is independent of \(\mathcal{F}_s\) and has distribution \(N(0,t-s)\) for \(0\le s<t\). All stochastic integrals below are Ito integrals. Their integrands are progressively measurable and belong to \(\mathcal{L}^2\) on each stated finite time interval: this means \(\mathbb{E}\int_0^T H_s^2\,ds<\infty\). Under this condition, the Ito integral is a square-integrable martingale, with conditional mean-zero increments and the Ito isometry.

Definition: The Ito correction in the formula for \(f(B_t)\) is the second-order term \(\tfrac12\int_0^t f''(B_s)\,ds\). It arises because Brownian motion has quadratic variation \([B]_t=t\), summarized by \(dB_t\,dB_t=dt\); the other differential products are \(dB_t\,dt=0\) and \(dt\,dt=0\).

We use the one-dimensional Ito formula, established in the earlier material on Ito’s formula for Brownian motion: for \(f\in C^2(\mathbb{R})\), it gives \(f(B_t)=f(B_0)+\int_0^t f'(B_s)\,dB_s+\tfrac12\int_0^t f''(B_s)\,ds\), provided the stochastic integral is defined. The applications below check that condition. The stochastic integrals are Ito, not Stratonovich integrals; in particular, the ordinary chain rule is not a rule for evaluating them.

The Square Identity

Proposition: For every finite \(T\ge0\), almost surely for all \(0\le t\le T\), $$ B_t^2=2\int_0^t B_s\,dB_s+t. $$ The integrand \(B_s\) is progressively measurable and belongs to \(\mathcal{L}^2\) on \([0,T]\).

Proof. Set \(f(x)=x^2\). Its derivatives are \(f'(x)=2x\) and \(f''(x)=2\). Ito’s formula, including its second-order term, therefore gives $$ B_t^2=B_0^2+\int_0^t 2B_s\,dB_s+\frac12\int_0^t 2\,ds. $$ Since \(B_0=0\), the last term is \(t\), giving the identity. To check that the stochastic integral is defined on \([0,T]\), use \(\mathbb{E}[B_s^2]=s\): $$ \mathbb{E}\int_0^T B_s^2\,ds=\int_0^T s\,ds=\frac{T^2}{2}<\infty. $$ The integrand is adapted with continuous paths, hence progressively measurable. The Ito integral is consequently square-integrable, and the asserted identity follows from Ito’s formula. \(\square\)

Worked Example: Checking the Square Identity at Time Two

Use the identity at \(t=2\) to calculate the mean and variance of \(B_2^2\), then check both against the normal distribution.

Write \(I=\int_0^2 B_s\,dB_s\). The integrability calculation in the proposition applies, and the Ito integral is a square-integrable martingale. Thus \(\mathbb{E}[I]=0\). By the Ito isometry, $$ \mathbb{E}[I^2]=\mathbb{E}\int_0^2 B_s^2\,ds=\int_0^2 s\,ds=\left.\frac{s^2}{2}\right|_0^2=2. $$ The square identity says \(B_2^2=2I+2\). Therefore $$ \mathbb{E}[B_2^2]=2\mathbb{E}[I]+2=2, \qquad \operatorname{Var}(B_2^2)=\operatorname{Var}(2I+2)=4\operatorname{Var}(I)=4\cdot2=8. $$ Here \(\operatorname{Var}(I)=\mathbb{E}[I^2]-(\mathbb{E}[I])^2=2\).

Check: \(B_2\sim N(0,2)\). Its second moment is \(2\), and its fourth moment is \(3\cdot2^2=12\). Hence the variance of its square is \(12-2^2=8\), agreeing with the identity-based calculation.

The Cube Identity

Proposition: For every finite \(T\ge0\), almost surely for all \(0\le t\le T\), $$ B_t^3=3\int_0^t B_s^2\,dB_s+3\int_0^t B_s\,ds. $$ The stochastic integrand \(B_s^2\) is progressively measurable and belongs to \(\mathcal{L}^2\) on \([0,T]\).

Proof. Set \(f(x)=x^3\). Then \(f'(x)=3x^2\) and \(f''(x)=6x\). Ito’s formula gives the first-order integral and the explicit correction term: $$ B_t^3=B_0^3+\int_0^t 3B_s^2\,dB_s+\frac12\int_0^t 6B_s\,ds. $$ Since \(B_0=0\), the correction is \(3\int_0^t B_s\,ds\), proving the displayed identity. For the stochastic integral, Brownian normal moments give \(\mathbb{E}[B_s^4]=3s^2\), so $$ \mathbb{E}\int_0^T (B_s^2)^2\,ds=\int_0^T 3s^2\,ds=T^3<\infty. $$ The process \(B_s^2\) is adapted and continuous, hence progressively measurable. Thus the Ito integral exists in the square-integrable sense, as required. \(\square\)

Worked Example: Checking the Mean of the Cubic Identity

Apply the cube identity at \(t=1\) and use it to compute \(\mathbb{E}[B_1^3]\). Verify the result directly from the distribution of \(B_1\).

The identity gives $$ B_1^3=3\int_0^1 B_s^2\,dB_s+3\int_0^1 B_s\,ds. $$ The stochastic integrand \(B_s^2\) satisfies \(\mathbb{E}\int_0^1 B_s^4\,ds=\int_0^1 3s^2\,ds=1<\infty\). Its Ito integral is a square-integrable martingale starting at zero, so its expectation at time \(1\) is zero. For the ordinary time integral, Fubini’s theorem applies because \(\int_0^1\mathbb{E}|B_s|\,ds\le\int_0^1\sqrt{\mathbb{E}[B_s^2]}\,ds=\int_0^1\sqrt{s}\,ds<\infty\). Since \(\mathbb{E}[B_s]=0\), this integral also has mean zero. Consequently \(\mathbb{E}[B_1^3]=0\).

Check: \(B_1\sim N(0,1)\), a distribution symmetric about zero. Its third moment is zero, in agreement with the calculation from Ito’s identity.

A Conditional Cubic-Moment Formula

The cube identity also determines a conditional expectation. The result reflects the contribution of the Brownian increment’s variance: conditionally on the present, the expected cube at a later time is not just the cube of the present value.

Theorem: For \(0\le s\le t<\infty\), $$ \mathbb{E}[B_t^3\mid\mathcal{F}_s]=B_s^3+3(t-s)B_s $$ almost surely.

Proof. Apply the cube identity at \(t\) and at \(s\), then subtract: $$ B_t^3-B_s^3=3\int_s^t B_u^2\,dB_u+3\int_s^t B_u\,du. $$ The first integral is an increment of a square-integrable Ito martingale: its integrand satisfies \(\mathbb{E}\int_0^t B_u^4\,du=t^3<\infty\). Therefore its conditional expectation given \(\mathcal{F}_s\) is zero. For the time integral, \(\mathbb{E}\int_s^t|B_u|\,du<\infty\), as follows from \(\mathbb{E}|B_u|\le\sqrt{u}\) on this finite interval. Conditional Fubini and \(\mathbb{E}[B_u\mid\mathcal{F}_s]=B_s\) for \(u\ge s\) give $$ \mathbb{E}\left[\int_s^t B_u\,du\mid\mathcal{F}_s\right] =\int_s^t\mathbb{E}[B_u\mid\mathcal{F}_s]\,du =\int_s^t B_s\,du=(t-s)B_s. $$ Taking conditional expectations in the subtracted identity proves the formula. When \(s=t\), the stochastic and time integrals over \([s,t]\) vanish, and the formula reduces to \(B_t^3=B_t^3\). \(\square\)

Worked Example: Conditional Cubic Moment from One Half to One

Specialize the theorem to \(s=\tfrac12\) and \(t=1\), and check the result by expanding the Brownian increment.

Substitution gives $$ \mathbb{E}[B_1^3\mid\mathcal{F}_{1/2}] =B_{1/2}^3+3\left(1-\frac12\right)B_{1/2} =B_{1/2}^3+\frac32B_{1/2}. $$ For an independent-increment check, write \(B_1=B_{1/2}+Z\), where \(Z=B_1-B_{1/2}\) is independent of \(\mathcal{F}_{1/2}\), has mean zero, second moment \(\tfrac12\), and third moment zero. Given \(\mathcal{F}_{1/2}\), set \(x=B_{1/2}\). Expanding the cube and taking the conditional expectation gives $$ \mathbb{E}[(x+Z)^3\mid\mathcal{F}_{1/2}] =x^3+3x^2\mathbb{E}[Z]+3x\mathbb{E}[Z^2]+\mathbb{E}[Z^3] =x^3+\frac32x. $$ This is exactly the formula obtained from Ito’s identity.

Check: The coefficient is \(3(t-s)=3\cdot\tfrac12=\tfrac32\), not \(3(t-s)^2\). The independent increment contributes through its second moment, which is \(t-s=\tfrac12\).

What the Correction Changes

For the square function, the ordinary chain rule would suggest \(B_t^2=2\int_0^t B_s\,dB_s\). The Ito identity instead has the additional \(t\). For the cube, omitting the second derivative term would remove \(3\int_0^t B_s\,ds\). Both omissions change the resulting identities, including their expectations and conditional expectations. In differential notation, the square calculation uses \(d(B_t^2)=2B_t\,dB_t+dt\), while the cube calculation uses \(d(B_t^3)=3B_t^2\,dB_t+3B_t\,dt\).

These are Ito-integral identities. They should not be confused with the Stratonovich chain rule, which uses the notation \(\circ\,dB_t\) and has no extra second-derivative term in its chain rule. The integrals in this tutorial are all written with \(dB_t\), not \(\circ\,dB_t\). The distinction matters: replacing one integral convention with the other without accounting for the correction changes the calculation.

Common mistake: applying the ordinary chain rule to \(B_t^2\) and concluding \(B_t^2=2\int_0^t B_s\,dB_s\). This would make the expectation of \(B_t^2\) equal to zero, because the integral is a square-integrable martingale starting at zero. But \(\mathbb{E}[B_t^2]=t\). The corrected identity \(B_t^2=2\int_0^t B_s\,dB_s+t\) gives \(\mathbb{E}[B_t^2]=t\), as required.

Check Your Understanding

Use the displayed identities and state which integrability or conditional-expectation property justifies each stochastic calculation.

  1. For \(f(x)=x^2\), write \(f'(x)\), \(f''(x)\), and the Ito identity for \(B_t^2\).
  2. Verify that \(B_s^2\) is an admissible Ito integrand on \([0,T]\) by computing \(\mathbb{E}\int_0^T B_s^4\,ds\).
  3. Use the square identity and the Ito isometry to compute \(\operatorname{Var}(B_T^2)\).
  4. Write the cube identity and identify its second-order correction term.
  5. Use the conditional cubic-moment formula when \(s=0\) to compute \(\mathbb{E}[B_t^3]\).