Applying Itô’s Lemma to the Square of a Geometric Brownian Motion
Summary
The document resolves a sign discrepancy when finding the dynamics and expected value of the square of a driftless geometric Brownian motion, a calculation relevant to the expectation of a squared forward rate. Applying Itô’s lemma directly to the logarithm of the square gives a stochastic term of twice the volatility and a negative volatility correction in the drift. The key error in the alternative derivation is treating the relative change in the squared process as though it were the change in its logarithm; those expressions are not interchangeable without another Itô correction.
Integrating the log dynamics yields a Gaussian exponent whose mean is negative and whose variance contributes a positive term to the exponential expectation. Together these give a positive volatility adjustment in the expected square. The explanation assumes constant volatility and zero drift as stated in the setup; it addresses this specific stochastic calculus step rather than the full pricing of an in-arrears swap.
Key ideas
- For a driftless geometric Brownian motion, Itô’s lemma gives the log of its square a negative volatility correction.
- The relative differential of a squared process is not itself the differential of its logarithm.
- The Gaussian exponent’s variance affects the expectation of its exponential.
- The expected square has a positive volatility adjustment despite the negative drift in its log dynamics.
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Full text
# Log of square of Geometric Brownian Motion
# Log of square of Geometric Brownian Motion
Which of the two calculations below, is wrong? Why?
$dF = \sigma F dW$
First:
$dF^2 = (F^2)' dF + \frac{1}{2}(F^2)''dF.dF$
$dF^2 = 2F dF + dF.dF$
$dF^2 = 2 \sigma F^2 dW + \sigma^2 F^2 dt$
$\frac{dF^2}{F^2}=2\sigma dW + \sigma^2 dt$
$d \ln F^2=2\sigma dW + \sigma^2 dt$
OR
Second:
$d \ln F^2 = (\ln F^2)' dF + \frac{1}{2}(\ln F^2)'' dF.dF$
$d \ln F^2 = \frac{2F}{F^2} dF + \frac{1}{2} (\frac{2F}{F^2})' dF.dF$
$d \ln F^2 = \frac{2}{F} dF +\frac{1}{2} (\frac{2}{F})' dF.dF$
$d \ln F^2 = \frac{2}{F} dF +\frac{1}{2} \frac{-2}{F^2} dF.dF$
$d \ln F^2 = \frac{2}{F} dF - \frac{1}{F^2} dF.dF$
$d \ln F^2 = 2\sigma dW - \sigma^2 dt$
Just for context, I am trying to understand the calculation of In-Arears Swap pricing. So, need to compute expectation of "Square of Forward rate".
The book (Brigo Mercurio) says $E(F(T)^2)=F(0)^2 e^{\sigma^2 T}$
My computations above (Second) tells me that $E(F(T)^2)=F(0)^2 e^{-\sigma^2 T}$
I am stuck and unable to explain the "-" sign before $\sigma^2 dt$ which I see.
Ref: Brigo and Mercurio "Interest Rates Models - Theory and Practice" Second Edition, Part V, Chapter 13, Equation 13.3
## Answer by Magic is in the chain (score 5, accepted)
https://quant.stackexchange.com/a/45310
The second solution is correct, so the solution at t is:
$F_t^2=F_0^2e^{2 \sigma W_t-\sigma^2t}$
Now apply expectation to both sides.
$ E\left[F_t^2\right]=F_0^2 \, E\left[e^{2 \sigma W_t-\sigma^2t}\right]$
The term in the exponent is just Gaussian so let’s call it X: $X=2 \sigma W_t-\sigma^2t$
It’s mean and variance are:
$E[X]=-\sigma^2t$
$V[X]=4 \sigma^2t$
And hence: $E[X]+\frac{1}{2}V[X]=\sigma^2t$
And therefore: $ E\left[F_t^2\right]=F_0^2 \, E\left[e^{X}\right] =F_0^2 e^{\sigma^2t}$
For the mean and half the variance business above, please see the discussion here:https://math.stackexchange.com/questions/176196/calculate-the-expected-value-of-y-ex-where-x-sim-n-mu-sigma2
## Answer by Raskolnikov (score 3)
https://quant.stackexchange.com/a/45298
The first one is wrong.
As I said in my comment, you seem to be shoving some terms under the rug. In fact:
$$d\ln F^2 = \frac{1}{F^2}dF^2 + \frac{1}{2}(-\frac{1}{F^4})dF^2\cdot dF^2 \; .$$
Which leads to
$$d\ln F^2 = \frac{1}{F^2}dF^2 - 2\sigma^2dt \; .$$
Hence with this correct substitution in the first computation, both computations will lead to the same result.
By the way, $\ln F^2 = 2\ln F$. This gives an even more straightforward confirmation that this is the correct formula.
## Answer by SmurfAcco (score 2)
https://quant.stackexchange.com/a/45326
I just want to offer an alternative approach to the problem. I simply used Ito's Lemma. We have $$ dF_t = \sigma F_t dW_t.$$ Now, we want to know the dynamics of $\ln F_t^2$ (https://en.wikipedia.org/wiki/It%C3%B4%27s_lemma). We set $f(t, x) = \ln x^2$ and get the derivatives $$ \frac{\partial f(t, x) }{\partial t} = 0, \quad \frac{\partial f(t, x)}{\partial x} = \frac{2}{x}, \quad \frac{\partial^2 f(t, x)}{\partial x^2 }= -\frac{2}{x^2}$$ It follows \begin{align*} df(t,F_t) & = \frac{\partial f(t, x) }{\partial t}dt + \frac{\partial f(t, x)}{\partial x} dF_t + \frac{1}{2} \frac{\partial^2 f(t, x)}{\partial x^2 }(dF_t)^2\\ & = 0 + \frac{2}{F_t}\sigma F_t dW_t + \frac{1}{2}\frac{-2}{F_t^2}\sigma^2F_t^2dt\\ & = 2\sigma dW_t -\sigma^2dt \end{align*}
You probabably did it the same way as I. However, this is also to show an easy application of Ito's Lemma to a maybe not so sophisticated reader.
## Answer by Cettt (score 1)
https://quant.stackexchange.com/a/45297
the second one is correct because you have used the right tools to compute $d \ln F^2$.
In the first one everything up to the last conclusion is correct.
However,
$$ \frac{dF^2}{F^2} = 2\sigma dW + \sigma^2dt $$
does not imply $$ d \ln F^2 = 2\sigma dW + \sigma^2 dt. $$
This is only true if $F$ would not be raised to the power of two.Shown in full with attribution under the source's licence. Licence: CC BY-SA 4.0 (Stack Exchange)
This summary was written by Stratmill's research agent from the original; it is not a copy of the source.