Let $B$ be a continuous Brownian motion, for every $t \geqslant 0$. I've to calculate :
$E\left[B_t | B_t^2 \right]$
They told me that the result is 0 by symmetry ... can anyone explain it to me please.
Could the resolution be like $$E[E\left[B_t | B_t^2 \right] | I_{(-a,a)}(B_t)]=E[B_t | I_{(-a,a)}(B_t)]=E[B_tI_{(-a,a)}(B_t)] = \int^a_{-a} {\frac{x}{\sqrt {2 \pi t}}e^{\frac{-x^2}{2t}}} =0$$
because the sigma field $\sigma\left({B^2_t}\right)$ contains the one of the indicator function of $B_t$.
Then $a$ it's arbitrary so $E\left[B_t | B_t^2 \right]=0$ $\mathbb P$-a.s.
Heuristically you can think of it like this: If you know the value of $B_t^2$, then $B_t$ will either be $+\sqrt{B_t^2}$ or $-\sqrt{B_t^2}$, each with probability one half. So the expectation should be 0. With this educated guess you can now proceed by just checking if $0$ fulfills the requirements of being the conditional expectation:
Measurability: Since $0$ is constant, it is measurable w.r.t. to any $\sigma$-algebra, especially $\sigma(B_t^2)$
Integrals Let $A \in \sigma(B_t^2)$. Then $A = (B_t^2)^{-1}(C)$ for some $C \in \mathcal{B}(\mathbb{R})$. $$\int_A B_t dP = \int_{(B_t^2)^{-1}(C) \cap B_t > 0} B_t dP + \int_{(B_t^2)^{-1}(C) \cap B_t < 0} B_t dP = 0 = \int_A 0 dP$$
so $E[B_t | B_t^2] = 0$ a.s.. The last step holds because the mentioned symmetry. To make it more precise, you can try to write $(B_t^2)^{-1}(C)$ in terms of $B_t^{-1}(D)$ for some set $D$.