Let $(B_t)_{t \geq 0}$ be a Brownian motion and $T \geq 0$. Find a constant $z_T \in \mathbb{R}$ and $(s,\omega) \in \mathcal{V}([0,T])$ such that $F_T(\omega) = z_T + \int_{0}^{T} \phi_T(s,\omega)dB_s(\omega)$ when $F_T(\omega) = \int_0^T B^3_s(\omega) ds$.
The idea is to rewrite $\int_0^T B^3_s ds$ using Itô's lemma, but it seems like I'm stuck in a loop. We have
\begin{equation*} \begin{split} d(tB_t^3) &= B_t^3dt + 3tB_t^2dB_t + 3t B_t d \langle B \rangle_t \iff \\ \int_0^T B_t^3 dt&= TB_T^3 - \int_0^T 3tB_t^2 d B_t - \int_0^T 3t B_t dt \end{split} \end{equation*}
Now two new terms appeared, $TB_T^3$ and $\int_0^T 3t B_t dt$. If we plug in
$$ TB_T^3 = \int_0^T B_t^3 dt + \int_0^T 3tB_t^2 d B_t + \int_0^T 3t B_t dt $$
everything cancels, yielding $0=0$. Otherwise we can proceed by using Itô on $\int_0^T 3t B_t dt $ to see what we get, but I'm not quite sure if that's gonna give anything. Any hints?
Edit, solution:
We have that
\begin{equation*} \begin{split} &\int_0^T 3t B_t dt = \frac{3}{2}T^2B_T - \int_0^T \frac{3}{2}t^2 dB_t \\ &TB_T^3 = \int_0^T 3T(B_t^2 +T -t) dB_t \\ &\frac{3}{2}T^2B_T = \frac{3}{2}T^2 \int_0^T dB_t \end{split} \end{equation*}
by some Itô engineering, yielding
$$ \int_0^T B^3_t dt = \int_0^T (T-t)(3T + 3B_t^2 + \frac{3}{2}(T+t))dB_t. $$
Seems I obtain something different which cannot be since the representation should be unique.