  We exhibit various restrictions about the wellposedness of the Schr\"odinger
product $$\mathcal{L}: z \longmapsto -\imath \int_0^t e^{\imath \Delta s}\big(
z_s\cdot \Psi_s\big) ds $$ where $\Psi$ refers to the so-called linear solution
of the stochastic Schr\"dinger problem. We focus more specifically on the case
where $\Psi$ satisfies $$(\imath \partial_t-\Delta)\Psi=\dot{B}, \quad
\Psi_0=0,\quad \quad t\in \mathbb{R}, \ x\in \mathbb{T},$$where $\dot{B}$ is a
white noise in space with fractional time covariance of index $H>\frac12$. As
an important consequence of our analysis, we obtain that if $H$ is close to
$\frac12$ (that is $\dot{B}$ is close to a space-time white noise), then it is
essentially impossible to treat the stochastic NLS problem $$(\imath
\partial_t-\Delta)u=\lambda\, u^{p} \overline{u}^q+\dot{B}, \quad u_0=0,\quad
\quad \lambda \in \{-1,1\}, \ p,q\geq 1, \ t\in \mathbb{R}, \ x\in
\mathbb{T},$$using only a first-order expansion of the solution ("$u=\Psi+z$").
