I think I found a solution and thatEdited because the original answer solved the problem for $\ell^1(\mathbf{Z})$ submodules not for $\ell^2(\mathbf{Z})$ ones.
An $\{0\}$$\ell^1(\mathbf{Z})$-submodule of $\ell^2(\mathbf{Z})$ is just an invariant subspace under the only simple moduleleft regular representation (in$\lambda$. If $P:\ell^2(\mathbf{Z}) \to \ell^2(\mathbf{Z})$ is the normprojection onto a $\lambda$-closed sense).
To obtain thatinvariant subspace, you have to usethen it lies in the following theorem of Wiener, see Theorem 4.64commutant of Folland's
4.64 Theorem. (Wiener's Theorem), if $J$ is a closed ideal in $L^1(G)$ and $\nu(J) = \emptyset$, then $J=L^1(G)$.
where $G$$\lambda[\mathbf{Z}]$, which is a LCH Abelian group andjust $\nu(J) \subset \widehat{G}$ is the nullset over the dual. You also$L^\infty(\mathbf{T})$ after conjugating with the following Theorem fromFourier transform and applying the same book:
4.67 Theorem. Suppose $J$ is a closed ideal in $L^1(G)$, $f \in L^l(G)$, and $\nu(J) \subset \nu(f)$. If $\partial \, \nu(J) \cap \partial \, \nu(f)$ contains no non empty perfect set, then $f \in J$.
If $J = \{0\}$, it is simplePlancherel theorem. Otherwise, there are two casesThis gives that, if $J = \ell^1(\mathbf{Z})$ after taking the Fourier transform, then there is nothing to prove. If $J$any closed submodule is smaller thanof the form $\ell^1(\mathbf{Z})$$\mathbf{1}_E \cdot L^2(\mathbf{T})$, then its nullfor a measurable set $S$ has to be non-empty by Wiener's Theorem$E$. ItThe reciprocal is also non-totaltrue. But thenEvery measurable set $\mathbf{T} \setminus S$ contains(up to measure zero differences) gives a small interval whose complement C has non-intersecting boundary with that of $S$submodule. The annihilator of $C$Thus, the only simple module is a closed submodule$\{0\}$.