In quantum chemistry, the wavefunction for a molecule can be viewed as the output of a function $\xi(m, n_1,..., n_k)$ with $m, n_i \in \mathbb{Z}^+$ that returns a $|\psi\rangle$ that satisfies a $H|\psi\rangle = E|\psi\rangle$. $H$ is the electrostatic Hamiltonian for $m$ electrons and $k$ nuclei with charges $\{+n_k\}$ (and the appropriate masses). I believe there is an injective mapping between $\xi$ and $|\psi\rangle$, right?
In which case, how are chemical isomers explained? All isomers for a given chemical formula are stable and have the same $\xi$, but they have different energy eigenvalues and different structures.