Linear square-well Schr"{o}dinger equation endowed with a singular logarithmic spike in the origin is studied. The study is methodical, motivated by the problem of non-gausson states , generated by nonlinear Schr"{o}dinger equations. Once the state-dependent self-interaction term is chosen logarithmic, , the nonlinear model develops the puzzling logarithmic (i.e., weakly singular) repulsive barriers near the nodal zeros of at . In our linearized approach the weak-coupling regime is shown reliably described by the routine Rayleigh-Schr"{o}dinger perturbation theory. It even provides the first-order picture of the spectrum in closed-form. Beyond the weak-coupling regime an amendment of the unperturbed Hamiltonian is recommended. Finally, an analytic insight into the nature of the singularity at is obtained, in a non-perturbative setting, after the change of variables .

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