Prove entireness of the linear-combination eigenfunctions for all N
Establish rigorously that the special linear combinations of solutions defined in equations (eq:eigenfeven) for even N and (eq:eigenfodd) for odd N exhibit complete pole cancellation and are entire functions of x for generic values of the parameters h_k and the energy, for arbitrary N.
References
Only for the special linear combinations eq:eigenfeven and eq:eigenfodd do these poles cancel, yielding a function that is entire in x. Although we do not have a rigorous proof of this statement, we have tested it for N=2,3,4,5,6 up to three orders in the Λ expansion.
— Eigenfunctions of deformed Schrödinger equations
(2511.10636 - François et al., 13 Nov 2025) in Section 2.3 (The eigenfunctions), Remarks item 1 and footnote