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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.

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Background

Each individual saddle solution of the finite-difference equation has poles at x = a_I + \hbar n. The authors construct explicit linear combinations (eqs. (eq:eigenfeven) and (eq:eigenfodd)) that are designed to cancel these poles and yield entire off-shell eigenfunctions for generic parameters, which become L2-normalizable only on a discrete energy spectrum.

They report extensive checks for N=2–6 up to several orders in the \Lambda expansion but note the lack of a rigorous proof that entireness holds generally. A formal proof would validate the exact solvability claim for all polynomial potentials considered.

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