Abstract
In an innovative inverse-problem construction the measured, experimental energies , , ... of a quantum bound-state system are assumed fitted by an N-plet of zeros of a classical orthogonal polynomial . We reconstruct the underlying Hamiltonian (in the most elementary nearest-neighbor-interaction form) and the underlying Hilbert space of states (the rich menu of non-equivalent inner products is offered). The Gegenbauer's ultraspherical polynomials are chosen for the detailed illustration of technicalities.
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