In an innovative inverse-problem construction the measured, experimental
energies E1, E2, ...EN of a quantum bound-state system are assumed
fitted by an N-plet of zeros of a classical orthogonal polynomial fN(E). We
reconstruct the underlying Hamiltonian H (in the most elementary
nearest-neighbor-interaction form) and the underlying Hilbert space H
of states (the rich menu of non-equivalent inner products is offered). The
Gegenbauer's ultraspherical polynomials fn(x)=Cnα(x) are chosen for
the detailed illustration of technicalities.Comment: 29 pp., 1 fi