Gegenbauer-solvable quantum chain model
arXiv:1011.4803 · doi:10.1103/PhysRevA.82.052113
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.
29 pp., 1 fig
References in corpus (20)
- Making Sense of Non-Hermitian Hamiltonians
- Exponentially Fragile PT-Symmetry in Lattices with Localized Eigenmodes
- A non-Hermitian symmetric Bose-Hubbard model: eigenvalue rings from unfolding higher-order exceptional points
- Three-Hilbert-Space Formulation of Quantum Mechanics
- PT Symmetry on the Lattice: The Quantum Group Invariant XXZ Spin-Chain
- Interface between Hermitian and non-Hermitian Hamiltonians in a model calculation
- A spin chain model with non-Hermitian interaction: The Ising quantum spin chain in an imaginary field
- Scattering theory with localized non-Hermiticities
- Tridiagonal PT-symmetric N by N Hamiltonians and a fine-tuning of their observability domains in the strongly non-Hermitian regime
- Maximal couplings in PT-symmetric chain-models with the real spectrum of energies
- Discrete PT-symmetric models of scattering
- Non-Hermitian Hamiltonians of Lie algebraic type
- Scattering theory using smeared non-Hermitian potentials
- Calculation of the metric in the Hilbert space of a PT-symmetric model via the spectral theorem
- Fundamental length in quantum theories with PT-symmetric Hamiltonians
- Conditional observability
- Fragile PT-symmetry in a solvable model
- Quantum Mechanics of Proca Fields
- Metrics and isospectral partners for the most generic cubic PT-symmetric non-Hermitian Hamiltonian
- Fundamental length in quantum theories with PT-symmetric Hamiltonians II: The case of quantum graphs