Exactly-solvable coupled-channel potential models of atom-atom magnetic Feshbach resonances from supersymmetric quantum mechanics
arXiv:0709.0343 · doi:10.1103/PhysRevA.77.012724
Abstract
Starting from a system of radial Schrödinger equations with a vanishing potential and finite threshold differences between the channels, a coupled exactly-solvable potential model is obtained with the help of a single non-conservative supersymmetric transformation. The obtained potential matrix, which subsumes a result obtained in the literature, has a compact analytical form, as well as its Jost matrix. It depends on unconstrained parameters and on one upper-bounded parameter, the factorization energy. A detailed study of the model is done for the case: a geometrical analysis of the zeros of the Jost-matrix determinant shows that the model has 0, 1 or 2 bound states, and 0 or 1 resonance; the potential parameters are explicitly expressed in terms of its bound-state energies, of its resonance energy and width, or of the open-channel scattering length, which solves schematic inverse problems. As a first physical application, exactly-solvable atom-atom interaction potentials are constructed, for cases where a magnetic Feshbach resonance interplays with a bound or virtual state close to threshold, which results in a large background scattering length.
19 pages, 15 figures
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- Eigenphase preserving two-channel SUSY transformations
- Shadow poles in a coupled-channel problem calculated with Berggren basis
- Coupling between scattering channels with SUSY transformations for equal thresholds
- Spectral properties of non-conservative multichannel SUSY partners of the zero potential
- Resonances and continued-fraction Green's functions in non-Hermitian Bose-Hubbard-like quantum models
- Multichannel generalization of eigen-phase preserving supersymmetric transformations