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Optics Communications

Dynamical supersymmetries of the Jaynes—Cummings hamiltonian

H. A. Schmitt, A. Mufti

Published Nov 1, 1990• 10 citations
Publisher
DOI
10.1016/0030-4018(90)90074-4

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We demonstrate how supersymmetries of Hamiltonians for coupled Bose-Fermi systems can be used to place the Hamiltonians of the Jaynes-Cummings model and Dicke model under the rotating wave approximation in matrix form and provide explicit analytic solutions for their eigenvalues. We then use this supersymmetry to place the Liouvillians of the associated Markovian open systems in matrix form and provide explicit solutions for their eigenvalues. These results are a consequence of the fact that the Hamiltonian of the Jaynes-Cummings model commutes with the linear Casimir invariant of the superalgebra u(1∣1)u(1|1)u(1∣1) and that the Hamiltonian of the Dicke model commutes both with the linear invariant of ∑iui(1∣1)\sum_{i} u_{i}(1|1)∑i​ui​(1∣1) and with the invariant of an additional su(2)su(2)su(2) algebra. Our methods apply to various coupled Bose-Fermi systems with u(1∣1)u(1|1)u(1∣1) and more generally with u(n∣m)u(n|m)u(n∣m) dynamical superalgebras, and may provide efficient tools for studying more complicated examples.
It is shown that for a given Hermitian Hamiltonian possessing supersymmetry, there is always a non-Hermitian Jaynes–Cummings-type Hamiltonian (JCTH) admitting entirely real spectra. The parent supersymmetric Hamiltonian and the corresponding non-Hermitian JCTH are simultaneously diagonalizable. The exact eigenstates of these non-Hermitian Hamiltonians are constructed algebraically for certain shape-invariant potentials, including a non-Hermitian version of the standard Jaynes–Cummings (JC) model for which the parent supersymmetric Hamiltonian is the superoscillator. It is also shown that a non-Hermitian version of the several physically motivated generalizations of the JC model admits entirely real spectra. The positive-definite metric operator in the Hilbert space is constructed explicitly along with the introduction of a new inner product structure, so that the eigenstates form a complete set of orthonormal vectors and the time evolution is unitary.