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arXiv:2606.12682 · Journal of Physics A Mathematical and Theoretical

Supersymmetry of dissipative Bose-Fermi systems with application to Jaynes-Cummings and Dicke models

Colin V. Coane, Francesco Iachello

quant-phmath-phSubmitted Jun 10, 2026• Announced Jun 12, 2026• 0 citations
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Abstract

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 $u(1|1)$ and that the Hamiltonian of the Dicke model commutes both with the linear invariant of $\sum_{i} u_{i}(1|1)$ and with the invariant of an additional $su(2)$ algebra. Our methods apply to various coupled Bose-Fermi systems with $u(1|1)$ and more generally with $u(n|m)$ dynamical superalgebras, and may provide efficient tools for studying more complicated examples.

Journal reference
J. Phys. A: Math. Theor. 59 345303 (2026)
DOI
10.1088/1751-8121/ae99a3
Comments
14 + 10 pages, 9 figures

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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.
The super-algebraic structure of a generalized version of the Jaynes–Cummings model is investigated. We find that a Z 2 graded extension of the so (2,1) Lie algebra is the underlying symmetry of this model. It is isomorphic to the four-dimensional super-algebra u (1/1) with two odd and two even elements. Differential matrix operators are taken as realization of the elements of the superalgebra to which the model Hamiltonian belongs. Several examples with various choices of superpotentials are presented. The energy spectrum and corresponding wavefunctions are obtained analytically.
Abstract A novel approach is proposed to analyze a rather vast counter-rotating Hamiltonian interaction in the context of quantum optics.The method relies upon the supersymmetric mapping of the corresponding rotating interaction and allows the analysis of thedynamics in the counter-rotating system in a fully general and exact analytical manner by diagonalizing the correspondingHamiltonian. Intriguing features of the counter-rotating system are revealed through the simple supersymmetric transformation.In turn, such interesting attributes have an important range of potential technological applications. In this way, supersymmetryemerges as a useful tool to both connect and construct exactly solvable photonic systems in quantum optics, as well as toanalyze the corresponding physical consequences and their possible technology implementations.
We analyze symmetries of the integrable generalizations of Jaynes–Cummings and Dicke models associated with simple Lie algebras g and their reductive subalgebras gK [T. Skrypnyk, “Generalized n-level Jaynes-Cummings and Dicke models, classical rational r-matrices and nested Bethe ansatz,” J. Phys. A: Math. Theor. 41, 475202 (2008)]. We show that their symmetry algebras contain commutative subalgebras isomorphic to the Cartan subalgebras of g, which can be added to the commutative algebras of quantum integrals generated with the help of the quantum Lax operators. We diagonalize additional commuting integrals and constructed with their help the most general integrable quantum Hamiltonian of the generalized n-level many-mode Jaynes–Cummings and Dicke-type models using nested algebraic Bethe ansatz.
We consider quantum integrable systems associated with non-skew-symmetric sl (2)-valued classical r -matrices. For a special class of such r -matrices we construct a one-parametric family of integrable modifications of the ‘two-level one-mode’ Jaynes–Cummings–Dicke Hamiltonians, with non-uniform coupling constants, containing additional Kerr- and Stark-type nonlinearities. We also construct a family of integrable Bose–Hubbard-type dimers and a family of integrable models that unifies Bose–Hubbard- and Jaynes–Cummings–Dicke-type models and may be called a ‘two-level, two-mode’ Jaynes–Cummings–Dicke model or a ‘spin generalization’ of a Bose–Hubbard dimer. We diagonalize the constructed models with the help of the algebraic Bethe ansatz technique in any irreducible representation of the sl (2) ⊕ N spin algebra.