Rabi Hamiltonian with three instead of two Pauli matrices This question was motivated by a question on Mathoverflow, in which a Hamiltonian is considered that looks like the Rabi Hamiltonian, but with three instead of two Pauli matrices:
$$H=\omega a^\dagger a+\Delta\sigma_z+g_x\sigma_x(a+a^\dagger)+ig_y\sigma_y(a-a^\dagger).$$
In the literature I have only found the Rabi Hamiltonian with $g_y=0$, so with two Pauli matrices. The case $g_y\neq 0$ with three Pauli matrices seems essentially different, at least if $g_x\neq g_y$ and one does not make the rotating wave approximation. Has it been considered before?
Since this model is so fundamental, I am a bit surprised at not having found this generalization, I may be missing something obvious.
 A: I probably should have searched more extensively before posting here, I did eventually find this Hamiltonian in Exceptional and regular spectra of a generalized Rabi model by Michael Tomka, Omar El Araby, Mikhail Pletyukhov, and Vladimir Gritsev. The context is different from quantum optics (which is probably why I could not locate it earlier), it is a model of a two-dimensional electron gas with parabolic confinement in one direction, with a Zeeman field and Rashba and Dresselhaus spin-orbit couplings. The three-Pauli-matrix Rabi Hamiltonian is also referred to as the anisotropic Rabi Hamiltonian (arXiv:1401.5865).
In my answer to the Mathoverflow question I made a conjecture for the ground state energy in the special case that $\Delta=2g_xg_y$:

The generalised Rabi Hamiltonian  $$H_0=\begin{pmatrix} a^\dagger
 a+\alpha^2&\alpha a+\beta a^\dagger\\ \alpha a^\dagger+ \beta
 a&a^\dagger a+ \beta^2 \end{pmatrix}$$ has a doubly degenerate ground state at zero energy
for any $\alpha,\beta\in\mathbb{R}$.

I now see that this conjecture follows from the Bethe Ansatz solution of the generalized Rabi Hamiltonian given in the Tomka et al. paper, section II.B.1. The case $\Delta=2g_xg_y$ corresponds to $\lambda_-=\delta$ in their notation, which is the "exceptional case"$^\ast$ in which the Rabi Hamiltonian has an eigenvalue $E_0=-\lambda_+=-(g_x^2+g_y^2)$. This corresponds to a zero eigenvalue for $H_0$, because the spectrum of $H_0$ is shifted relative to the Rabi spectrum by $(\alpha^2+\beta^2)/2=g_x^2+g_y^2$.
The zero eigenvalue is the ground state, because $H_0$ is positive definite,
$$H_0=Q^\dagger Q,\;\;\text{for}\;\;Q=\begin{pmatrix} \alpha&a\\ a&\beta \end{pmatrix}.$$
The two ground state wave functions, such that $Q\Psi_\pm=0$, are $\Psi_\pm={{\sqrt\beta}\choose{\mp\sqrt\alpha}}|\!\pm\!\!\sqrt{\alpha\beta}\rangle$, in terms of the coherent state $|\gamma\rangle$ with $a|\gamma\rangle=\gamma|\gamma\rangle$.

$^\ast$ In arXiv:1407.5213 the symmetry is identified that enforces the doubly degenerate ground state.
