Covering models of the asymmetric quantum Rabi model: $\eta$-shifted non-commutative harmonic oscillators

Abstract

The non-commutative harmonic oscillator (NCHO) is a matrix valued differential operator originally introduced as a generalization of the quantum harmonic oscillator having a weaker $\mathfrak{sl}_2(\mathbb{R})$-symmetry. The spectrum of the NCHO has remarkable properties, including the presence of number theoretical structures such as modular forms, elliptic curves and Eichler cohomology observed in the special values of the associated spectral zeta function. In addition, the Heun ODE picture of the eigenvalue problem of the NCHO reveals a connection with the quantum Rabi model (QRM), a fundamental interaction model from quantum optics. In this paper we introduce an $\eta$-shifted NCHO ($\eta$-NCHO) that has an analogous relation with the asymmetric quantum Rabi model (AQRM) and describe its basic properties. Even though the shift factor does not break the parity symmetry of the NCHO, a certain type of degeneracies appears for $\eta \in \frac12 \mathbb{Z}$, as if mirroring the situation of the AQRM. We give furthermore a detailed description of the confluence process, that we call iso-parallel confluence process due to the fact that it requires a parallel transformation of two parameters describing the spectrum of $\eta$-NCHO and representations of $\mathfrak{sl}_2(\mathbb{R})$. We relate the eigenvalues of the two models under the iso-parallel confluence process, including how the quasi-exact eigenfunctions of the $\eta$-NCHO correspond to Juddian solutions of the AQRM. From the point of view of this confluence process, a family of $\eta$-NCHO corresponds to a single AQRM, thus we may regard the $\eta$-NCHO as a covering of the AQRM. We expect the study of the $\eta$-NCHO and the AQRM from this point of view to be helpful for the clarification of several questions on the AQRM, including the hidden symmetry and the number of Juddian solutions.