Quantum jumps in open cavity optomechanics and Liouvillian versus Hamiltonian exceptional points
Aritra Ghosh, M. Bhattacharya

TL;DR
This paper investigates the nature of exceptional points in cavity optomechanics, distinguishing between Liouvillian and Hamiltonian types, and introduces a hybrid spectral framework to understand their interplay and robustness.
Contribution
It clarifies the differences between Liouvillian and Hamiltonian exceptional points in optomechanics and develops a unified spectral framework using thermofield formalism.
Findings
Liouvillian exceptional points are temperature-independent.
Hamiltonian exceptional points are thermally shifted due to conditional damping.
Exceptional points are robust under small hybrid perturbations.
Abstract
Exceptional points, where two or more eigenstates of a non-Hermitian system coalesce, are now of interest across many fields of physics, from the perspective of open-system dynamics, sensing, nonreciprocal transport, and topological phase transitions. In this work, we investigate exceptional points in cavity optomechanics, a platform of interest to diverse communities working on gravitational-wave detection, macroscopic quantum mechanics, quantum transduction, etc. Specifically, we clarify the role of quantum jumps in making a clear distinction between Liouvillian and Hamiltonian exceptional points in optomechanical systems. While the Liouvillian exceptional point arises from the unconditional Lindblad dynamics and is independent of the phonon-bath temperature, the Hamiltonian exceptional point emerges from the conditional no-jump evolution and acquires a thermal shift due to an…
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Taxonomy
TopicsMechanical and Optical Resonators · Quantum Mechanics and Non-Hermitian Physics · Quantum many-body systems
