Quantum heat engines: limit cycles and exceptional points

Abstract

We show that the inability of a quantum Otto cycle to reach a limit cycle is connected with the propagator of the cycle being non-compact. For a working fluid consisting of quantum harmonic oscillators, the transition point in parameter space where this instability occurs is associated with a non-hermitian degeneracy (exceptional point) of the eigenvalues of the propagator. In particular, a third-order exceptional point is observed at the transition from the region where the eigenvalues are complex numbers to the region where all the eigenvalues are real. Within this region we find another exceptional point, this time of second order, at which the trajectory becomes divergent. The onset of the divergent behavior corresponds to the modulus of one of the eigenvalues becoming larger than one. The physical origin of this phenomenon is that the hot and cold heat baths are unable to dissipate the frictional internal heat generated in the adiabatic strokes of the cycle. This behavior is contrasted with that of quantum spins as working fluid which have a compact Hamiltonian and thus no exceptional points. All arguments are rigorously proved in terms of the systems' associated Lie algebras.

References in corpus (3)

• Bloch vectors for qudits
• The quantum harmonic Otto cycle
• The Quantum Refrigerator: The quest for absolute zero

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• Quantumness and thermodynamic uncertainty relation of finite-time Otto cycle
• Photonic chiral state transfer near the Liouvillian exceptional point
• A Quantum Otto Engine with Shortcuts to Thermalization and Adiabaticity
• A Finite-Time Quantum Otto Engine subject to Control Noise and Enhancement Techniques
• Periodically-driven quantum thermal machines from warming up to limit cycle