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This theoretical study demonstrates how dipole-dipole interactions in a Rydberg-atom cavity system can fundamentally alter dissipative phase transitions, potentially enabling superradiant phases at weaker coupling strengths. Such precise control over criticality is vital for advancing quantum state engineering and improving the sensitivity of future quantum sensors. The research offers fundamental insights into nonequilibrium dynamics without relying on current commercial AI or hardware products.
Multicritical dissipative phase transitions manipulated by dipole--dipole interactions
arXiv:2607.20905v1 Announce Type: new Abstract: Precise control of criticality in superradiant phase transitions is essential for quantum state engineering and the simulation of nonequilibrium phase transitions. Here, we investigate theoretically multicritical phenomena in a dissipative two-Rydberg-atom cavity--QED system. The intrinisic dipole--dipole interaction between the two Rydberg atoms restructures the energy-level landscape of the atomic subsystem, thereby significantly modifying the boundary of the continuous second-order superradiant phase transition, and shifting both the phase boundary and the multicritical point toward weaker atom--cavity strengths. For sufficiently strong dipole--dipole interactions, the continuous second-order phase transition and the multicritical point both disappear, leaving only a discontinuous first--order phase transition that enables the emergence of a superradiant phase even at arbitrarily weak atom--cavity coupling. This work is of fundamental interest for studying dissipative quantum phase transitions, with potential implications for quantum precision measurement and quantum sensing.
Abstract:Precise control of criticality in superradiant phase transitions is essential for quantum state engineering and the simulation of nonequilibrium phase transitions. Here, we investigate theoretically multicritical phenomena in a dissipative two-Rydberg-atom cavity--QED system. The intrinisic dipole--dipole interaction between the two Rydberg atoms restructures the energy-level landscape of the atomic subsystem, thereby significantly modifying the boundary of the continuous second-order superradiant phase transition, and shifting both the phase boundary and the multicritical point toward weaker atom--cavity strengths. For sufficiently strong dipole--dipole interactions, the continuous second-order phase transition and the multicritical point both disappear, leaving only a discontinuous first--order phase transition that enables the emergence of a superradiant phase even at arbitrarily weak atom--cavity coupling. This work is of fundamental interest for studying dissipative quantum phase transitions, with potential implications for quantum precision measurement and quantum sensing.
arXiv:2607.20905 [quant-ph]
(or arXiv:2607.20905v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2607.20905 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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