Collective spin systems in dispersive optical cavity QED: Quantum phase transitions and entanglement

Simple item page
dc.creatorMorrison, S.
dc.creatorParkins, A. S.
dc.date2007-11-15
dc.date2008-05-07
dc.date.accessioned2026-07-07T09:37:11Z
dc.date.available2026-07-07T09:37:11Z
dc.descriptionWe propose a cavity QED setup which implements a dissipative Lipkin-Meshkov-Glick model -- an interacting collective spin system. By varying the external model parameters the system can be made to undergo both first-and second-order quantum phase transitions, which are signified by dramatic changes in cavity output field properties, such as the probe laser transmission spectrum. The steady-state entanglement between pairs of atoms is shown to peak at the critical points and can be experimentally determined by suitable measurements on the cavity output field. The entanglement dynamics also exhibits pronounced variations in the vicinities of the phase transitions.
dc.description19 pages, 18 figures, shortened version
dc.identifierhttps://arxiv.org/abs/0711.2325
dc.identifierhttp://arxiv.org/abs/0711.2325
dc.identifierPhys. Rev. A 77, 043810 (2008)
dc.identifierdoi:10.1103/PhysRevA.77.043810
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/160367
dc.subjectQuantum Physics
dc.subjectOther Condensed Matter
dc.titleCollective spin systems in dispersive optical cavity QED: Quantum phase transitions and entanglement
dc.typetext

Files

Collections

arXiv