Long linear chains of trapped ions concentrate the motional spectrum to revive strong carrier excitation of narrow optical transitions outside the Lamb-Dicke regime.
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Kinetically constrained superradiance splits Dicke superradiance into selective collective decay channels that trap finite-momentum spin waves and produce dissipation-generated entanglement.
In diverse superradiant models the normal phase occupies the origin and the transition occurs only once along radial coupling vectors under mean-field theory at finite temperature, permitting concise boundary calculations.
citing papers explorer
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Carrier Revival in Long Trapped-Ion Chains
Long linear chains of trapped ions concentrate the motional spectrum to revive strong carrier excitation of narrow optical transitions outside the Lamb-Dicke regime.
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Kinetically constrained superradiance
Kinetically constrained superradiance splits Dicke superradiance into selective collective decay channels that trap finite-momentum spin waves and produce dissipation-generated entanglement.
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General phase diagram features of superradiant phase transitions
In diverse superradiant models the normal phase occupies the origin and the transition occurs only once along radial coupling vectors under mean-field theory at finite temperature, permitting concise boundary calculations.