Room-temperature cavity with AlGaAs coatings achieves 4.2×10^{-17} fractional frequency instability, with birefringence fluctuations identified as a leading noise source and acceleration noise mitigated by feed-forward.
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In the subradiant regime of a bad-cavity laser, a dissipative phase transition maps to a switch from detailed-balance Markov chains to ones with time-asymmetric currents and N-scaling entropy production, producing observable self-pulsing.
The maximum photon emission rate in atomic ensembles scales universally as atom number times optical depth at fixed density, unifying ordered and disordered systems from independent emission to the Dicke limit.
Superradiance in disordered 1D waveguide QED keeps its ideal N² peak-rate scaling, driven by spins that spontaneously order their phases according to their random positions.
In a minimal model of partially pumped atomic ensembles, collective dissipation induces interference that allows tuning linewidth from size-independent to extensive and photon statistics from antibunched to bunched via phase and pump rate.
citing papers explorer
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Laser stabilized to a room temperature cavity with AlGaAs coatings reaching $4.2 \times 10^{-17}$ fractional frequency instability
Room-temperature cavity with AlGaAs coatings achieves 4.2×10^{-17} fractional frequency instability, with birefringence fluctuations identified as a leading noise source and acceleration noise mitigated by feed-forward.
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Dynamical aspects of steady-state subradiance: Detailed balance and its breakdown
In the subradiant regime of a bad-cavity laser, a dissipative phase transition maps to a switch from detailed-balance Markov chains to ones with time-asymmetric currents and N-scaling entropy production, producing observable self-pulsing.
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Optical depth dictates universal bounds on many-body decay in atomic ensembles
The maximum photon emission rate in atomic ensembles scales universally as atom number times optical depth at fixed density, unifying ordered and disordered systems from independent emission to the Dicke limit.
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Robust Superradiance and Spontaneous Spin Ordering in Disordered Waveguide Quantum Electrodynamics
Superradiance in disordered 1D waveguide QED keeps its ideal N² peak-rate scaling, driven by spins that spontaneously order their phases according to their random positions.
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One knob to tune them all: Phase-controlled photon statistics and linewidth in partially pumped atomic ensembles
In a minimal model of partially pumped atomic ensembles, collective dissipation induces interference that allows tuning linewidth from size-independent to extensive and photon statistics from antibunched to bunched via phase and pump rate.