Steady-state susceptibility to a control parameter yields a universal lower bound on relaxation and second-order correlation times of driven-dissipative quantum systems.
Time-resolved second-order autocorrelation function of parametric downconversion
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abstract
We study a possibility of measuring the time-resolved second-order autocorrelation function of one of two beams generated in type-II parametric downconversion by means of temporal magnification of this beam, bringing its correlation time from the picosecond to the nanosecond scale, which can be resolved by modern photodetectors. We show that such a measurement enables one to infer directly the degree of global coherence of that beam, which is linked by a simple relation to the number of modes characterizing the entanglement between the two generated beams. We illustrate the proposed method by an example of photon pairs generated in a periodically poled KTP crystal with a symmetric group velocity matching for various durations of the pump pulse, resulting in different numbers of modes. Our theoretical model also shows that the magnified double-heralded autocorrelation function of one beam exhibits a local maximum around zero delay time, corresponding to photon bunching at a short time scale.
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Time correlations from steady-state expectation values
Steady-state susceptibility to a control parameter yields a universal lower bound on relaxation and second-order correlation times of driven-dissipative quantum systems.