2013
DOI: 10.1103/physrevlett.110.133605
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UltrasensitiveN-Photon Interferometric Autocorrelator

Abstract: We demonstrate a novel method to measure Nth-order (N=1,2,3,4) interferometric autocorrelation with high sensitivity and temporal resolution. It is based on the combination of linear absorption and nonlinear detection in a superconducting nanodetector, providing much higher efficiency than methods based on all-optical nonlinearities. Its temporal resolution is only limited by the quasiparticle energy relaxation time, which is directly measured to be in the 20 ps range for the NbN films used in this work. We pr… Show more

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Cited by 32 publications
(36 citation statements)
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References 33 publications
(38 reference statements)
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“…It is crucial for this experiment that the pulse duration is shorter than the lifetime of an excitation, which was measured to be several tens of picoseconds 19,25,35 . If the pulse duration is longer than that, it is possible to have a pulse which produces two excitations which are far enough apart in time that one has died out before the second is created; this will therefore not result in a multiphoton excitation.…”
Section: Methodsmentioning
confidence: 99%
“…It is crucial for this experiment that the pulse duration is shorter than the lifetime of an excitation, which was measured to be several tens of picoseconds 19,25,35 . If the pulse duration is longer than that, it is possible to have a pulse which produces two excitations which are far enough apart in time that one has died out before the second is created; this will therefore not result in a multiphoton excitation.…”
Section: Methodsmentioning
confidence: 99%
“…In a bias current range from 0.45 to 0.65 I b /I c , the excitation lifetime changes by an order of magnitude. In contrast, in NbN [31,32], the lifetime is constant over a similar range of bias currents (0.3 -0.55 I b /I c ).…”
mentioning
confidence: 98%
“…In particular, the pulses which the light source sends out should be shorter than the lifetime of an excitation in the detector. This number can be determined in a separate experiment [121] and is 20 ps for NbN SNSPDs. Moreover, the pulses should be separated by more than the dead time of the detector, to make sure that each individual pulse corresponds to a separate probing of the detector, uncorrelated to the previous ones.…”
Section: Appendix A2 Experimental Considerationsmentioning
confidence: 99%