|
|
|
|
LEADER |
02763 am a22003373u 4500 |
001 |
110756 |
042 |
|
|
|a dc
|
100 |
1 |
0 |
|a Calandri, Niccolo
|e author
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science
|e contributor
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Research Laboratory of Electronics
|e contributor
|
100 |
1 |
0 |
|a Calandri, Niccolo
|e contributor
|
100 |
1 |
0 |
|a Zhao, Qingyuan
|e contributor
|
100 |
1 |
0 |
|a Zhu, Di
|e contributor
|
100 |
1 |
0 |
|a Dane, Andrew E.
|e contributor
|
100 |
1 |
0 |
|a Berggren, Karl K
|e contributor
|
700 |
1 |
0 |
|a Zhao, Qingyuan
|e author
|
700 |
1 |
0 |
|a Zhu, Di
|e author
|
700 |
1 |
0 |
|a Dane, Andrew E.
|e author
|
700 |
1 |
0 |
|a Berggren, Karl K
|e author
|
245 |
0 |
0 |
|a Superconducting nanowire detector jitter limited by detector geometry
|
260 |
|
|
|b American Institute of Physics (AIP),
|c 2017-07-18T15:32:38Z.
|
856 |
|
|
|z Get fulltext
|u http://hdl.handle.net/1721.1/110756
|
520 |
|
|
|a Detection jitter quantifies variance introduced by the detector in the determination of photon arrival time. It is a crucial performance parameter for systems using superconducting nanowire single photon detectors (SNSPDs). In this work, we have demonstrated that the detection timing jitter is limited in part by the spatial variation of the photon detection events along the length of the wire. We define this jitter source as a geometric jitter since it is related to the length and area of the SNSPD. To characterize the geometric jitter, we have constructed a differential cryogenic readout with less than 7 ps of an electronic jitter that can amplify the pulses generated from the two ends of an SNSPD. By differencing the measured arrival times of the two electrical pulses, we were able to partially cancel out the difference of the propagation times and thus reduce the uncertainty of the photon arrival time. We proved that the variation of the differential propagation time was a few ps for a 3 μm × 3 μm device, while it increased up to 50 ps for a 20 μm × 20 μm device. In a 20 μm × 20 μm large SNSPD, we achieved a 20% reduction in the overall detection timing jitter for detecting the telecom-wavelength photons by using the differential cryogenic readout.
|
520 |
|
|
|a National Science Foundation (U.S.) (ECCS1-509486)
|
520 |
|
|
|a United States. Air Force. Office of Scientific Research (ECCS1-509486)
|
520 |
|
|
|a Roberto Rocca Foundation
|
520 |
|
|
|a Singapore. Agency for Science, Technology and Research (National Science Scholarship)
|
520 |
|
|
|a United States. National Aeronautics and Space Administration (Space Technology Research Fellowship Grant NNX14AL48H)
|
546 |
|
|
|a en_US
|
655 |
7 |
|
|a Article
|
773 |
|
|
|t Applied Physics Letters
|