scholarly journals On-chip time resolved detection of quantum dot emission using integrated superconducting single photon detectors

2013 ◽  
Vol 3 (1) ◽  
Author(s):  
G. Reithmaier ◽  
S. Lichtmannecker ◽  
T. Reichert ◽  
P. Hasch ◽  
K. Müller ◽  
...  
2006 ◽  
Vol 12 (6) ◽  
pp. 1255-1268 ◽  
Author(s):  
Martin J. Stevens ◽  
Robert H. Hadfield ◽  
Robert E. Schwall ◽  
Sae Woo Nam ◽  
Richard P. Mirin

2006 ◽  
Vol 89 (15) ◽  
pp. 153510 ◽  
Author(s):  
S. S. Hees ◽  
B. E. Kardynal ◽  
P. See ◽  
A. J. Shields ◽  
I. Farrer ◽  
...  

2013 ◽  
Vol 62 (19) ◽  
pp. 194205
Author(s):  
Wang Hong-Pei ◽  
Wang Guang-Long ◽  
Ni Hai-Qiao ◽  
Xu Ying-Qiang ◽  
Niu Zhi-Chuan ◽  
...  

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Samuel Gyger ◽  
Julien Zichi ◽  
Lucas Schweickert ◽  
Ali W. Elshaari ◽  
Stephan Steinhauer ◽  
...  

AbstractIntegrated quantum photonics offers a promising path to scale up quantum optics experiments by miniaturizing and stabilizing complex laboratory setups. Central elements of quantum integrated photonics are quantum emitters, memories, detectors, and reconfigurable photonic circuits. In particular, integrated detectors not only offer optical readout but, when interfaced with reconfigurable circuits, allow feedback and adaptive control, crucial for deterministic quantum teleportation, training of neural networks, and stabilization of complex circuits. However, the heat generated by thermally reconfigurable photonics is incompatible with heat-sensitive superconducting single-photon detectors, and thus their on-chip co-integration remains elusive. Here we show low-power microelectromechanical reconfiguration of integrated photonic circuits interfaced with superconducting single-photon detectors on the same chip. We demonstrate three key functionalities for photonic quantum technologies: 28 dB high-extinction routing of classical and quantum light, 90 dB high-dynamic range single-photon detection, and stabilization of optical excitation over 12 dB power variation. Our platform enables heat-load free reconfigurable linear optics and adaptive control, critical for quantum state preparation and quantum logic in large-scale quantum photonics applications.


Nanophotonics ◽  
2018 ◽  
Vol 7 (11) ◽  
pp. 1725-1758 ◽  
Author(s):  
Simone Ferrari ◽  
Carsten Schuck ◽  
Wolfram Pernice

AbstractIntegration of superconducting nanowire single-photon detectors with nanophotonic waveguides is a key technological step that enables a broad range of classical and quantum technologies on chip-scale platforms. The excellent detection efficiency, timing and noise performance of these detectors have sparked growing interest over the last decade and have found use in diverse applications. Almost 10 years after the first waveguide-coupled superconducting detectors were proposed, here, we review the performance metrics of these devices, compare both superconducting and dielectric waveguide material systems and present prominent emerging applications.


2014 ◽  
Vol 104 (5) ◽  
pp. 051113 ◽  
Author(s):  
Q. C. Weng ◽  
Z. H. An ◽  
Z. Q. Zhu ◽  
J. D. Song ◽  
W. J. Choi

2021 ◽  
Vol 7 (1) ◽  
Author(s):  
Fabian Beutel ◽  
Helge Gehring ◽  
Martin A. Wolff ◽  
Carsten Schuck ◽  
Wolfram Pernice

AbstractQuantum key distribution (QKD) can greatly benefit from photonic integration, which enables implementing low-loss, alignment-free, and scalable photonic circuitry. At the same time, superconducting nanowire single-photon detectors (SNSPD) are an ideal detector technology for QKD due to their high efficiency, low dark-count rate, and low jitter. We present a QKD receiver chip featuring the full photonic circuitry needed for different time-based protocols, including single-photon detectors. By utilizing waveguide-integrated SNSPDs we achieve low dead times together with low dark-count rates and demonstrate a QKD experiment at 2.6 GHz clock rate, yielding secret-key rates of 2.5 Mbit/s for low channel attenuations of 2.5 dB without detector saturation. Due to the broadband 3D polymer couplers the reciver chip can be operated at a wide wavelength range in the telecom band, thus paving the way for highly parallelized wavelength-division multiplexing implementations.


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