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Absolute Measurement of Detector Quantum Efficiency Using Parametric Downconversion
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Absolute Efficiency and Time-Response Measurement of Single-Photon Detectors
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Measuring Absolute Infrared Spectral Radiance with Correlated Visible Photons: Technique Verification and Measurement Uncertainty
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Quantum Efficiency and Dead Time of Single-Photon Counting Photodiodes: A Ccomparison Between Two Measurement Techniques
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Towards an Uncertainty Budget in Quantum-Efficiency Measurements with Parametric Fluorescence
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Radiometric reference for weak radiations: Comparison of methods
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Detector calibration at INM using a correlated photons source
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2942724599
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Quantum Key Distribution with 1.25 Gbps Clock Synchronization
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for example
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for example, J. C. Bienfang, A. J. Gross, A. Mink, B. J. Hershman, A. Nakassis, X. Tang, R. Lu, D. H. Su, C. W. Clark, C. J. Williams, E. W. Hagley and Jesse Wen, "Quantum Key Distribution with 1.25 Gbps Clock Synchronization," Opt. Express 12, 2011-2016 (2004).
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19
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28644448875
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Measurement-induced entanglement for excitation stored in remote atomic ensembles
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for example
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for example, C. W. Chou, H. de Riedmatten, D. Felinto, S. V. Polyakov, S. J. van Enk, H. J. Kimble, "Measurement-induced entanglement for excitation stored in remote atomic ensembles," Nature 438, 828-832 (2005).
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3142520038
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Single-photon Detector Characterization Using Correlated Photons: The March from Feasibility to Metrology
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84894396447
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Determination of the Spectrum Responsivity of Optical Radiation Detectors, Publ. 64 (Commission Internationale de L'Éclairage, Paris, 1984).
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Determination of the Spectrum Responsivity of Optical Radiation Detectors, Publ. 64 (Commission Internationale de L'Éclairage, Paris, 1984).
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Optical Radiation Measurements
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84894399382
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Photon Counting Module, product datasheet, available at
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SPCM-AQR Single Photon Counting Module, product datasheet, available at: http://optoelectronics.perkinelmer.com/content/Datasheets/SPCM-AOR.pdf.
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Single, S.P.C.M.-A.Q.1
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25
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84894389326
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-
Perkin-Elmer APD SPCM-AQR-12 (trigger detector: s/n 12432, DUT: s/n 12433)
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Perkin-Elmer APD SPCM-AQR-12 (trigger detector: s/n 12432, DUT: s/n 12433)
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26
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84894399269
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Certain commercial equipment, instruments or materials are identified in this paper to foster understanding. Such identification does not imply recommendation or endorsement by the National Institute of Standards and Technology, nor does it imply that the materials or equipment are necessarily the best available for the purpose
-
Certain commercial equipment, instruments or materials are identified in this paper to foster understanding. Such identification does not imply recommendation or endorsement by the National Institute of Standards and Technology, nor does it imply that the materials or equipment are necessarily the best available for the purpose.
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27
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84894391836
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Gamma Scientific Silicon Photodiode p/n: 19830-3 s/n: ND0104
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Gamma Scientific Silicon Photodiode p/n: 19830-3 s/n: ND0104
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28
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84894401196
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Calibrating Photon-Counting Detectors to High Accuracy: Background and Deadtime Issues
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to appear
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M. Ware, A. L. Migdall, J. C. Bienfang, and S. V. Polyakov, "Calibrating Photon-Counting Detectors to High Accuracy: Background and Deadtime Issues," J. Mod. Opt., to appear.
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Facility for spectral irradiance and radiance responsivity calibrations using uniform sources
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0001584312
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Accurate 2nd-order Susceptibility Measurements of Visible and Infrared Nonlinear Crystals
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84894392065
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Establishing transmittance with desired accuracy requires temporal stability of associated irradiance measurements. The experimental setup consisted of a He-Ne laser followed by a spatial filter pinhole, and two trap detectors with a high degree of spatial uniformity. One trap detector monitored the laser's power and the other measured the transmitted power with and without the crystal. The maximum observed long-term drift of the system was 0.004 %/h, and the rms of the signal, normalized to laser power, was 0.02
-
Establishing transmittance with desired accuracy requires temporal stability of associated irradiance measurements. The experimental setup consisted of a He-Ne laser followed by a spatial filter (pinhole), and two trap detectors with a high degree of spatial uniformity. One trap detector monitored the laser's power and the other measured the transmitted power with and without the crystal. The maximum observed long-term drift of the system was 0.004 %/h, and the rms of the signal, normalized to laser power, was 0.02 %.
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35
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84894400428
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High Accuracy Lens Transmittance Measurements
-
submitted to
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J. Cheung, J. Gardner, A. L. Migdall, S. V. Polyakov, and M. Ware, "High Accuracy Lens Transmittance Measurements," submitted to Appl. Opt.
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Appl. Opt
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Cheung, J.1
Gardner, J.2
Migdall, A.L.3
Polyakov, S.V.4
Ware, M.5
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