Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method
The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measu...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Samoylenko, A. A. [verfasserIn] Ivanov, A. D. [verfasserIn] Levin, G. G. [verfasserIn] |
|---|
| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2020 |
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| Schlagwörter: |
spontaneous parametric scattering |
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| Übergeordnetes Werk: |
Enthalten in: Measurement techniques - New York, NY [u.a.] : Consultants Bureau, 1958, 63(2020), 8 vom: Nov., Seite 619-628 |
|---|---|
| Übergeordnetes Werk: |
volume:63 ; year:2020 ; number:8 ; month:11 ; pages:619-628 |
| Links: |
|---|
| DOI / URN: |
10.1007/s11018-020-01831-y |
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| Katalog-ID: |
SPR042252377 |
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| 520 | |a The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. | ||
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| 650 | 4 | |a reference calibration of single-photon detectors |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a heterodyning |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Ivanov, A. D. |e verfasserin |4 aut | |
| 700 | 1 | |a Levin, G. G. |e verfasserin |4 aut | |
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10.1007/s11018-020-01831-y doi (DE-627)SPR042252377 (DE-599)SPRs11018-020-01831-y-e (SPR)s11018-020-01831-y-e DE-627 ger DE-627 rakwb eng 620 ASE 50.21 bkl 33.00 bkl Samoylenko, A. A. verfasserin aut Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. spontaneous parametric scattering (dpeaa)DE-He213 reference calibration of single-photon detectors (dpeaa)DE-He213 heterodyning (dpeaa)DE-He213 Ivanov, A. D. verfasserin aut Levin, G. G. verfasserin aut Enthalten in Measurement techniques New York, NY [u.a.] : Consultants Bureau, 1958 63(2020), 8 vom: Nov., Seite 619-628 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:63 year:2020 number:8 month:11 pages:619-628 https://dx.doi.org/10.1007/s11018-020-01831-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 ASE 33.00 ASE AR 63 2020 8 11 619-628 |
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10.1007/s11018-020-01831-y doi (DE-627)SPR042252377 (DE-599)SPRs11018-020-01831-y-e (SPR)s11018-020-01831-y-e DE-627 ger DE-627 rakwb eng 620 ASE 50.21 bkl 33.00 bkl Samoylenko, A. A. verfasserin aut Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. spontaneous parametric scattering (dpeaa)DE-He213 reference calibration of single-photon detectors (dpeaa)DE-He213 heterodyning (dpeaa)DE-He213 Ivanov, A. D. verfasserin aut Levin, G. G. verfasserin aut Enthalten in Measurement techniques New York, NY [u.a.] : Consultants Bureau, 1958 63(2020), 8 vom: Nov., Seite 619-628 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:63 year:2020 number:8 month:11 pages:619-628 https://dx.doi.org/10.1007/s11018-020-01831-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 ASE 33.00 ASE AR 63 2020 8 11 619-628 |
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10.1007/s11018-020-01831-y doi (DE-627)SPR042252377 (DE-599)SPRs11018-020-01831-y-e (SPR)s11018-020-01831-y-e DE-627 ger DE-627 rakwb eng 620 ASE 50.21 bkl 33.00 bkl Samoylenko, A. A. verfasserin aut Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. spontaneous parametric scattering (dpeaa)DE-He213 reference calibration of single-photon detectors (dpeaa)DE-He213 heterodyning (dpeaa)DE-He213 Ivanov, A. D. verfasserin aut Levin, G. G. verfasserin aut Enthalten in Measurement techniques New York, NY [u.a.] : Consultants Bureau, 1958 63(2020), 8 vom: Nov., Seite 619-628 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:63 year:2020 number:8 month:11 pages:619-628 https://dx.doi.org/10.1007/s11018-020-01831-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 ASE 33.00 ASE AR 63 2020 8 11 619-628 |
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10.1007/s11018-020-01831-y doi (DE-627)SPR042252377 (DE-599)SPRs11018-020-01831-y-e (SPR)s11018-020-01831-y-e DE-627 ger DE-627 rakwb eng 620 ASE 50.21 bkl 33.00 bkl Samoylenko, A. A. verfasserin aut Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. spontaneous parametric scattering (dpeaa)DE-He213 reference calibration of single-photon detectors (dpeaa)DE-He213 heterodyning (dpeaa)DE-He213 Ivanov, A. D. verfasserin aut Levin, G. G. verfasserin aut Enthalten in Measurement techniques New York, NY [u.a.] : Consultants Bureau, 1958 63(2020), 8 vom: Nov., Seite 619-628 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:63 year:2020 number:8 month:11 pages:619-628 https://dx.doi.org/10.1007/s11018-020-01831-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 ASE 33.00 ASE AR 63 2020 8 11 619-628 |
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10.1007/s11018-020-01831-y doi (DE-627)SPR042252377 (DE-599)SPRs11018-020-01831-y-e (SPR)s11018-020-01831-y-e DE-627 ger DE-627 rakwb eng 620 ASE 50.21 bkl 33.00 bkl Samoylenko, A. A. verfasserin aut Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. spontaneous parametric scattering (dpeaa)DE-He213 reference calibration of single-photon detectors (dpeaa)DE-He213 heterodyning (dpeaa)DE-He213 Ivanov, A. D. verfasserin aut Levin, G. G. verfasserin aut Enthalten in Measurement techniques New York, NY [u.a.] : Consultants Bureau, 1958 63(2020), 8 vom: Nov., Seite 619-628 (DE-627)325573468 (DE-600)2037682-0 1573-8906 nnns volume:63 year:2020 number:8 month:11 pages:619-628 https://dx.doi.org/10.1007/s11018-020-01831-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 ASE 33.00 ASE AR 63 2020 8 11 619-628 |
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Samoylenko, A. A. |
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Samoylenko, A. A. ddc 620 bkl 50.21 bkl 33.00 misc spontaneous parametric scattering misc reference calibration of single-photon detectors misc heterodyning Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method |
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620 ASE 50.21 bkl 33.00 bkl Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method spontaneous parametric scattering (dpeaa)DE-He213 reference calibration of single-photon detectors (dpeaa)DE-He213 heterodyning (dpeaa)DE-He213 |
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ddc 620 bkl 50.21 bkl 33.00 misc spontaneous parametric scattering misc reference calibration of single-photon detectors misc heterodyning |
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ddc 620 bkl 50.21 bkl 33.00 misc spontaneous parametric scattering misc reference calibration of single-photon detectors misc heterodyning |
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ddc 620 bkl 50.21 bkl 33.00 misc spontaneous parametric scattering misc reference calibration of single-photon detectors misc heterodyning |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method |
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(DE-627)SPR042252377 (DE-599)SPRs11018-020-01831-y-e (SPR)s11018-020-01831-y-e |
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Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method |
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Samoylenko, A. A. |
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Measurement techniques |
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eng |
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Samoylenko, A. A. Ivanov, A. D. Levin, G. G. |
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Samoylenko, A. A. |
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10.1007/s11018-020-01831-y |
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verfasserin |
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detection efficiency measurement of single-photon detectors based on spontaneous parametric scattering process using the heterodyning method |
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Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method |
| abstract |
The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. |
| abstractGer |
The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. |
| abstract_unstemmed |
The article presents the various problems in the metrological support for the components of quantum information systems and uses the Klyshko reference method given in the international ETSI standard, which works on the principle of spontaneous parametric scattering effect. It is found that the measurement time has increased by an order of magnitude at noise level with a high power density at low frequencies when compared to desired signal level for single-photon detectors. So, the heterodyning method is proposed to increase the efficiency of signal accumulation. The method consists in accumulating a signal at a higher frequency and introducing modulation into the standard Klyshko scheme. The method proposed is simulated numerically and the signal-to-noise ratio is increased by a factor of 14 compared to simple signal accumulation has been established experimentally. |
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8 |
| title_short |
Detection Efficiency Measurement of Single-Photon Detectors Based on Spontaneous Parametric Scattering Process Using the Heterodyning Method |
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https://dx.doi.org/10.1007/s11018-020-01831-y |
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Ivanov, A. D. Levin, G. G. |
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Ivanov, A. D. Levin, G. G. |
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| doi_str |
10.1007/s11018-020-01831-y |
| up_date |
2024-07-04T01:25:22.718Z |
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