Non-Markovian property of afterpulsing effect in single-photon avalanche detector
The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Wang, Fang-Xiang [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2016 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Journal of lightwave technology - New York, NY : IEEE, 1983, (2016), Seite 1-1 |
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| Übergeordnetes Werk: |
year:2016 ; pages:1-1 |
| Links: |
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| DOI / URN: |
10.1109/JLT.2016.2577141 |
|---|
| Katalog-ID: |
OLC1977981542 |
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| 520 | |a The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. | ||
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| 700 | 1 | |a Chen, Wei |4 oth | |
| 700 | 1 | |a Li, Ya-Ping |4 oth | |
| 700 | 1 | |a He, Deyong |4 oth | |
| 700 | 1 | |a Wang, Chao |4 oth | |
| 700 | 1 | |a Han, Yun-Guang |4 oth | |
| 700 | 1 | |a Wang, Shuang |4 oth | |
| 700 | 1 | |a Yin, Zhen-Qiang |4 oth | |
| 700 | 1 | |a Han, Zheng-fu |4 oth | |
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10.1109/JLT.2016.2577141 doi PQ20160719 (DE-627)OLC1977981542 (DE-599)GBVOLC1977981542 (PRQ)a791-f902c25ba78d00b09c9688972ac7aa8d012ac752ea267cb77d60cf10697e8b330 (KEY)0124889820160000000000000001nonmarkovianpropertyofafterpulsingeffectinsingleph DE-627 ger DE-627 rakwb eng 530 600 620 DNB Wang, Fang-Xiang verfasserin aut Non-Markovian property of afterpulsing effect in single-photon avalanche detector 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. Instrumentation and Detectors Physics Chen, Wei oth Li, Ya-Ping oth He, Deyong oth Wang, Chao oth Han, Yun-Guang oth Wang, Shuang oth Yin, Zhen-Qiang oth Han, Zheng-fu oth Enthalten in Journal of lightwave technology New York, NY : IEEE, 1983 (2016), Seite 1-1 (DE-627)129620882 (DE-600)246121-3 (DE-576)015127214 0733-8724 nnns year:2016 pages:1-1 http://dx.doi.org/10.1109/JLT.2016.2577141 Volltext http://arxiv.org/abs/1606.01728 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_185 AR 2016 1-1 |
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10.1109/JLT.2016.2577141 doi PQ20160719 (DE-627)OLC1977981542 (DE-599)GBVOLC1977981542 (PRQ)a791-f902c25ba78d00b09c9688972ac7aa8d012ac752ea267cb77d60cf10697e8b330 (KEY)0124889820160000000000000001nonmarkovianpropertyofafterpulsingeffectinsingleph DE-627 ger DE-627 rakwb eng 530 600 620 DNB Wang, Fang-Xiang verfasserin aut Non-Markovian property of afterpulsing effect in single-photon avalanche detector 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. Instrumentation and Detectors Physics Chen, Wei oth Li, Ya-Ping oth He, Deyong oth Wang, Chao oth Han, Yun-Guang oth Wang, Shuang oth Yin, Zhen-Qiang oth Han, Zheng-fu oth Enthalten in Journal of lightwave technology New York, NY : IEEE, 1983 (2016), Seite 1-1 (DE-627)129620882 (DE-600)246121-3 (DE-576)015127214 0733-8724 nnns year:2016 pages:1-1 http://dx.doi.org/10.1109/JLT.2016.2577141 Volltext http://arxiv.org/abs/1606.01728 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_185 AR 2016 1-1 |
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10.1109/JLT.2016.2577141 doi PQ20160719 (DE-627)OLC1977981542 (DE-599)GBVOLC1977981542 (PRQ)a791-f902c25ba78d00b09c9688972ac7aa8d012ac752ea267cb77d60cf10697e8b330 (KEY)0124889820160000000000000001nonmarkovianpropertyofafterpulsingeffectinsingleph DE-627 ger DE-627 rakwb eng 530 600 620 DNB Wang, Fang-Xiang verfasserin aut Non-Markovian property of afterpulsing effect in single-photon avalanche detector 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. Instrumentation and Detectors Physics Chen, Wei oth Li, Ya-Ping oth He, Deyong oth Wang, Chao oth Han, Yun-Guang oth Wang, Shuang oth Yin, Zhen-Qiang oth Han, Zheng-fu oth Enthalten in Journal of lightwave technology New York, NY : IEEE, 1983 (2016), Seite 1-1 (DE-627)129620882 (DE-600)246121-3 (DE-576)015127214 0733-8724 nnns year:2016 pages:1-1 http://dx.doi.org/10.1109/JLT.2016.2577141 Volltext http://arxiv.org/abs/1606.01728 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_185 AR 2016 1-1 |
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10.1109/JLT.2016.2577141 doi PQ20160719 (DE-627)OLC1977981542 (DE-599)GBVOLC1977981542 (PRQ)a791-f902c25ba78d00b09c9688972ac7aa8d012ac752ea267cb77d60cf10697e8b330 (KEY)0124889820160000000000000001nonmarkovianpropertyofafterpulsingeffectinsingleph DE-627 ger DE-627 rakwb eng 530 600 620 DNB Wang, Fang-Xiang verfasserin aut Non-Markovian property of afterpulsing effect in single-photon avalanche detector 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. Instrumentation and Detectors Physics Chen, Wei oth Li, Ya-Ping oth He, Deyong oth Wang, Chao oth Han, Yun-Guang oth Wang, Shuang oth Yin, Zhen-Qiang oth Han, Zheng-fu oth Enthalten in Journal of lightwave technology New York, NY : IEEE, 1983 (2016), Seite 1-1 (DE-627)129620882 (DE-600)246121-3 (DE-576)015127214 0733-8724 nnns year:2016 pages:1-1 http://dx.doi.org/10.1109/JLT.2016.2577141 Volltext http://arxiv.org/abs/1606.01728 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_185 AR 2016 1-1 |
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10.1109/JLT.2016.2577141 doi PQ20160719 (DE-627)OLC1977981542 (DE-599)GBVOLC1977981542 (PRQ)a791-f902c25ba78d00b09c9688972ac7aa8d012ac752ea267cb77d60cf10697e8b330 (KEY)0124889820160000000000000001nonmarkovianpropertyofafterpulsingeffectinsingleph DE-627 ger DE-627 rakwb eng 530 600 620 DNB Wang, Fang-Xiang verfasserin aut Non-Markovian property of afterpulsing effect in single-photon avalanche detector 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. Instrumentation and Detectors Physics Chen, Wei oth Li, Ya-Ping oth He, Deyong oth Wang, Chao oth Han, Yun-Guang oth Wang, Shuang oth Yin, Zhen-Qiang oth Han, Zheng-fu oth Enthalten in Journal of lightwave technology New York, NY : IEEE, 1983 (2016), Seite 1-1 (DE-627)129620882 (DE-600)246121-3 (DE-576)015127214 0733-8724 nnns year:2016 pages:1-1 http://dx.doi.org/10.1109/JLT.2016.2577141 Volltext http://arxiv.org/abs/1606.01728 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_185 AR 2016 1-1 |
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Non-Markovian property of afterpulsing effect in single-photon avalanche detector |
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Wang, Fang-Xiang |
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Journal of lightwave technology |
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Journal of lightwave technology |
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eng |
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2016 |
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Wang, Fang-Xiang |
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Wang, Fang-Xiang |
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10.1109/JLT.2016.2577141 |
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530 600 620 |
| title_sort |
non-markovian property of afterpulsing effect in single-photon avalanche detector |
| title_auth |
Non-Markovian property of afterpulsing effect in single-photon avalanche detector |
| abstract |
The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. |
| abstractGer |
The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. |
| abstract_unstemmed |
The single-photon avalanche photodiode(SPAD) has been widely used in research on quantum optics. The afterpulsing effect, which is an intrinsic character of SPAD, affects the system performance in most experiments and needs to be carefully handled. For a long time, afterpulsing has been presumed to be determined by the pre-ignition avalanche. We studied the afterpulsing effect of a commercial InGaAs/InP SPAD (The avalanche photodiode model is: Princeton Lightwave PGA-300) and demonstrated that its afterpulsing is non-Markovian, with a memory effect in the avalanching history. Theoretical analysis and experimental results clearly indicate that the embodiment of this memory effect is the afterpulsing probability, which increases as the number of ignition-avalanche pulses increase. This conclusion makes the principle of the afterpulsing effect clearer and is instructive to the manufacturing processes and afterpulsing evaluation of high-count-rate SPADs. It can also be regarded as a fundamental premise to handle the afterpulsing signals in many applications, such as quantum communication and quantum random number generation. |
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| title_short |
Non-Markovian property of afterpulsing effect in single-photon avalanche detector |
| url |
http://dx.doi.org/10.1109/JLT.2016.2577141 http://arxiv.org/abs/1606.01728 |
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false |
| author2 |
Chen, Wei Li, Ya-Ping He, Deyong Wang, Chao Han, Yun-Guang Wang, Shuang Yin, Zhen-Qiang Han, Zheng-fu |
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Chen, Wei Li, Ya-Ping He, Deyong Wang, Chao Han, Yun-Guang Wang, Shuang Yin, Zhen-Qiang Han, Zheng-fu |
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| up_date |
2024-07-03T20:12:11.624Z |
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