Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data
Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimat...
Ausführliche Beschreibung
Autor*in: |
Adhikari, P. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2021 |
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Anmerkung: |
© The Author(s) 2021 |
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Übergeordnetes Werk: |
Enthalten in: The European physical journal / C - Springer Berlin Heidelberg, 1998, 81(2021), 9 vom: Sept. |
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Übergeordnetes Werk: |
volume:81 ; year:2021 ; number:9 ; month:09 |
Links: |
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DOI / URN: |
10.1140/epjc/s10052-021-09514-w |
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Katalog-ID: |
OLC2077170700 |
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100 | 1 | |a Adhikari, P. |e verfasserin |4 aut | |
245 | 1 | 0 | |a Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data |
264 | 1 | |c 2021 | |
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500 | |a © The Author(s) 2021 | ||
520 | |a Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. | ||
700 | 1 | |a Ajaj, R. |4 aut | |
700 | 1 | |a Alpízar-Venegas, M. |4 aut | |
700 | 1 | |a Amaudruz, P.-A. |4 aut | |
700 | 1 | |a Auty, D. J. |4 aut | |
700 | 1 | |a Batygov, M. |4 aut | |
700 | 1 | |a Beltran, B. |4 aut | |
700 | 1 | |a Benmansour, H. |4 aut | |
700 | 1 | |a Bina, C. E. |4 aut | |
700 | 1 | |a Bonatt, J. |4 aut | |
700 | 1 | |a Bonivento, W. |4 aut | |
700 | 1 | |a Boulay, M. G. |4 aut | |
700 | 1 | |a Broerman, B. |4 aut | |
700 | 1 | |a Bueno, J. F. |4 aut | |
700 | 1 | |a Burghardt, P. M. |4 aut | |
700 | 1 | |a Butcher, A. |4 aut | |
700 | 1 | |a Cadeddu, M. |4 aut | |
700 | 1 | |a Cai, B. |4 aut | |
700 | 1 | |a Cárdenas-Montes, M. |4 aut | |
700 | 1 | |a Cavuoti, S. |4 aut | |
700 | 1 | |a Chen, M. |4 aut | |
700 | 1 | |a Chen, Y. |4 aut | |
700 | 1 | |a Cleveland, B. T. |4 aut | |
700 | 1 | |a Corning, J. M. |4 aut | |
700 | 1 | |a Cranshaw, D. |4 aut | |
700 | 1 | |a Daugherty, S. |4 aut | |
700 | 1 | |a DelGobbo, P. |4 aut | |
700 | 1 | |a Dering, K. |4 aut | |
700 | 1 | |a DiGioseffo, J. |4 aut | |
700 | 1 | |a Di Stefano, P. |4 aut | |
700 | 1 | |a Doria, L. |4 aut | |
700 | 1 | |a Duncan, F. A. |4 aut | |
700 | 1 | |a Dunford, M. |4 aut | |
700 | 1 | |a Ellingwood, E. |4 aut | |
700 | 1 | |a Erlandson, A. |4 aut | |
700 | 1 | |a Farahani, S. S. |4 aut | |
700 | 1 | |a Fatemighomi, N. |4 aut | |
700 | 1 | |a Fiorillo, G. |4 aut | |
700 | 1 | |a Florian, S. |4 aut | |
700 | 1 | |a Flower, T. |4 aut | |
700 | 1 | |a Ford, R. J. |4 aut | |
700 | 1 | |a Gagnon, R. |4 aut | |
700 | 1 | |a Gallacher, D. |4 aut | |
700 | 1 | |a García Abia, P. |4 aut | |
700 | 1 | |a Garg, S. |4 aut | |
700 | 1 | |a Giampa, P. |4 aut | |
700 | 1 | |a Goeldi, D. |4 aut | |
700 | 1 | |a Golovko, V. |4 aut | |
700 | 1 | |a Gorel, P. |4 aut | |
700 | 1 | |a Graham, K. |4 aut | |
700 | 1 | |a Grant, D. R. |4 aut | |
700 | 1 | |a Grobov, A. |4 aut | |
700 | 1 | |a Hallin, A. L. |4 aut | |
700 | 1 | |a Hamstra, M. |4 aut | |
700 | 1 | |a Harvey, P. J. |4 aut | |
700 | 1 | |a Hearns, C. |4 aut | |
700 | 1 | |a Hugues, T. |4 aut | |
700 | 1 | |a Ilyasov, A. |4 aut | |
700 | 1 | |a Joy, A. |4 aut | |
700 | 1 | |a Jigmeddorj, B. |4 aut | |
700 | 1 | |a Jillings, C. J. |4 aut | |
700 | 1 | |a Kamaev, O. |4 aut | |
700 | 1 | |a Kaur, G. |4 aut | |
700 | 1 | |a Kemp, A. |4 aut | |
700 | 1 | |a Kochanek, I. |4 aut | |
700 | 1 | |a Kuźniak, M. |4 aut | |
700 | 1 | |a Lai, M. |4 aut | |
700 | 1 | |a Langrock, S. |4 aut | |
700 | 1 | |a Lehnert, B. |4 aut | |
700 | 1 | |a Leonhardt, A. |4 aut | |
700 | 1 | |a Levashko, N. |4 aut | |
700 | 1 | |a Li, X. |4 aut | |
700 | 1 | |a Lidgard, J. |4 aut | |
700 | 1 | |a Lindner, T. |4 aut | |
700 | 1 | |a Lissia, M. |4 aut | |
700 | 1 | |a Lock, J. |4 aut | |
700 | 1 | |a Longo, G. |4 aut | |
700 | 1 | |a Machulin, I. |4 aut | |
700 | 1 | |a McDonald, A. B. |4 aut | |
700 | 1 | |a McElroy, T. |4 aut | |
700 | 1 | |a McGinn, T. |4 aut | |
700 | 1 | |a McLaughlin, J. B. |4 aut | |
700 | 1 | |a Mehdiyev, R. |4 aut | |
700 | 1 | |a Mielnichuk, C. |4 aut | |
700 | 1 | |a Monroe, J. |4 aut | |
700 | 1 | |a Nadeau, P. |4 aut | |
700 | 1 | |a Nantais, C. |4 aut | |
700 | 1 | |a Ng, C. |4 aut | |
700 | 1 | |a Noble, A. J. |4 aut | |
700 | 1 | |a O’Dwyer, E. |4 aut | |
700 | 1 | |a Oliviéro, G. |4 aut | |
700 | 1 | |a Ouellet, C. |4 aut | |
700 | 1 | |a Pal, S. |4 aut | |
700 | 1 | |a Pasuthip, P. |4 aut | |
700 | 1 | |a Peeters, S. J. M. |4 aut | |
700 | 1 | |a Perry, M. |4 aut | |
700 | 1 | |a Pesudo, V. |4 aut | |
700 | 1 | |a Picciau, E. |4 aut | |
700 | 1 | |a Piro, M.-C. |4 aut | |
700 | 1 | |a Pollmann, T. R. |4 aut | |
700 | 1 | |a Rand, E. T. |4 aut | |
700 | 1 | |a Rethmeier, C. |4 aut | |
700 | 1 | |a Retière, F. |4 aut | |
700 | 1 | |a Rodríguez-García, I. |4 aut | |
700 | 1 | |a Roszkowski, L. |4 aut | |
700 | 1 | |a Ruhland, J. B. |4 aut | |
700 | 1 | |a Sánchez-García, E. |4 aut | |
700 | 1 | |a Santorelli, R. |4 aut | |
700 | 1 | |a Sinclair, D. |4 aut | |
700 | 1 | |a Skensved, P. |4 aut | |
700 | 1 | |a Smith, B. |4 aut | |
700 | 1 | |a Smith, N. J. T. |4 aut | |
700 | 1 | |a Sonley, T. |4 aut | |
700 | 1 | |a Soukup, J. |4 aut | |
700 | 1 | |a Stainforth, R. |4 aut | |
700 | 1 | |a Stone, C. |4 aut | |
700 | 1 | |a Strickland, V. |4 aut | |
700 | 1 | |a Stringer, M. |4 aut | |
700 | 1 | |a Sur, B. |4 aut | |
700 | 1 | |a Tang, J. |4 aut | |
700 | 1 | |a Vázquez-Jáuregui, E. |4 aut | |
700 | 1 | |a Viel, S. |4 aut | |
700 | 1 | |a Walding, J. |4 aut | |
700 | 1 | |a Waqar, M. |4 aut | |
700 | 1 | |a Ward, M. |4 aut | |
700 | 1 | |a Westerdale, S. |4 aut | |
700 | 1 | |a Willis, J. |4 aut | |
700 | 1 | |a Zuñiga-Reyes, A. |4 aut | |
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10.1140/epjc/s10052-021-09514-w doi (DE-627)OLC2077170700 (DE-He213)s10052-021-09514-w-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Adhikari, P. verfasserin aut Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data 2021 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2021 Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. Ajaj, R. aut Alpízar-Venegas, M. aut Amaudruz, P.-A. aut Auty, D. J. aut Batygov, M. aut Beltran, B. aut Benmansour, H. aut Bina, C. E. aut Bonatt, J. aut Bonivento, W. aut Boulay, M. G. aut Broerman, B. aut Bueno, J. F. aut Burghardt, P. M. aut Butcher, A. aut Cadeddu, M. aut Cai, B. aut Cárdenas-Montes, M. aut Cavuoti, S. aut Chen, M. aut Chen, Y. aut Cleveland, B. T. aut Corning, J. M. aut Cranshaw, D. aut Daugherty, S. aut DelGobbo, P. aut Dering, K. aut DiGioseffo, J. aut Di Stefano, P. aut Doria, L. aut Duncan, F. A. aut Dunford, M. aut Ellingwood, E. aut Erlandson, A. aut Farahani, S. S. aut Fatemighomi, N. aut Fiorillo, G. aut Florian, S. aut Flower, T. aut Ford, R. J. aut Gagnon, R. aut Gallacher, D. aut García Abia, P. aut Garg, S. aut Giampa, P. aut Goeldi, D. aut Golovko, V. aut Gorel, P. aut Graham, K. aut Grant, D. R. aut Grobov, A. aut Hallin, A. L. aut Hamstra, M. aut Harvey, P. J. aut Hearns, C. aut Hugues, T. aut Ilyasov, A. aut Joy, A. aut Jigmeddorj, B. aut Jillings, C. J. aut Kamaev, O. aut Kaur, G. aut Kemp, A. aut Kochanek, I. aut Kuźniak, M. aut Lai, M. aut Langrock, S. aut Lehnert, B. aut Leonhardt, A. aut Levashko, N. aut Li, X. aut Lidgard, J. aut Lindner, T. aut Lissia, M. aut Lock, J. aut Longo, G. aut Machulin, I. aut McDonald, A. B. aut McElroy, T. aut McGinn, T. aut McLaughlin, J. B. aut Mehdiyev, R. aut Mielnichuk, C. aut Monroe, J. aut Nadeau, P. aut Nantais, C. aut Ng, C. aut Noble, A. J. aut O’Dwyer, E. aut Oliviéro, G. aut Ouellet, C. aut Pal, S. aut Pasuthip, P. aut Peeters, S. J. M. aut Perry, M. aut Pesudo, V. aut Picciau, E. aut Piro, M.-C. aut Pollmann, T. R. aut Rand, E. T. aut Rethmeier, C. aut Retière, F. aut Rodríguez-García, I. aut Roszkowski, L. aut Ruhland, J. B. aut Sánchez-García, E. aut Santorelli, R. aut Sinclair, D. aut Skensved, P. aut Smith, B. aut Smith, N. J. T. aut Sonley, T. aut Soukup, J. aut Stainforth, R. aut Stone, C. aut Strickland, V. aut Stringer, M. aut Sur, B. aut Tang, J. aut Vázquez-Jáuregui, E. aut Viel, S. aut Walding, J. aut Waqar, M. aut Ward, M. aut Westerdale, S. aut Willis, J. aut Zuñiga-Reyes, A. aut Enthalten in The European physical journal / C Springer Berlin Heidelberg, 1998 81(2021), 9 vom: Sept. (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:81 year:2021 number:9 month:09 https://doi.org/10.1140/epjc/s10052-021-09514-w lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 81 2021 9 09 |
spelling |
10.1140/epjc/s10052-021-09514-w doi (DE-627)OLC2077170700 (DE-He213)s10052-021-09514-w-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Adhikari, P. verfasserin aut Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data 2021 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2021 Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. Ajaj, R. aut Alpízar-Venegas, M. aut Amaudruz, P.-A. aut Auty, D. J. aut Batygov, M. aut Beltran, B. aut Benmansour, H. aut Bina, C. E. aut Bonatt, J. aut Bonivento, W. aut Boulay, M. G. aut Broerman, B. aut Bueno, J. F. aut Burghardt, P. M. aut Butcher, A. aut Cadeddu, M. aut Cai, B. aut Cárdenas-Montes, M. aut Cavuoti, S. aut Chen, M. aut Chen, Y. aut Cleveland, B. T. aut Corning, J. M. aut Cranshaw, D. aut Daugherty, S. aut DelGobbo, P. aut Dering, K. aut DiGioseffo, J. aut Di Stefano, P. aut Doria, L. aut Duncan, F. A. aut Dunford, M. aut Ellingwood, E. aut Erlandson, A. aut Farahani, S. S. aut Fatemighomi, N. aut Fiorillo, G. aut Florian, S. aut Flower, T. aut Ford, R. J. aut Gagnon, R. aut Gallacher, D. aut García Abia, P. aut Garg, S. aut Giampa, P. aut Goeldi, D. aut Golovko, V. aut Gorel, P. aut Graham, K. aut Grant, D. R. aut Grobov, A. aut Hallin, A. L. aut Hamstra, M. aut Harvey, P. J. aut Hearns, C. aut Hugues, T. aut Ilyasov, A. aut Joy, A. aut Jigmeddorj, B. aut Jillings, C. J. aut Kamaev, O. aut Kaur, G. aut Kemp, A. aut Kochanek, I. aut Kuźniak, M. aut Lai, M. aut Langrock, S. aut Lehnert, B. aut Leonhardt, A. aut Levashko, N. aut Li, X. aut Lidgard, J. aut Lindner, T. aut Lissia, M. aut Lock, J. aut Longo, G. aut Machulin, I. aut McDonald, A. B. aut McElroy, T. aut McGinn, T. aut McLaughlin, J. B. aut Mehdiyev, R. aut Mielnichuk, C. aut Monroe, J. aut Nadeau, P. aut Nantais, C. aut Ng, C. aut Noble, A. J. aut O’Dwyer, E. aut Oliviéro, G. aut Ouellet, C. aut Pal, S. aut Pasuthip, P. aut Peeters, S. J. M. aut Perry, M. aut Pesudo, V. aut Picciau, E. aut Piro, M.-C. aut Pollmann, T. R. aut Rand, E. T. aut Rethmeier, C. aut Retière, F. aut Rodríguez-García, I. aut Roszkowski, L. aut Ruhland, J. B. aut Sánchez-García, E. aut Santorelli, R. aut Sinclair, D. aut Skensved, P. aut Smith, B. aut Smith, N. J. T. aut Sonley, T. aut Soukup, J. aut Stainforth, R. aut Stone, C. aut Strickland, V. aut Stringer, M. aut Sur, B. aut Tang, J. aut Vázquez-Jáuregui, E. aut Viel, S. aut Walding, J. aut Waqar, M. aut Ward, M. aut Westerdale, S. aut Willis, J. aut Zuñiga-Reyes, A. aut Enthalten in The European physical journal / C Springer Berlin Heidelberg, 1998 81(2021), 9 vom: Sept. (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:81 year:2021 number:9 month:09 https://doi.org/10.1140/epjc/s10052-021-09514-w lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 81 2021 9 09 |
allfields_unstemmed |
10.1140/epjc/s10052-021-09514-w doi (DE-627)OLC2077170700 (DE-He213)s10052-021-09514-w-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Adhikari, P. verfasserin aut Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data 2021 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2021 Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. Ajaj, R. aut Alpízar-Venegas, M. aut Amaudruz, P.-A. aut Auty, D. J. aut Batygov, M. aut Beltran, B. aut Benmansour, H. aut Bina, C. E. aut Bonatt, J. aut Bonivento, W. aut Boulay, M. G. aut Broerman, B. aut Bueno, J. F. aut Burghardt, P. M. aut Butcher, A. aut Cadeddu, M. aut Cai, B. aut Cárdenas-Montes, M. aut Cavuoti, S. aut Chen, M. aut Chen, Y. aut Cleveland, B. T. aut Corning, J. M. aut Cranshaw, D. aut Daugherty, S. aut DelGobbo, P. aut Dering, K. aut DiGioseffo, J. aut Di Stefano, P. aut Doria, L. aut Duncan, F. A. aut Dunford, M. aut Ellingwood, E. aut Erlandson, A. aut Farahani, S. S. aut Fatemighomi, N. aut Fiorillo, G. aut Florian, S. aut Flower, T. aut Ford, R. J. aut Gagnon, R. aut Gallacher, D. aut García Abia, P. aut Garg, S. aut Giampa, P. aut Goeldi, D. aut Golovko, V. aut Gorel, P. aut Graham, K. aut Grant, D. R. aut Grobov, A. aut Hallin, A. L. aut Hamstra, M. aut Harvey, P. J. aut Hearns, C. aut Hugues, T. aut Ilyasov, A. aut Joy, A. aut Jigmeddorj, B. aut Jillings, C. J. aut Kamaev, O. aut Kaur, G. aut Kemp, A. aut Kochanek, I. aut Kuźniak, M. aut Lai, M. aut Langrock, S. aut Lehnert, B. aut Leonhardt, A. aut Levashko, N. aut Li, X. aut Lidgard, J. aut Lindner, T. aut Lissia, M. aut Lock, J. aut Longo, G. aut Machulin, I. aut McDonald, A. B. aut McElroy, T. aut McGinn, T. aut McLaughlin, J. B. aut Mehdiyev, R. aut Mielnichuk, C. aut Monroe, J. aut Nadeau, P. aut Nantais, C. aut Ng, C. aut Noble, A. J. aut O’Dwyer, E. aut Oliviéro, G. aut Ouellet, C. aut Pal, S. aut Pasuthip, P. aut Peeters, S. J. M. aut Perry, M. aut Pesudo, V. aut Picciau, E. aut Piro, M.-C. aut Pollmann, T. R. aut Rand, E. T. aut Rethmeier, C. aut Retière, F. aut Rodríguez-García, I. aut Roszkowski, L. aut Ruhland, J. B. aut Sánchez-García, E. aut Santorelli, R. aut Sinclair, D. aut Skensved, P. aut Smith, B. aut Smith, N. J. T. aut Sonley, T. aut Soukup, J. aut Stainforth, R. aut Stone, C. aut Strickland, V. aut Stringer, M. aut Sur, B. aut Tang, J. aut Vázquez-Jáuregui, E. aut Viel, S. aut Walding, J. aut Waqar, M. aut Ward, M. aut Westerdale, S. aut Willis, J. aut Zuñiga-Reyes, A. aut Enthalten in The European physical journal / C Springer Berlin Heidelberg, 1998 81(2021), 9 vom: Sept. (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:81 year:2021 number:9 month:09 https://doi.org/10.1140/epjc/s10052-021-09514-w lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 81 2021 9 09 |
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10.1140/epjc/s10052-021-09514-w doi (DE-627)OLC2077170700 (DE-He213)s10052-021-09514-w-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Adhikari, P. verfasserin aut Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data 2021 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2021 Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. Ajaj, R. aut Alpízar-Venegas, M. aut Amaudruz, P.-A. aut Auty, D. J. aut Batygov, M. aut Beltran, B. aut Benmansour, H. aut Bina, C. E. aut Bonatt, J. aut Bonivento, W. aut Boulay, M. G. aut Broerman, B. aut Bueno, J. F. aut Burghardt, P. M. aut Butcher, A. aut Cadeddu, M. aut Cai, B. aut Cárdenas-Montes, M. aut Cavuoti, S. aut Chen, M. aut Chen, Y. aut Cleveland, B. T. aut Corning, J. M. aut Cranshaw, D. aut Daugherty, S. aut DelGobbo, P. aut Dering, K. aut DiGioseffo, J. aut Di Stefano, P. aut Doria, L. aut Duncan, F. A. aut Dunford, M. aut Ellingwood, E. aut Erlandson, A. aut Farahani, S. S. aut Fatemighomi, N. aut Fiorillo, G. aut Florian, S. aut Flower, T. aut Ford, R. J. aut Gagnon, R. aut Gallacher, D. aut García Abia, P. aut Garg, S. aut Giampa, P. aut Goeldi, D. aut Golovko, V. aut Gorel, P. aut Graham, K. aut Grant, D. R. aut Grobov, A. aut Hallin, A. L. aut Hamstra, M. aut Harvey, P. J. aut Hearns, C. aut Hugues, T. aut Ilyasov, A. aut Joy, A. aut Jigmeddorj, B. aut Jillings, C. J. aut Kamaev, O. aut Kaur, G. aut Kemp, A. aut Kochanek, I. aut Kuźniak, M. aut Lai, M. aut Langrock, S. aut Lehnert, B. aut Leonhardt, A. aut Levashko, N. aut Li, X. aut Lidgard, J. aut Lindner, T. aut Lissia, M. aut Lock, J. aut Longo, G. aut Machulin, I. aut McDonald, A. B. aut McElroy, T. aut McGinn, T. aut McLaughlin, J. B. aut Mehdiyev, R. aut Mielnichuk, C. aut Monroe, J. aut Nadeau, P. aut Nantais, C. aut Ng, C. aut Noble, A. J. aut O’Dwyer, E. aut Oliviéro, G. aut Ouellet, C. aut Pal, S. aut Pasuthip, P. aut Peeters, S. J. M. aut Perry, M. aut Pesudo, V. aut Picciau, E. aut Piro, M.-C. aut Pollmann, T. R. aut Rand, E. T. aut Rethmeier, C. aut Retière, F. aut Rodríguez-García, I. aut Roszkowski, L. aut Ruhland, J. B. aut Sánchez-García, E. aut Santorelli, R. aut Sinclair, D. aut Skensved, P. aut Smith, B. aut Smith, N. J. T. aut Sonley, T. aut Soukup, J. aut Stainforth, R. aut Stone, C. aut Strickland, V. aut Stringer, M. aut Sur, B. aut Tang, J. aut Vázquez-Jáuregui, E. aut Viel, S. aut Walding, J. aut Waqar, M. aut Ward, M. aut Westerdale, S. aut Willis, J. aut Zuñiga-Reyes, A. aut Enthalten in The European physical journal / C Springer Berlin Heidelberg, 1998 81(2021), 9 vom: Sept. (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:81 year:2021 number:9 month:09 https://doi.org/10.1140/epjc/s10052-021-09514-w lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 81 2021 9 09 |
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10.1140/epjc/s10052-021-09514-w doi (DE-627)OLC2077170700 (DE-He213)s10052-021-09514-w-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Adhikari, P. verfasserin aut Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data 2021 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2021 Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. Ajaj, R. aut Alpízar-Venegas, M. aut Amaudruz, P.-A. aut Auty, D. J. aut Batygov, M. aut Beltran, B. aut Benmansour, H. aut Bina, C. E. aut Bonatt, J. aut Bonivento, W. aut Boulay, M. G. aut Broerman, B. aut Bueno, J. F. aut Burghardt, P. M. aut Butcher, A. aut Cadeddu, M. aut Cai, B. aut Cárdenas-Montes, M. aut Cavuoti, S. aut Chen, M. aut Chen, Y. aut Cleveland, B. T. aut Corning, J. M. aut Cranshaw, D. aut Daugherty, S. aut DelGobbo, P. aut Dering, K. aut DiGioseffo, J. aut Di Stefano, P. aut Doria, L. aut Duncan, F. A. aut Dunford, M. aut Ellingwood, E. aut Erlandson, A. aut Farahani, S. S. aut Fatemighomi, N. aut Fiorillo, G. aut Florian, S. aut Flower, T. aut Ford, R. J. aut Gagnon, R. aut Gallacher, D. aut García Abia, P. aut Garg, S. aut Giampa, P. aut Goeldi, D. aut Golovko, V. aut Gorel, P. aut Graham, K. aut Grant, D. R. aut Grobov, A. aut Hallin, A. L. aut Hamstra, M. aut Harvey, P. J. aut Hearns, C. aut Hugues, T. aut Ilyasov, A. aut Joy, A. aut Jigmeddorj, B. aut Jillings, C. J. aut Kamaev, O. aut Kaur, G. aut Kemp, A. aut Kochanek, I. aut Kuźniak, M. aut Lai, M. aut Langrock, S. aut Lehnert, B. aut Leonhardt, A. aut Levashko, N. aut Li, X. aut Lidgard, J. aut Lindner, T. aut Lissia, M. aut Lock, J. aut Longo, G. aut Machulin, I. aut McDonald, A. B. aut McElroy, T. aut McGinn, T. aut McLaughlin, J. B. aut Mehdiyev, R. aut Mielnichuk, C. aut Monroe, J. aut Nadeau, P. aut Nantais, C. aut Ng, C. aut Noble, A. J. aut O’Dwyer, E. aut Oliviéro, G. aut Ouellet, C. aut Pal, S. aut Pasuthip, P. aut Peeters, S. J. M. aut Perry, M. aut Pesudo, V. aut Picciau, E. aut Piro, M.-C. aut Pollmann, T. R. aut Rand, E. T. aut Rethmeier, C. aut Retière, F. aut Rodríguez-García, I. aut Roszkowski, L. aut Ruhland, J. B. aut Sánchez-García, E. aut Santorelli, R. aut Sinclair, D. aut Skensved, P. aut Smith, B. aut Smith, N. J. T. aut Sonley, T. aut Soukup, J. aut Stainforth, R. aut Stone, C. aut Strickland, V. aut Stringer, M. aut Sur, B. aut Tang, J. aut Vázquez-Jáuregui, E. aut Viel, S. aut Walding, J. aut Waqar, M. aut Ward, M. aut Westerdale, S. aut Willis, J. aut Zuñiga-Reyes, A. aut Enthalten in The European physical journal / C Springer Berlin Heidelberg, 1998 81(2021), 9 vom: Sept. (DE-627)235469777 (DE-600)1397769-6 (DE-576)061879150 1434-6044 nnns volume:81 year:2021 number:9 month:09 https://doi.org/10.1140/epjc/s10052-021-09514-w lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 81 2021 9 09 |
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The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. 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Adhikari, P. |
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Adhikari, P. ddc 530 Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data |
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530 VZ Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data |
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title |
Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data |
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(DE-627)OLC2077170700 (DE-He213)s10052-021-09514-w-p |
title_full |
Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data |
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Adhikari, P. |
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Adhikari, P. Ajaj, R. Alpízar-Venegas, M. Amaudruz, P.-A. Auty, D. J. Batygov, M. Beltran, B. Benmansour, H. Bina, C. E. Bonatt, J. Bonivento, W. Boulay, M. G. Broerman, B. Bueno, J. F. Burghardt, P. M. Butcher, A. Cadeddu, M. Cai, B. Cárdenas-Montes, M. Cavuoti, S. Chen, M. Chen, Y. Cleveland, B. T. Corning, J. M. Cranshaw, D. Daugherty, S. DelGobbo, P. Dering, K. DiGioseffo, J. Di Stefano, P. Doria, L. Duncan, F. A. Dunford, M. Ellingwood, E. Erlandson, A. Farahani, S. S. Fatemighomi, N. Fiorillo, G. Florian, S. Flower, T. Ford, R. J. Gagnon, R. Gallacher, D. García Abia, P. Garg, S. Giampa, P. Goeldi, D. Golovko, V. Gorel, P. Graham, K. Grant, D. R. Grobov, A. Hallin, A. L. Hamstra, M. Harvey, P. J. Hearns, C. Hugues, T. Ilyasov, A. Joy, A. Jigmeddorj, B. Jillings, C. J. Kamaev, O. Kaur, G. Kemp, A. Kochanek, I. Kuźniak, M. Lai, M. Langrock, S. Lehnert, B. Leonhardt, A. Levashko, N. Li, X. Lidgard, J. Lindner, T. Lissia, M. Lock, J. Longo, G. Machulin, I. McDonald, A. B. McElroy, T. McGinn, T. McLaughlin, J. B. Mehdiyev, R. Mielnichuk, C. Monroe, J. Nadeau, P. Nantais, C. Ng, C. Noble, A. J. O’Dwyer, E. Oliviéro, G. Ouellet, C. Pal, S. Pasuthip, P. Peeters, S. J. M. Perry, M. Pesudo, V. Picciau, E. Piro, M.-C. Pollmann, T. R. Rand, E. T. Rethmeier, C. Retière, F. Rodríguez-García, I. Roszkowski, L. Ruhland, J. B. Sánchez-García, E. Santorelli, R. Sinclair, D. Skensved, P. Smith, B. Smith, N. J. T. Sonley, T. Soukup, J. Stainforth, R. Stone, C. Strickland, V. Stringer, M. Sur, B. Tang, J. Vázquez-Jáuregui, E. Viel, S. Walding, J. Waqar, M. Ward, M. Westerdale, S. Willis, J. Zuñiga-Reyes, A. |
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Adhikari, P. |
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10.1140/epjc/s10052-021-09514-w |
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title_sort |
pulse-shape discrimination against low-energy ar-39 beta decays in liquid argon with 4.5 tonne-years of deap-3600 data |
title_auth |
Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data |
abstract |
Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. © The Author(s) 2021 |
abstractGer |
Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. © The Author(s) 2021 |
abstract_unstemmed |
Abstract The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $$^{39}\text{ Ar }$$ beta decays and is suppressed using pulse-shape discrimination (PSD). We use two types of PSD estimator: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the mean single-photoelectron charge, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulse shape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. © The Author(s) 2021 |
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9 |
title_short |
Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data |
url |
https://doi.org/10.1140/epjc/s10052-021-09514-w |
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Ajaj, R. Alpízar-Venegas, M. Amaudruz, P.-A. Auty, D. J. Batygov, M. Beltran, B. Benmansour, H. Bina, C. E. Bonatt, J. Bonivento, W. Boulay, M. G. Broerman, B. Bueno, J. F. Burghardt, P. M. Butcher, A. Cadeddu, M. Cai, B. Cárdenas-Montes, M. Cavuoti, S. Chen, M. Chen, Y. Cleveland, B. T. Corning, J. M. Cranshaw, D. Daugherty, S. DelGobbo, P. Dering, K. DiGioseffo, J. Di Stefano, P. Doria, L. Duncan, F. A. Dunford, M. Ellingwood, E. Erlandson, A. Farahani, S. S. Fatemighomi, N. Fiorillo, G. Florian, S. Flower, T. Ford, R. J. Gagnon, R. Gallacher, D. García Abia, P. Garg, S. Giampa, P. Goeldi, D. Golovko, V. Gorel, P. Graham, K. Grant, D. R. Grobov, A. Hallin, A. L. Hamstra, M. Harvey, P. J. Hearns, C. Hugues, T. Ilyasov, A. Joy, A. Jigmeddorj, B. Jillings, C. J. Kamaev, O. Kaur, G. Kemp, A. Kochanek, I. Kuźniak, M. Lai, M. Langrock, S. Lehnert, B. Leonhardt, A. Levashko, N. Li, X. Lidgard, J. Lindner, T. Lissia, M. Lock, J. Longo, G. Machulin, I. McDonald, A. B. McElroy, T. McGinn, T. McLaughlin, J. B. Mehdiyev, R. Mielnichuk, C. Monroe, J. Nadeau, P. Nantais, C. Ng, C. Noble, A. J. O’Dwyer, E. Oliviéro, G. Ouellet, C. Pal, S. Pasuthip, P. Peeters, S. J. M. Perry, M. Pesudo, V. Picciau, E. Piro, M.-C. Pollmann, T. R. Rand, E. T. Rethmeier, C. Retière, F. Rodríguez-García, I. Roszkowski, L. Ruhland, J. B. Sánchez-García, E. Santorelli, R. Sinclair, D. Skensved, P. Smith, B. Smith, N. J. T. Sonley, T. Soukup, J. Stainforth, R. Stone, C. Strickland, V. Stringer, M. Sur, B. Tang, J. Vázquez-Jáuregui, E. Viel, S. Walding, J. Waqar, M. Ward, M. Westerdale, S. Willis, J. Zuñiga-Reyes, A. |
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