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Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data.

Authors :
Adhikari P
Ajaj R
Alpízar-Venegas M
Amaudruz PA
Auty DJ
Batygov M
Beltran B
Benmansour H
Bina CE
Bonatt J
Bonivento W
Boulay MG
Broerman B
Bueno JF
Burghardt PM
Butcher A
Cadeddu M
Cai B
Cárdenas-Montes M
Cavuoti S
Chen M
Chen Y
Cleveland BT
Corning JM
Cranshaw D
Daugherty S
DelGobbo P
Dering K
DiGioseffo J
Di Stefano P
Doria L
Duncan FA
Dunford M
Ellingwood E
Erlandson A
Farahani SS
Fatemighomi N
Fiorillo G
Florian S
Flower T
Ford RJ
Gagnon R
Gallacher D
García Abia P
Garg S
Giampa P
Goeldi D
Golovko V
Gorel P
Graham K
Grant DR
Grobov A
Hallin AL
Hamstra M
Harvey PJ
Hearns C
Hugues T
Ilyasov A
Joy A
Jigmeddorj B
Jillings CJ
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 AB
McElroy T
McGinn T
McLaughlin JB
Mehdiyev R
Mielnichuk C
Monroe J
Nadeau P
Nantais C
Ng C
Noble AJ
O'Dwyer E
Oliviéro G
Ouellet C
Pal S
Pasuthip P
Peeters SJM
Perry M
Pesudo V
Picciau E
Piro MC
Pollmann TR
Rand ET
Rethmeier C
Retière F
Rodríguez-García I
Roszkowski L
Ruhland JB
Sánchez-García E
Santorelli R
Sinclair D
Skensved P
Smith B
Smith NJT
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
Source :
The European physical journal. C, Particles and fields [Eur Phys J C Part Fields] 2021; Vol. 81 (9), pp. 823. Date of Electronic Publication: 2021 Sep 16.
Publication Year :
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 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.<br /> (© The Author(s) 2021.)

Details

Language :
English
ISSN :
1434-6044
Volume :
81
Issue :
9
Database :
MEDLINE
Journal :
The European physical journal. C, Particles and fields
Publication Type :
Academic Journal
Accession number :
34720726
Full Text :
https://doi.org/10.1140/epjc/s10052-021-09514-w