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1. Precision measurement of the specific activity of $$^{39}$$ 39 Ar in atmospheric argon with the DEAP-3600 detector

Author

P. Adhikari, R. Ajaj, M. Alpízar-Venegas, P.-A. Amaudruz, J. Anstey, G. R. Araujo, D. J. Auty, M. Baldwin, M. Batygov, B. Beltran, H. Benmansour, C. E. Bina, J. Bonatt, W. Bonivento, M. G. Boulay, B. Broerman, J. F. Bueno, P. M. Burghardt, A. Butcher, M. Cadeddu, B. Cai, M. Cárdenas-Montes, S. Cavuoti, M. Chen, Y. Chen, S. Choudhary, B. T. Cleveland, J. M. Corning, R. Crampton, D. Cranshaw, S. Daugherty, P. DelGobbo, K. Dering, P. Di Stefano, J. DiGioseffo, G. Dolganov, L. Doria, F. A. Duncan, M. Dunford, E. Ellingwood, A. Erlandson, S. S. Farahani, N. Fatemighomi, G. Fiorillo, S. Florian, A. Flower, R. J. Ford, R. Gagnon, D. Gallacher, P. García Abia, S. Garg, P. Giampa, A. Giménez-Alcázar, D. Goeldi, V. V. Golovko, P. Gorel, K. Graham, D. R. Grant, A. Grobov, A. L. Hallin, M. Hamstra, P. J. Harvey, S. Haskins, C. Hearns, J. Hu, J. Hucker, T. Hugues, A. Ilyasov, B. Jigmeddorj, C. J. Jillings, A. Joy, O. Kamaev, G. Kaur, A. Kemp, M. Kuźniak, F. La Zia, M. Lai, S. Langrock, B. Lehnert, A. Leonhardt, J. LePage-Bourbonnais, N. Levashko, J. Lidgard, T. Lindner, M. Lissia, J. Lock, L. Luzzi, I. Machulin, P. Majewski, A. Maru, J. Mason, A. B. McDonald, T. McElroy, T. McGinn, J. B. McLaughlin, R. Mehdiyev, C. Mielnichuk, L. Mirasola, J. Monroe, P. Nadeau, C. Nantais, C. Ng, A. J. Noble, E. O’Dwyer, G. Oliviéro, C. Ouellet, S. Pal, D. Papi, P. Pasuthip, S. J. M. Peeters, M. Perry, V. Pesudo, E. Picciau, M.-C. Piro, T. R. Pollmann, F. Rad, E. T. Rand, C. Rethmeier, F. Retière, I. Rodríguez García, L. Roszkowski, J. B. Ruhland, R. Santorelli, F. G. Schuckman II, N. Seeburn, S. Seth, V. Shalamova, K. Singhrao, P. Skensved, N. J. T. Smith, B. Smith, K. Sobotkiewich, T. Sonley, J. Sosiak, J. Soukup, R. Stainforth, C. Stone, V. Strickland, M. Stringer, B. Sur, J. Tang, E. Vázquez-Jáuregui, L. Veloce, S. Viel, B. Vyas, M. Walczak, J. Walding, M. Ward, S. Westerdale, J. Willis, A. Zuñiga-Reyes, and DEAP Collaboration

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract The specific activity of the $$\beta $$ β decay of $$^{39}$$ 39 Ar in atmospheric argon is measured using the DEAP-3600 detector. DEAP-3600, located 2 km underground at SNOLAB, uses a total of (3269 ± 24) kg of liquid argon distilled from the atmosphere to search for dark matter. This detector is well-suited to measure the decay of $$^{39}$$ 39 Ar owing to its very low background levels. This is achieved in two ways: it uses low background construction materials; and it uses pulse-shape discrimination to differentiate between nuclear recoils and electron recoils. With 167 live-days of data, the measured specific activity at the time of atmospheric extraction is (0.964 ± 0.001 $$_\textrm{stat}$$ stat ± 0.024 $$_\textrm{sys}$$ sys ) Bq/kg $$_\textrm{atmAr}$$ atmAr , which is consistent with results from other experiments. A cross-check analysis using different event selection criteria and a different statistical method confirms the result.

Published
2023
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2. Pulse-shape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data

Author

P. Adhikari, R. Ajaj, M. Alpízar-Venegas, P.-A. Amaudruz, D. J. Auty, M. Batygov, B. Beltran, H. Benmansour, C. E. Bina, J. Bonatt, W. Bonivento, M. G. Boulay, B. Broerman, J. F. Bueno, P. M. Burghardt, A. Butcher, M. Cadeddu, B. Cai, M. Cárdenas-Montes, S. Cavuoti, M. Chen, Y. Chen, B. T. Cleveland, J. M. Corning, D. Cranshaw, S. Daugherty, P. DelGobbo, K. Dering, J. DiGioseffo, P. Di Stefano, L. Doria, F. A. Duncan, M. Dunford, E. Ellingwood, A. Erlandson, S. S. Farahani, N. Fatemighomi, G. Fiorillo, S. Florian, T. Flower, R. J. Ford, R. Gagnon, D. Gallacher, P. García Abia, S. Garg, P. Giampa, D. Goeldi, V. Golovko, P. Gorel, K. Graham, D. R. Grant, A. Grobov, A. L. Hallin, M. Hamstra, P. J. Harvey, C. Hearns, T. Hugues, A. Ilyasov, A. Joy, B. Jigmeddorj, C. J. Jillings, O. Kamaev, G. Kaur, A. Kemp, I. Kochanek, M. Kuźniak, M. Lai, S. Langrock, B. Lehnert, A. Leonhardt, N. Levashko, X. Li, J. Lidgard, T. Lindner, M. Lissia, J. Lock, G. Longo, I. Machulin, A. B. McDonald, T. McElroy, T. McGinn, J. B. McLaughlin, R. Mehdiyev, C. Mielnichuk, J. Monroe, P. Nadeau, C. Nantais, C. Ng, A. J. Noble, E. O’Dwyer, G. Oliviéro, C. Ouellet, S. Pal, P. Pasuthip, S. J. M. Peeters, M. Perry, V. Pesudo, E. Picciau, M.-C. Piro, T. R. Pollmann, E. T. Rand, C. Rethmeier, F. Retière, I. Rodríguez-García, L. Roszkowski, J. B. Ruhland, E. Sánchez-García, R. Santorelli, D. Sinclair, P. Skensved, B. Smith, N. J. T. Smith, T. Sonley, J. Soukup, R. Stainforth, C. Stone, V. Strickland, M. Stringer, B. Sur, J. Tang, E. Vázquez-Jáuregui, S. Viel, J. Walding, M. Waqar, M. Ward, S. Westerdale, J. Willis, A. Zuñiga-Reyes, and DEAP Collaboration

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
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 $$^{39}\text{ Ar }$$ 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.

Published
2021
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3. The liquid-argon scintillation pulseshape in DEAP-3600

Author

DEAP Collaboration, P. Adhikari, R. Ajaj, G. R. Araujo, M. Batygov, B. Beltran, C. E. Bina, M. G. Boulay, B. Broerman, J. F. Bueno, A. Butcher, B. Cai, M. Cárdenas-Montes, S. Cavuoti, Y. Chen, B. T. Cleveland, J. M. Corning, S. J. Daugherty, P. Di Stefano, K. Dering, L. Doria, F. A. Duncan, M. Dunford, A. Erlandson, N. Fatemighomi, G. Fiorillo, A. Flower, R. J. Ford, R. Gagnon, D. Gallacher, E. A. Garcés, P. García Abia, S. Garg, P. Giampa, D. Goeldi, V. V. Golovko, P. Gorel, K. Graham, D. R. Grant, A. Grobov, A. L. Hallin, M. Hamstra, P. J. Harvey, C. Hearns, A. Ilyasov, A. Joy, C. J. Jillings, O. Kamaev, G. Kaur, A. Kemp, I. Kochanek, M. Kuźniak, S. Langrock, F. La Zia, B. Lehnert, N. Levashko, X. Li, O. Litvinov, J. Lock, G. Longo, I. Machulin, P. Majewski, A. B. McDonald, T. McElroy, T. McGinn, J. B. McLaughlin, R. Mehdiyev, C. Mielnichuk, J. Monroe, P. Nadeau, C. Nantais, C. Ng, A. J. Noble, G. Oliviéro, C. Ouellet, S. Pal, P. Pasuthip, S. J. M. Peeters, V. Pesudo, M.-C. Piro, T. R. Pollmann, E. T. Rand, C. Rethmeier, F. Retière, E. Sanchez García, T. Sánchez-Pastor, R. Santorelli, N. Seeburn, P. Skensved, B. Smith, N. J. T. Smith, T. Sonley, R. Stainforth, C. Stone, V. Strickland, M. Stringer, B. Sur, E. Vázquez-Jáuregui, L. Veloce, S. Viel, J. Walding, M. Waqar, M. Ward, S. Westerdale, J. Willis, and A. Zuñiga-Reyes

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract DEAP-3600 is a liquid-argon scintillation detector looking for dark matter. Scintillation events in the liquid argon (LAr) are registered by 255 photomultiplier tubes (PMTs), and pulseshape discrimination (PSD) is used to suppress electromagnetic background events. The excellent PSD performance of LAr makes it a viable target for dark matter searches, and the LAr scintillation pulseshape discussed here is the basis of PSD. The observed pulseshape is a combination of LAr scintillation physics with detector effects. We present a model for the pulseshape of electromagnetic background events in the energy region of interest for dark matter searches. The model is composed of (a) LAr scintillation physics, including the so-called intermediate component, (b) the time response of the TPB wavelength shifter, including delayed TPB emission at $${\mathcal {O}}$$ O (ms) time-scales, and c) PMT response. TPB is the wavelength shifter of choice in most LAr detectors. We find that approximately 10% of the intensity of the wavelength-shifted light is in a long-lived state of TPB. This causes light from an event to spill into subsequent events to an extent not usually accounted for in the design and data analysis of LAr-based detectors.

Published
2020
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4. Pulse-shape discrimination against low-energy Ar-39 β decays in liquid argon with 4.5 tonne-years of DEAP-3600 data

Author

P. Adhikari, R. Ajaj, M. Alpízar-Venegas, P.-A. Amaudruz, D. J. Auty, M. Batygov, B. Beltran, H. Benmansour, C. E. Bina, J. Bonatt, W. Bonivento, M. G. Boulay, B. Broerman, J. F. Bueno, P. M. Burghardt, A. Butcher, M. Cadeddu, B. Cai, M. Cárdenas-Montes, S. Cavuoti, M. Chen, Y. Chen, B. T. Cleveland, J. M. Corning, D. Cranshaw, S. Daugherty, P. DelGobbo, K. Dering, J. DiGioseffo, P. Di Stefano, L. Doria, F. A. Duncan, M. Dunford, E. Ellingwood, A. Erlandson, S. S. Farahani, N. Fatemighomi, G. Fiorillo, S. Florian, T. Flower, R. J. Ford, R. Gagnon, D. Gallacher, P. García Abia, S. Garg, P. Giampa, D. Goeldi, V. Golovko, P. Gorel, K. Graham, D. R. Grant, A. Grobov, A. L. Hallin, M. Hamstra, P. J. Harvey, C. Hearns, T. Hugues, A. Ilyasov, A. Joy, B. Jigmeddorj, C. J. Jillings, O. Kamaev, G. Kaur, A. Kemp, I. Kochanek, M. Kuźniak, M. Lai, S. Langrock, B. Lehnert, A. Leonhardt, N. Levashko, X. Li, J. Lidgard, T. Lindner, M. Lissia, J. Lock, G. Longo, I. Machulin, A. B. McDonald, T. McElroy, T. McGinn, J. B. McLaughlin, R. Mehdiyev, C. Mielnichuk, J. Monroe, P. Nadeau, C. Nantais, C. Ng, A. J. Noble, E. O’Dwyer, G. Oliviéro, C. Ouellet, S. Pal, P. Pasuthip, S. J. M. Peeters, M. Perry, V. Pesudo, E. Picciau, M.-C. Piro, T. R. Pollmann, E. T. Rand, C. Rethmeier, F. Retière, I. Rodríguez-García, L. Roszkowski, J. B. Ruhland, E. Sánchez-García, R. Santorelli, D. Sinclair, P. Skensved, B. Smith, N. J. T. Smith, T. Sonley, J. Soukup, R. Stainforth, C. Stone, V. Strickland, M. Stringer, B. Sur, J. Tang, E. Vázquez-Jáuregui, S. Viel, J. Walding, M. Waqar, M. Ward, S. Westerdale, J. Willis, A. Zuñiga-Reyes, DEAP Collaboration, and Astroparticle Physics (IHEF, IoP, FNWI)

Subjects
Physics - Instrumentation and Detectors, Photon, Physics and Astronomy (miscellaneous), Regular Article - Experimental Physics, Physics::Instrumentation and Detectors, Dark matter, FOS: Physical sciences, QC770-798, Astrophysics, Computer Science::Digital Libraries, 01 natural sciences, 7. Clean energy, Signal, DEAP, Nuclear and particle physics. Atomic energy. Radioactivity, 0103 physical sciences, 010306 general physics, Instrumentation and Methods for Astrophysics (astro-ph.IM), Engineering (miscellaneous), Physics, Scintillation, 010308 nuclear & particles physics, Scattering, Detector, Instrumentation and Detectors (physics.ins-det), 3. Good health, Computational physics, Pulse (physics), QB460-466, Computer Science::Mathematical Software, Astrophysics - Instrumentation and Methods for Astrophysics
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 pulseshape discrimination (PSD). We use two types of PSD algorithm: 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 charge of a single photoelectron, 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 pulseshape 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., 14 pages, 9 figures

Published
2021

5. Constraints on dark matter-nucleon effective couplings in the presence of kinematically distinct halo substructures using the DEAP-3600 detector

Author

Miguel Cárdenas-Montes, G. Oliviéro, Luca Doria, M. G. Boulay, A. Kemp, G. Kaur, R. Stainforth, Stefano Cavuoti, Bei Cai, O. Litvinov, P. Gorel, M. C. Piro, Monica Dunford, O. Kamaev, F. Retiere, S. Viel, P. Skensved, Xiujiang Li, C. Rethmeier, S. S. Farahani, I. Kochanek, J. Lock, A. Zuñiga-Reyes, C. Jillings, T. Hugues, N. J. T. Smith, D. Gallacher, C. E. Bina, C. Mielnichuk, M. Cadeddu, S. Westerdale, Bhaskar Sur, S. Langrock, J. B. McLaughlin, M. Hamstra, T. Pollmann, P. DelGobbo, S. Garg, M. Kuźniak, V. Pesudo, T. Sonley, B. Jigmeddorj, Jocelyn Monroe, David A. Sinclair, Leszek Roszkowski, A. C. Vincent, S. J. M. Peeters, G. Fiorillo, W. Bonivento, J. Walding, R. Santorelli, J. M. Corning, P. Giampa, T. Sánchez-Pastor, B. C. Smith, A. Ilyasov, D. J. Auty, I. N. Machulin, M. Lai, M. Stringer, A. B. McDonald, N. Fatemighomi, R. Ajaj, P. Adhikari, E. Sanchez Garcia, A. Erlandson, Martin Ward, Giuseppe Longo, E. T. Rand, E. Vázquez-Jáuregui, P. Garcia Abia, S. Pal, A. Joy, J. Willis, B. Lehnert, N. Levashko, A. L. Hallin, B. T. Cleveland, M. Waqar, E. A. Garcés, A. Grobov, K. Graham, I. Rodríguez-García, S. J. Daugherty, Y. Chen, D. Goeldi, T. McElroy, P. Di Stefano, Adhikari, P., Ajaj, R., Auty, D. J., Bina, C. E., Bonivento, W., Boulay, M. G., Cadeddu, M., Cai, B., Cardenas-Montes, M., Cavuoti, S., Chen, Y., Cleveland, B. T., Corning, J. M., Daugherty, S., Delgobbo, P., Di Stefano, P., Doria, L., Dunford, M., Erlandson, A., Farahani, S. S., Fatemighomi, N., Fiorillo, G., Gallacher, D., Garces, E. A., Abia, P. Garcia, Garg, S., Giampa, P., Goeldi, D., Gorel, P., Graham, K., Grobov, A., Hallin, A. L., Hamstra, M., Hugues, T., Ilyasov, A., Joy, A., Jigmeddorj, B., Jillings, C. J., Kamaev, O., Kaur, G., Kemp, A., Kochanek, I, Kuzniak, M., Lai, M., Langrock, S., Lehnert, B., Levashko, N., Li, X., Litvinov, O., Lock, J., Longo, G., Machulin, I, Mcdonald, A. B., Mcelroy, T., Mclaughlin, J. B., Mielnichuk, C., Monroe, J., Oliviero, G., Pal, S., Peeters, S. J. M., Pesudo, V, Piro, M-C, Pollmann, T. R., Rand, E. T., Rethmeier, C., Retiere, F., Rodriguez-Garcia, I, Roszkowski, L., Sanchez Garcia, E., Sanchez-Pastor, T., Santorelli, R., Sinclair, D., Skensved, P., Smith, B., Smith, N. J. T., Sonley, T., Stainforth, R., Stringer, M., Sur, B., Vazquez-Jauregui, E., Viel, S., Vincent, A. C., Walding, J., Waqar, M., Ward, M., Westerdale, S., Willis, J., and Zuniga-Reyes, A.

Subjects
Physics, Particle physics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Isovector, 010308 nuclear & particles physics, Isoscalar, Dark matter, FOS: Physical sciences, Astrophysics::Cosmology and Extragalactic Astrophysics, 01 natural sciences, Astrophysics - Astrophysics of Galaxies, High Energy Physics - Experiment, Dark matter halo, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), Weakly interacting massive particles, Astrophysics of Galaxies (astro-ph.GA), 0103 physical sciences, Effective field theory, Halo, 010306 general physics, Magnetic dipole, Astrophysics::Galaxy Astrophysics, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract

DEAP-3600 is a single-phase liquid argon detector aiming to directly detect Weakly Interacting Massive Particles (WIMPs), located at SNOLAB (Sudbury, Canada). After analyzing data taken during the first year of operation, a null result was used to place an upper bound on the WIMP-nucleon spin-independent, isoscalar cross section. This study reinterprets this result within a Non-Relativistic Effective Field Theory framework, and further examines how various possible substructures in the local dark matter halo may affect these constraints. Such substructures are hinted at by kinematic structures in the local stellar distribution observed by the Gaia satellite and other recent astronomical surveys. These include the Gaia Sausage (or Enceladus), as well as a number of distinct streams identified in recent studies. Limits are presented for the coupling strength of the effective contact interaction operators $\mathcal{O}_1$, $\mathcal{O}_3$, $\mathcal{O}_5$, $\mathcal{O}_8$, and $\mathcal{O}_{11}$, considering isoscalar, isovector, and xenonphobic scenarios, as well as the specific operators corresponding to millicharge, magnetic dipole, electric dipole, and anapole interactions. The effects of halo substructures on each of these operators are explored as well, showing that the $\mathcal{O}_5$ and $\mathcal{O}_8$ operators are particularly sensitive to the velocity distribution, even at dark matter masses above 100 GeV/$c^2$.

Published
2020

6. Electromagnetic backgrounds and potassium-42 activity in the DEAP-3600 dark matter detector

Author

C. Rethmeier, Laurelle Maria Veloce, C. Jillings, C. E. Bina, S. Langrock, T. Sonley, C. M. Nantais, Stefano Cavuoti, Peter Majewski, M. C. Piro, V. V. Golovko, K. Graham, N. J. T. Smith, O. Litvinov, P. Skensved, J. B. McLaughlin, Darren Grant, E. Sanchez Garcia, P. Nadeau, O. Kamaev, I. Kochanek, M. G. Boulay, Min Chen, Martin Ward, D. Gallacher, R. J. Ford, J. Lock, A. Zuñiga-Reyes, F. La Zia, N. Fatemighomi, Giuseppe Longo, T. McGinn, S. Viel, A. B. McDonald, Y. Chen, M. Hamstra, P. J. Harvey, A. Erlandson, D. Goeldi, B. Lehnert, V. Pesudo, N. Seeburn, V. Strickland, E. T. Rand, S. Garg, R. Gagnon, K. Dering, C. Mielnichuk, R. Santorelli, Bhaskar Sur, P. Pasuthip, T. McElroy, A. J. Noble, P. Gorel, Xiujiang Li, S. J. M. Peeters, R. Ajaj, B. Beltran, A. Flower, C. Ng, Jocelyn Monroe, A. Joy, J. Walding, M. Waqar, A. Kemp, G. Kaur, J. Willis, M. Batygov, C. Hearns, T. Pollmann, J. F. Bueno, G. R. Araujo, R. Mehdiyev, A. L. Hallin, G. Fiorillo, B. T. Cleveland, F. Retiere, Miguel Cárdenas-Montes, B. C. Smith, M. Kuźniak, C. Stone, S. Westerdale, F. A. Duncan, R. Stainforth, B. Broerman, A. Butcher, Bei Cai, C. Ouellet, M. Dunford, E. Vázquez-Jáuregui, P. M. Burghardt, P. Giampa, P. Garcia Abia, Ajaj, R., Araujo, G. R., Batygov, M., Beltran, B., Bina, C. E., Boulay, M. G., Broerman, B., Bueno, J. F., Burghardt, P. M., Butcher, A., Cai, B., Cárdenas-Montes, M., Cavuoti, S., Chen, M., Chen, Y., Cleveland, B. T., Dering, K., Duncan, F. A., Dunford, M., Erlandson, A., Fatemighomi, N., Fiorillo, G., Flower, A., Ford, R. J., Gagnon, R., Gallacher, D., García Abia, P., Garg, S., Giampa, P., Goeldi, D., Golovko, V. V., Gorel, P., Graham, K., Grant, D. R., Hallin, A. L., Hamstra, M., Harvey, P. J., Hearns, C., Joy, A., Jillings, C. J., Kamaev, O., Kaur, G., Kemp, A., Kochanek, I., Kuźniak, M., Langrock, S., La Zia, F., Lehnert, B., Li, X., Litvinov, O., Lock, J., Longo, G., Majewski, P., 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., Ouellet, C., Pasuthip, P., Peeters, S. J. M., Pesudo, V., Piro, M. -C., Pollmann, T. R., Rand, E. T., Rethmeier, C., Retière, F., Sanchez García, E., Santorelli, R., Seeburn, N., Skensved, P., Smith, B., Smith, N. J. T., Sonley, T., Stainforth, R., Stone, C., Strickland, V., Sur, B., Vázquez-Jáuregui, E., Veloce, L., Viel, S., Walding, J., Waqar, M., Ward, M., Westerdale, S., Willis, J., and Zuñiga-Reyes, A.

Subjects
Dark matter, Analytical chemistry, FOS: Physical sciences, nucl-ex, 01 natural sciences, Atomic, DEAP, Particle and Plasma Physics, 0103 physical sciences, Nuclear, Nuclear Experiment (nucl-ex), Single phase, 010306 general physics, Nuclear Experiment, Instrumentation and Methods for Astrophysics (astro-ph.IM), ComputingMilieux_MISCELLANEOUS, QC, Prior information, Physics, Quantum Physics, 010308 nuclear & particles physics, Molecular, Nuclear & Particles Physics, Liquid argon, Astrophysics - Instrumentation and Methods for Astrophysics, Astronomical and Space Sciences, astro-ph.IM
Abstract

Author(s): Ajaj, R; Araujo, GR; Batygov, M; Beltran, B; Bina, CE; Boulay, MG; Broerman, B; Bueno, JF; Burghardt, PM; Butcher, A; Cai, B; Cardenas-Montes, M; Cavuoti, S; Chen, M; Chen, Y; Cleveland, BT; Dering, K; Duncan, FA; Dunford, M; Erlandson, A; Fatemighomi, N; Fiorillo, G; Flower, A; Ford, RJ; Gagnon, R; Gallacher, D; Garcia Abia, P; Garg, S; Giampa, P; Goeldi, D; Golovko, VV; Gorel, P; Graham, K; Grant, DR; Hallin, AL; Hamstra, M; Harvey, PJ; Hearns, C; Joy, A; Jillings, CJ; Kamaev, O; Kaur, G; Kemp, A; Kochanek, I; Kuźniak, M; Langrock, S; La Zia, F; Lehnert, B; Li, X; Litvinov, O; Lock, J; Longo, G; Majewski, P; McDonald, AB; McElroy, T; McGinn, T; McLaughlin, JB; Mehdiyev, R; Mielnichuk, C; Monroe, J; Nadeau, P; Nantais, C; Ng, C; Noble, AJ; Ouellet, C; Pasuthip, P; Peeters, SJM; Pesudo, V; Piro, MC; Pollmann, TR; Rand, ET; Rethmeier, C; Retiere, F; Sanchez Garcia, E; Santorelli, R; Seeburn, N; Skensved, P; Smith, B; Smith, NJT; Sonley, T; Stainforth, R; Stone, C; Strickland, V; Sur, B; Vazquez-Jauregui, E | Abstract: The DEAP-3600 experiment is searching for weakly interacting massive particles dark matter with a 3.3 ×103 kg single phase liquid argon (LAr) target, located 2.1 km underground at SNOLAB. The experimental signature of dark matter interactions is kilo electron volt-scale Ar40 nuclear recoils producing 128 nm LAr scintillation photons observed by photomultiplier tubes. The largest backgrounds in DEAP-3600 are electronic recoils (ERs) induced by β and γ rays originating from internal and external radioactivity in the detector material. A background model of the ER interactions in DEAP-3600 was developed and is described in this work. The model is based on several components which are expected from radioisotopes in the LAr, from ex situ material assay measurements, and from dedicated independent in situ analyses. This prior information is used in a Bayesian fit of the ER components to a 247.2 d dataset to model the radioactivity in the surrounding detector materials. Pulse-shape discrimination separates ER and NR events. However, detailed knowledge of the ER background and activity of detector components sets valuable constraints on NR backgrounds including neutrons and alphas. In addition, the activity of Ar42 in LAr in DEAP-3600 is determined by measuring the daughter decay of K42. This cosmogenically activated trace isotope is a relevant background at higher energies for other rare event searches using atmospheric argon, e.g., DarkSide-20k, GERDA, or LEGEND. The specific activity of Ar42 in the atmosphere is found to be 40.4±5.9 μBq/kg of argon.

Published
2019

7. Design and construction of the DEAP-3600 dark matter detector

Author

C. Hearns, B. Lehnert, P. Gorel, Randall White, S. Florian, J. B. McLaughlin, A. Kemp, T. Pollmann, S. J. M. Peeters, C. Lim, A. J. Noble, R. Mathew, D. Bishop, K. Olchanski, J. F. Bueno, N. Seeburn, A. Muir, Y. Linn, W. Rau, Shuai Liu, P. Liimatainen, T. McElroy, C. Rethmeier, Stephen Kam-wah Chan, T. Bromwich, Monica Dunford, K. S. Olsen, C. Ouellet, R. Chouinard, P. Nadeau, C. Nantais, C. Ohlmann, C. Ng, Laurelle Maria Veloce, O. Kamaev, S. Langrock, R. Gagnon, P. Amaudruz, A. Butcher, M. Hamstra, Jocelyn Monroe, C. Mielnichuk, B. T. Cleveland, Bhaskar Sur, F. Duncan, F. Retiere, Min Chen, K. W. McFarlane, A. Hall, O. Li, J. Tang, P. Giampa, J. Walding, J. Soukup, M. Batygov, K. Graham, K. Singhrao, R. Stainforth, T. Lindner, A. B. McDonald, Martin Ward, Darren Grant, S. Mead, B. Smith, Bei Cai, R. Gornea, Mark Guy Boulay, Peter Majewski, N. Fatemighomi, P. Skensved, P. Pasuthip, P. M. Burghardt, R. Ford, J. DiGioseffo, J. Lidgard, J. Bonatt, C. Stone, M. Kuźniak, S. Westerdale, N. J. T. Smith, B. Broerman, E. Vázquez-Jáuregui, A. Flower, Joanne Taylor, E. Grace, T. Sonley, P. J. Harvey, R. Mehdiyev, A. Erlandson, F. La Zia, V. V. Golovko, T. McGinn, K. Dering, E. Gulyev, E. O'Dwyer, B. Beltran, S. Dittmeier, E. Woolsey, A. L. Hallin, Gary Boorman, C. J. Jillings, M. Baldwin, B. Shaw, E. T. Rand, C. E. Bina, J. Zielinski, V. Strickland, S. Churchwell, and D. Cranshaw

Subjects
Physics::Instrumentation and Detectors, Dark matter, FOS: Physical sciences, chemistry.chemical_element, Astrophysics::Cosmology and Extragalactic Astrophysics, 01 natural sciences, High Energy Physics - Experiment, Nuclear physics, DEAP, High Energy Physics - Experiment (hep-ex), WIMP, 0103 physical sciences, Instrumentation and Methods for Astrophysics (astro-ph.IM), 010303 astronomy & astrophysics, QC, Physics, Argon, 010308 nuclear & particles physics, Scattering, Detector, Astrophysics::Instrumentation and Methods for Astrophysics, Astronomy and Astrophysics, chemistry, Weakly interacting massive particles, Nucleon, Astrophysics - Instrumentation and Methods for Astrophysics
Abstract

The Dark matter Experiment using Argon Pulse-shape discrimination (DEAP) has been designed for a direct detection search for particle dark matter using a single-phase liquid argon target. The projected cross section sensitivity for DEAP-3600 to the spin-independent scattering of Weakly Interacting Massive Particles (WIMPs) on nucleons is $10^{-46}~\rm{cm}^{2}$ for a 100 GeV/$c^2$ WIMP mass with a fiducial exposure of 3 tonne-years. This paper describes the physical properties and construction of the DEAP-3600 detector., minor corrections in version 2. 70 pages, 24 figures, to be submitted to Astroparticle Physics Journal

Published
2019

8. In-situ characterization of the Hamamatsu R5912-HQE photomultiplier tubes used in the DEAP-3600 experiment

Author

J. B. McLaughlin, V. Strickland, M. Batygov, P. Nadeau, C. E. Bina, P. Skensved, T. Pollmann, T. Sonley, Y. Linn, B. Lehnert, C. Stone, W. Rau, S. Westerdale, J. F. Bueno, N. Seeburn, T. McElroy, J. Walding, B. Broerman, J. Lidgard, C. Ng, K. Olchanski, C. Rethmeier, Laurelle Maria Veloce, S. J. M. Peeters, A. Muir, T. Lindner, D. Bishop, K. Graham, K. Singhrao, S. Mead, C. Hearns, K. W. McFarlane, M. Kuźniak, E. T. Rand, P. Gorel, T. Bromwich, A. J. Noble, S. Churchwell, A. Kemp, Joanne Taylor, C. Lim, P. Liimatainen, C. Mielnichuk, E. O'Dwyer, Bhaskar Sur, B. Smith, P. Giampa, E. Grace, Bei Cai, N. Fatemighomi, R. Gornea, R. Ford, R. Mathew, D. Cranshaw, K. Dering, Monica Dunford, P. Pasuthip, O. Kamaev, M. Hamstra, R. Mehdiyev, V. V. Golovko, P. J. Harvey, Martin Ward, Min Chen, N. J. T. Smith, J. Zielinski, A. Erlandson, Gary Boorman, E. Gulyev, F. La Zia, E. Vázquez-Jáuregui, Stephen Kam-wah Chan, S. Langrock, B. T. Cleveland, A. Hall, Mark Guy Boulay, R. Gagnon, Pierre-Andre Amaudruz, Jocelyn Monroe, Shuai Liu, J. Bonatt, R. Stainforth, A. B. McDonald, O. Li, J. Tang, B. Beltran, S. Dittmeier, E. Woolsey, A. L. Hallin, C. J. Jillings, C. Ouellet, C. Nantais, A. Butcher, B. Shaw, R. Chouinard, C. Ohlmann, F. Duncan, F. Retiere, Darren Grant, Randall White, and K. S. Olsen

Subjects
Physics, Nuclear and High Energy Physics, Photomultiplier, Optical fiber, Physics - Instrumentation and Detectors, 010308 nuclear & particles physics, business.industry, Physics::Instrumentation and Detectors, Detector, Dark matter, FOS: Physical sciences, Instrumentation and Detectors (physics.ins-det), 01 natural sciences, 7. Clean energy, Noise (electronics), law.invention, DEAP, Optics, law, 0103 physical sciences, Neutrino, 010306 general physics, business, Instrumentation, Dark current
Abstract

The Hamamatsu R5912-HQE photomultiplier-tube (PMT) is a novel high-quantum efficiency PMT. It is currently used in the DEAP-3600 dark matter detector and is of significant interest for future dark matter and neutrino experiments where high signal yields are needed. We report on the methods developed for in-situ characterization and monitoring of DEAP's 255 R5912-HQE PMTs. This includes a detailed discussion of typical measured single-photoelectron charge distributions, correlated noise (afterpulsing), dark noise, double, and late pulsing characteristics. The characterization is performed during the detector commissioning phase using laser light injected through a light diffusing sphere and during normal detector operation using LED light injected through optical fibres.

Published
2017
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9. First Direct Detection Constraints on Planck-Scale Mass Dark Matter with Multiple-Scatter Signatures Using the DEAP-3600 Detector.

Author

Adhikari P, Ajaj R, Alpízar-Venegas M, Auty DJ, Benmansour H, Bina CE, Bonivento W, Boulay MG, Cadeddu M, Cai B, Cárdenas-Montes M, Cavuoti S, Chen Y, Cleveland BT, Corning JM, Daugherty S, DelGobbo P, Di Stefano P, Doria L, Dunford M, Ellingwood E, Erlandson A, Farahani SS, Fatemighomi N, Fiorillo G, Gallacher D, García Abia P, Garg S, Giampa P, Goeldi D, Gorel P, Graham K, Grobov A, Hallin AL, Hamstra M, 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, Lissia M, Litvinov O, Lock J, Longo G, Machulin I, McDonald AB, McElroy T, McLaughlin JB, Mielnichuk C, Mirasola L, Monroe J, Oliviéro G, Pal S, Peeters SJM, Perry M, Pesudo V, Picciau E, Piro MC, Pollmann TR, Raj N, Rand ET, Rethmeier C, Retière F, Rodríguez-García I, Roszkowski L, Ruhland JB, Sanchez García E, Sánchez-Pastor T, Santorelli R, Seth S, Sinclair D, Skensved P, Smith B, Smith NJT, Sonley T, Stainforth R, Stringer M, Sur B, Vázquez-Jáuregui E, Viel S, Walding J, Waqar M, Ward M, Westerdale S, Willis J, and Zuñiga-Reyes A

Abstract

Dark matter with Planck-scale mass (≃10^{19}  GeV/c^{2}) arises in well-motivated theories and could be produced by several cosmological mechanisms. A search for multiscatter signals from supermassive dark matter was performed with a blind analysis of data collected over a 813 d live time with DEAP-3600, a 3.3 t single-phase liquid argon-based detector at SNOLAB. No candidate signals were observed, leading to the first direct detection constraints on Planck-scale mass dark matter. Leading limits constrain dark matter masses between 8.3×10^{6} and 1.2×10^{19}  GeV/c^{2}, and ^{40}Ar-scattering cross sections between 1.0×10^{-23} and 2.4×10^{-18}  cm^{2}. These results are interpreted as constraints on composite dark matter models with two different nucleon-to-nuclear cross section scalings.

Published
2022
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10. First Results from the DEAP-3600 Dark Matter Search with Argon at SNOLAB.

Author

Amaudruz PA, Baldwin M, Batygov M, Beltran B, Bina CE, Bishop D, Bonatt J, Boorman G, Boulay MG, Broerman B, Bromwich T, Bueno JF, Burghardt PM, Butcher A, Cai B, Chan S, Chen M, Chouinard R, Cleveland BT, Cranshaw D, Dering K, DiGioseffo J, Dittmeier S, Duncan FA, Dunford M, Erlandson A, Fatemighomi N, Florian S, Flower A, Ford RJ, Gagnon R, Giampa P, Golovko VV, Gorel P, Gornea R, Grace E, Graham K, Gulyev E, Hakobyan R, Hall A, Hallin AL, Hamstra M, Harvey PJ, Hearns C, Jillings CJ, Kamaev O, Kemp A, Kuźniak M, Langrock S, La Zia F, Lehnert B, Lidgard JJ, Lim C, Lindner T, Linn Y, Liu S, Majewski P, Mathew R, McDonald AB, McElroy T, McGinn T, McLaughlin JB, Mead S, Mehdiyev R, Mielnichuk C, Monroe J, Muir A, Nadeau P, Nantais C, Ng C, Noble AJ, O'Dwyer E, Ohlmann C, Olchanski K, Olsen KS, Ouellet C, Pasuthip P, Peeters SJM, Pollmann TR, Rand ET, Rau W, Rethmeier C, Retière F, Seeburn N, Shaw B, Singhrao K, Skensved P, Smith B, Smith NJT, Sonley T, Soukup J, Stainforth R, Stone C, Strickland V, Sur B, Tang J, Taylor J, Veloce L, Vázquez-Jáuregui E, Walding J, Ward M, Westerdale S, Woolsey E, and Zielinski J

Abstract

This Letter reports the first results of a direct dark matter search with the DEAP-3600 single-phase liquid argon (LAr) detector. The experiment was performed 2 km underground at SNOLAB (Sudbury, Canada) utilizing a large target mass, with the LAr target contained in a spherical acrylic vessel of 3600 kg capacity. The LAr is viewed by an array of PMTs, which would register scintillation light produced by rare nuclear recoil signals induced by dark matter particle scattering. An analysis of 4.44 live days (fiducial exposure of 9.87 ton day) of data taken during the initial filling phase demonstrates the best electronic recoil rejection using pulse-shape discrimination in argon, with leakage <1.2×10^{-7} (90% C.L.) between 15 and 31  keV&#95;{ee}. No candidate signal events are observed, which results in the leading limit on weakly interacting massive particle (WIMP)-nucleon spin-independent cross section on argon, <1.2×10^{-44}  cm^{2} for a 100  GeV/c^{2} WIMP mass (90% C.L.).

Published
2018
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