B. Beltran
University of Alberta
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Featured researches published by B. Beltran.
Physics Letters B | 2009
S. Archambault; F. Aubin; M. Auger; E. Behnke; B. Beltran; K. Clark; X. Dai; A. Davour; J. Farine; R. Faust; M.-H. Genest; G. Giroux; R. Gornea; C. Krauss; S. Kumaratunga; I. Lawson; C. Leroy; L. Lessard; C. Levy; I. Levine; R. MacDonald; J. P. Martin; P. Nadeau; A.J. Noble; M.-C. Piro; S. Pospisil; T. Shepherd; N. Starinski; I. Stekl; C. Storey
The PICASSO experiment at SNOLAB uses super?heated C4F10 droplets suspended in a gel as a target sensitive to WIMP?proton spin?dependent elastic scattering. The phase II setup has been improved substantially in sensitivity by using an array of 32 detectors with an active mass of ~65 g each and largely reduced background. First results are presented for a subset of two detectors with target masses of 19F of 65 g and 69 g respectively and a total exposure of 13.75 ? 0.48 kgd. No dark matter signal was found and for WIMP masses around 24 GeV/c2 new limits have been obtained on the spin?dependent cross section on 19F of ?F = 13.9 pb (90% C.L.) which can be converted into cross section limits on protons and neutrons of ?p = 0.15 pb and ?n = 2.45 pb respectively (90% C.L). The obtained limits on protons restrict recent interpretations of the DAMA/LIBRA annual modulations in terms of spin-dependent interactions.
Astroparticle Physics | 2016
P.-A. Amaudruz; M. Batygov; B. Beltran; J. Bonatt; K. Boudjemline; M.G. Boulay; B. Broerman; J.F. Bueno; A. Butcher; B. Cai; T. Caldwell; M. Chen; R. Chouinard; B.T. Cleveland; D. Cranshaw; K. Dering; F. Duncan; N. Fatemighomi; R. Ford; R. Gagnon; P. Giampa; F. Giuliani; M. Gold; V.V. Golovko; P. Gorel; E. Grace; K. Graham; D. Grant; R. Hakobyan; A. L. Hallin
The DEAP-1 low-background liquid argon detector was used to measure scintillation pulse shapes of electron and nuclear recoil events and to demonstrate the feasibility of pulse-shape discrimination (PSD) down to an electron-equivalent energy of 20 keV. In the surface dataset using a triple-coincidence tag we found the fraction of beta events that are misidentified as nuclear recoils to be <1.4×10 −7 (90% C.L.) for energies between 43-86 keVee and for a nuclear recoil acceptance of at least 90%, with 4% systematic uncertainty on the absolute energy scale. The discrimination measurement on surface was limited by nuclear recoils induced by cosmic-ray generated neutrons. This was improved by moving the detector to the SNOLAB underground laboratory, where the reduced background rate allowed the same measurement with only a double-coincidence tag. The combined data set contains 1.23×10 8 events. One of those, in the underground data set, is in the nuclear-recoil region of interest. Taking into account the expected background of 0.48 events coming from random pileup, the resulting upper limit on the electronic recoil contamination is <2.7×10 −8 (90% C.L.) between 44-89 keVee and for a nuclear recoil acceptance of at least 90%, with 6% systematic uncertainty on the absolute energy scale. We developed a general mathematical framework to describe PSD parameter distributions and used it to build an analytical model of the distributions observed in DEAP-1. Using this model, we project a misidentification fraction of approx. 10 −10 for an electron-equivalent energy threshold of 15 keV for a detector with 8 PE/keVee light yield. This reduction enables a search for spin-independent scattering of WIMPs from 1000 kg of liquid argon with a WIMP-nucleon cross-section sensitivity of 10 −46 cm 2 , assuming negligible contribution from nuclear recoil backgrounds.
Nuclear and Particle Physics Proceedings | 2016
M. Kuźniak; P.-A. Amaudruz; M. Batygov; B. Beltran; J. Bonatt; M.G. Boulay; B. Broerman; J.F. Bueno; A. Butcher; B. Cai; M. Chen; R. Chouinard; B.T. Cleveland; K. Dering; J. DiGioseffo; F. Duncan; T. Flower; R. Ford; P. Giampa; P. Gorel; K. Graham; D. Grant; E. Guliyev; A. L. Hallin; M. Hamstra; P.J. Harvey; C.J. Jillings; I. Lawson; O. Li; P. Liimatainen
The DEAP-3600 experiment is located 2 km underground at SNOLAB, in Sudbury, Ontario. It is a single-phase detector that searches for dark matter particle interactions within a 1000-kg fiducial mass target of liquid argon. A first generation prototype detector (DEAP-1) with a 7-kg liquid argon target mass demonstrated a high level of pulse-shape discrimination (PSD) for reducing / backgrounds and helped to develop low radioactivity techniques to mitigate surface-related backgrounds. Construction of the DEAP-3600 detector is nearly complete and commissioning is starting in 2014. The target sensitivity to spin-independent scattering of Weakly Interacting Massive Particles (WIMPs) on nucleons of 10 46 cm 2 will allow one order of magnitude improvement in sensitivity over current searches at 100 GeV WIMP mass. This paper presents an overview and status of the DEAP-3600 project and discusses plans for a future multi-tonne experiment, DEAP-50T.
New Journal of Physics | 2011
S Archambault; F. Aubin; M. Auger; M Beleshi; E. Behnke; J Behnke; B. Beltran; K. Clark; X. Dai; M Das; A. Davour; F. Debris; J. Farine; M-H Genest; G. Giroux; R. Gornea; R. Faust; H Hinnefeld; A. Kamaha; C. Krauss; M. Lafrenière; M. Laurin; I Lawson; Claude Leroy; C. Levy; L. Lessard; I. Levine; J.-P. Martin; S. Kumaratunga; R. MacDonald
We report new results obtained from calibrations of superheated liquid droplet detectors used in dark matter searches with different radiation sources (n, α, γ). In particular, detectors were spiked with α-emitters located inside and outside the droplets. It is shown that the responses have different temperature thresholds, depending on whether α-particles or recoil nuclei create the signals. The measured temperature threshold for recoiling 210Pb nuclei from 214Po α-decays was found to be in agreement with test beam measurements using mono-energetic neutrons. A comparison of the threshold data with theoretical predictions shows deviations, especially at high temperatures. It is shown that signals produced simultaneously by recoil nuclei and α-particles have more acoustic energy than signals produced by one or the other separately. A model is presented that describes how the observed intensities of particle-induced acoustic signals can be related to the dynamics of bubble growth in superheated liquids. A growth scenario that is limited by the inertia of the surrounding liquid shows a trend that is supported by the data. An improved understanding of the bubble dynamics is an important first step in obtaining better discrimination between particle types interacting in detectors of this kind.
Astroparticle Physics | 2015
M. Akashi-Ronquest; P.-A. Amaudruz; M. Batygov; B. Beltran; M. Bodmer; M.G. Boulay; B. Broerman; B. Buck; A. Butcher; B. Cai; T. Caldwell; M. Chen; Y. Chen; B.T. Cleveland; Kevin J. Coakley; K. Dering; F. Duncan; Joseph A. Formaggio; R. Gagnon; Daniel Gastler; F. Giuliani; M. Gold; V.V. Golovko; P. Gorel; K. Graham; E. Grace; N. Guerrero; V. Guiseppe; A. L. Hallin; P.J. Harvey
Many current and future dark matter and neutrino detectors are designed to measure scintillation light with a large array of photomultiplier tubes (PMTs). The energy resolution and particle identification capabilities of these detectors depend in part on the ability to accurately identify individual photoelectrons in PMT waveforms despite large variability in pulse amplitudes and pulse pileup. We describe a Bayesian technique that can identify the times of individual photoelectrons in a sampled PMT waveform without deconvolution, even when pileup is present. To demonstrate the technique, we apply it to the general problem of particle identification in single-phase liquid argon dark matter detectors. Using the output of the Bayesian photoelectron counting algorithm described in this paper, we construct several test statistics for rejection of backgrounds for dark matter searches in argon. Compared to simpler methods based on either observed charge or peak finding, the photoelectron counting technique improves both energy resolution and particle identification of low energy events in calibration data from the DEAP-1 detector and simulation of the larger MiniCLEAN dark matter detector.
New Journal of Physics | 2011
B. Beltran; H Bichsel; B. Cai; G. A. Cox; H. Deng; J. Detwiler; J. Formaggio; S. Habib; A. L. Hallin; A. Hime; M. Huang; C. Kraus; H R Leslie; J.C. Loach; R. Martin; S. McGee; M. L. Miller; B. Monreal; J. Monroe; N.S. Oblath; S.J.M. Peeters; A.W.P. Poon; G. Prior; K. Rielage; R. G. H. Robertson; M W E Smith; L.C. Stonehill; N. Tolich; T.D. Van Wechel; H. Wan Chan Tseung
The third phase of the Sudbury Neutrino Observatory (SNO) experiment added an array of 3He proportional counters to the detector. The purpose of this neutral-current detection (NCD) array was to observe neutrons resulting from neutral-current solar-neutrino–deuteron interactions. We have developed a detailed simulation of current pulses from NCD array proportional counters, from the primary neutron capture on 3He through NCD array signal-processing electronics. This NCD array MC simulation was used to model the alpha-decay background in SNOs third-phase 8B solar-neutrino measurement.
Workshop on Calculation of Double-Beta-Decay Matrix Elements, MEDEX '09 | 2009
S. Archambault; F. Aubin; M. Auger; E. Behnke; B. Beltran; B. Biskup; K. Clark; X. Dai; A. Davour; J. Farine; M.-H. Genest; G. Giroux; R. Gornea; R. Faust; C. Krauss; I. Lawson; C. Leroy; C. Levy; L. Lessard; I. Levine; J. P. Martin; S. Kumaratunga; R. MacDonald; P. Nadeau; A.J. Noble; M.-C. Piro; S. Pospisil; T. Shepherd; J. Sodomka; N. Starinski
The PICASSO experiment searches WIMPs via their spin‐dependent interactions with nuclei. At their operating temperatures, PICASSO threshold detectors are not sensitive to γ‐rays, while it is necessary to suppress neutron and α‐ray backgrounds. The different types of neutron shielding (water, polyethylene, borated water and polyethylene doped with different compounds of boron and lithium) were studied via the Monte Carlo method using MCNPX code. Efficiencies of these different types of neutron shielding were compared from the point of view of neutron suppression as well as number of newly born y‐rays. The neutrons and γ‐rays were followed up to the PICASSO detector active material. The most suitable neutron shielding for the PICASSO experiment was determined following these simulations.
Journal of Physics: Conference Series | 2008
B. Beltran; J. Monroe; N.S. Oblath; G. Prior; K. Rielage; R. G. H. Robertson; H. Wan Chan Tseung
In the third phase of the Sudbury Neutrino Observatory (SNO) experiment an array of 3He proportional counters was added deployed in the heavy-water volume of the SNO detector. This Neutral-Current Detection (NCD) Array detected the neutrons from the neutral-current interaction of 8B solar neutrinos with deuterium. Before we can determine the neutrino flux we must separate the neutron-capture pulses from pulses due to alpha particles and instrumental backgrounds. We have created a unique, detailed simulation of the current pulses from the proportional counters that includes energy straggling, ion drift, electron diffusion, space charge, and electronics effects. We have conducted extensive studies to determine the accuracy of the simulation. In the solar neutrino analysis the NCD Monte Carlo is used to determine the energy spectrum of the alpha background, as well as the applicable systematic effects. In the near future it will be used to fit the data pulses to separate neutron-capture and alpha pulses. With this pulse-shape analysis method the differences between pulse characteristics can be associated directly with the physical mechanisms of track formation and charge motion in the counter gas.
Astroparticle Physics | 2015
P.-A. Amaudruz; M. Batygov; B. Beltran; K. Boudjemline; M.G. Boulay; B. Cai; T. Caldwell; M. Chen; R. Chouinard; B.T. Cleveland; D. Contreras; K. Dering; F. Duncan; R. Ford; R. Gagnon; F. Giuliani; M. Gold; V.V. Golovko; P. Gorel; K. Graham; D. Grant; R. Hakobyan; A. L. Hallin; P.J. Harvey; C. Hearns; C.J. Jillings; M. Kuźniak; I.T. Lawson; O. Li; J. Lidgard