D. Reyna
Sandia National Laboratories
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Featured researches published by D. Reyna.
Physical Review Letters | 2011
P. S. Barbeau; N. S. Bowden; B. Cabrera-Palmer; J. Colaresi; J. I. Collar; S. Dazeley; P. De Lurgio; J. E. Fast; N. Fields; C. Greenberg; Todd W. Hossbach; Martin E. Keillor; Jeremy D. Kephart; M. G. Marino; Harry S. Miley; M. L. Miller; John L. Orrell; D. C. Radford; D. Reyna; O. Tench; T.D. Van Wechel; J. F. Wilkerson; K. M. Yocum
We report on several features in the energy spectrum from an ultralow-noise germanium detector operated deep underground. By implementing a new technique able to reject surface events, a number of cosmogenic peaks can be observed for the first time. We discuss an irreducible excess of bulklike events below 3 keV in ionization energy. These could be caused by unknown backgrounds, but also dark matter interactions consistent with DAMA/LIBRA. It is not yet possible to determine their origin. Improved constraints are placed on a cosmological origin for the DAMA/LIBRA effect.
Physical Review Letters | 2008
P. S. Barbeau; D. G. Cerdeno; J. Colaresi; J. I. Collar; P. De Lurgio; Gary Drake; J. E. Fast; C. Greenberg; Todd W. Hossbach; Jeremy D. Kephart; M. G. Marino; Harry S. Miley; John L. Orrell; D. Reyna; R. G. H. Robertson; R. L. Talaga; O. Tench; T.D. Van Wechel; J. F. Wilkerson; K. M. Yocum
A claim for evidence of dark matter interactions in the DAMA experiment has been recently reinforced. We employ a new type of germanium detector to conclusively rule out a standard isothermal galactic halo of weakly interacting massive particles as the explanation for the annual modulation effect leading to the claim. Bounds are similarly imposed on a suggestion that dark pseudoscalars might lead to the effect. We describe the sensitivity to light dark matter particles achievable with our device, in particular, to next-to-minimal supersymmetric model candidates.
Science | 2017
D. Akimov; J. B. Albert; P. An; C. Awe; P.S. Barbeau; B. Becker; V. Belov; A. Brown; A. Bolozdynya; B. Cabrera-Palmer; M. Cervantes; J. I. Collar; R. J. Cooper; R.L. Cooper; C. Cuesta; D.J. Dean; J. A. Detwiler; A. Eberhardt; Y. V. Efremenko; S. R. Elliott; E. M. Erkela; L. Fabris; M. Febbraro; N. Fields; W. Fox; Z. Fu; A. Galindo-Uribarri; M. P. Green; M. Hai; M.R. Heath
A 14.6-kilogram sodium-doped CsI scintillator is used to detect a neutrino scattering process with a 6.7σ confidence level. Nailing down an elusive process Detecting neutrinos—elementary particles that barely interact with other matter—usually requires detectors of enormous size. A particular interaction of neutrinos with atomic nuclei, called the coherent elastic neutrino-nucleus scattering (CEνNS), is predicted to occur with relatively high probability, and it could be used to drastically reduce the size of neutrino detectors. However, observing this interaction requires a source of low-energy neutrinos and detectors that contain nuclei of optimal mass. Akimov et al. observed CEνNS with a 6.7σ confidence by using a comparatively tiny, 14.6-kg sodium-doped CsI scintillator exposed to neutrinos from a spallation neutron facility (see the Perspective by Link). The discovery places tighter bounds on exotic, beyond-the-standard-model interactions involving neutrinos. Science, this issue p. 1123; see also p. 1098 The coherent elastic scattering of neutrinos off nuclei has eluded detection for four decades, even though its predicted cross section is by far the largest of all low-energy neutrino couplings. This mode of interaction offers new opportunities to study neutrino properties and leads to a miniaturization of detector size, with potential technological applications. We observed this process at a 6.7σ confidence level, using a low-background, 14.6-kilogram CsI[Na] scintillator exposed to the neutrino emissions from the Spallation Neutron Source at Oak Ridge National Laboratory. Characteristic signatures in energy and time, predicted by the standard model for this process, were observed in high signal-to-background conditions. Improved constraints on nonstandard neutrino interactions with quarks are derived from this initial data set.
arXiv: Instrumentation and Detectors | 2015
D. Akimov; A. Sosnovchev; J. I. Collar; S. Penttila; S. Suchyta; W. Lu; M. P. Green; P. An; R. Tayloe; R.T. Thornton; D. Rudik; A. Melikyan; N. Fields; L. J. Kaufman; A. Khromov; W.M. Snow; A. V. Kumpan; P. Naumov; B. Suh; A. Konovalev; K. Miller; N. Herman; A. Burenkov; B. Cabrera-Palmer; J. Newby; B. Becker; S. Hedges; A. Bolozdynya; A. Tolstukhin; K. Vetter
The COHERENT collaborations primary objective is to measure coherent elastic neutrino-nucleus scattering (CEvNS) using the unique, high-quality source of tens-of-MeV neutrinos provided by the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory (ORNL). In spite of its large cross section, the CEvNS process has never been observed, due to tiny energies of the resulting nuclear recoils which are out of reach for standard neutrino detectors. The measurement of CEvNS has now become feasible, thanks to the development of ultra-sensitive technology for rare decay and weakly-interacting massive particle (dark matter) searches. The CEvNS cross section is cleanly predicted in the standard model; hence its measurement provides a standard model test. It is relevant for supernova physics and supernova-neutrino detection, and enables validation of dark-matter detector background and detector-response models. In the long term, precision measurement of CEvNS will address questions of nuclear structure. COHERENT will deploy multiple detector technologies in a phased approach: a 14-kg CsI[Na] scintillating crystal, 15 kg of p-type point-contact germanium detectors, and 100 kg of liquid xenon in a two-phase time projection chamber. Following an extensive background measurement campaign, a location in the SNS basement has proven to be neutron-quiet and suitable for deployment of the COHERENT detector suite. The simultaneous deployment of the three COHERENT detector subsystems will test the
Journal of Physics: Conference Series | 2017
D. Akimov; J. B. Albert; C. Awe; P.S. Barbeau; B. Becker; V. Belov; A. Bolozdynya; A Burenkov; B. Cabrera-Palmer; M. Cervantes; J. I. Collar; R. J. Cooper; R.L. Cooper; C. Cuesta; D.J. Dean; M. del Valle Coello; J. A. Detwiler; A G Dolgolenko; M D’Onofrio; A. Eberhardt; Y. V. Efremenko; S. R. Elliott; A. Etenko; Lorenzo Fabris; N. Fields; W. Fox; A Galindo-Uribarri; M. P. Green; M.R. Heath; S. Hedges
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arXiv: High Energy Physics - Experiment | 2013
D. Akimov; A. Bernstein; BarbeauP.; P. J. Barton; A. Bolozdynya; B. Cabrera-Palmer; F. Cavanna; V. Cianciolo; J. I. Collar; R. J. Cooper; D.J. Dean; Yuri Efremenko; A. Etenko; N. Fields; M. Foxe; Enectali Figueroa-Feliciano; N. Fomin; F. Gallmeier; I. Garishvili; M. Gerling; M. P. Green; G. Greene; A. Hatzikoutelis; R. Henning; R. Hix; D. Hogan; D. Hornback; I. Jovanovic; T.W. Hossbach; Erik B Iverson
dependence of the cross section and ensure an unambiguous discovery of CEvNS. This document describes concisely the COHERENT physics motivations, sensitivity and plans for measurements at the SNS to be accomplished on a four-year timescale.
Physical Review Letters | 2009
P. S. Barbeau; D. G. Cerdeno; J. Colaresi; J. I. Collar; P. De Lurgio; G. Drake; Jim Fast; C. Greenberg; T.W. Hossbach; Jeremy D. Kephart; M. G. Marino; Harry S. Miley; John L. Orrell; D. Reyna; R. G. H. Robertson; R. L. Talaga; O. Tench; T.D. Van Wechel; J. F. Wilkerson; K. M. Yocum
The COHERENT Collaboration is realizing a long term neutrino physics research program. The main goals of the program are to detect and study elastic neutrino-nucleus scattering (CEνNS). This process is predicted by Standard Model but it has never been observed experimentally because of the very low energy of the recoil nucleus. COHERENT is using different detector technologies: CsI[Na] and NaI scintillator crystals, a single-phase liquid Ar and a Ge detectors. The placement of all the detector setups is in the basement of the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory (ORNL). The current status of the COHERENT experimental program is presented.
arXiv: Nuclear Experiment | 2018
D. Akimov; J. I. Collar; J. Daughhetee; R. L. Varner; A. Khromov; J. Yoo; J. Newby; A. Galindo-Uribarri; D. Reyna; M. Kaemingk; S. R. Klein; C. Cuesta; H. Ray; E.B. Iverson; M. Kremer; H. Moreno; M. Hai; P. An; John L. Orrell; M. Cervantes; C. Awe; Cory T. Overman; D.J. Salvat; W. Lu; D. Rudik; M. Febbraro; G. Sinev; B. Suh; S. Ki; G. Perumpilly
arXiv: Instrumentation and Detectors | 2018
D. Akimov; J. I. Collar; S. Hedges; S. Penttila; D.J. Salvat; W. Lu; J. Newby; J. Daughhetee; P. An; R. Tayloe; R.T. Thornton; D. Rudik; V. Sosnovtsev; M. Febbraro; N. Fields; A. Khromov; Lorenzo Fabris; J. Yoo; A. V. Kumpan; P. Naumov; B. Suh; S. Ki; L. J. Kaufman; B. Scholz; G. Perumpilly; W.M. Snow; A. Burenkov; B. Cabrera-Palmer; E.B. Iverson; B. Becker
Bulletin of the American Physical Society | 2008
J. I. Collar; P. S. Barbeau; A. Bernstein; N. S. Bowden; J. Colaresi; S. Dazeley; P. De Lurgio; G. Drake; Jim Fast; C. Greenberg; T.W. Hossbach; Jeremy D. Kephart; J. Lund; M. G. Marino; Harry S. Miley; John L. Orrell; D. Reyna; R. G. H. Robertson; L. Sadler; R. L. Talaga; O. Tench; T.D. Van Wechel; J. F. Wilkerson; M. Yocum