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Featured researches published by R. L. Varner.


Advances in High Energy Physics | 2014

The MAJORANA DEMONSTRATOR Neutrinoless Double-Beta Decay Experiment

N. Abgrall; E. Aguayo; Frank T. Avignone; A. S. Barabash; F. E. Bertrand; Melissa Boswell; V. Brudanin; M. Busch; A. S. Caldwell; Y.D. Chan; C. D. Christofferson; D. C. Combs; J. A. Detwiler; P. J. Doe; Y. V. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; J. Esterline; J. E. Fast; P. Finnerty; F. M. Fraenkle; A. Galindo-Uribarri; G. K. Giovanetti; J. Goett; M. P. Green; J. Gruszko; V. E. Guiseppe; K. Gusev; A. L. Hallin

The MAJORANA DEMONSTRATOR will search for the neutrinoless double-beta decay of the isotope Ge with a mixed array of enriched and natural germanium detectors. The observation of this rare decay would indicate that the neutrino is its own antiparticle, demonstrate that lepton number is not conserved, and provide information on the absolute mass scale of the neutrino. The DEMONSTRATOR is being assembled at the 4850-foot level of the Sanford Underground Research Facility in Lead, South Dakota. The array will be situated in a low-background environment and surrounded by passive and active shielding. Here we describe the science goals of the DEMONSTRATOR and the details of its design.


Science | 2017

Observation of coherent elastic neutrino-nucleus scattering

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.


Journal of Physics G | 2016

The PROSPECT Physics Program

J. Ashenfelter; A. B. Balantekin; H. R. Band; G. Barclay; C. D. Bass; D. Berish; L. J. Bignell; N. S. Bowden; A. Bowes; J. P. Brodsky; C. D. Bryan; J. J. Cherwinka; R. Chu; T. Classen; K. Commeford; A. Conant; D. Davee; D. J. Dean; G. Deichert; M. V. Diwan; M. J. Dolinski; J. Dolph; M. Duvernois; Anna Erickson; M. T. Febbraro; J. K. Gaison; A. Galindo-Uribarri; K. Gilje; A. Glenn; B. W. Goddard

The Precision Reactor Oscillation and Spectrum Experiment, PROSPECT, is designed to make a precise measurement of the antineutrino spectrum from a highly-enriched uranium reactor and probe eV-scale sterile neutrinos by searching for neutrino oscillations over meter-long distances. PROSPECT is conceived as a 2-phase experiment utilizing segmented


arXiv: Nuclear Experiment | 2012

The MAJORANA demonstrator: A search for neutrinoless double-beta decay of germanium-76

J. F. Wilkerson; E. Aguayo; Frank T. Avignone; H. O. Back; A. S. Barabash; James R. Beene; M. Bergevin; F. E. Bertrand; Melissa Boswell; V. Brudanin; M. Busch; Y.D. Chan; C. D. Christofferson; J. I. Collar; D. C. Combs; R. J. Cooper; J. A. Detwiler; P. J. Doe; Yu. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; J. Esterline; J. E. Fast; N. Fields; P. Finnerty; F. M. Fraenkle; V. M. Gehman; G K Giovanetti; M. P. Green

^6


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016

The Majorana Demonstrator radioassay program

N. Abgrall; I. J. Arnquist; F. T. Avignone; H. O. Back; A. S. Barabash; F. E. Bertrand; Melissa Boswell; A. W. Bradley; V. Brudanin; M. Busch; M. Buuck; D. Byram; A. S. Caldwell; Y.D. Chan; C. D. Christofferson; Pinghan Chu; C. Cuesta; J. A. Detwiler; J. A. Dunmore; Yu. Efremenko; H. Ejiri; S. R. Elliott; P. Finnerty; A. Galindo-Uribarri; V. M. Gehman; T. Gilliss; G. K. Giovanetti; J. Goett; M. P. Green; J. Gruszko

Li-doped liquid scintillator detectors for both efficient detection of reactor antineutrinos through the inverse beta decay reaction and excellent background discrimination. PROSPECT Phase I consists of a movable 3-ton antineutrino detector at distances of 7 - 12 m from the reactor core. It will probe the best-fit point of the


Physical Review C | 2007

Fusion of radioactive Sn-132 with Ni-64

J. F. Liang; D. Shapira; J.R. Beene; C. J. Gross; R. L. Varner; A. Galindo-Uribarri; J. Gomez del Campo; Paul Hausladen; P. E. Mueller; D. W. Stracener; H. Amro; J. J. Kolata; J. D. Bierman; A. L. Caraley; K. L. Jones; Y. Larochelle; W. Loveland; D. Peterson

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Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2000

Study of resonant reactions with radioactive ion beams

A. Galindo-Uribarri; J. Gomez del Campo; J.R. Beene; C. J. Gross; J. F. Liang; S.D. Paul; D. Shapira; D. W. Stracener; R. L. Varner; E. Chávez; A. Huerta; M.E. Ortiz; E. Padilla; S. Pascual

disappearance experiments at 4


Physics Letters B | 1996

Temperature dependence of the giant dipole resonance width in 208Pb

E. Ramakrishnan; A. Azhari; J.R. Beene; R. J. Charity; M. L. Halbert; P.-F. Hua; R.A. Kryger; P. E. Mueller; R. Pfaff; D. G. Sarantites; L. G. Sobotka; M. Thoennessen; G. Van Buren; R. L. Varner; S. Yokoyama

\sigma


Physics Letters B | 2003

Radiative fusion from very symmetric reactions: the giant dipole resonance in the 179Au nucleus

F. Camera; A. Bracco; V. Nanal; M. P. Carpenter; F. Della Vedova; S. Leoni; B. Million; S. Mantovani; M. Pignanelli; O. Wieland; B. B. Back; A. Heinz; R. V. F. Janssens; D Jenkins; T. L. Khoo; F. G. Kondev; T. Lauritsen; C. J. Lister; B. McClintock; S Mitsuoka; E. F. Moore; D. Seweryniak; R.H. Siemssen; R. van Swol; D. J. Hofman; M. Thoennessen; K Eisenman; P. Heckman; J Seitz; R. L. Varner

in 1 year and the favored region of the sterile neutrino parameter space at


Physical Review C | 2003

Low-lying E 1 strength in 20 O

E. Tryggestad; T. Baumann; P. Heckman; M. Thoennessen; T. Aumann; D. Bazin; Y. Blumenfeld; J.R. Beene; T. A. Lewis; D. C. Radford; D. Shapira; R. L. Varner; M. Chartier; M.L. Halbert; J. F. Liang

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A. Galindo-Uribarri

Oak Ridge National Laboratory

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J.R. Beene

Oak Ridge National Laboratory

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D. Shapira

Oak Ridge National Laboratory

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J. F. Liang

Oak Ridge Associated Universities

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C. J. Gross

Oak Ridge National Laboratory

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D. W. Stracener

Oak Ridge National Laboratory

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P. E. Mueller

Oak Ridge National Laboratory

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F. E. Bertrand

Oak Ridge National Laboratory

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