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Dive into the research topics where John L. Orrell is active.

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Featured researches published by John L. Orrell.


Physical Review Letters | 2011

Results from a Search for Light-Mass Dark Matter with a p -Type Point Contact Germanium Detector

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 D | 2013

CoGeNT: A Search for Low-Mass Dark Matter using p-type Point Contact Germanium Detectors

K. M. Yocum; J. I. Collar; J. Colaresi; M. L. Miller; J. Diaz Leon; A. Knecht; J. E. Fast; M. G. Marino; P. S. Barbeau; Kos; John L. Orrell; Todd W. Hossbach; N. Fields; Harry S. Miley

CoGeNT employs


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

p


Physical Review Letters | 2008

Experimental constraints on a dark matter origin for the DAMA annual modulation effect

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

-type point-contact (PPC) germanium detectors to search for weakly interacting massive particles (WIMPs). By virtue of its low-energy threshold and ability to reject surface backgrounds, this type of device allows an emphasis on low-mass dark matter candidates (


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

{m}_{\ensuremath{\chi}}\ensuremath{\sim}10\text{ }\text{ }\mathrm{GeV}/{c}^{2}


Physical Review D | 2017

Projected sensitivity of the SuperCDMS SNOLAB experiment

R. Agnese; A. J. Anderson; T. Aramaki; I. J. Arnquist; W. Baker; D. Barker; R. Basu Thakur; D. A. Bauer; A. W. Borgland; M.A. Bowles; P. L. Brink; R. Bunker; B. Cabrera; David O. Caldwell; R. Calkins; C. Cartaro; D. G. Cerdeno; H. Chagani; Yan Chen; J. Cooley; B. Cornell; P. Cushman; M. Daal; P. Di Stefano; T. Doughty; L. Esteban; S. Fallows; E. Figueroa-Feliciano; M. Fritts; G. Gerbier

). We report on the characteristics of the PPC detector presently taking data at the Soudan Underground Laboratory, elaborating on aspects of shielding, data acquisition, instrumental stability, data analysis, and background estimation. A detailed background model is used to investigate the low-energy excess of events previously reported and to assess the possibility of temporal modulations in the low-energy event rate. Extensive simulations of all presently known backgrounds do not provide a viable background explanation for the excess of low-energy events in the CoGeNT data or the previously observed temporal variation in the event rate. Also reported for the first time is a determination of the surface (slow pulse rise time) event contamination in the data as a function of energy. We conclude that the CoGeNT detector technology is well suited to search for the annual modulation signature expected from dark matter particle interactions in the region of WIMP mass and coupling favored by the DAMA/LIBRA results.


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

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.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015

Coherent neutrino-nucleus scattering detection with a CsI[Na] scintillator at the SNS spallation source

J. I. Collar; N. Fields; M. Hai; T.W. Hossbach; John L. Orrell; Cory T. Overman; G. Perumpilly; B. Scholz

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.


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

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: Nuclear Experiment | 2006

The Majorana Project

S. R. Elliott; M. Akashi-Ronquest; Mark Amman; J. F. Amsbaugh; Frank T. Avignone; H. O. Back; C. Baktash; A. S. Barabash; P.S. Barbeau; J. R. Beene; M. Bergevin; F. E. Bertrand; M. Boswell; V. Brudanin; W. Bugg; T. H. Burritt; Y.D. Chan; T.V. Cianciolo; J. I. Collar; Richard J. Creswick; M. Cromaz; J. A. Detwiler; P. J. Doe; J. A. Dunmore; Yu. Efremenko; V. Egorov; H. Ejiri; James H. Ely; J. Esterline; Horacio A. Farach

SuperCDMS SNOLAB will be a next-generation experiment aimed at directly detecting low-mass particles (with masses ≤ 10 GeV/c^2) that may constitute dark matter by using cryogenic detectors of two types (HV and iZIP) and two target materials (germanium and silicon). The experiment is being designed with an initial sensitivity to nuclear recoil cross sections ∼ 1×10^(−43) cm^2 for a dark matter particle mass of 1 GeV/c^2, and with capacity to continue exploration to both smaller masses and better sensitivities. The phonon sensitivity of the HV detectors will be sufficient to detect nuclear recoils from sub-GeV dark matter. A detailed calibration of the detector response to low-energy recoils will be needed to optimize running conditions of the HV detectors and to interpret their data for dark matter searches. Low-activity shielding, and the depth of SNOLAB, will reduce most backgrounds, but cosmogenically produced ^3H and naturally occurring ^(32)Si will be present in the detectors at some level. Even if these backgrounds are 10 times higher than expected, the science reach of the HV detectors would be over 3 orders of magnitude beyond current results for a dark matter mass of 1 GeV/c^2. The iZIP detectors are relatively insensitive to variations in detector response and backgrounds, and will provide better sensitivity for dark matter particles with masses ≳ 5 GeV/c^2. The mix of detector types (HV and iZIP), and targets (germanium and silicon), planned for the experiment, as well as flexibility in how the detectors are operated, will allow us to maximize the low-mass reach, and understand the backgrounds that the experiment will encounter. Upgrades to the experiment, perhaps with a variety of ultra-low-background cryogenic detectors, will extend dark matter sensitivity down to the “neutrino floor,” where coherent scatters of solar neutrinos become a limiting background.

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F. E. Bertrand

Oak Ridge National Laboratory

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S. R. Elliott

Los Alamos National Laboratory

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V. Brudanin

Joint Institute for Nuclear Research

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J. A. Detwiler

University of Washington

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J. E. Fast

Pacific Northwest National Laboratory

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C. D. Christofferson

South Dakota School of Mines and Technology

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G. K. Giovanetti

University of North Carolina at Chapel Hill

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