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Dive into the research topics where D. C. Radford is active.

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Featured researches published by D. C. Radford.


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.


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.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000

Performance of the Recoil Mass Spectrometer and its Detector Systems at the Holifield Radioactive Ion Beam Facility

C. J. Gross; Thomas Nelson Ginter; D. Shapira; W.T. Milner; J. W. McConnell; A.N. James; J.W. Johnson; J. F. Mas; P.F. Mantica; R.L. Auble; J.J. Das; J.L. Blankenship; Jonathan H. Hamilton; R.L. Robinson; Y.A. Akovali; C. Baktash; J. C. Batchelder; Carrol R Bingham; M.J. Brinkman; H.K. Carter; R.A. Cunningham; Thomas Davinson; J.D. Fox; A. Galindo-Uribarri; R. Grzywacz; J.F. Liang; B. D. MacDonald; Jim MacKenzie; S.D. Paul; A. Piechaczek

The recently commissioned Recoil Mass Spectrometer (RMS) at the Holifield Radioactive Ion Beam Facility (HRIBF) is described. Consisting of a momentum separator followed by an E-D-E Rochester-type mass spectrometer, the RMS is the centerpiece of the nuclear structure endstation at the HRIBF. Designed to transport ions with rigidities near K = 100, the RMS has acceptances of +/- 10% in energy and +/- 4.9% in mass-to-charge ratio. Recent experimental results are used to illustrate the detection capabilities of the RMS, which is compatible with many detectors and devices


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 observation of neutrinoless double-beta decay would determine whether the neutrino is a Majorana particle and provide information on the absolute scale of neutrino mass. The MAJORANA Collaboration is constructing the DEMONSTRATOR, an array of germanium detectors, to search for neutrinoless double-beta decay of 76-Ge. The DEMONSTRATOR will contain 40 kg of germanium; up to 30 kg will be enriched to 86% in 76-Ge. The DEMONSTRATOR will be deployed deep underground in an ultra-low-background shielded environment. Operation of the DEMONSTRATOR aims to determine whether a future tonne-scale germanium experiment can achieve a background goal of one count per tonne-year in a 4-keV region of interest around the 76-Ge neutrinoless double-beta decay Q-value of 2039 keV.


Physics of Atomic Nuclei | 2004

The Majorana neutrinoless double-beta decay experiment

Dale N. Anderson; R. Arthur; Frank T. Avignone; C. Baktash; T. Ball; A. S. Barabash; R. L. Brodzinski; V. Brudanin; W. Bugg; A.E. Champagne; Y.D. Chan; T.V. Cianciolo; J. I. Collar; R. W. Creswick; P. J. Doe; G. Dunham; S. Easterday; Yu. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; J. Ely; P. Fallon; Horacio A. Farach; R.J. Gaitskell; V. Gehman; R. Grzywacz; R. Hazma; H. Hime; T. Hossbach

The proposed Majorana double-beta decay experiment is based on an array of segmented intrinsic Ge detectors with a total mass of 500 kg of Ge isotopically enriched to 86% in 76Ge. A discussion is given of background reduction by material selection, detector segmentation, pulse shape analysis, and electroformation of copper parts and granularity. Predictions of the experimental sensitivity are given. For an experimental running time of 10 years over the construction and operation oft he Majorana setup, a sensitivity of T1/20ν∼4×1027 yr is predicted. This corresponds to 〈mν〉∼0.003−0.004 eV according to recent QRPA and RQRPA matrix element calculations.


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

Abstract The Majorana collaboration is constructing the Majorana Demonstrator at the Sanford Underground Research Facility at the Homestake gold mine, in Lead, SD. The apparatus will use Ge detectors, enriched in isotope 76 Ge, to demonstrate the feasibility of a large-scale Ge detector experiment to search for neutrinoless double beta decay. The long half-life of this postulated process requires that the apparatus be extremely low in radioactive isotopes whose decays may produce backgrounds to the search. The radioassay program conducted by the collaboration to ensure that the materials comprising the apparatus are sufficiently pure is described. The resulting measurements from gamma-ray counting, neutron activation and mass spectroscopy of the radioactive-isotope contamination for the materials studied for use in the detector are reported. We interpret these numbers in the context of the expected background for the experiment.


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

Building a Ovββ experiment with the ability to probe neutrino mass in the inverted hierarchy region requires the combination of a large detector mass sensitive to Ovββ, on the order of 1-tonne, and unprecedented background levels, on the order of or less than 1 count per year in the Ovβ β signal region. The MAJORANA Collaboration proposes a design based on using high-purity enriched 76Ge crystals deployed in ultralow background electroformed Cu cryostats and using modern analysis techniques that should be capable of reaching the required sensitivity while also being scalable to a 1-tonne size. To demonstrate feasibility, the collaboration plans to construct a prototype system, the MAJORANA DEMONSTRATOR, consisting of 30 kg of 86% enriched 76Ge detectors and 30 kg of natural or isotope-76-depleted Ge detectors. We plan to deploy and evaluate two different Ge detector technologies, one based on a p-type configuration and the other on n-type.


arXiv: Nuclear Experiment | 2009

The MAJORANA DEMONSTRATOR: An R&D project towards a tonne-scale germanium neutrinoless double-beta decay search

Mark Amman; J. F. Amsbaugh; Frank T. Avignone; H. O. Back; A. S. Barabash; P.S. Barbeau; James R. Beene; M. Bergevin; F. E. Bertrand; M. Boswell; V. Brudanin; W. Bugg; T. H. Burritt; Y.D. Chan; J. I. Collar; R. J. Cooper; Richard J. Creswick; J. A. Detwiler; P. J. Doe; Yu. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; James H. Ely; J. Esterline; Horacio A. Farach; J. E. Fast; N. Fields; P. Finnerty; B. K. Fujikawa

The MAJORANA collaboration is pursuing the development of the so‐called MAJORANA DEMONSTRATOR. The DEMONSTRATOR is intended to perform research and development towards a tonne‐scale germanium‐based experiment to search for the neutrinoless double‐beta decay of 76Ge. The DEMONSTRATOR can also perform a competitive direct dark matter search for light WIMPs in the 1–10 GeV/c2 mass range. It will consist of approximately 60 kg of germanium detectors in an ultra‐low background shield located deep underground at the Sanford Underground Laboratory in Lead, SD. The DEMONSTRATOR will also perform background and technology studies, and half of the detector mass will be enriched germanium. This talk will review the motivation, design, technology and status of the Demonstrator.


arXiv: Instrumentation and Detectors | 2015

The COHERENT Experiment at the Spallation Neutron Source

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


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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C. Baktash

Oak Ridge National Laboratory

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C. J. Gross

Oak Ridge Institute for Science and Education

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J.R. Beene

Oak Ridge National Laboratory

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S. R. Elliott

Los Alamos National Laboratory

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F. E. Bertrand

Oak Ridge National Laboratory

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J. A. Detwiler

University of Washington

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V. Brudanin

Joint Institute for Nuclear Research

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