M. P. Green
Oak Ridge National Laboratory
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Featured researches published by M. P. Green.
Advances in High Energy Physics | 2014
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 | 2008
D.S. Leonard; P. Grinberg; P. Weber; E. Baussan; Z. Djurcic; G. Keefer; A. Piepke; A. Pocar; J.-L. Vuilleumier; J.-M. Vuilleumier; D. Akimov; A. Bellerive; M. Bowcock; M. Breidenbach; A. Burenkov; R. Conley; W. Craddock; M. Danilov; R. DeVoe; M. S. Dixit; A. Dolgolenko; I. Ekchtout; W. Fairbank; J. Farine; P. Fierlinger; B. Flatt; G. Gratta; M. P. Green; C. Hall; K. Hall
The Enriched Xenon Observatory (EXO) will search for double beta decays of 136Xe. We report the results of a systematic study of trace concentrations of radioactive impurities in a wide range of raw materials and finished parts considered for use in the construction of EXO-200, the first stage of the EXO experimental program. Analysis techniques employed, and described here, include direct gamma counting, alpha counting, neutron activation analysis, and high-sensitivity mass spectrometry.
Journal of Environmental Radioactivity | 2012
S. MacMullin; G. K. Giovanetti; M. P. Green; R. Henning; R. Holmes; K. Vorren; J. F. Wilkerson
We present measurement results of airborne fission products in Chapel Hill, NC, USA, from 62 d following the March 11, 2011, accident at the Fukushima Dai-ichi nuclear power plant. Airborne particle samples were collected daily in air filters and radio-assayed with two high-purity germanium (HPGe) detectors. The fission products (131)I and (137)Cs were measured with maximum activity concentrations of 4.2 ± 0.6 mBq/m(3) and 0.42 ± 0.07 mBq/m(3) respectively. Additional activity from (131,132)I, (134,136,137)Cs and (132)Te were measured in the same air filters using a low-background HPGe detector at the Kimballton Underground Research Facility (KURF).
arXiv: Nuclear Experiment | 2012
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.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016
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.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009
R. Neilson; F. LePort; A. Pocar; K.S. Kumar; A. Odian; C.Y. Prescott; V. Tenev; Nicole Ackerman; D. Akimov; M. Auger; C. Benitez-Medina; M. Breidenbach; A. Burenkov; R. Conley; S. Cook; R. DeVoe; M. J. Dolinski; W. Fairbank; J. Farine; P. Fierlinger; B. Flatt; R. Gornea; G. Gratta; M. P. Green; C. Hall; K. Hall; D. Hallman; C. Hargrove; S. Herrin; J. Hodgson
EXO-200 uses 468 large area avalanche photodiodes (LAAPDs) for detection of scintillation light in an ultra-lowbackground liquid xenon (LXe) detector. We describe initial measurements of dark noise, gain and response to xenon scintillation light of LAAPDs at temperatures from room temperature to 169 K—the temperature of liquid xenon. We also describe the individual characterization of more than 800 LAAPDs for selective installation in the EXO-200 detector.
arXiv: Instrumentation and Detectors | 2017
N. Abgrall; A. Abramov; N. Abrosimov; I. Abt; M. Agostini; M. Agartioglu; A. Ajjaq; S. I. Alvis; F. T. Avignone; X. Bai; M. Balata; I. Barabanov; A. S. Barabash; P. J. Barton; L. Baudis; L. Bezrukov; T. Bode; A. Bolozdynya; D. Borowicz; A. J. Boston; H. Boston; S. T.P. Boyd; R. Breier; V. Brudanin; R. Brugnera; M. Busch; M. Buuck; A. Caldwell; T. S. Caldwell; T. Camellato
The observation of neutrinoless double-beta decay (0νββ) would show that lepton number is violated, reveal that neu-trinos are Majorana particles, and provide information on neutrino mass. A discovery-capable experiment covering the inverted ordering region, with effective Majorana neutrino masses of 15 - 50 meV, will require a tonne-scale experiment with excellent energy resolution and extremely low backgrounds, at the level of ∼0.1 count /(FWHM·t·yr) in the region of the signal. The current generation 76Ge experiments GERDA and the Majorana Demonstrator, utilizing high purity Germanium detectors with an intrinsic energy resolution of 0.12%, have achieved the lowest backgrounds by over an order of magnitude in the 0νββ signal region of all 0νββ experiments. Building on this success, the LEGEND collaboration has been formed to pursue a tonne-scale 76Ge experiment. The collaboration aims to develop a phased 0νββ experimental program with discovery potential at a half-life approaching or at 1028 years, using existing resources as appropriate to expedite physics results.
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
Physical Review A | 2007
M. P. Green; J. Wodin; R. DeVoe; P. Fierlinger; B. Flatt; G. Gratta; F. LePort; M. Montero Díez; R. Neilson; K. O'Sullivan; A. Pocar; S. Waldman; D.S. Leonard; A. Piepke; U Alabama; C. Hargrove; D. Sinclair; V. Strickland; U Carleton; W. Fairbank; K. Hall; B. Mong; M. K. Moe; U Laurentian; U Neuchatel
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Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2011
A. Dobi; C. Hall; S. Herrin; A. Odian; C.Y. Prescott; P.C. Rowson; Nicole Ackerman; B. Aharmin; M. Auger; P.S. Barbeau; K. Barry; C. Benitez-Medina; M. Breidenbach; S. Cook; I. Counts; T. Daniels; R. DeVoe; M. J. Dolinski; K. Donato; W. Fairbank; J. Farine; G. Giroux; R. Gornea; K. Graham; G. Gratta; M. P. Green; C. Hagemann; K. Hall; D. Hallman; C. Hargrove
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.