N. Fields
University of Chicago
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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 D | 2013
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
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
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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
-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 (
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015
J. I. Collar; N. Fields; M. Hai; T.W. Hossbach; John L. Orrell; Cory T. Overman; G. Perumpilly; B. Scholz
{m}_{\ensuremath{\chi}}\ensuremath{\sim}10\text{ }\text{ }\mathrm{GeV}/{c}^{2}
arXiv: Nuclear Experiment | 2009
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
). 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: 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
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.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2013
Ricco Bonicalzi; J. I. Collar; J. Colaresi; J. E. Fast; N. Fields; Erin S. Fuller; M. Hai; Todd W. Hossbach; Marek S. Kos; John L. Orrell; Cory T. Overman; Douglas J. Reid; Brent A. VanDevender; Clinton G. Wiseman; K. M. Yocum
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.
12th International Conference on Topics in Astroparticle and Underground Physics, TAUP 2011 | 2012
G K Giovanetti; E. Aguayo; F. T. Avignone; H. O. Back; A. S. Barabash; James R. Beene; M. Bergevin; F. E. Bertrand; M. 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; M. P. Green; V. E. Guiseppe
We study the possibility of using CsI[Na] scintillators as an advantageous target for the detection of coherent elastic neutrino-nucleus scattering (CENNS), using the neutrino emissions from the SNS spallation source at Oak Ridge National Laboratory. The response of this material to low-energy nuclear recoils like those expected from this process is characterized. Backgrounds are studied using a 2 kg low-background prototype crystal in a dedicated radiation shield. The conclusion is that a planned 14 kg detector should measure approximately 550 CENNS events per year above a demonstrated ~7keVnr low-energy threshold, with a signal-to-background ratio sufficient for a first measurement of the CENNS cross-section. The cross-section for the Pb208(νe,e−)Bi208 reaction, of interest for future supernova neutrino detection, can be simultaneously obtained.
arXiv: Nuclear Experiment | 2014
P. Finnerty; E. Aguayo; Mark Amman; F. T. Avignone; A. S. Barabash; Paul Barton; James R. Beene; F. E. Bertrand; M. 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; F. M. Fraenkle; A. Galindo-Uribarri; V. M. Gehman; G. K. Giovanetti; M. P. Green
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.