P. J. Doe
University of Washington
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by P. J. Doe.
Modern Physics Letters A | 2002
Frank T. Avignone; A. S. Barabash; F. Boehm; R. L. Brodzinski; J. I. Collar; P. J. Doe; H. Ejiri; Stephen R. Elliott; E. Fiorini; R.J. Gaitskell; G. Gratta; R. Hazama; K. Kazkaz; G. S. King; Richard T. Kouzes; Harry S. Miley; M. Moe; A. Morales; J. Morales; A. Piepke; R. G. H. Robertson; W. Tornow; P. G. Vogel; Ray A. Warner; J. F. Wilkerson
We comment on the recent claim for the experimental observation of neutrinoless double-beta decay. We discuss several limitations in the analysis provided in that paper and conclude that there is no basis for the presented claim.
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 | 2007
J.F. Amsbaugh; Juan-Manuel Anaya; J. Banar; T. J. Bowles; M.C. Browne; T.V. Bullard; T.H. Burritt; G.A. Cox-Mobrand; X. Dai; H. Deng; M. Di Marco; P. J. Doe; M.R. Dragowsky; C.A. Duba; F.A. Duncan; E.D. Earle; S. R. Elliott; Ernst I. Esch; H. Fergani; J. Formaggio; M. M. Fowler; J.E. Franklin; P. Geissbühler; J.V. Germani; A. Goldschmidt; E. Guillian; A. L. Hallin; G. Harper; P.J. Harvey; R. Hazama
An array of Neutral-Current Detectors (NCDs) has been built in order to make a unique measurement of the total active ux of solar neutrinos in the Sudbury Neutrino Observatory (SNO). Data in the third phase of the SNO experiment were collected between November 2004 and November 2006, after the NCD array was added to improve the neutral-current sensitivity of the SNO detector. This array consisted of 36 strings of proportional counters lled with a mixture of 3He and CF4 gas capable of detecting the neutrons liberated by the neutrino-deuteron neutral current reaction in the D2O, and four strings lled with a mixture of 4He and CF4 gas for background measurements. The proportional counter diameter is 5 cm. The total deployed array length was 398 m. The SNO NCD array is the lowest-radioactivity large array of proportional counters ever produced. This article describes the design, construction, deployment, and characterization of the NCD array, discusses the electronics and data acquisition system, and considers event signatures and backgrounds.
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.
Physical Review Letters | 2015
D. M. Asner; R. F. Bradley; L. de Viveiros; P. J. Doe; Justin L. Fernandes; M Fertl; Erin C. Finn; Joseph A. Formaggio; D. Furse; A M Jones; J. N. Kofron; B H LaRoque; M. Leber; E.L. McBride; Michael Miller; Prajwal Mohanmurthy; B. Monreal; N.S. Oblath; R. G. H. Robertson; L.J. Rosenberg; G. Rybka; D. Rysewyk; Matthew Sternberg; Jonathan R. Tedeschi; Brent A. VanDevender; N. L. Woods
It has been understood since 1897 that accelerating charges must emit electromagnetic radiation. Although first derived in 1904, cyclotron radiation from a single electron orbiting in a magnetic field has never been observed directly. We demonstrate single-electron detection in a novel radio-frequency spectrometer. The relativistic shift in the cyclotron frequency permits a precise electron energy measurement. Precise beta electron spectroscopy from gaseous radiation sources is a key technique in modern efforts to measure the neutrino mass via the tritium decay end point, and this work demonstrates a fundamentally new approach to precision beta spectroscopy for future neutrino mass experiments.
Physics of Atomic Nuclei | 2004
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 | 2015
J.F. Amsbaugh; J. Barrett; A. Beglarian; Till Bergmann; H. Bichsel; L. I. Bodine; J. Bonn; N.M. Boyd; T.H. Burritt; Z. Chaoui; Suren Chilingaryan; T.J. Corona; P. J. Doe; J.A. Dunmore; S. Enomoto; Joseph A. Formaggio; F.M. Fränkle; D. Furse; H. Gemmeke; F. Glück; F. Harms; G. Harper; J. Hartmann; M. A. Howe; A. Kaboth; J. Kelsey; M. Knauer; Andreas Kopmann; M. Leber; E.L. Martin
Abstract The focal-plane detector system for the KArlsruhe TRItium Neutrino (KATRIN) experiment consists of a multi-pixel silicon p-i-n-diode array, custom readout electronics, two superconducting solenoid magnets, an ultra high-vacuum system, a high-vacuum system, calibration and monitoring devices, a scintillating veto, and a custom data-acquisition system. It is designed to detect the low-energy electrons selected by the KATRIN main spectrometer. We describe the system and summarize its performance after its final installation.
arXiv: Nuclear Experiment | 2006
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
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.
Journal of the Physical Society of Japan | 2007
Hidehito Nakamura; P. J. Doe; H. Ejiri; S. R. Elliott; J. Engel; Miroslav Finger; Michael Finger Jr; K. Fushimi; Victor M. Gehman; Mark Greenfield; Vo Hong Hai; R. Hazama; Hitoshi Imaseki; Petr Kavitov; V. Kekelidze; Hisashi Kitamura; K. Matsuoka; M. Nomachi; Takeo Ogama; A. Para; R. G. Hamish Robertson; Takuya Sakiuchi; T. Shima; Milos Slunecka; G. Shirkov; A. N. Sissakian; A.I. Titov; Yukio Uchihori; S. Umehara; Atsushi Urano
An ensemble of multilayer scintillators is discussed as an option of the high-sensitivity detector MOON (Mo Observatory of Neutrinos) for spectroscopic measurements of neutrinoless double beta decays. A prototype detector MOON-1, which consists of 6-layer plastic scintillator plates, was built to study the photon responses of the MOON-type detector. The photon responses, i.e., the number of scintillation photons collected and the energy resolution, which are key elements for high-sensitivity experiments, are found to be 1835 � 30 photoelectrons for 976 keV electrons and � ¼ 2:9 � 0:1% (� E=E ¼ 6:8 � 0:3% in FWHM) at the Q�� � 3 MeV region, respectively. The multilayer plastic scintillator structure with high energy resolution as well as a good signal for the background suppression of � –� rays is crucial for the MOON-type detector to achieve inverted-hierarchy neutrino-mass sensitivity. It will also be useful for medical and other rare-decay experiments as well.