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Dive into the research topics where G. L. Greene is active.

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Featured researches published by G. L. Greene.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009

Nab: Measurement principles, apparatus and uncertainties

D. Pocanic; R. Alarcon; L.P. Alonzi; S. Baeßler; S. Balascuta; J. D. Bowman; M. Bychkov; J. Byrne; J. R. Calarco; V. Cianciolo; C. Crawford; E. Frlež; M. T. Gericke; G. L. Greene; R. Grzywacz; Vladimir Gudkov; F. W. Hersman; Andreas Klein; J. Martin; S. A. Page; A. Palladino; S. I. Penttilä; K. Rykaczewski; W. S. Wilburn; A. R. Young; G. R. Young

The Nab collaboration will perform a precise measurement of a, the electron-neutrino correlation parameter, and b, the Fierz interference term in neutron beta decay, in the Fundamental Neutron Physics Beamline at the SNS, using a novel electric/magnetic field spectrometer and detector design. The experiment is aiming at the 10{sup -3} accuracy level in {Delta}a/a, and will provide an independent measurement of {lambda} = G{sub A}/G{sub V}, the ratio of axial-vector to vector coupling constants of the nucleon. Nab also plans to perform the first ever measurement of b in neutron decay, which will provide an independent limit on the tensor weak coupling.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2010

Study of the dependence of 198Au half-life on source geometry

Richard M. Lindstrom; Ephraim Fischbach; J. B. Buncher; G. L. Greene; Jere H. Jenkins; D. E. Krause; J. J. Mattes; Andrew Yue

We report the results of an experiment to determine whether the half-life of {sup 198}Au depends on the shape of the source. This study was motivated by recent suggestions that nuclear decay rates may be affected by solar activity, perhaps arising from solar neutrinos. If this were the case then the {beta}-decay rates, or half-lives, of a thin foil sample and a spherical sample of gold of the same mass and activity could be different. We find for {sup 198}Au, (T{sub 1/2}){sub foil}/(T{sub 1/2}){sub sphere} = 0.999 {+-} 0.002, where T{sub 1/2} is the mean half-life. The maximum neutrino flux at the sample in our experiments was several times greater than the flux of solar neutrinos at the surface of the Earth. We show that this increase in flux leads to a significant improvement in the limits that can be inferred on a possible solar contribution to nuclear decays.


Physical Review C | 2006

General classification and analysis of neutron β-decay experiments

Vladimir Gudkov; G. L. Greene; J. R. Calarco

A general analysis of the sensitivities of neutron ensuremath{beta}-decay experiments to manifestations of possible interaction beyond the standard model is carried out. In a consistent fashion, we take into account all known radiative and recoil corrections arising in the standard model. This provides a description of angular correlations in neutron decay in terms of one parameter, which is accurate to the level of


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

Fundamental neutron physics beamline at the spallation neutron source at ORNL

N. Fomin; G. L. Greene; R.R. Allen; V. Cianciolo; C. Crawford; T.M. Tito; P.R. Huffman; Erik B. Iverson; R. Mahurin; W.M. Snow

~{10}^{ensuremath{-}5}


arXiv: Nuclear Experiment | 2006

Precision Measurement of Parity Violation in Polarized Cold Neutron Capture on the Proton: the NPDγ Experiment

B. Lauss; J. D. Bowman; R. Carlini; Timothy E. Chupp; W. Chen; S. Corvig; M. Dabaghyan; D. Desai; Stuart J. Freedman; Thomas R. Gentile; M. T. Gericke; R. C. Gillis; G. L. Greene; F. W. Hersman; Takashi Ino; Takeyasu M. Ito; G. L. Jones; M. Kandes; M. Leuschner; B. Lozowski; R. Mahurin; M. Mason; Y. Masuda; J. Mei; G. S. Mitchell; S. Muto; H. Nann; S. A. Page; S. I. Penttilä; W. D. Ramsay

. Based on this general expression, we present an analysis of the sensitivities to new physics for selected neutron decay experiments. We emphasize that the usual parametrization of experiments in terms of the tree-level coefficients


Journal of Research of the National Institute of Standards and Technology | 1993

Facilities for Fundamental Neutron Physics Research at the NIST Cold Neutron Research Facility

Muhammad Arif; Maynard S. Dewey; G. L. Greene; W. M. Snow

a,A


11TH CONFERENCE ON THE INTERSECTIONS OF PARTICLE AND NUCLEAR PHYSICS: (CIPANP 2012) | 2013

Neutron Beta Decay Studies with Nab

S. Baeßler; R. Alarcon; L.P. Alonzi; S. Balascuta; L. Barrón-Palos; J. D. Bowman; M. Bychkov; J. Byrne; J. R. Calarco; T. Chupp; T. V. Cianciolo; C. Crawford; E. Frlež; M. T. Gericke; F. Glück; G. L. Greene; R. Grzywacz; Vladimir Gudkov; D. Harrison; F. W. Hersman; T. Ito; M. Makela; J. Martin; P. L. McGaughey; S. McGovern; S. A. Page; S. I. Penttilä; D. Pocanic; K. Rykaczewski; A. Salas-Bacci

, and B is inadequate when the experimental sensitivities are at the same or higher level relative to the size of the corrections to the tree-level description.


Physical Review C | 2006

Upper Bounds on Parity Violating Gamma-Ray Asymmetries in Compound Nuclei from Polarized Cold Neutron Capture.

M. T. Gericke; J. D. Bowman; R. Carlini; Tim Chupp; Kevin Patrick Coulter; M. Dabaghyan; M. Dawkins; D. Desai; Stuart J. Freedman; Thomas R. Gentile; R. C. Gillis; G. L. Greene; F. W. Hersman; Takashi Ino; G. L. Jones; M. Kandes; B. Lauss; M. Leuschner; W. R. Lozowski; R. Mahurin; M. Mason; Y. Masuda; G. S. Mitchell; S. Muto; H. Nann; S. A. Page; S. I. Penttilä; W. D. Ramsay; S. Santra; P.‐N. Seo

Abstract We describe the Fundamental Neutron Physics Beamline (FnPB) facility located at the Spallation Neutron Source at Oak Ridge National Laboratory. The FnPB was designed for the conduct of experiments that investigate scientific issues in nuclear physics, particle physics, astrophysics and cosmology using a pulsed slow neutron beam. We present a detailed description of the design philosophy, beamline components, and measured fluxes of the polychromatic and monochromatic beams.


Nuclear Physics | 2003

Parity-violating gamma-ray asymmetry in the neutron-proton capture

Y. Masuda; J. D. Bowman; R. Carlini; T. Case; T. E. Chupp; Kevin Patrick Coulter; S. J. Freedman; Thomas R. Gentile; M. Gericke; G. L. Greene; F.W. Hersmann; Takashi Ino; S. Ishimoto; G. L. Jones; M. Leuschner; G. S. Mitchell; K. Morimoto; S. Muto; H. Nann; S. A. Page; S.I. Pentilla; W. D. Ramsay; E. I. Sharapov; T. B. Smith; W. M. Snow; S.W. Wilburn; Y.W. Yuan

The NPDγ experiment at the Los Alamos Neutron Science Center (LANSCE) is dedicated to measure with high precision the parity violating asymmetry in the γ emission after capture of spin polarized cold neutrons in para‐hydrogen. The measurement will determine unambiguously the weak pion‐nucleon‐nucleon (πNN) coupling constant fπ1.The NPDGamma experiment at the Los Alamos Neutron Science Center (LANSCE) is dedicated to measure with high precision the parity violating asymmetry in the


Journal of Physics: Conference Series | 2010

NPDGamma: A measurement of the parity-violating gamma asymmetry A γ in n-p capture

R. C. Gillis; R. Alarcon; Septimiu Balascuta; L. Barrón-Palos; J. D. Bowman; R. Carlini; W. Chen; T. E. Chupp; C. Crawford; S. Covrig; M. Dabaghyan; N. Fomin; S. J. Freedman; Thomas R. Gentile; M. T. Gericke; G. L. Greene; F. W. Hersman; T. Ino; G. L. Jones; B. Lauss; M. Leuschner; W. R. Lozowski; R. Mahurin; Y. Masuda; J. Mei; G. S. Mitchell; S. Muto; H. Nann; S. A. Page; S. I. Penttilä

gamma

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J. D. Bowman

Los Alamos National Laboratory

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S. I. Penttilä

Oak Ridge National Laboratory

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G. S. Mitchell

Los Alamos National Laboratory

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Thomas R. Gentile

National Institute of Standards and Technology

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H. Nann

Indiana University Bloomington

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S. A. Page

University of Manitoba

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F. W. Hersman

University of New Hampshire

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R. Carlini

Thomas Jefferson National Accelerator Facility

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