Mark Bancroft Leuschner
University of New Hampshire
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Featured researches published by Mark Bancroft Leuschner.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
W.M. Snow; Anatoliy V. Bazhenov; C.S Blessinger; J. D. Bowman; T. E. Chupp; Kevin Patrick Coulter; S. J. Freedman; B. K. Fujikawa; Thomas R. Gentile; Geoffrey L. Greene; G. L. Hansen; Gary E. Hogan; S. Ishimoto; Gordon L. Jones; J. N. Knudson; E. Kolomenski; S. K. Lamoreaux; Mark Bancroft Leuschner; A. Masaike; Y. Masuda; Y. Matsuda; G. L. Morgan; Kimio Morimoto; C. L. Morris; H. Nann; S. I. Penttilä; A. Pirozhkov; V.R. Pomeroy; Donald Rich; Anatolii P. Serebrov
The weak pion-nucleon coupling constant H{sub {pi}}{sup 1} remains poorly determined, despite many years of effort. The recent measurement of the {sup 133}Cs anapole moment has been interpreted to give a value of H{sub {pi}}{sup 1} almost an order of magnitude larger than the limit established in the {sup 18}F parity doublet experiments. A measurement of the gamma ray directional asymmetry A{sub {gamma}} for the capture of polarized neutrons by hydrogen has been proposed at Los Alamos National Laboratory. This experiment will determine H{sub {pi}}{sup 1} independent of nuclear structure effects. However, since the predicted asymmetry is small, A{sub {gamma}} {approximately} 5 x 10{sup {minus}8}, systematic effects must be reduced to < 5 x 10{sup {minus}9}. The design of the experiment will is presented, with an emphasis on the techniques used for controlling systematic errors.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
D.R. Rich; J. D. Bowman; B. E. Crawford; P. P. J. Delheij; M.A. Espy; T. Haseyama; Gordon L. Jones; C.D. Keith; J. N. Knudson; Mark Bancroft Leuschner; A. Masaike; Y. Masuda; Y. Matsuda; S. I. Penttilä; V.R. Pomeroy; Debbie Smith; W. M. Snow; J.J. Szymanski; S. L. Stephenson; Alan K. Thompson; V. W. Yuan
Abstract The capability of performing accurate absolute measurements of neutron beam polarization opens a number of exciting opportunities in fundamental neutron physics and in neutron scattering. At the LANSCE pulsed neutron source we have measured the neutron beam polarization with an absolute accuracy of 0.3% in the neutron energy range from 40 meV to 10 eV using an optically pumped polarized 3 He spin filter and a relative transmission measurement technique. 3 He was polarized using the Rb spin-exchange method. We describe the measurement technique, present our results, and discuss some of the systematic effects associated with the method.
Nuclear Physics | 1995
A. Zondervan; L.J. de Bever; E. Jans; J. Konijn; M. Kruijer; J. J. M. Steijger; J.L. Visschers; P.J. Countryman; W.H.A. Hesselink; N. Kalantar-Nayestanaki; L.J.H.M. Kester; J.H. Mitchell; A. Pellegrino; J. R. Calarco; F.W. Hersman; Mark Bancroft Leuschner; Timothy Smith; Th. Bauer; M.W. Kelder; C. Giusti; F.D. Pacati; Jan Ryckebusch; Marc Vanderhaeghen
Abstract Coincidence cross sections for the 12 C(e, e′pp) and 12 C(e, e′p) reactions have been measured in the Δ-resonance region. The 12 C(e, e′pp) reaction has been measured at three different angular settings of the proton detectors to investigate the angular correlation between the emitted protons. The data, which have a low statistical accuracy, are compared with a calculation based on the direct-knockout mechanism, which includes one- and two-body currents. NN-correlations are accounted for via a correlation function, Δ-excitation via a two-body current and final-state interactions of the emitted protons via an optical potential. The 12 C(e, e′p) data, taken at large proton-emission angles, cover the region of high missing-energy values (145–275 MeV). The data are compared to results of a calculation taking into account meson exchange, intermediate Δ-excitation and pion production. This comparison shows that there is ample evidence for processes leading to multi-nucleon knockout.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2004
G. S. Mitchell; C. Blessinger; J. D. Bowman; T. E. Chupp; Kevin Patrick Coulter; M.T. Gericke; G. L. Jones; Mark Bancroft Leuschner; H. Nann; S. A. Page; S. I. Penttilä; T. B. Smith; W. M. Snow; W. S. Wilburn
Abstract An apparatus for measuring parity-violating asymmetries in gamma-ray emission following polarized cold neutron capture was constructed as a 1/10th scale test of the design for the forthcoming n → + p → d + γ experiment at LANSCE. The elements of the polarized neutron beam, including a polarized 3 He neutron spin filter and a radio frequency neutron spin rotator, are described. Using CsI(Tl) detectors and photodiode current mode readout, measurements were made of asymmetries in gamma-ray emission following neutron capture on 35 Cl , 113 Cd , and 139 La targets. Upper limits on the parity-allowed asymmetry s n ·( k γ × k n ) were set at the level of 7×10 −6 for all three targets. Parity-violating asymmetries s n · k γ were observed in 35 Cl , A γ =(−29.1±6.7)×10 −6 , and 139 La , A γ =(−15.5±7.1)×10 −6 , values consistent with previous measurements.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003
W. M. Snow; W. S. Wilburn; J. D. Bowman; Mark Bancroft Leuschner; S. I. Penttilä; V.R. Pomeroy; D.R. Rich; E. I. Sharapov; V. W. Yuan
Abstract A proof-of-principle experiment using unpolarized low-energy neutron capture on polyethylene and an array of 12 CsI detectors operated in current mode has been performed to test the possibility of measuring at LANSCE the parity-violating asymmetry A γ in the angular distribution of 2.23 MeV gamma rays from the n → + p → d + γ reaction. Results of this experiment including the current mode signal, electronic noise and detector sensitivity to magnetic fields are reported. The motivation and conceptual design for a new experiment aimed at a 10-fold improvement in the accuracy of A γ are outlined.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2004
G. S. Mitchell; Christopher S Blessinger; J. D. Bowman; T. E. Chupp; Kevin Patrick Coulter; M. Gericke; G. L. Jones; Mark Bancroft Leuschner; H. Nann; S. A. Page; S. I. Penttilä; T. B. Smith; W. M. Snow; W. S. Wilburn
Abstract An apparatus for measuring parity-violating asymmetries in gamma-ray emission following polarized cold neutron capture was constructed as a 1/10th scale test of the design for the forthcoming n → + p → d + γ experiment at LANSCE. The elements of the polarized neutron beam, including a polarized 3 He neutron spin filter and a radio frequency neutron spin rotator, are described. Using CsI(Tl) detectors and photodiode current mode readout, measurements were made of asymmetries in gamma-ray emission following neutron capture on 35 Cl , 113 Cd , and 139 La targets. Upper limits on the parity-allowed asymmetry s n ·( k γ × k n ) were set at the level of 7×10 −6 for all three targets. Parity-violating asymmetries s n · k γ were observed in 35 Cl , A γ =(−29.1±6.7)×10 −6 , and 139 La , A γ =(−15.5±7.1)×10 −6 , values consistent with previous measurements.
Journal of Research of the National Institute of Standards and Technology | 2005
Brian Collett; R. Anderman; Sergey Balashov; Fred B. Bateman; J. Byrne; Maynard S. Dewey; Brendan Michael Fisher; Lynn R. Goldin; G. L. Jones; Alexander Karl Komives; T. Konopka; Mark Bancroft Leuschner; Yu. Mostovoy; Jeffrey S. Nico; Alan K. Thompson; C. Trull; F. E. Wietfeldt; Richard Wilson; B. G. Yerozolimsky
Currently, the beta-neutrino asymmetry has the largest uncertainty (4 %) of the neutron decay angular correlations. Without requiring polarimetry this decay parameter can be used to measure λ (ga/gv), test Cabibbo-Kobayashi-Maskawa (CKM) unitarity limit scalar and tensor currents, and search for Charged Vector Current (CVC) violation. We propose to measure the beta-neutrino asymmetry coeffcient, a, using time-of-flight for the recoil protons. We hope to achieve a systematic uncertainty of σa / a ≈ 1.0 %. After tests at Indiana University’s Low Energy Neutron Source (LENS), the apparatus will be moved to the National Institute of Standards and Technology (NIST) where the measurement can achieve a statistical uncertainty of 1 % to 2 % in about 200 beam days.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2004
G. S. Mitchell; Christopher S Blessinger; J. D. Bowman; T. E. Chupp; Kevin Patrick Coulter; M. T. Gericke; Gordon Lyman Jones; Mark Bancroft Leuschner; H. Nann; S. A. Page; S. I. Penttilä; T. B. Smith; W. M. Snow; W. S. Wilburn
Abstract An apparatus for measuring parity-violating asymmetries in gamma-ray emission following polarized cold neutron capture was constructed as a 1/10th scale test of the design for the forthcoming n → + p → d + γ experiment at LANSCE. The elements of the polarized neutron beam, including a polarized 3 He neutron spin filter and a radio frequency neutron spin rotator, are described. Using CsI(Tl) detectors and photodiode current mode readout, measurements were made of asymmetries in gamma-ray emission following neutron capture on 35 Cl , 113 Cd , and 139 La targets. Upper limits on the parity-allowed asymmetry s n ·( k γ × k n ) were set at the level of 7×10 −6 for all three targets. Parity-violating asymmetries s n · k γ were observed in 35 Cl , A γ =(−29.1±6.7)×10 −6 , and 139 La , A γ =(−15.5±7.1)×10 −6 , values consistent with previous measurements.
Proceedings of the Eleventh International Symposium | 2003
S. I. Penttilä; J. D. Bowman; R. Carlini; T. Case; W C. Chen; T. E. Chupp; Kevin Patrick Coulter; S. J. Freedman; Thomas R. Gentile; M. T. Gericke; G. L. Greene; B. Hersmann; S. Ishimoto; G. L. Jones; Mark Bancroft Leuschner; Y. Masuda; G. S. Mitchell; K. Morimoto; H. Nann; S. A. Page; W. D. Ramsay; E. I. Sharapov; T. B. Smith; W. M. Snow; S. W. Wilburn; Y. W. Yuan
The {rvec n} + p {yields} d + {gamma} experiment under construction at LANSCE studies the weak interaction between neutrons and protons. The experiments will measure the directional dependence of the parity-violating {gamma}-ray asymmetry, A{sub {gamma}}, in the polarized cold neutron capture by para-hydrogen. The goal is to measure A{sub {gamma}} with uncertainty of 0.5 x 10{sup -8}, 10% of its predicted value. A{sub {gamma}} primarily isolates the {Delta}I = 1 component of the hadronic weak interaction and thus will determine the long-range weak pion-nucleon coupling constant H{sub {pi}}{sup 1}. The experiment is carefully designed for the LANSCE pulsed spallation neutron source to achieve the proposed statistical precision and to control systematic errors. We discuss the experiment and its status.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
W. M. Snow; J. D. Bowman; S. I. Penttilä; J. N. Knudson; Kevin Patrick Coulter; B. K. Fujikawa; Y. Masuda; T. E. Chupp; G. L. Greene; G. L. Morgan; D.R. Rich; V. W. Yuan; Christopher S Blessinger; H. Nann; Gary Hansen; Robert C. Welsh; E. I. Sharapov; Kimio Morimoto; Anatoliy V. Bazhenov; F. E. Wietfeldt; Thomas R. Gentile; G. L. Jones; Mark Bancroft Leuschner; Y. Matsuda; S.K. Lamoureaux; Anatolii P. Serebrov; Gary E. Hogan; S. J. Freedman; E. Kolomensky; T. B. Smith
The weak pion-nucleon coupling constant H{sub {pi}}{sup 1} remains poorly determined, despite many years of effort. The recent measurement of the {sup 133}Cs anapole moment has been interpreted to give a value of H{sub {pi}}{sup 1} almost an order of magnitude larger than the limit established in the {sup 18}F parity doublet experiments. A measurement of the gamma ray directional asymmetry A{sub {gamma}} for the capture of polarized neutrons by hydrogen has been proposed at Los Alamos National Laboratory. This experiment will determine H{sub {pi}}{sup 1} independent of nuclear structure effects. However, since the predicted asymmetry is small, A{sub {gamma}} {approximately} 5 x 10{sup {minus}8}, systematic effects must be reduced to < 5 x 10{sup {minus}9}. The design of the experiment will is presented, with an emphasis on the techniques used for controlling systematic errors.