Richard Coleman
Fermilab
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Featured researches published by Richard Coleman.
European Physical Journal C | 1992
E. Oltman; P. S. Auchincloss; R.E. Blair; C. Haber; S.R. Mishra; M. Ruiz; F. Sciulli; Michael H. Shaevitz; W. H. Smith; F. S. Merritt; M. J. Oreglia; P. G. Reutens; Richard Coleman; H. E. Fis; D. Levinthal; W. Marsh; P. A. Rapidis; H. B. White; D. Yovanovitch; Arie Bodek; F. Borcherding; N. Giokaris; K. Lang; I. E. Stockdale
Structure functions obtained from high energy neutrino and antineutrino scattering from an iron target are presented. These were extracted from the combined data of Fermilab experiments E616 and E701; these utilized narrow band beam runs between 1979–1982. The structure functions are used to test the validity of quarkparton model (QPM) predictions and to extract the QCD scale parameter Λ from fits to the Altarelli-Parisi equations.
European Physical Journal A | 1987
K. Lang; Arie Bodek; F. Borcherding; N. Giokaris; I. E. Stockdale; P. S. Auchincloss; R.E. Blair; C. Haber; S. Mishra; E. Oltman; M. Ruiz; F. Sciulli; Michael H. Shaevitz; W. H. Smith; R. Zhu; Y. K. Chu; D. B. MacFarlane; R. L. Messner; D. B. Novikoff; M. V. Purohit; David Garfinkle; Frank Merritt; Mark Oreglia; P. G. Reutens; Richard Coleman; H. E. Fisk; Y. Fukushima; O. Kerns; B. Jin; D. Levinthal
AbstractNeutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437vμ and 31
NEUTRINO FACTORIES, SUPERBEAMS, AND BETA BEAMS: 11th International Workshop on Neutrino Factories, Superbeams and Beta Beams—NuFact09 | 2010
Richard Coleman
Physical Review Letters | 1983
R.E. Blair; Barry C. Barish; Y. K. Chu; B. Jin; David Brian Macfarlane; R. L. Messner; J. Lee; J. Ludwig; D. B. Novikoff; M. Purohit; P. S. Auchincloss; F. Sciulli; M. H. Shaevitz; F. Bartlett; D. Edwards; H. Edwards; H. E. Fisk; Y. Fukushima; Q. A. Kerns; T. Kondo; P. A. Rapidis; S. Segler; R. Stefanski; D. Theriot; D. Yovanovitch; A. Bodek; Richard Coleman; W. Marsh; O. Fackler; K. A. Jenkins
\bar v_\mu
Physical Review Letters | 1980
Jack L. Ritchie; A. Bodek; Richard Coleman; W. Marsh; S. L. Olsen; B. Barish; R. L. Messner; M. H. Shaevitz; E. J. Siskind; H. E. Fisk; Y. Fukushima; G. J. Donaldson; F. S. Merritt; S. G. Wojcicki
Physical Review Letters | 1989
V. Papadimitriou; L. Gibbons; J. R. Patterson; Y.W. Wah; B. Winstein; R. Winston; Marcella C. Woods; H. Yamamoto; E. C. Swallow; G. J. Bock; Richard Coleman; Yee Bob Hsiung; K. Stanfield; R. Stefanski; Tatsuhiko Yamanaka; G. D. Gollin; M. Karlsson; J. K. Okamitsu; P. Debu; B. Peyaud; R. Turlay; B. Vallage
opposite sign dimuon events withPμ>4.3 GeV/c are used to measure the strange quark content of the nucleon:
Physical Review Letters | 1988
L. Gibbons; V. Papadimitriou; J. R. Patterson; Y.W. Wah; B. Winstein; R. Winston; Marcella C. Woods; H. Yamamoto; E. C. Swallow; G. J. Bock; Richard Coleman; Yee Bob Hsiung; K. Stanfield; R. Stefanski; Tatsuhiko Yamanaka; G.A. Blair; G. D. Gollin; M. Karlsson; J. K. Okamitsu; P. Debu; B. Peyaud; R. Turlay; B. Vallage
Physics Letters B | 1985
P. G. Reutens; F. S. Merritt; David Brian Macfarlane; R. L. Messner; D. B. Novikoff; M. Purohit; R.E. Blair; F. Sciulli; Michael H. Shaevitz; H. E. Fisk; Yasunori Fukushima; B. N. Jin; Takashi Kondo; P. A. Rapidis; D. Yovanovitch; A. Bodek; Richard Coleman; W. Marsh; Orrin D. Fackler; Keith A. Jenkins
\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}
European Physical Journal C | 1985
I. E. Stockdale; A. Bodek; F. O. Borcherding; Nikos D. Giokaris; Kevin J. Lang; David Garfinkle; F. S. Merritt; M. J. Oreglia; P. G. Reutens; Priscilla Auchincloss; R.E. Blair; C. Haber; Mariano Ruiz; F. Sciulli; Michael H. Shaevitz; Walter H. F. Smith; Rong-Yi Zhu; Richard Coleman; H. E. Fisk; B. N. Jin; Daniel A. Levinthal; W. Marsh; P. A. Rapidis; H. B. White; D. Yovanovitch
Archive | 1984
C. Haber; F. S. Merritt; K. Lang; P. G. Reutens; W. Marsh; M. J. Oreglia; David Garfinkle; D. Levinthal; H. B. White; A. Bodek; B. N. Jin; I. E. Stockdale; R. Zhu; F. Sciulli; N. Giokaris; P. A. Rapidis; R. E. Blair; Richard Coleman; W. H. Smith; M. Ruiz; D. Yovanovitch; M. H. Shaevitz; P. Auchincloss; H. E. Fisk; F. Borcherding
using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine+e− collisions and neutrino emulsion data.
