NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = V.Cupps Found 19 matches. 2011KA42 J.Korean Phys.Soc. 59, 2063s (2011) Y.Kasugai, N.Matsuda, Y.Iwamoto, Y.Sakamoto, H.Nakashima, H.Matsumura, N.Kinoshita, H.Iwase, T.Sanami, M.Hagiwara, H.Hirayama, H.Yashima, N.Sigyo, H.Arakawa, K.Ishibashi, N.Mokhov, A.Leveling, D.Boehnlein, K.Vaziri, G.Lauten, S.Wayne, V.Cupps, B.Kershisnik, S.Benesch, T.Nakamura, K.Oishi, K.Niita Shielding Experiments under JASMIN Collaboration at Fermilab (I) Overview of the Research Activities
doi: 10.3938/jkps.59.2063
1996SI01 Phys.Rev. C53, 30 (1996) A.J.Simon, G.Glass, M.W.McNaughton, T.Noro, K.H.McNaughton, P.J.Riley, E.Gulmez, C.A.Whitten, Jr., V.R.Cupps, R.D.Ransome, D.L.Adams Absolute pp-Elastic Cross Sections from 492 to 793 MeV using CH2 Targets NUCLEAR REACTIONS 1H(p, p), E=492-793 MeV; measured absolute σ(θ). Polyethylene targets.
doi: 10.1103/PhysRevC.53.30
1993BA37 Phys.Rev. C48, 1106 (1993) F.T.Baker, D.Beatty, L.Bimbot, V.Cupps, C.Djalali, R.W.Fergerson, C.Glashausser, G.Graw, A.Green, K.Jones, M.Morlet, S.K.Nanda, A.Sethi, B.H.Storm, W.Unkelbach, A.Willis Separation of ΔS = 0 and ΔS = 1 in the Response of 12C to 318 MeV Protons NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=318 MeV; measured σ(θ, Ep), spin-flip probability; deduced model parameters. 12C deduced ΔS=0, ΔS=1 multipole transition strength distributions. RPA, DWIA analysis.
doi: 10.1103/PhysRevC.48.1106
1993GR02 Phys.Rev.Lett. 70, 734 (1993) A.Green, W.Unkelbach, F.T.Baker, D.Beatty, L.Bimbot, X.Y.Chen, V.R.Cupps, C.Djalali, G.Edwards, R.W.Fergerson, C.Glashausser, K.W.Jones, M.K.Jones, G.Kumbartzki, A.Sethi, B.Storm, J.Wambach Spin-Longitudinal and Spin-Transverse Response of 40Ca to 500 MeV Protons at Low Momentum Transfer NUCLEAR REACTIONS 40Ca(polarized p, p'), E=497, 581 MeV; measured spin-transfer observables; deduced longitudinal, transverse spin-flip probabilities. DWIA analysis, finite nucleus RPA.
doi: 10.1103/PhysRevLett.70.734
1993GU03 Nucl.Phys. A551, 621 (1993) E.Gulmez, A.G.Ling, C.A.Whitten, Jr., M.W.McNaughton, D.L.Adams, V.R.Cupps, G.Glass, A.J.Simon, K.H.McNaughton Absolute Differential Cross-Section Measurements for p + p → π+ + d Reaction at 500-800 MeV NUCLEAR REACTIONS 1H(p, π+), E=492, 576, 642, 728, 793 MeV; measured σ(θ). Liquid H2 target, scintillator beam-counting system, wire-chamber detectors, two arms.
doi: 10.1016/0375-9474(93)90269-4
1993JO11 Phys.Rev. C48, 2800 (1993) M.K.Jones, R.D.Ransome, V.R.Cupps, R.W.Fergerson, C.L.Morris, J.A.McGill, J.D.Zumbro, J.R.Comfort, B.G.Ritchie, J.R.Tinsley, P.C.Gugelot, C.F.Moore Pion Absorption Above the Δ(1232) Resonance NUCLEAR REACTIONS 12C, 58Ni, 90Zr, 118Sn, 208Pb(π+, xp), E=250-500 MeV; measured σ vs missing energy for x=2, 3; deduced total absorption σ.
doi: 10.1103/PhysRevC.48.2800
1993SI08 Phys.Rev. C48, 662 (1993) A.J.Simon, G.Glass, M.W.McNaughton, T.Noro, K.H.McNaughton, P.J.Riley, E.Gulmez, C.A.Whitten, Jr., V.R.Cupps, R.D.Ransome, D.L.Adams Absolute pp-Elastic Cross Sections from 492 to 793 MeV NUCLEAR REACTIONS 1H(p, p), E=492-793 MeV; measured absolute σ(E, θ), uncertainties less than 1%.
doi: 10.1103/PhysRevC.48.662
1992RA01 Phys.Rev. C45, R509 (1992) R.D.Ransome, C.L.Morris, V.R.Cupps, R.W.Fergerson, J.A.McGill, D.L.Watson, J.D.Zumbro, B.G.Ritchie, J.R.Comfort, J.R.Tinsley, R.A.Loveman, S.Dawson, A.Green, P.C.Gugelot, C.F.Moore Pion Absorption in Heavy Nuclei NUCLEAR REACTIONS 6Li, 12C, 27Al, 58Ni, 118Sn, 208Pb, 238U(π+, xp), (π+, d), E=50-200 MeV; measured σ vs missing energy; deduced pion absorption mechanism. Large solid angle bismuth germanate detector array.
doi: 10.1103/PhysRevC.45.R509
1991BA26 Phys.Rev. C44, 93 (1991) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, M.Vetterli, R.Abegg, D.Beatty, B.Bonin, B.Castel, X.Y.Chen, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, K.Nakayama, S.K.Nanda, R.Sawafta, S.Yen Spin Decomposition of the Responses of 44Ca and 48Ca to 300 MeV Protons NUCLEAR REACTIONS 44Ca(polarized p, p'), E=290 MeV; 48Ca(polarized p, p'), E=318 MeV; measured σ(θ, Ep), analyzing power, spin-flip σ(θ). 44,48Ca deduced giant, spin resonance strength distributions.
doi: 10.1103/PhysRevC.44.93
1991GU01 Phys.Rev. C43, 2067 (1991) E.Gulmez, S.Beedoe, T.Jaroszewicz, A.G.Ling, C.A.Whitten, Jr., M.W.McNaughton, J.R.Santana, D.L.Adams, V.R.Cupps, A.J.Simon, M.L.Barlett, K.H.McNaughton, P.J.Riley Absolute Differential Cross Section Measurements for Proton-Deuteron Elastic Scattering at 641.3 and 792.7 MeV NUCLEAR REACTIONS 2H(p, p), E=641.3, 792.7 MeV; measured absolute σ(θ). Relativistic impulse approximation.
doi: 10.1103/PhysRevC.43.2067
1990BA14 Phys.Lett. 237B, 337 (1990) F.T.Baker, L.Bimbot, B.Castel, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, S.K.Nanda, R.D.Smith, M.Vetterli, J.Wambach, R.Abegg, D.Beatty, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, J.Lisantti, M.Morlet, R.Sawafta, W.Unkelbach, A.Willis, S.Yen The Nuclear Spin Response to Intermediate Energy Protons NUCLEAR REACTIONS 12C, 90Zr, 40,44,48Ca, 24Mg, 54Fe(polarized p, p'), E ≈ 300 MeV; 40Ca(polarized p, p'), E=800 MeV; measured spin-flip transition probability; deduced enhanced spin response features. Continuum RPA.
doi: 10.1016/0370-2693(90)91185-E
1990BI09 Phys.Rev. C42, 2367 (1990) L.Bimbot, R.W.Fergerson, C.Glashausser, K.W.Jones, F.T.Baker, D.Beatty, V.Cupps, A.Green, S.Nanda Nuclear Spin Response of 40Ca to 800 MeV Polarized Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=800 MeV; measured missing mass spectra, σ(θ, Ep), spin-flip probability; deduced reaction mechanism. 40Ca deduced nuclear spin response.
doi: 10.1103/PhysRevC.42.2367
1990RA05 Phys.Rev.Lett. 64, 372 (1990) R.D.Ransome, V.R.Cupps, S.Dawson, R.W.Fergerson, A.Green, C.L.Morris, J.A.McGill, J.R.Comfort, B.G.Ritchie, J.Tinsley, J.D.Zumbro, R.A.Loveman, P.C.Gugelot, D.L.Watson, C.F.Moore Charged-Particle Multiplicities following Pion Absorption on 6Li NUCLEAR REACTIONS 6Li(π+, X), E=150 MeV; measured charged particle spectra following pion absorption; deduced multi-proton emission σ.
doi: 10.1103/PhysRevLett.64.372
1990RA20 Phys.Rev. C42, 1500 (1990) R.D.Ransome, V.R.Cupps, S.Dawson, R.W.Fergerson, A.Green, C.L.Morris, J.A.McGill, J.R.Comfort, B.G.Ritchie, J.R.Tinsley, J.D.Zumbro, R.A.Loveman, P.C.Gugelot, D.L.Watson, C.F.Moore Systematics of Pion Absorption on 6Li NUCLEAR REACTIONS 6Li(π+, 2pX), E=50-200 MeV; measured missing energy distributions, σ(θ) for 2p, 2pn, 3p, 2pd final states; deduced pion absorption mechanism.
doi: 10.1103/PhysRevC.42.1500
1990ST20 Phys.Rev. C42, 2562 (1990) E.J.Stephenson, A.D.Bacher, G.P.A.Berg, V.R.Cupps, C.C.Foster, N.Hodiwalla, P.Li, J.Lisantti, D.A.Low, D.W.Miller, C.Olmer, A.K.Opper, B.K.Park, R.Sawafta, S.W.Wissink, J.A.Tostevin, D.A.Coley, R.C.Johnson Enhancement of the Near-Side Component in Quasiadiabatic Calculations of the 66Zn(d, p)67Zn Reaction NUCLEAR REACTIONS 67Zn(polarized p, p), E=91.8 MeV; 66Zn(polarized d, p), E=88.2 MeV; measured σ(θ), proton polarization, analyzing power vs θ; deduced model parameters. Quasiadiabatic model.
doi: 10.1103/PhysRevC.42.2562
1987CU04 Nucl.Phys. A469, 445 (1987) V.R.Cupps, J.D.Brown, C.C.Foster, W.P.Jones, D.W.Miller, H.Nann, P.Schwandt, E.J.Stephenson, J.A.Tostevin The 116Sn(d, p)117Sn l = 0 Reaction Mechanism at Intermediate Energies NUCLEAR REACTIONS 116Sn(d, p), (polarized d, p), E=79.2 MeV; measured σ(θ), A(θ), P(θ); deduced reaction mechanism. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(87)90032-7
1987PI01 Phys.Rev. C35, 37 (1987) M.A.Pickar, H.J.Karwowski, J.D.Brown, J.R.Hall, M.Hugi, R.E.Pollock, V.R.Cupps, M.Fatyga, A.D.Bacher Proton Radiative Capture by Deuterium between 100 and 200 MeV NUCLEAR REACTIONS, MECPD 2H(polarized p, γ), E=100-200 MeV; measured σ(θ), A(θ); deduced quasideuteron role. Coincidence measurement. Quasideuteron model calculations.
doi: 10.1103/PhysRevC.35.37
1987ST16 Nucl.Phys. A469, 467 (1987) E.J.Stephenson, V.R.Cupps, J.A.Tostevin, R.C.Johnson, J.D.Brown, C.C.Foster, W.P.Jones, D.W.Miller, H.Nann, P.Schwandt The Effects of Far-Side Dominance on the j-Dependence of the Medium Energy 116Sn(d, p)117Sn Reaction NUCLEAR REACTIONS 116Sn(d, p), (polarized d, p), E=79.2 meV; measured σ(E(p), θ), A(E(p), θ); deduced reaction mechanism. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(87)90033-9
1986ST06 Phys.Lett. 171B, 358 (1986) E.J.Stephenson, R.C.Johnson, J.A.Tostevin, V.R.Cupps, J.D.Brown, C.C.Foster, J.A.Gering, W.P.Jones, D.A.Low, D.W.Miller, H.Nann, C.Olmer, A.K.Opper, P.Schwandt, J.W.Seubert, S.W.Wissink Inplications of Far-Side Dominance for the Disagreement between Distorted Wave Theory and Well-Matched Intermediate Energy (d, p) Reactions NUCLEAR REACTIONS 116Sn(polarized d, p), E=90 MeV; analyzed σ(θ), analyzing power vs θ. 66Zn(polarized d, p), E=88.1 MeV; measured proton polarization vs θ; deduced far-side dominance insignificance.
doi: 10.1016/0370-2693(86)91420-6
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