NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.McGill Found 61 matches. 1998MO09 Phys.Lett. 419B, 25 (1998) C.L.Morris, J.D.Zumbro, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Reidel, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, J.Ouyang, R.J.Peterson, J.E.Wise Evidence for Δ+ Components in Nuclei NUCLEAR REACTIONS 12,13C, 90Zr, 208Pb(π+, π+p), (π+, π-p), E=500 MeV; measured σ(DCX)/σ(NCX); deduced nuclear wave function Δ+ components.
doi: 10.1016/S0370-2693(97)01453-6
1997KA22 Phys.Rev. C55, 2533 (1997) G.Kahrimanis, G.Burleson, C.M.Chen, B.C.Clark, K.Dhuga, D.J.Ernst, J.A.Faucett, H.T.Fortune, S.Hama, A.Hussein, M.F.Jiang, K.W.Johnson, L.Kurth Kerr, S.Mathews, J.McGill, C.F.Moore, S.Mordechai, C.L.Morris, J.O'Donnell, M.Snell, M.Rawool-Sullivan, L.Ray, C.Whitley, A.L.Williams Pion-Nucleus Elastic Scattering on 12C, 40Ca, 90Zr, and 208Pb at 400 and 500 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(π+, π+), (π-, π-), E=400, 500 MeV; 90Zr(π+, π+), E=400, 500 MeV; 90Zr(π-, π-), E=400 MeV; measured σ(θ). 208Pb(π+, π+), (π-, π-), E=662.7 MeV; 40Ca(π+, π+), (π-, π-), 12C(π+, π+), E=672.5 MeV; 12C(π-, π-), E=672.5, 486.2 MeV; analyzed σ(θ). Impulse approximation approach.
doi: 10.1103/PhysRevC.55.2533
1994YE06 Phys.Rev. C50, 897 (1994) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, M.A.Franey, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.I.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=130-180 MeV; 13C(π+, π+), E=223 MeV; 13C(π-, π-), E=226 MeV; measured analyzing power A(y)(θ), σ(θ); deduced spin-flip transition quadrupole component role. Polarized, unpolarized target. DWIA calculations, optical, Δ-hole models.
doi: 10.1103/PhysRevC.50.897
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
1993KO17 Phys.Rev. C48, 250 (1993) C.M.Kormanyos, R.J.Peterson, J.Applegate, J.Beck, T.D.Averett, B.G.Ritchie, C.L.Morris, J.McGill, D.S.Oakley Low-Energy Pion Scattering to 1- States in 12C NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=40, 50, 65 MeV; measured σ(θ). 12C deduced level energies, Γ, sum rule strengths. DWIA analysis.
doi: 10.1103/PhysRevC.48.250
1993SM01 Phys.Rev. C47, 1053 (1993) D.A.Smith, H.T.Fortune, J.M.O'Donnell, J.D.Silk, B.Gluckman, R.Crittenden, N.Claytor, C.L.Morris, J.A.McGill Pion Double Charge Exchange on 56Fe at T(π) = 400 MeV NUCLEAR REACTIONS 56Fe(π+, π-), E=400 MeV; measured σ(θ). 56Ni deduced double dipole resonance components J, π, excitation σ.
doi: 10.1103/PhysRevC.47.1053
1993WI15 Phys.Rev. C48, 1840 (1993) J.E.Wise, M.R.Braunstein, S.Hoibraten, M.D.Kohler, B.J.Kriss, J.Ouyang, R.J.Peterson, J.A.McGill, C.L.Morris, S.J.Seestrom, R.M.Whitton, J.D.Zumbro, C.M.Edwards, A.L.Williams Quasifree Pion Scattering at 500 MeV NUCLEAR REACTIONS C(π+, π+), (π-, π-), E=500 MeV; measured σ(θ) vs energy loss, σ(θ). Ca, Zr, Pb(π+, π+), (π-, π-), E=500 MeV; measured σ(θ); deduced surface single nucleon knockout evidence.
doi: 10.1103/PhysRevC.48.1840
1993ZU01 Phys.Rev.Lett. 71, 1796 (1993) J.D.Zumbro, C.L.Morris, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Edwards, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, R.J.Peterson, J.Ouyang, J.E.Wise, W.R.Gibbs Inclusive Scattering of 500-MeV Pions from Carbon NUCLEAR REACTIONS C(π+, π+X), (π-, π-X), E=500 MeV; measured inclusive σ(θ, E(π)); deduced comparison with (e, e'X).
doi: 10.1103/PhysRevLett.71.1796
1992BR12 Phys.Rev. C45, 2343 (1992) M.L.Brooks, B.Bassalleck, B.D.Dieterle, R.A.Reeder, D.M.Lee, J.A.McGill, M.E.Schillaci, R.A.Ristinen, W.R.Smythe Neutron Induced Pion Production on C, Al, Cu, and W at 200-600 MeV NUCLEAR REACTIONS C, 27Al, Cu, N(n, π+), (n, π-), E=200, 600 MeV; measured σ(θ, E), θ=(25°, 125°); deduced π- to π+ ratio. Intranuclear cascade model.
doi: 10.1103/PhysRevC.45.2343
1992JO01 Phys.Lett. 278B, 419 (1992) M.K.Jones, B.G.Ritchie, C.L.Morris, R.D.Ransome, J.A.McGill, D.L.Watson, C.F.Moore, D.Clayton, K.Pujara, I.Brown, P.Campbell Energy Dependence of the Total 12C(π+, 2p) Cross Section NUCLEAR REACTIONS 12C(π+, 2p), E=19-140 MeV; measured absorption σ(E); deduced energy dependence. Large solid angle bismuth germanate multi-element detection system.
doi: 10.1016/0370-2693(92)90578-R
1992OD02 Nucl.Instrum.Methods Phys.Res. A317, 445 (1992) J.M.O'Donnell, J.Davis, R.A.DeHaven, E.Gray, R.Johnson, R.E.Lomax, B.J.McCloud, J.A.McGill, C.L.Morris, J.Novak, B.Rusnak, G.Tubb, J.M.Applegate, T.D.Averett, J.Beck, B.G.Ritchie, E.Haebel, D.Kiehlmann, U.Klein, M.Peiniger, P.Schafer, H.Vogel, H.Ward, C.F.Moore A Superconducting Radio-Frequency Cavity for Manipulating the Phase Space of Pion Beams at LAMPF NUCLEAR REACTIONS 93Nb(π+, π+), E=50 MeV; 12C(π+, π+'), E=50 MeV; measured spectra. Superconducting radio-frequency cavity, pion beam phase space manipulation.
doi: 10.1016/0168-9002(92)90988-G
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
1992RA11 Phys.Rev. C46, 273 (1992) R.D.Ransome, C.L.Morris, M.K.Jones, B.G.Ritchie, D.L.Watson, J.A.McGill, K.Pujara, D.B.Clayton, I.Brown, P.Campbell, C.F.Moore Pion Absorption in Light Nuclei NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 12,13C(π+, 2p), (π+, 3p), E=50-180 MeV; measured missing mass spectra; deduced σ(E), pion absorption mechanism.
doi: 10.1103/PhysRevC.46.273
1991AK05 Nucl.Phys. A534, 478 (1991) M.Akei, J.F.Amann, J.Chiba, H.Ejiri, Y.Iseki, M.Fukuda, T.Fukuda, O.Hashimoto, A.Higashi, S.Homma, T.Irie, A.Kashitani, S.Kato, K.Kimura, T.Kishimoto, K.Maeda, Y.Matsuyama, J.A.McGill, T.Nagae, H.Nagasawa, C.Nagoshi, H.Noumi, M.Nomachi, H.Ohsumi, K.Okuda, K.Omata, H.Sano, O.Sasaki, T.Shibata, F.Soga, F.Takeuchi, H.A.Thiessen, S.Toyama, K.H.Tanaka, Y.Umeda, N.Yoshikawa, Y.Yamanoi The (π+, K+) Reaction on 12C and 56Fe NUCLEAR REACTIONS 12C, Fe(π+, K+), E at 1.07 GeV/c; measured σ(θ), θ=3°. DWIA analysis.
doi: 10.1016/0375-9474(91)90457-H
1991WI03 Phys.Rev. C43, 766 (1991) A.L.Williams, J.A.McGill, C.L.Morris, G.R.Burleson, J.A.Faucett, D.S.Oakley, M.Burlein, H.T.Fortune, J.M.O'Donnell, G.P.Kahrimanis, C.F.Moore Pion Double Charge Exchange on 42,44,48Ca for 300 ≤ T(π) ≤ 550 MeV NUCLEAR REACTIONS 42,44,48Ca(π+, π-), E=300-550 MeV; measured σ(θ), σ(E(π)); deduced two-amplitude model parameters.
doi: 10.1103/PhysRevC.43.766
1991WI13 Phys.Rev. C44, 2025 (1991) A.L.Williams, K.W.Johnson, G.P.Kahrimanis, H.Ward, C.F.Moore, J.A.McGill, C.L.Morris, G.R.Burleson, J.A.Faucett, M.Rawool-Sullivan, D.S.Oakley, M.Burlein, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith Mass Dependence of High-Energy Pion Double Charge Exchange NUCLEAR REACTIONS 26Mg, 46,50Ti, 54,56Fe, 52Cr, 80Se, 90Zr, 197Au, 208Pb(π+, π-), E=450, 500 MeV; measured σ(θ), θ=5°; deduced mass dependence, two-amplitude model parameters. Double isobaric analog state excitation.
doi: 10.1103/PhysRevC.44.2025
1991YE01 Phys.Rev.Lett. 66, 1959 (1991) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Asymmetry Measurement of Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=132-226 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.1959
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
1990YE06 J.Phys.(Paris), Colloq.C-6, 587 (1990) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.Gorgen, B.Ritchie, J.R.Tinsley, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, S.Hoibraten, M.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the [3, 3] Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=114-226 MeV; measured analyzing power vs θ. Polarized target. DWIA analyses.
1989AD02 Phys.Lett. 219B, 399 (1989) G.S.Adams, B.Hoistad, J.M.Laget, B.Aas, K.Jones, J.A.McGill, G.S.Blanpied, C.S.Mishra, G.Pignault, C.S.Whisnant, G.Pauletta Analyzing Powers for p(pol) + d → 3He + π0 at 800 MeV NUCLEAR REACTIONS 2H(polarized p, π0), E=800 MeV; measured missing mass spectra, analyzing power; deduced Δ-isobar role.
doi: 10.1016/0370-2693(89)91084-8
1989AK02 Nuovo Cim. 102A, 457 (1989) M.Akei, H.Ejiri, M.Fukuda, T.Irie, Y.Iseki, A.Kashitani, T.Kishimoto, H.Nagasawa, H.Noumi, H.Ohsumi, K.Okuda, Y.Umeda, T.Fukuda, T.Shibata, O.Hashimoto, S.Homma, Y.Matsuyama, T.Nagae, C.Nagoshi, K.Omata, F.Soga, S.Toyama, N.Yoshikawa, Y.Yamanoi, J.F.Amann, J.A.McGill, H.A.Thiessen, J.Chiba, M.Nomachi, S.Sasaki, K.H.Tanaka, S.Kato, K.Kimura, F.Takeuchi, K.Maeda, H.Sano Study of 12C(Lambda) and 56Fe(Lambda) Hypernuclei by (π+, K+) Reactions at the KEK 12 GeV PS NUCLEAR REACTIONS 12C, 56Fe(π+, K+), E ≈ 720 MeV/c; measured σ(θ) vs lambda binding energy.
doi: 10.1007/BF02734864
1989AK04 Nucl.Instrum.Methods Phys.Res. A283, 46 (1989) M.Akei, J.F.Amann, J.Chiba, H.Ejiri, M.Fukuda, T.Fukuda, O.Hashimoto, S.Homma, T.Irie, Y.Iseki, A.Kashitani, S.Kato, K.Kimura, T.Kishimoto, K.Maeda, Y.Matsuyama, J.A.McGill, T.Nagae, H.Nagasawa, C.Nagoshi, M.Nomachi, H.Noumi, H.Ohsumi, K.Okuda, K.Omata, H.Sano, O.Sasaki, T.Shibata, F.Soga, F.Takeuchi, H.A.Thiessen, S.Toyama, K.H.Tanaka, Y.Yamanoi, N.Yoshikawa A Broad Range Spectrometer PIK for Medium-Energy Meson Spectroscopy NUCLEAR REACTIONS 12C(π+, K+), E at 1.05 GeV/c; 12C, 1H(π+, p), E at 490 MeV/c; measured missing mass spectra. CH2 target, broad range spectrometer.
doi: 10.1016/0168-9002(89)91254-0
1989WI02 Phys.Lett. 216B, 11 (1989) A.L.Williams, L.Agnew, L.G.Atencio, H.W.Baer, M.Burlein, G.R.Burleson, K.S.Dhuga, H.T.Fortune, G.S.Kyle, J.A.McGill, C.F.Moore, C.L.Morris, S.Mordechai, J.M.O'Donnell, M.W.Rawool, S.Schilling, J.D.Silk, J.D.Zumbro Pion Double Charge Exchange Above the Δ(1232) Resonance NUCLEAR REACTIONS 14C, 18O(π+, π-), E=300, 400, 500 MeV; measured σ(E(π), θ(π)). 14N, 18Ne deduced double IAS excitation.
doi: 10.1016/0370-2693(89)91360-9
1988AD01 Phys.Rev. C37, 1341 (1988) G.S.Adams, B.Hoistad, J.M.Laget, B.Aas, K.Jones, J.A.McGill, G.S.Blanpied, C.S.Mishra, W.K.Mize, G.Pignault, C.S.Whisnant, S.M.Whitlow, G.Pauletta Analyzing Powers for the Reaction 2H(p(pol), γ)3He at 800 MeV NUCLEAR REACTIONS 2H(polarized p, γ), E=800 MeV; measured A(θ); deduced meson exchange currents.
doi: 10.1103/PhysRevC.37.1341
1988BL04 Phys.Rev. C37, 1304 (1988) G.S.Blanpied, B.G.Ritchie, M.L.Barlett, R.W.Fergerson, J.A.McGill, B.H.Wildenthal Elastic and Inelastic Scattering of 0.8 GeV Protons from 40Ar NUCLEAR REACTIONS 40Ar(p, p), (p, p'), E=0.8 GeV; measured σ(θ); deduced optical model parameters. 40Ar levels deduced deformation parameters. Collective model transition densities.
doi: 10.1103/PhysRevC.37.1304
1988BL08 Phys.Rev. C37, 1987 (1988) G.S.Blanpied, B.G.Ritchie, M.L.Barlett, G.W.Hoffmann, J.A.McGill, E.C.Milner, K.W.Jones, S.K.Nanda, R.de Swiniarski Elastic and Inelastic Scattering of 0.8 GeV Polarized Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ. 24,26Mg deduced levels, L, deformation lengths, β(l).
doi: 10.1103/PhysRevC.37.1987
1988BL13 Phys.Rev. C38, 2180 (1988) G.S.Blanpied, B.G.Ritchie, M.L.Barlett, R.W.Fergerson, G.W.Hoffmann, J.A.McGill, B.H.Wildenthal Elastic and Inelastic Scattering of 0.8 GeV Protons from 20Ne and 22Ne NUCLEAR REACTIONS 20,22Ne(p, p), (p, p'), E=0.8 GeV; measured σ(Ep), σ(θ). 22,20Ne levels deduced multipole moments, deformation lengths.
doi: 10.1103/PhysRevC.38.2180
1988FE09 Phys.Rev. C38, 2193 (1988) R.Fergerson, J.McGill, C.Glashausser, K.Jones, S.Nanda, Sun Zuxun, M.Barlett, G.Hoffmann, J.Marshall, J.McClelland Polarization Transfer for Inclusive Proton-Nucleus Inelastic Scattering at 800 MeV NUCLEAR REACTIONS 12C, 1,2H(polarized p, pX), E=800 MeV; measured polarization transfer parameters. Quasielastic, isobar excitations.
doi: 10.1103/PhysRevC.38.2193
1988HI01 Phys.Rev. C37, 692 (1988) N.M.Hintz, D.Cook, M.Gazzaly, M.A.Franey, M.L.Barlett, G.W.Hoffmann, R.Fergerson, J.McGill, G.Pauletta, R.L.Boudrie, J.B.McClelland, K.W.Jones Energy Dependence of Neutron-Proton Matrix Element Ratios Derived from 25-800 MeV Energy Proton Scattering NUCLEAR REACTIONS 58Ni, 208Pb(p, p), (p, p'), E=318-800 MeV; measured σ(θ); deduced potential deformation lengths. 40Ca, 58Ni, 208Pb levels deduced neutron, proton matrix element ratio. Other data input.
doi: 10.1103/PhysRevC.37.692
1988HO01 Phys.Rev. C37, 397 (1988) G.W.Hoffmann, M.L.Barlett, R.W.Fergerson, J.A.Marshall, J.A.McGill, E.C.Milner, L.Ray, J.F.Amann Differential Cross Section and Analyzing Power Measurements for p + p Elastic Scattering at 497.5 MeV NUCLEAR REACTIONS 1H(polarized p, p), (p, p), E ≈ 497.5 MeV; measured σ(θ), analyzing power for (θ(cm)=16°-97°). Phase shift analysis.
doi: 10.1103/PhysRevC.37.397
1987NA06 Phys.Lett. 188B, 177 (1987) S.K.Nanda, M.Gazzaly, C.Glashausser, J.McGill, K.W.Jones, T.A.Carey, L.B.Rees, H.Ohnuma Spin Transfer Measurements in the 51V(p(pol), p(pol)')51V* Reaction NUCLEAR REACTIONS 51V(polarized p, p'), E=319 MeV; measured σ(θ), analyzing power, spin-flip σ(E(p'), θ). 51V deduced M1 resonance.
doi: 10.1016/0370-2693(87)90002-5
1987RI06 Phys.Lett. 197B, 23 (1987) P.J.Riley, M.Bachman, C.L.Hollas, K.H.McNaughton, S.-W.Xu, B.E.Bonner, O.B.Van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet Polarization Observables for the Reaction pp → ppπ0 at 800 MeV NUCLEAR REACTIONS 1H(polarized p, pπ0), E=647, 733, 800 MeV; measured induced polarization, analyzing power, Wolfenstein parameters. Orthogonal beam polarization.
doi: 10.1016/0370-2693(87)90334-0
1986HO23 Phys.Lett. 177B, 299 (1986) B.Hoistad, M.Barlett, G.S.Adams, M.Gazzaly, B.Aas, G.Pauletta, F.Irom, K.Jones, J.A.McGill The (p(pol), π(±)) Reactions on Be at 650 MeV NUCLEAR REACTIONS 9Be(polarized p, π+), (polarized p, π-), E=650 MeV; measured σ(θ), analyzing power vs θ. Trigger system, high resolution spectrometer.
doi: 10.1016/0370-2693(86)90756-2
1986MO26 Phys.Lett. 182B, 151 (1986) C.L.Morris, K.W.Jones, J.A.McGill, M.A.Bryan, C.F.Moore, R.Gilman, C.Glashausser, S.J.Seestrom-Morris The Observation of Energetic Protons in Coincidence with Pion-Induced Double Charge Exchange on 12C and 48Ca NUCLEAR REACTIONS 12C, 48Ca(π+, π-p), (π+, π+p), (π-, π-p), E=250 MeV; measured σ(θ(π), θp) vs pion momentum. Enriched Ca target, energetic pion spectrometer.
doi: 10.1016/0370-2693(86)91567-4
1985BA30 Phys.Rev. C32, 239 (1985) M.L.Barlett, G.W.Hoffmann, J.A.McGill, B.Hoistad, L.Ray, R.W.Fergerson, E.C.Milner, J.A.Marshall, J.F.Amann, B.E.Bonner, J.B.McClelland Proton-Nucleon Spin-Rotation and -Depolarization Parameters at 800 MeV NUCLEAR REACTIONS 1H, 1n(polarized p, p), E=800 MeV; measured spin polarization, depolarization parameters vs θ. Liquid deuterium target.
doi: 10.1103/PhysRevC.32.239
1985BL22 Phys.Rev. C32, 2152 (1985) G.S.Blanpied, B.G.Ritchie, M.L.Barlett, G.W.Hoffmann, J.A.McGill, M.A.Franey, M.Gazzaly Elastic Scattering of 0.8 GeV Protons from the Non-Zero-Spin Nuclei 13C and 14N NUCLEAR REACTIONS 12,13C, 14N(p, p), (polarized p, p), E=0.8 GeV; measured σ(θ), analyzing power vs θ; deduced optical potential parameters.
doi: 10.1103/PhysRevC.32.2152
1985HO16 Phys.Rev.Lett. 55, 29 (1985) C.L.Hollas, K.H.McNaughton, P.J.Riley, Shen-wu Xu, B.E.Bonner, O.B.van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet Wolfenstein Polarization Observables for the Reaction p(pol)p → p(pol)πn at 800 MeV NUCLEAR REACTIONS 1H(polarized p, pπ+), E=650, 733, 800 MeV; measured Wolfenstein polarization parameters, induced polarization, σ(θ1, θ2) vs proton momentum.
doi: 10.1103/PhysRevLett.55.29
1985MI04 Phys.Rev.Lett. 54, 1237 (1985) C.Milner, M.Barlett, G.W.Hoffmann, S.Bart, R.E.Chrien, P.Pile, P.D.Barnes, G.B.Franklin, R.Grace, H.S.Plendl, J.F.Amann, T.S.Bhatia, T.Kozlowski, J.C.Peng, R.R.Silbar, H.A.Thiessen, C.Glashausser, J.A.McGill, R.Hackenburg, E.V.Hungerford, R.L.Stearns Observation of Lambda-Hypernuclei in the Reaction 12C(π+, K+)12C(Lamdba) NUCLEAR REACTIONS 12C(π+, K+), E at 716, 728 MeV/c; measured σ(θ); deduced 12C hypernuclear levels.
doi: 10.1103/PhysRevLett.54.1237
1985SE14 Phys.Lett. 158B, 23 (1985) K.K.Seth, D.Barlow, A.Saha, R.Soundranayagam, S.Iversen, M.Kaletka, M.Bosko, D.Smith, G.W.Hoffmann, M.L.Barlett, R.Fergerson, J.McGill, E.C.Milner Polarized Proton Inelastic Scattering from 40Ca and 48Ca at 500 MeV NUCLEAR REACTIONS 40,48Ca(polarized p, p'), E=500 MeV; measured σ(θ), analyzing power vs θ. 40Ca(polarized p, p), E=500 MeV; analyzed spin rotation parameter vs θ; deduced optical potential parameters. 40,48Ca deduced mass deformation parameters, lengths.
doi: 10.1016/0370-2693(85)90731-2
1984BA33 Phys.Rev. C30, 279 (1984) M.L.Barlett, G.W.Hoffmann, J.A.McGill, R.W.Fergerson, E.C.Milner, J.A.Marshall, J.F.Amann, B.E.Bonner, J.B.McClelland Forward-Angle Elastic p(pol)p Spin-Depolarization and -Rotation Parameters at 0.8 GeV NUCLEAR REACTIONS 1H(polarized p, p), E=800 MeV; measured spin rotation, spin depolarization parameters vs θ. Global phase shift analysis.
doi: 10.1103/PhysRevC.30.279
1984BL14 Phys.Rev. C30, 1233 (1984) G.S.Blanpied, G.A.Balchin, G.E.Langston, B.G.Ritchie, M.L.Barlett, G.W.Hoffmann, J.A.McGill, M.A.Franey, M.Gazzaly, B.H.Wildenthal Excitation of the Ground State Rotational Band in 20Ne by 0.8 GeV Protons NUCLEAR REACTIONS 20Ne(polarized p, p'), E=0.8 GeV; measured σ(θ), analyzing power vs θ, σ(Ep'); deduced potential parameters. 20Ne levels deduced β, B(λ). Coupled-channels calculation.
doi: 10.1103/PhysRevC.30.1233
1984HI10 Phys.Rev. C30, 1976 (1984) N.M.Hintz, M.A.Franey, M.M.Gazzaly, D.Cook, G.S.Kyle, D.Dehnhard, S.J.Seestrom-Morris, G.W.Hoffmann, M.Barlett, G.S.Blanpied, J.A.McGill, J.B.McClelland, R.L.Boudrie, F.Irom, G.Pauletta High Spin States in 28Si and 58Ni NUCLEAR REACTIONS 28Si, 58Ni(p, p'), E=333, 498, 800 MeV; measured σ(θ), σ(Ep). 28Si, 58Ni levels deduced transition densities. DWIA, other (p, p'), (e, e') data analysis.
doi: 10.1103/PhysRevC.30.1976
1984MC02 Phys.Rev. C29, 204 (1984) J.A.McGill, G.W.Hoffmann, M.L.Barlett, R.W.Fergerson, E.C.Milner, R.E.Chrien, R.J.Sutter, T.Kozlowski, R.L.Stearns Proton + Nucleus Inclusive (p, p') Scattering at 800 MeV NUCLEAR REACTIONS 1,2H, 12C, 40Ca, 208Pb(p, p'X), E=800 MeV; measured σ(θ, Ep); deduced angle integrated σ, pion production mechansim. Quasifree scattering formalism.
doi: 10.1103/PhysRevC.29.204
1984MC04 Phys.Lett. 134B, 157 (1984) J.A.McGill, C.Glashausser, K.Jones, S.K.Nanda, M.Barlett, R.Fergerson, J.A.Marshall, E.C.Milner, G.W.Hoffmann Inclusive (p, p') Cross Sections and Analyzing Powers for 1H and 12C in the Delta Region NUCLEAR REACTIONS 1H, 12C(polarized p, p'X), E=800 MeV; measured σ(θ), analyzing power vs θ.
doi: 10.1016/0370-2693(84)90661-0
1984NA02 Phys.Rev. C29, 660 (1984) S.K.Nanda, C.Glashausser, K.W.Jones, J.A.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, J.R.Comfort, S.Levenson, R.Segel, H.Ohnuma 10.23 MeV M1 Transition in the 48Ca(p(pol), p'(pol))48Ca Reaction at 319 MeV NUCLEAR REACTIONS 48Ca(polarized p, p'), E=319 MeV; measured σ(θ), analyzing power, spin-flip probability vs θ. 48Ca deduced M1 transition strength, energy. DWIA analysis.
doi: 10.1103/PhysRevC.29.660
1984NA14 J.Phys.(Paris), Colloq.C4, 459 (1984); See 1984Na29 S.K.Nanda, C.Glashausser, K.W.Jones, J.S.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, J.R.Comfort, S.Levenson, R.Segel, H.Ohnuma Spin Flip Strength at High Excitation Energy in the 90Zr(p(pol), p(pol)')90Zr Reaction
1984NA29 J.Phys.(Paris), Colloq.C-4, 459 (1984) S.K.Nanda, C.Glashausser, K.W.Jones, J.S.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, J.R.Comfort, S.Levenson, R.Segel, H.Ohnuma Spin Flip Strength at High Excitation Energy in the 90Zr(p(pol), p(pol)')90Zr Reaction NUCLEAR REACTIONS 90Zr(polarized p, p'), E=319 MeV; measured σ(Ep', θp'), σ(θ), analyzing power, spin-flip σ, probability. 90Zr deduced possible M1 transitions. DWIA calculations.
1983BA05 Phys.Rev. C27, 682 (1983) M.L.Barlett, G.W.Hoffmann, J.A.McGill, B.Hoistad, L.Ray, R.W.Fergerson, E.C.Milner, J.A.Marshall, J.F.Amann, B.E.Bonner, J.B.McClelland, G.S.Blanpied, R.A.Arndt Forward-Angle Elastic and Quasielastic Proton-Nucleon Cross Sections and Analyzing Powers at 0.8 GeV NUCLEAR REACTIONS 1H(p, p), (polarized p, p), E=800 MeV; measured σ(θ), analyzing power vs θ. 2H(polarized p, 2p), (polarized p, pn), E=800 MeV; measured analyzing power vs θ, quasielastic scattering; deduced proton nucleus amplitudes. Liquid hydrogen, deuterium, CH, CH2 targets. 40Ca(polarized p, p), E=800 MeV; analyzed σ(θ), analyzing power data; deduced medium correction effects. Kerman-McManus-Thaler formalism, amplitude input from present data.
doi: 10.1103/PhysRevC.27.682
1983MO04 Phys.Lett. 123B, 37 (1983) C.L.Morris, J.F.Amann, S.J.Seestrom-Morris, J.A.McGill, C.Glashausser, K.Jones, S.Nanda, M.Barlett, G.W.Hoffmann, C.Milner, C.F.Moore, J.R.Comfort, L.C.Bland, R.Gilman Low-Momentum Delta Production in the 13C(p, d)12C Reaction NUCLEAR REACTIONS 13C(p, d), E=800 MeV; measured inclusive deuteron production σ, dp-, dπ-, dpp-coin; deduced isobar-hole admixtures in 12C.
doi: 10.1016/0370-2693(83)90953-X
1983NA20 Phys.Rev.Lett. 51, 1526 (1983) S.K.Nanda, C.Glashausser, K.W.Jones, J.A.McGill, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, H.Ohnuma, M.Franey, M.Gazzaly, N.Hintz Fine Structure and Spin Excitations in the Giant Resonance Region of 90Zr NUCLEAR REACTIONS 90Zr(polarized p, p'), E=319 MeV; measured σ(θ), σ(Ep'), analyzing power vs θ, spin-flip probabilities. 90Zr deduced M1 giant resonance, fine structure.
doi: 10.1103/PhysRevLett.51.1526
1982BL01 Phys.Rev. C25, 422 (1982) G.S.Blanpied, N.M.Hintz, G.S.Kyle, M.A.Franey, S.J.Seestrom-Morris, R.K.Owen, J.W.Palm, D.Dehnhard, M.L.Barlett, C.J.Harvey, G.W.Hoffmann, J.A.McGill, R.P.Liljestrand, L.Ray Elastic and Inelastic Scattering of 0.8 GeV Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(p, p), (p, p'), E=0.8 GeV; measured σ(θ). 24,26Mg deduced deformation lengths, multipole moments. Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.25.422
1982BL08 Phys.Rev. C25, 2550 (1982) G.S.Blanpied, M.L.Barlett, G.W.Hoffmann, J.A.McGill Scattering of 0.8 GeV Protons from 14N NUCLEAR REACTIONS 14N(p, p'), E=0.8 GeV; measured σ(θ), σ(Ep'). 14N levels deduced deformation lengths. DWBA analysis.
doi: 10.1103/PhysRevC.25.2550
1982BL10 Phys.Rev. C25, 2563 (1982) E.Bleszynski, M.Bleszynski, S.Hajisaeid, G.J.Igo, F.Irom, J.B.McClelland, G.Pauletta, A.Rahbar, A.T.Wang, C.A.Whitten, Jr., G.Adams, M.Barlett, G.W.Hoffmann, J.A.McGill, R.Boudrie, G.Kyle Large Angle Elastic and Inelastic Scattering of Protons from 40Ca at 800 MeV NUCLEAR REACTIONS 40Ca(p, p), (p, p'), (polarized p, p), (polarized p, p'), E=0.8 GeV; measured σ(Ep'), σ(θ), A(θ). 40Ca deduced ground state density distribution, correlation length, deformation parameters β2, β3, β5. Glauber multiple scattering theory.
doi: 10.1103/PhysRevC.25.2563
1981BL07 Phys.Rev. C23, 2599 (1981) G.S.Blanpied, G.W.Hoffmann, M.L.Barlett, J.A.McGill, S.J.Greene, L.Ray, O.B.Van Dyck, J.Amann, H.A.Thiessen Large Angle Scattering of 0.8 GeV Protons from 12C NUCLEAR REACTIONS 12C(p, p'), E=800 MeV; measured σ(θ). 12C deduced charge density multipole moments M(E2), M(E4). Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.23.2599
1981HO20 Phys.Rev. C24, 541 (1981) G.W.Hoffmann, L.Ray, M.Barlett, W.R.Coker, J.McGill, G.S.Adams, G.J.Igo, F.Irom, A.T.M.Wang, C.A.Whitten, Jr., R.L.Boudrie, J.F.Amann, C.Glashausser, N.M.Hintz, G.S.Kyle, G.S.Blanpied A(y)(θ) for p(pol) + 208Pb Elastic Scattering at 0.8 GeV and a Test of Multiple Scattering Theory NUCLEAR REACTIONS 208Pb(polarized p, p), E=0.8 GeV; measured analyzing power vs θ. Microscopic optical model, second-order Kerman-McManus-Thaler multiple scattering approach, electromagnetic spin-orbit term.
doi: 10.1103/PhysRevC.24.541
1981HO26 Phys.Rev.Lett. 47, 1436 (1981) G.W.Hoffmann, L.Ray, M.L.Barlett, R.Fergerson, J.McGill, E.C.Milner, K.K.Seth, D.Barlow, M.Bosko, S.Iversen, M.Kaletka, A.Saha, D.Smith Elastic Scattering of 500-MeV Polarized Protons from 40,48Ca, 90Zr, and 208Pb, and Breakdown of the Impulse Approximation at Small Momentum Transfer NUCLEAR REACTIONS 40,48Ca, 90Zr, 208Pb(polarized p, p), E=500 MeV; measured σ(θ), A(θ); deduced impulse approximation breakdown. Second-order. Kerman-McManus-Thaler optical potential.
doi: 10.1103/PhysRevLett.47.1436
1981RA02 Phys.Rev. C23, 828 (1981) L.Ray, G.W.Hoffmann, M.Barlett, J.McGill, J.Amann, G.Adams, G.Pauletta, M.Gazzaly, G.S.Blanpied Proton Elastic Scattering from 40,42,44,48Ca at 800 MeV NUCLEAR REACTIONS 40,42,44,48Ca(p, p), E=800 MeV; measured σ(θ); analyzed analyzing power data. 40,42,44,48Ca deduced neutron, isotopic density differences. Second-order Kerman-McManus-Thaler optical potential.
doi: 10.1103/PhysRevC.23.828
1980BA30 Phys.Rev. C22, 1168 (1980) M.L.Bartlett, J.A.McGill, L.Ray, M.M.Bartlett, G.W.Hoffmann, N.M.Hintz, G.S.Kyle, M.A.Franey, G.Blanpied Proton Scattering from 154Sm and 176Yb at 0.8 GeV NUCLEAR REACTIONS 154Sm, 176Yb(p, p), (p, p'), E=0.8 GeV; measured σ(θ); deduced optical model parameters. 154Sm, 176Yb levels deduced deformation lengths. DWBA, coupled channel analysis, rotational model. Enriched targets.
doi: 10.1103/PhysRevC.22.1168
1980HO09 Phys.Rev. C21, 1488 (1980) G.W.Hoffman, L.Ray, M.Barlett, J.McGill, G.S.Adams, G.J.Igo, F.Irom, A.T.M.Wang, C.A.Whitten, Jr., R.L.Boudrie, J.F.Amann, C.Glashausser, N.M.Hintz, G.S.Kyle, G.S.Blanpied 0.8 GeV p + 208Pb Elastic Scattering and the Quantity Δr(np) NUCLEAR REACTIONS 208Pb(p, p), E=0.8 GeV; measured σ(θ); deduced neutron, proton rms radius difference. Microscopic optical model analysis.
doi: 10.1103/PhysRevC.21.1488
1976BO32 Phys.Rev.Lett. 37, 1206 (1976) J.E.Bolger, W.J.Braithwaite, J.J.Kraushaar, J.McGill, C.F.Moore, C.L.Morris, R.J.Peterson, R.A.Ristinen, G.Smith, L.E.Smith, H.A.Thiessen, J.Whitenton Comparison of Neutron Removal from 7Li by π± with Free Pion-Nucleon Results NUCLEAR REACTIONS 7Li(π-, π-n), (π+, π+n), E=50-290 MeV; measured σ(E).
doi: 10.1103/PhysRevLett.37.1206
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