NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.C.Phillips Found 136 matches. Showing 1 to 100. [Next]1990BO06 Phys.Rev. D41, 13 (1990) B.E.Bonner, J.A.Buchanan, J.M.Clement, M.D.Corcoran, N.M.Krishna, J.W.Kruk, H.E.Miettinen, R.M.Moss, G.S.Mutchler, F.Nessi-Tedaldi, M.Nessi, G.C.Phillips, J.B.Roberts, P.M.Stevenson, S.R.Tonse, A.Birman, S.U.Chung, A.Etkin, R.C.Fernow, H.Kirk, S.D.Protopopescu, H.Willutzki, T.Hallman, L.Madansky, Z.Bar-Yam, J.Dowd, W.Kern, E.King, B.W.Mayes, L.S.Pinsky Analyzing Power of Inclusive Production of π+, π-, and K(S)0 by Polarized Protons at 13.3 and 18.5 GeV/c NUCLEAR REACTIONS Be(polarized p, π+), (polarized p, π-), (polarized p, K0), E at 13.3, 18.5 GeV/c; measured meson production analyzing power.
doi: 10.1103/PhysRevD.41.13
1988PA22 Phys.Rev. C38, 2716 (1988) P.V.Pancella, G.S.Mutchler, S.D.Baker, J.W.Kruk, I.M.Duck, M.D.Corcoran, G.C.Phillips, J.M.Clement, J.A.Buchanan, B.W.Mayes, L.S.Pinsky, W.von Witsch, E.Andrade, H.Garcilazo, J.M.Laget Measurement of π+d → Δ++n at Intermediate Energy NUCLEAR REACTIONS 2H(π+, π+p), E at 312-600 MeV/c; measured σ(θ(π), θ(p)) vs pion momentum; deduced σ(θ) for reaction 2H(π+, Δ++).
doi: 10.1103/PhysRevC.38.2716
1985MA06 Phys.Rev. D31, 966 (1985) W.P.Madigan, D.A.Bell, J.A.Buchanan, M.M.Calkin, J.M.Clement, M.Copel, M.D.Corcoran, K.A.Johns, J.D.Lesikar, H.E.Miettinen, G.S.Mutchler, C.J.Naudet, G.P.Pepin, G.C.Phillips, J.B.Roberts, S.E.Turpin, E.V.Hungerford, B.W.Mayes, A.D.Hancock, L.S.Pinsky, K.K.Sekharan, C.L.Hollas, P.J.Riley, J.C.Allred, B.E.Bonner, P.Cameron, S.T.Linn, W.von Witsch, M.Furic, V.Valkovic Transverse-Spin Dependence of the p-p Total Cross Section Δσ(T) from 0.8 to 2.5 GeV/c NUCLEAR REACTIONS 1H(polarized p, p), E at 0.8-2.5 GeV/c; measured σ asymmetry, transverse spin dependence. Polarized target.
doi: 10.1103/PhysRevD.31.966
1984PH01 Nucl.Instrum.Methods 221, 334 (1984) G.C.Phillips, E.A.Umland, G.S.Mutchler, J.B.Roberts, M.Duong-Van, J.A.Buchanan, J.B.Donahue, J.C.Allred, B.W.Noel, T.A.Mulera, B.Aas, B.W.Mayes A Novel Neutrino Detection System NUCLEAR REACTIONS 1H(ν-bar, e+), E=40 MeV; measured e+n(t); deduced potential neutrino experiment applications. Liquid scintillator modules, drift chambers.
doi: 10.1016/0167-5087(84)90004-8
1983HA11 Phys.Rev. C27, 2742 (1983) A.D.Hancock, R.W.Hackenburg, J.M.Hungerford, B.W.Mayes, L.S.Pinsky, J.C.Allred, T.M.Williams, S.D.Baker, J.A.Buchanan, J.M.Clement, M.Copel, I.M.Duck, G.S.Mutchler, G.P.Pepin, E.A.Umland, G.C.Phillips, M.W.McNaughton, C.Hwang, M.Furic Asymmetries and Cross Sections for the Reaction p(pol) + p → p + π+ + n at 800 MeV NUCLEAR REACTIONS 1H(polarized p, π+p), E=800 MeV; measured σ(θp, σ(π)) vs proton momemtum, analyzing power. Polarized target.
doi: 10.1103/PhysRevC.27.2742
1981HO01 Phys.Rev. C23, 407 (1981) J.H.Hoftiezer, S.D.Baker, J.M.Clement, W.H.Dragoset, I.M.Duck, R.D.Felder, D.M.Judd, G.S.Mutchler, G.P.Pepin, G.C.Phillips, E.A.Umland, J.C.Allred, E.V.Hungerford III, B.W.Mayes, L.S.Pinsky, T.M.Williams, M.Furic, W.von Witsch Reaction πd → pπn in the Δ Resonance Region NUCLEAR REACTIONS 2H(π+, π+p), (π-, π-p), E at 340 MeV/c; measured σ(θp, θ(π), proton momentum). DWIA model, dibaryon resonances.
doi: 10.1103/PhysRevC.23.407
1981LO05 Phys.Rev. C23, 1656 (1981) J.W.Low, E.V.Hungerford, J.C.Allred, B.W.Mayes, L.S.Pinsky, M.L.Warneke, T.M.Williams, J.M.Clement, W.H.Dragoset, R.D.Felder, J.H.Hoftiezer, J.Hudomalj-Gabitzsch, G.S.Mutchler, G.C.Phillips Angular Distribution of the Reaction pd → 3Heπ0 at 800 MeV NUCLEAR REACTIONS 2H(p, 3He), E=800 MeV; measured σ(θ). Magnetic spectrometer. Ruderman model.
doi: 10.1103/PhysRevC.23.1656
1980AN06 Nucl.Phys. A337, 365 (1980) E.Andrade, D.Miljanic, G.C.Phillips Analysis of Angular Distribution of Proton-Neutron FSI in the Reaction 2H(p, pn)1H at E = 12.5 MeV NUCLEAR REACTIONS 2H(p, pn), E=12.5 MeV; measured pn-coin; deduced angular dependence of final state interaction. Watson-Migdal, exact three-body models.
doi: 10.1016/0375-9474(80)90148-7
1980BE29 Phys.Lett. B94, 310 (1980) D.A.Bell, J.A.Buchanan, M.M.Calkin, J.M.Clement, W.H.Dragoset, M.Furic, K.A.Johns, J.D.Lesikar, H.E.Miettinen, T.A.Mulera, G.S.Mutchler, G.C.Phillips, J.B.Roberts, S.E.Turpin Measurement of the Spin Parameters A and A(nn) in pp Elastic Scattering in the 1-3 GeV/c Region NUCLEAR REACTIONS 1H(polarized p, p), E at 1.1, 2.75 GeV/c; measured asymmetry, spin correlation parameter vs θ. Polarized target.
doi: 10.1016/0370-2693(80)90885-0
1979HO26 Phys.Lett. 88B, 73 (1979) J.H.Hoftiezer, M.Furic, G.S.Mutchler, I.M.Duck, W.H.Dragoset, J.M.Clement, D.M.Judd, R.D.Felder, G.P.Pepin, W.von Witsch, G.C.Phillips, J.C.Allred, E.V.Hungerford, B.W.Mayes, L.S.Pinsky, T.M.Williams Reaction Mechanisms and Isospin Effects for the π+ + D → p + π+ + n Processes at Pπ = 340 MeV/c NUCLEAR REACTIONS 2H(π+, π+p), (π-, π-p), E at 340 MeV/c; measured σ; deduced reaction mechanism, isospin effects, role of spectator particle.
doi: 10.1016/0370-2693(79)90117-5
1979LO08 Phys.Rev. C20, 1479 (1979) J.W.Lo, E.V.Hungerford, J.C.Allred, B.W.Mayes, L.S.Pinsky, M.L.Warneke, T.M.Williams, J.M.Clement, W.H.Dragoset, R.D.Felder, J.H.Hoftiezer, J.Hudomalj-Gabitzsch, G.S.Mutchler, G.C.Phillips Pion Production in the Reaction d(p;d, π)n at 800 MeV with a Spectator Neutron NUCLEAR REACTIONS 2H(p, π+d), E=800 MeV; measured σ(θd, θπ); deduced validity of spectator model.
doi: 10.1103/PhysRevC.20.1479
1978HO03 Phys.Rev. C17, 259 (1978) K.R.Hogstrom, G.S.Mutchler, T.R.Witten, J.Hudomalj-Gabitzsch, J.M.Clement, R.D.Felder, W.H.Dragoset, W.P.Madigan, J.A.Buchanan, G.C.Phillips, E.V.Hungerford, B.W.Mayes, L.Pinsky, L.Y.Lee, T.M.Williams, J.C.Allred Pion Production from the pd → dπ+n Reaction at 585 MeV NUCLEAR REACTIONS 2H(p, π+d), E=585 MeV; measured σ(Ed, Eπ+, θπ+) in kinematically complete experiment.
doi: 10.1103/PhysRevC.17.259
1978HU13 Phys.Rev. C18, 2666 (1978) J.Hudomalj-Gabitzsch, I.M.Duck, M.Furic, G.S.Mutchler, J.M.Clement, R.D.Felder, W.H.Dragoset, G.C.Phillips, J.C.Allred, E.V.Hungerford, B.W.Mayes, L.S.Pinsky, T.M.Williams Production of the Δ++ in the Reaction pp → pπ+n at 800 MeV NUCLEAR REACTIONS 1H(p, p'π+), E=800 MeV; measured σ(Ep', θp, θπ); deduced form factor range parameters, Δ++ intermediate state.
doi: 10.1103/PhysRevC.18.2666
1977FE06 Nucl.Phys. A280, 308 (1977) R.D.Felder, T.M.Williams, G.S.Mutchler, I.Duck, J.Hudomalj-Gabitzsch, M.Furic, D.Mann, N.D.Gabitzsch, J.M.Clement, G.C.Phillips, T.R.Witten, E.V.Hungerford, M.Warneke, B.W.Mayes, L.Y.Lee, J.C.Allred Final State Interactions in Deuteron Breakup by Protons at 585 and 800 MeV NUCLEAR REACTIONS 2H(p, 2p), E=585, 800 MeV; measured σ(θ); deduced singlet, triplet contributions in pn final state interactions.
doi: 10.1016/0375-9474(77)90607-8
1977MI13 Nucl.Phys. A290, 27 (1977) D.Miljanic, E.Andrade, J.Hudomalj-Gabitzsch, G.S.Mutchler, G.C.Phillips Mechanisms in d + 6Li Three-Body Reactions at Low Bombarding Energies NUCLEAR REACTIONS 6Li(d, 2d), (d, dα), (d, pt), (d, pα), (d, tα), E=7.5, 9, 10, 10.5 MeV; measured (E;E1, E2, θ1, θ2); deduced reaction mechanisms. Enriched target.
doi: 10.1016/0375-9474(77)90662-5
1976FE05 Nucl.Phys. A264, 397 (1976) R.D.Felder, T.R.Witten, T.M.Williams, M.Furic, G.S.Mutchler, N.D.Gabitzsch, J.Hudomalj-Gabitzsch, J.M.Clement, Jr., G.C.Phillips, E.V.Hungerford, L.Y.Lee, M.Warneke, B.W.Mayes, J.C.Allred Quasi-Free Scattering in Proton-Induced Deuteron Breakup at 585 and 800 MeV NUCLEAR REACTIONS 2H(p, 2p), (p, pn), E=585, 800 MeV; measured σ(Ep, θ1, θ2); deduced deuteron momentum distribution via spectator model.
doi: 10.1016/0375-9474(76)90413-9
1976PL01 Nucl.Phys. A256, 189 (1976) R.Plasek, V.Valkovic, G.C.Phillips A Study of the Neutron-Proton Final State Interaction in Proton-Induced Deuteron Breakup NUCLEAR REACTIONS 2H(p, 2p), (p, pn), E=8-12 MeV; measured σ(E;Ep, En, θp, θn).
doi: 10.1016/0375-9474(76)90103-2
1975CH25 Phys.Rev. A12, 52 (1975) R.P.Chaturvedi, R.M.Wheeler, R.B.Liebert, D.J.Miljanic, T.Zabel, G.C.Phillips L-Shell X-Ray Production Cross Sections of Pd, Ag, and Sn for Incident Proton Energies in the Range 3-12 MeV and Oxygen Ions in the Range 15-40 MeV NUCLEAR REACTIONS Pd, Ag, Sn(p, p), E=3-12 MeV; Pd, Ag, Sn(16O, 16O), E=15-40 MeV; measured absolute L-shell X-ray σ.
doi: 10.1103/PhysRevA.12.52
1975MU06 Phys.Rev. C11, 1873 (1975) G.S.Mutchler, C.R.Fletcher, L.V.Coulson, D.Mann, N.D.Gabitzsch, G.C.Phillips, B.W.Mayes, E.V.Hungerford, L.Y.Lee, C.Goodman, J.C.Allred Nuclear-Coulomb Interference in π±-16O Scattering NUCLEAR REACTIONS 16O(π+, π+), (π-, π-), E=155, 185, 213 MeV; measured σ(θ); deduced real part of forward scattering amplitude.
doi: 10.1103/PhysRevC.11.1873
1975VA04 Nucl.Phys. A239, 260 (1975) V.Valkovic, D.Miljanic, R.B.Liebert, G.C.Phillips Energy Dependence of the Cross Sections for the d + 10B → 3α and the p + 11B → 3α Reactions NUCLEAR REACTIONS 10B(d, α), E=2.5-4.5 MeV; measured σ(E, Eα, θ), αα-coin, absolute σ. 11B(p, α), E=7.5-10.5 MeV; measured σ(E, Eα), αα-coin.
doi: 10.1016/0375-9474(75)90450-9
1975WI29 Nucl.Phys. A254, 269 (1975) T.R.Witten, M.Furic, G.S.Mutchler, C.R.Fletcher, N.D.Gabitzsch, G.C.Phillips, J.Hudomalj, L.Y.Lee, B.W.Mayes, J.Allred, C.Goodman Quasi-Free Scattering and Final State Interactions in the Reaction 2H(p, 2p)n at 585 MeV NUCLEAR REACTIONS 2H(p, 2p), E=585 MeV; measured σ; deduced 2H momentum distribution.
doi: 10.1016/0375-9474(75)90216-X
1974MA37 Nucl.Phys. A230, 515 (1974) B.W.Mayes, L.Y.Lee, J.C.Allred, C.Goodman, G.S.Mutchler, E.V.Hungerford, M.L.Scott, G.C.Phillips Pion Small-Angle Multiple Scattering at Energies Spanning the (3, 3) Resonance NUCLEAR REACTIONS C, Al, Cu, Pb(π+, π+), (π-, π-), E=139-220 MeV; measured Coulomb multiple scattering; deduced gaussian width. calculated multiple scattering distribution.
doi: 10.1016/0375-9474(74)90154-7
1974MI10 Phys.Lett. 50B, 330 (1974) D.Miljanic, J.Hudomalj, G.S.Mutchler, E.Andrade, G.C.Phillips Quasi-Free Contributions in the d + 6Li Reactions at Low Energies NUCLEAR REACTIONS 6Li(d, 2d), (d, αd), (d, tp), E=7.5-10.5 MeV; measured σ, deduced reaction mechanism.
doi: 10.1016/0370-2693(74)90682-0
1974MU03 Phys.Rev. C9, 1198 (1974) G.S.Mutchler, M.L.Scott, C.R.Fletcher, E.V.Hungerford, L.V.Coulson, N.D.Gabitzsch, G.C.Phillips, B.W.Mayes, L.Y.Lee, J.C.Allred, C.Goodman Nuclear-Coulomb Interference in π+-12C Scattering NUCLEAR REACTIONS 12C(π+, π+), E=115-242 MeV; measured σ(θ); deduced forward-scattering amplitude.
doi: 10.1103/PhysRevC.9.1198
1974VA16 Lett.Nuovo Cim. 10, 461 (1974) V.Valkovic, R.B.Liebert, R.Plasek, R.M.Wheeler, T.Zabel, G.C.Phillips Neutron-Proton Coincidences from the 12C(16O, np)26Al Reaction NUCLEAR REACTIONS 12C(16O, np), E=30, 36 MeV; measured np-coin, deduced missing mass spectrum. 26Al deduced levels.
1974VA31 Nucl.Instrum.Methods 122, 533 (1974) V.Valkovic, R.B.Liebert, G.C.Phillips (16O, np) and (16O, nα) Reactions on Some Light Nuclei NUCLEAR REACTIONS 9Be, 12,13C(16O, np), (16O, nα), E=30, 36 MeV; measured np-, nα-coin; deduced missing mass spectrum.
1973AN25 Nucl.Instrum.Methods 113, 93 (1973) E.Andrade, D.Rendic, V.A.Otte, G.C.Phillips Charged Particle Mass Identification by Energy-Time-of-Flight Technique NUCLEAR REACTIONS 12C(d, X), E=12 MeV; measured σ(E(X), mass(X)).
doi: 10.1016/0029-554X(73)90483-7
1973FU12 Phys.Lett. 47B, 241 (1973) M.Furic, C.R.Fletcher, N.D.Gabitzsch, G.S.Mutchler, T.R.Witten, G.C.Phillips, J.Hudomalj, D.Y.Lee, P.A.M.Gram, B.W.Mayes, J.Allred, C.Goodman Neutron-Proton Final State Interaction in p-d Breakup at E = 585 MeV NUCLEAR REACTIONS 2H(p, n2p), E=585 MeV; measured σ, pp-coin.
doi: 10.1016/0370-2693(73)90720-X
1973GA20 Phys.Lett. 47B, 234 (1973) N.D.Gabitzsch, G.S.Mutchler, C.R.Fletcher, E.V.Hungerford, L.Coulson, D.Mann, T.Witten, M.Furic, G.C.Phillips, B.Mayes, L.Y.Lee, J.Hudomalj, J.C.Allred, C.Goodman Pion-Nuclear Total Cross Sections Near the 3/2, 3/2 Resonance NUCLEAR REACTIONS 9Be, 12C, 16O, 27Al(π+, X), (π-, X), E=114-210 MeV; measured σ(E).
doi: 10.1016/0370-2693(73)90718-1
1973HO43 Nucl.Phys. A215, 598 (1973) K.R.Hogstrom, B.W.Mayes, L.Y.Lee, J.C.Allred, C.Goodman, G.S.Mutchler, C.R.Fletcher, G.C.Phillips Measurements of 12C(π+, πN)11C and 19F(π+, πN)18F Cross Sections Near the 3/2, 3/2 Resonance RADIOACTIVITY 11C, 18F; measured T1/2. NUCLEAR REACTIONS 12C, 19F(π+, πn); E(π+)=134-200 MeV; measured σ(R)(E(π+)).
doi: 10.1016/0375-9474(73)90492-2
1973MI20 Nucl.Phys. A215, 221 (1973) D.Miljanic, T.Zabel, R.B.Liebert, G.C.Phillips, V.Valkovic Quasi-Free Scattering in the 6Li(d, dd)4He Reaction at Low Bombarding Energies NUCLEAR REACTIONS 6Li(d, 2d), E=6, 7, 8, 8.5, 9, 10, 11 MeV; measured σ(E;E(d1), E(d2), θ(d)). Enriched target.
doi: 10.1016/0375-9474(73)90651-9
1973SA03 Nucl.Phys. A202, 49 (1973) J.Sandler, G.S.Mutchler, W.von Witsch, V.A.Otte, G.C.Phillips, D.Rendic Rescattering and Neutron-Proton Final-State Interaction in the 12C(d, pn)12C Reaction NUCLEAR REACTIONS 12C(d, np), E=5.00, 5.15, 5.39, 5.50, 9.20, 9.85 MeV; measured σ(Ep, θ(p)=θ(n)); deduced p-n final-state interaction.
doi: 10.1016/0375-9474(73)90240-6
1973VO06 Phys.Rev. C8, 403 (1973) W.von Witsch, G.S.Mutchler, G.C.Phillips, D.Miljanic Spatial Localization Effects in the 2H(d, pd)n Reaction NUCLEAR REACTIONS 2H(d, pd), E=8, 9, 10, 11, 12, 13 MeV; calculated σ(Ep).
doi: 10.1103/PhysRevC.8.403
1972AN02 Nucl.Phys. A183, 145 (1972) E.Andrade, V.Valkovic, D.Rendic, G.C.Phillips Angular Distributions of Quasi-Free Scattering Contributions in Deuteron Break-up by Protons and Deuterons NUCLEAR REACTIONS 2H(p, pn), E=12.5 MeV; 2H(d, pn), E=12.5 MeV; measured σ(E(p1), E(p2), Ep, En, θ(1)=-θ(2)=15-60°), (Ed, Ep, Ed, En, θ(1)=-θ(2)=15-40°).
doi: 10.1016/0375-9474(72)90935-9
1972CO11 Nucl.Phys. A184, 437 (1972) D.M.Corley, N.S.Wall, H.Palevsky, J.L.Friedes, R.J.Sutter, G.W.Bennett, W.D.Simpson, G.C.Phillips, G.W.Igo, R.L.Stearns Quasifree Scattering of 1 GeV Protons from 12C and 40Ca NUCLEAR REACTIONS 12C(p, p'), 40Ca(p, p')E=1 GeV; measured σ(Ep', θ). Quasifree spectrum.
doi: 10.1016/0375-9474(72)90418-6
1972CO42 Nucl.Instrum.Methods 101, 247 (1972) L.V.Coulson, C.R.Fletcher, E.V.Hungerford, G.S.Mutchler, G.C.Phillips, M.L.Scott, J.C.Allred, C.Goodman, B.W.Mayes An In-Flight Pion Beam Flux Monitor
doi: 10.1016/0029-554X(72)90196-6
1972DU12 Phys.Rev.Lett. 29, 875 (1972) I.M.Duck, V.Valkovic, G.C.Phillips Off-Energy-Shell Effects in Deuteron-Induced Deuteron Breakup NUCLEAR REACTIONS 2H(d, np), E=6-14 MeV; measured σ(Ed, Ep).
doi: 10.1103/PhysRevLett.29.875
1972HU12 Nucl.Phys. A197, 515 (1972) E.V.Hungerford, G.S.Mutchler, G.C.Phillips, M.L.Scott, J.C.Allred, L.Y.Lee, B.W.Mayes, C.Goodman Proton Small Angle Multiple Scattering at 600 MeV NUCLEAR REACTIONS C, Al, Cu, Cd, Pb(n, n), E=600 MeV; measured small-angle multiple scattering σ.
doi: 10.1016/0375-9474(72)91026-3
1972NI02 Nucl.Phys. A179, 263 (1972) A.Niiler, R.J.Spiger, W.von Witsch, G.C.Phillips Three-Body Break-up in the 3He+d Reaction NUCLEAR REACTIONS 3He(d, p3He), 3He(d, pt), E=10.92 MeV; measured yield of three-body break-up reactions. Enriched target.
doi: 10.1016/0375-9474(72)90368-5
1972SC18 Phys.Rev.Lett. 28, 1209 (1972) M.L.Scott, G.S.Mutchler, C.R.Fletcher, E.V.Hungerford, L.V.Coulson, G.C.Phillips, B.W.Mayes, L.Y.Lee, J.C.Allred, C.Goodman Nuclear-Coulomb Interference in π+-12C Scattering NUCLEAR REACTIONS 12C(π+, π+), E=115, 167, 242 MeV; measured σ(θ); deduced Coulomb-nuclear interference effects, real part of forward nuclear amplitude.
doi: 10.1103/PhysRevLett.28.1209
1972TA04 Nucl.Phys. A182, 558 (1972) M.C.Taylor, V.Valkovic, G.C.Phillips Study of the 9Be(3He, αα)4He Reaction NUCLEAR REACTIONS 9Be(3He, αα), E=3, 4 MeV; measured σ(E(α1), E(α2), θ(α1), θ(α2)).
doi: 10.1016/0375-9474(72)90535-0
1972VA04 Nucl.Phys. A182, 225 (1972) V.Valkovic, N.Gabitzsch, D.Rendic, I.Duck, G.C.Phillips Coincidence Spectra from d + d → d + p + n and p + d → p + p + n Reactions with Neutron Detection at Zero Degrees NUCLEAR REACTIONS 2H(p, pn), E=10 MeV; 2H(d, np), E=10 MeV; measured σ(Ep, En, θ(n)=0°, θ(p)=15-40°), σ(Ep, En, θ(n)=0°, θ(d)=15-35°).
doi: 10.1016/0375-9474(72)90273-4
1972VA05 Nucl.Phys. A183, 126 (1972) V.Valkovic, I.Duck, W.E.Sweeney, G.C.Phillips Three-Body Break-up in the d+d → d+p+n Reaction NUCLEAR REACTIONS 2H(d, pn), E=6-13 MeV; measured σ(E;Ed, Ep, En, θ=θ(1)=-θ(2)=20°).
doi: 10.1016/0375-9474(72)90934-7
1972VA35 Phys.Lett. 42B, 191 (1972) V.Valkovic, I.M.Duck, G.C.Phillips Coulomb Effects in Deuteron-Induced Deuteron Break-up
doi: 10.1016/0370-2693(72)90057-3
1972VO01 Nucl.Phys. A180, 402 (1972) W.von Witsch, M.Ivanovich, D.Rendic, V.Valkovic, G.C.Phillips, K.Schafer Decay of 12C via the 11B(p, 2α)α Reaction NUCLEAR REACTIONS 11B(p, 2α)α, E=1.39, 1.98, 2.62 MeV; measured σ(E(α1), E(α2), θ(α1), θ(α2)). 12C resonance deduced J, π. Enriched target.
doi: 10.1016/0375-9474(72)90869-X
1971EM01 Nucl.Phys. A169, 317 (1971) S.T.Emerson, V.Valkovic, W.R.Jackson, C.Joseph, A.Niiler, W.D.Simpson, G.C.Phillips Final-State Interactions in the 9Be + p → d + 2α Reaction NUCLEAR REACTIONS 9Be(p, dα), (p, αα), (p, αd), E = 9 MeV; measured σ(Ed, Eα, θ(d), θ(α)), σ(E(α1), E(α2), θ(α1), θ(α2)), σ(Eα, Ed, θ(α), θ(d)).
doi: 10.1016/0375-9474(71)90887-6
1971JA08 Nucl.Phys. A166, 525 (1971) W.R.Jackson, V.Valkovic, S.T.Emerson, W.D.Simpson, C.Joseph, Y.S.Chen, M.C.Taylor, G.C.Phillips The 2H(p, pn)p Reaction at 9.0 MeV NUCLEAR REACTIONS 2H(p, pn), E=9 MeV; measured σ(Ep, En, θ(p), θ(n)); deduced final state interactions, quasifree scattering contributions.
doi: 10.1016/0375-9474(71)90904-3
1971MU18 Nucl.Phys. A172, 469 (1971) G.S.Mutchler, D.Rendic, D.E.Velkley, W.E.Sweeney, Jr., G.C.Phillips The (d, n) Reaction on 1p Shell Nuclei at E = 11.8 MeV NUCLEAR REACTIONS 10,11B(d, n), 12,13C(d, n), E=11.8 MeV; measured σ(En, θ). 11,12C, 13,14N deduced absolute S. Enriched targets.
doi: 10.1016/0375-9474(71)90038-8
1971OT02 Phys.Rev. C4, 322 (1971) V.A.Otte, W.von Witsch, J.Sandler, D.Rendic, G.C.Phillips Singlet Deuteron p-n Correlations in the 13C(p, pn)12C Reaction NUCLEAR REACTIONS 13C(p, pn), E=7.9-12.5 MeV; measured σ(E;Ep, θ(p), θ(n)); deduced singlet deuteron contribution.
doi: 10.1103/PhysRevC.4.322
1971RE19 Nucl.Phys. A178, 49 (1971) D.Rendic, N.D.Gabitzsch, V.Valkovic, W.von Witsch, G.C.Phillips d + 11B → 3α + n Four-Body Break-up and States in 9Be NUCLEAR REACTIONS 11B(d, 3α)n, E=10.425, 12.0 MeV; measured α-α, α-n coin spectra. Enriched target.
doi: 10.1016/0375-9474(71)90184-9
1971SW10 Phys.Lett. 37B, 183 (1971) W.E.Sweeney, Jr., V.Valkovic, D.Rendic, G.C.Phillips On the Observation of Rescattering Effects in the Reaction 7Li(d, nα)4He NUCLEAR REACTIONS 7Li(d, nα), E=2.07, 2.09 MeV; measured σ(En, Eα, θ(n), θ(α)); deduced rescattering effects.
doi: 10.1016/0370-2693(71)90046-3
1971VA03 Phys.Rev.Lett 26, 394 (1971) V.Valkovic, D.Rendic, V.A.Otte, G.C.Phillips Comparison of p-p and n-p Quasi-Free Scattering in p + d → p + p + n Reaction NUCLEAR REACTIONS 2H(p, 2p), (p, pn), E=12 MeV; measured σ(Ep1, Ep2), σ(Ep, En).
doi: 10.1103/PhysRevLett.26.394
1971VA14 Nucl.Phys. A166, 547 (1971) V.Valkovic, D.Rendic, V.A.Otte, W.von Witsch, G.C.Phillips Nucleon-Nucleon Quasi-Free Scattering in the p + d → p + p + n Reaction at Low Bombarding Energies NUCLEAR REACTIONS 2H(p, 2p)n, E=4.5-13 MeV; measured σ(E;Ep, En, θ(p), θ(n)); deduced p-p, p-n quasi-free scattering contributions.
doi: 10.1016/0375-9474(71)90906-7
1971VA28 Phys.Rev. C4, 2289 (1971) V.Valkovic, I.M.Duck, W.E.Sweeney, Jr., E.Andrade, G.C.Phillips Nuclear-Deuteron Quasifree Scattering in the Reaction d + d → d + p + n at Low Bombarding Energies NUCLEAR REACTIONS 2H(d, np), E=6-13 MeV; measured σ(E;Ed, En, θ(d), θ(n)), σ(E;Ed, Ep, θ(d), θ(p)).
doi: 10.1103/PhysRevC.4.2289
1971VO07 Nucl.Phys. A172, 633 (1971) W.von Witsch, M.Ivanovich, V.A.Otte, D.Rendic, G.C.Phillips Final-State Interactions in the 6Li(d;6Li, p)n Reaction NUCLEAR REACTIONS 6Li(d, 6Li)pn , E=10 MeV; measured σ(E(6Li), Ep, θ(6Li), θ(p)). Enriched target.
doi: 10.1016/0375-9474(71)90050-9
1970IV03 Nucl.Phys. A156, 616 (1970) M.Ivanovich, W.von Witsch, E.V.Hungerford III, G.C.Phillips Proton-Proton Final-State Interaction in the 2H(p, pn)p Reaction NUCLEAR REACTIONS 2H(p, pn), E=8-13 MeV; measured σ(Ep, En); deduced pp scattering length.
doi: 10.1016/0375-9474(70)90257-5
1970NI05 Phys.Rev. C1, 1342 (1970) A.Niiler, W.von Witsch, G.C.Phillips, C.Joseph, V.Valkovic The D(p, d*)p Cross Section from the D(p, 2p)n Reaction NUCLEAR REACTIONS 2H(p, 2p), E=9-13 MeV; measured σ(E;E(p1), E(p2), θ(p1), θ(p2)). 3He deduced 12.4-MeV state.
doi: 10.1103/PhysRevC.1.1342
1970SI01 Nucl.Phys. A140, 201 (1970) W.D.Simpson, J.L.Friedes, H.Palevsky, R.J.Sutter, G.W.Bennett, B.Gottschalk, G.Igo, R.L.Stearns, N.S.Wall, D.M.Corley, G.C.Phillips The 12C(p, 2p) and 2H(p, 2p) Reactions at 1.0 GeV NUCLEAR REACTIONS 12C(p, 2p), 2H(p, 2p), E=1 GeV; measured σ(Ep1, Ep2, θ(p1), θ(p2)); deduced distorted momentum distributions for P-, S-shells of C, the triplet state of D.
doi: 10.1016/0375-9474(70)90896-1
1970VA25 Phys.Lett. 33B, 208 (1970) V.Valkovic, W.Von Witsch, D.Rendic, G.C.Phillips Proton-Proton Quasi-Free Scattering in the p + d → p + p + n Reaction For E = 4.5-13.0 MeV NUCLEAR REACTIONS 2H(p, 2p)n, E=4.5-13 MeV; measured σ(E;Ep1, Ep2, θ(p1), θ(p2)).
doi: 10.1016/0370-2693(70)90573-3
1970VO06 Nucl.Phys. A150, 461 (1970) W.von Witsch, A.Niiler, J.Sandler, R.J.Spiger, G.C.Phillips Neutron-Neutron Final State Interactions in the Reaction 2H(d, pp)2n NUCLEAR REACTIONS 2H(d, 2p)2n, E=12 MeV; measured σ(Ep1, Ep2, θ(p1), θ(p2)). Enriched target.
doi: 10.1016/0375-9474(70)90410-0
1970VO15 Phys.Rev. C2, 2144 (1970) W.von Witsch, M.Ivanovich, D.Rendic, J.Sandler, G.C.Phillips Proton-Neutron Final-State Interactions in the D(d, dp)n Reaction NUCLEAR REACTIONS 2H(d, dp), E=11, 13 MeV; measured σ(Ep, Ed); deduced p-n final-state interaction.
doi: 10.1103/PhysRevC.2.2144
1969BO55 Nucl.Phys. A128, 183 (1969) B.E.Bonner, E.B.Paul, G.C.Phillips The Elastic Scattering of Fast Neutrons by Deuterons NUCLEAR REACTIONS 2H(n, n), E=5.64, 7.01, 9.04 MeV; measured σ(E;θ).
doi: 10.1016/0375-9474(69)90984-1
1969NI08 Phys.Rev. 182, 1083 (1969) A.Niiler, C.Joseph, V.Valkovic, W.Von Witsch, G.C.Phillips p + D→p + p + n Reaction at 6.5 < E < 13 MeV NUCLEAR REACTIONS 2H(p, 2p), E=6.5-13 MeV; measured σ(E;En, Ep, θ); deduced n-p scattering length.
doi: 10.1103/PhysRev.182.1083
1969TA05 Nucl.Phys. A126, 615 (1969) A Study of the Reaction 9Be(3He, 6Li)6Li NUCLEAR REACTIONS 9Be(3He, 6Li), E=4.0-10.0 MeV; measured σ(E; θ); deduced orbital angular momentum transfer.
doi: 10.1016/0375-9474(69)90851-3
1969WI01 Nucl.Phys. A126, 193(1969) A.S.Wilson, M.C.Taylor, J.C.Legg, G.C.Phillips The Elastic Scattering of Deuterons by Deuterium NUCLEAR REACTIONS 2H(d, d), E=3.5-12.25 MeV; measured σ(Ed, θ). Gas target.
doi: 10.1016/0375-9474(69)90406-0
1969WI07 Nucl.Phys. A130, 624 (1969) A.S.Wilson, M.C.Taylor, J.C.Legg, G.C.Phillips The Elastic Scattering of Protons by Deuterium NUCLEAR REACTIONS 2H(p, p), E=4.5-11.5 MeV; measured σ(Ep, θ). Enriched gas target.
doi: 10.1016/0375-9474(69)90873-2
1968CH01 Nucl.Phys. A106, 1 (1968) Y.S.Chen, S.T.Emerson, W.R.Jackson, W.D.Simpson, G.C.Phillips The 11B(p, 2α)4He Reaction at 163 keV Resonance NUCLEAR REACTIONS 11B(p, 2α)4He, E = 163 keV; measured σ(Eα1, Eα2, θ(1), θ(2)). Enriched target.
doi: 10.1016/0375-9474(67)90823-8
1968VA02 Nucl.Phys. A106, 138 (1968) V.Valkovic, C.Joseph, S.T.Emerson, G.C.Phillips Two-Particle Coincidence Spectra from the p+6Li→p+d+α Reaction NUCLEAR REACTIONS 6Li(p, pd), (p, pα), (p, dα), E = 9, 10 MeV; measured σ(Ep, Ed, Eα, θ(p), θ(d), θ(α)). Enriched target.
doi: 10.1016/0375-9474(67)90834-2
1968VA12 Nucl.Phys. A116, 497(1968) V.Valkovic, C.Joseph, A.Niiler, G.C.Phillips Rescattering Effects in Reactions with Three Particles in the Final State NUCLEAR REACTIONS 7Li(d, 2α)n, Ed=3.0, 3.2, 3.6, 5.9 MeV; measured σ(Eα1, Eα2, θ(α1), θ(α2)), enriched target.
doi: 10.1016/0375-9474(68)90387-4
1967PA25 Phys.Rev.Letters 18, 1200 (1967) H.Palevsky, J.L.Friedes, R.J.Sutter, G.W.Bennett, G.J.Igo, W.D.Simpson, G.C.Phillips, D.M.Corley, N.S.Wall, R.L.Stearns, B.Gottschalk Elastic Scattering of 1-BeV Protons from Hydrogen, Helium, Carbon, and Oxygen Nuclei NUCLEAR REACTIONS 2H, 4He, 12C, 16O(p, p), E=1 bev; measured σ(θ).
doi: 10.1103/PhysRevLett.18.1200
1967SI12 Nucl.Phys. A103, 97 (1967) W.D.Simpson, W.R.Jackson, G.C.Phillips The 2H(p, 2p)n Reaction at 9.0 and 10.5 MeV NUCLEAR REACTIONS 2H(p, 2p), E=9.0, 10.5 MeV; measured σ(Ep, θ(p1), Ep2, θ(p2)). Enriched target.
doi: 10.1016/0375-9474(67)90791-9
1967VA11 Nucl.Phys. A96, 241 (1967) V.Valkovic, W.R.Jackson, Y.S.Chen, S.T.Emerson, G.C.Phillips Three-Body Break-Up in 7Li(d, nα)4He and 7Li(d, αα)n Reactions NUCLEAR REACTIONS 7Li(d, αn), 7Li(d, 2α), E=2.6-4.0 MeV; measured σ(En, Eα, θ(n), θ(α)), σ(Eα1, Eα2, θ(α1), θ(α2)). Enriched target.
doi: 10.1016/0375-9474(67)90709-9
1966BO20 Nucl.Phys. 86, 187(1966) B.E.Bonner, G.Rickards, D.L.Bernard, G.C.Phillips Absolute Energy Calibration of Neutron Thresholds NUCLEAR REACTIONS 13C, 27Al, 60Ni, 58Ni(p, n), E = 3.2-9.5 MeV; measured thresholds absolutely, Q. Enriched targets.
doi: 10.1016/0029-5582(66)90299-9
1966RI09 Nucl.Phys. 86, 167 (1966) G.Rickards, B.E.Bonner, G.C.Phillips Measurement of (p, n) Thresholds at Tandem Energies NUCLEAR REACTIONS 13C, 27Al, 52Cr, 58Ni, 60Ni, 62Ni(p, n), E = 3.2-9.5 MeV; measured σ(E); deduced Q. 13N, 27Si, 52,53Mn, 60,61,62,63Cu deduced levels. Enriched targets.
doi: 10.1016/0029-5582(66)90298-7
1965BA15 Phys.Rev.Letters 15, 115 (1965) S.D.Baker, G.Roy, G.C.Phillips, G.K.Walters Reaction He3(d, p)He4 with a Polarized Target NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.15.115
1965BE12 Nucl.Phys. 65, 545 (1965) R.C.Bearse, J.C.Legg, G.C.Phillips, A.A.Rollefson, G.Roy Triple Correlation of the 12C(p, p'γ)12C Reaction NUCLEAR REACTIONS 12C(p, p'γ), E=5.37 MeV; measured σ(θ(p, p') θ(p, γ)); deduced S-matrix elements. Natural target.
doi: 10.1016/0029-5582(65)90324-X
1965BR18 Nucl.Phys. 68, 241 (1965) J.D.Bronson, W.D.Simpson, W.R.Jackson, G.C.Phillips Three α-Particle Decay of C12 NUCLEAR STRUCTURE 12C, 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(65)90643-7
1965JA02 Bull.Am.Phys.Soc. 10, No.2, 155, A6 (1965) W.R.Jackson, W.D.Simpson, G.C.Phillips 2H(p, pn)p Reaction Using Coincidence and Time-of-Flight Techniques NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.
1965RO02 Bull.Am.Phys.Soc. 10, No.1, 51, DC4 (1965) G.Roy, S.D.Baker, G.C.Phillips, G.K.Walters He3(d, p)He4 Reaction with Polarized Target NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
1965RO04 Nucl.Phys. 63, 561(1965) A.A.Rollefson, R.C.Bearse, J.C.Legg, G.C.Phillips, G.Roy The Cr52(d, pγ)Cr53 Reaction NUCLEAR REACTIONS 52Cr(d, pγ), E=4.0 MeV; measured σ(Ep), Eγ, Iγ, pγ-coin. 53Cr deduced levels, J, π. Enriched target.
doi: 10.1016/0029-5582(65)90742-X
1965SI01 Bull.Am.Phys.Soc. 10, No.2, 155, A5 (1965) W.D.Simpson, W.R.Jackson, G.C.Phillips Evidence for the Singlet Deuteron and Diproton in the 2H(p, 2p)n and 1H(d, 2p)n reactions
1964BA09 Nucl. Phys. 50, 629 (1964) A.C.L.Barnard, C.M.Jones, G.C.Phillips The Scattering of He3 by He4 NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90235-4
1964BE09 Bull. Am. Phys. Soc. 9, No. 4, 408, CA12 (1964) R.C.Bearse, A.A.Rollefson, J.C.Legg, G.Roy, G.C.Phillips Study of the p-γ Angular Correlation in the 12C(p, p'γ)12C Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1964BR05 Bull. Am. Phys. Soc. 9, No. 4, 406, CA4 (1964) J.D.Bronson, W.D.Simpson, W.R.Jackson, G.C.Phillips Reaction-Mechanism Study of 11B(p, 2α)4He NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1964PH03 Proc.Intern.Conf.Nuclidic Masses, 2nd, Vienna, Austria (1963), W.H.Johnson, Jr., Ed., Springer-Verlag, Vienna, p.261 (1964) Absolute Energy Standards for Van de Graaff Accelerators
1964RO06 Bull.Am.Phys.Soc. 9, No.4, 470, HA1 (1964) A.A.Rollefson, R.C.Bearse, J.C.Legg, G.C.Phillips 52Cr(d, pγ)53Cr Reaction NUCLEAR STRUCTURE 53Cr; measured not abstracted; deduced nuclear properties.
1964RO15 WASH-1048, p.105 (1964) A.A.Rollefson, R.C.Bearse, J.C.Legg, G.C.Phillips Excited States of Cr53 NUCLEAR STRUCTURE 53Cr; measured not abstracted; deduced nuclear properties.
1963BO02 Bull.Am.Phys.Soc. 8, No.2, 114, I3 (1963) B.E.Bonner, J.Rickards, G.C.Phillips Neutron Thresholds from the Proton Bombardment of C13, Al27, Cr52, Ni58, Ni60, and Ni62 NUCLEAR STRUCTURE 58Cu, 52Mn, 62Cu, 60Cu, 13C, 27Si; measured not abstracted; deduced nuclear properties.
1963BR03 Bull.Am.Phys.Soc. 8, No.2, 125, U8 (1963) J.D.Bronson, W.D.Simpson, G.C.Phillips 3-α Decay from Protons on B11 NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1963GI02 Bull.Am.Phys.Soc. 8, No.2, 126, V2 (1963) W.W.Givens, R.C.Bearse, G.C.Phillips, A.A.Rollefson Parity of the 95-keV 1st-Excited Level of O19 NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.
1963GI09 Nucl.Phys. 43, 553 (1963) W.W.Givens, R.C.Bearse, G.C.Phillips, A.A.Rollefson The Spin Sequence of the First and Second Excited Levels of Ne19 NUCLEAR STRUCTURE 19Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90376-6
1963GI12 Nucl.Phys. 46, 519 (1963) W.W.Givens, R.C.Bearse, G.C.Phillips, A.A.Rollefson The Parity of the 95 keV First-Excited Level of O19 NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90621-7
1963PI04 Nucl.Phys. 48, 75 (1963) A.E.Pitts, J.D.Bronson, T.A.Belote, G.C.Phillips Evidence for Sequential Two-Body Decay in the C12(d, p, N)C12 Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90144-5
1963RI12 WASH-1042, p.40 (1963) G.Rickards, B.Bonner, G.C.Phillips Neutron Threshold Studies NUCLEAR STRUCTURE 58Cu, 60Cu, 52Mn; measured not abstracted; deduced nuclear properties.
1963RO03 Bull.Am.Phys.Soc. 8, No.2, 126, V3 (1963) A.A.Rollefson, R.C.Bearse, W.W.Givens, G.C.Phillips Angular Correlation of γ-Rays from O19 NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.
1962BR09 Bull.Am.Phys.Soc. 7, No.2, 119, J4 (1962) J.D.Bronson, Jr., E.H.Beckner, G.C.Phillips The 1.7-MeV Anomaly in Be9 NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1962HA37 Nuclear Phys. 38, 259 (1962) R.W.Harris, G.C.Phillips, C.M.Jones Phase Shift Analysis of the Elastic Scattering of Protons from Oxygen NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)91033-7
1962JO01 Bull.Am.Phys.Soc. 7, No.2, 119, J2 (1962) C.M.Jones, A.C.L.Barnard, G.C.Phillips Elastic Scattering of He3 from He4 NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
1962JO09 Nuclear Phys. 37, 1 (1962) C.M.Jones, G.C.Phillips, R.W.Harris, E.H.Beckner The Scattering of Alpha Particles from C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90242-0
1962TO12 Nuclear Phys. 39, 541 (1962); Erratum Nucl.Phys. 43, 528 (1963) T.A.Tombrello, C.Miller Jones, G.C.Phillips, J.L.Weil The Scattering of Protons from He3 NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90412-1
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