NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = C.Goodman Found 160 matches. Showing 1 to 100. [Next]2009BH09 Phys.Rev. C 80, 055501 (2009); Pub note Phys.Rev. C 80, 069901 (2009) M.Bhattacharya, C.D.Goodman, A.Garcia Weak-interaction strength from charge-exchange reactions versus β decay in the A=40 isoquintet NUCLEAR REACTIONS 40Ar(p, n), E=120, 160 MeV; measured E(n), I(n) by time-of-flight method using peak-shape fitting parameters from 13C(p, n)13N, E=120, 160 MeV reaction. 40K; deduced levels and B(GT). Comparison of B(GT) strengths from 40Ti(β+). 40Ar(ν, e)40K; deduced capture cross section.
doi: 10.1103/PhysRevC.80.055501
2002HA14 Phys.Rev. C65, 034612 (2002) C.Hautala, J.Rapaport, M.Palarczyk, D.L.Prout, D.A.Cooper, G.Savopulos, B.Anderson, A.Baldwin, C.C.Foster, C.D.Goodman, K.Hicks, R.Howes, M.S.Islam, B.A.Luther, D.M.Manley, R.Madey, E.Sugarbaker, T.N.Taddeucci, I.Van Heerden, J.Watson, X.Yang, W.-M.Zhang Polarization Transfer in Quasifree (p(pol), n(pol)) Reactions on C, Ca, and Pb Targets at 197 MeV NUCLEAR REACTIONS 12C, 40Ca, Pb(polarized p, n), E=197 MeV; measured polarization transfer coefficients, σ(E, θ). Comparison with model predictions.
doi: 10.1103/PhysRevC.65.034612
2002PR04 Phys.Rev. C65, 034611 (2002) D.L.Prout, J.Rapaport, M.Palarczyk, D.A.Cooper, G.Savopulos, C.Hautala, B.Anderson, A.Baldwin, C.C.Foster, W.Gloeckle, C.D.Goodman, R.Howes, M.S.Islam, B.A.Luther, R.Madey, D.M.Manley, J.Sowinski, E.Sugarbaker, T.N.Taddeucci, I.Van Heerden, J.Watson, H.Witala, X.Yang, W.-M.Zhang Polarization Transfer in Quasifree (p(pol), n(pol)) Reactions on 2H and 3, 4He Targets at 197 MeV NUCLEAR REACTIONS 2H, 3,4He(polarized p, nX), E=197 MeV; measured polarization transfer coefficients, σ(E, θ). Comparison with model predictions.
doi: 10.1103/PhysRevC.65.034611
2001AU02 Phys.Rev. C63, 034322 (2001) S.M.Austin, E.Adamides, A.Galonsky, T.Nees, W.A.Sterrenburg, D.E.Bainum, J.Rapaport, E.Sugarbaker, C.C.Foster, C.D.Goodman, D.J.Horen, C.A.Goulding, M.B.Greenfield Splitting of the Dipole and Spin-Dipole Resonances NUCLEAR REACTIONS 90,92,94Zr(p, n), E=79.2, 119.4 MeV; measured σ(E, θ); deduced splitting between GDR and spin-dipole resonance. NUCLEAR STRUCTURE 90,92,94Zr, 112,116,124Sn, 208Pb; calculated resonance energies, dipole-spin-dipole splitting.
doi: 10.1103/PhysRevC.63.034322
2001GO25 Nucl.Instrum.Methods Phys.Res. A462, 545 (2001) C.D.Goodman, M.Bhattacharya, M.B.Aufderheide, S.D.Bloom, P.Zupranski Data Analysis Techniques for Extracting Gamow-Teller Strengths from 0° (p, n) Data NUCLEAR REACTIONS 7Li, 13C, 23Na(p, n), E=120, 160 MeV; analyzed neutron spectra; deduced Gamow-Teller matrix elements.
doi: 10.1016/S0168-9002(00)01317-6
2001PR02 Phys.Rev. C63, 014603 (2001) D.L.Prout, J.Rapaport, E.Sugarbaker, D.Cooper, S.Delucia, B.Luther, C.D.Goodman, B.K.Park, L.Rybarcyk, T.N.Taddeucci, J.Ullmann Observation of the Spin Isovector Monopole Resonance using the Pb(p(pol), n(pol))Bi Reaction at 795 MeV NUCLEAR REACTIONS 12C, 90Zr, 208Pb(polarized p, n), E=795 MeV; measured neutron spectra, σ(E), polarization transfer observables; deduced spin isovector monopole resonance features. DWIA calculations. Comparison with previous results.
doi: 10.1103/PhysRevC.63.014603
2000BH10 Phys.Rev.Lett. 85, 4446 (2000) M.Bhattacharya, C.D.Goodman, R.S.Raghavan, M.Palarczyk, A.Garcia, J.Rapaport, I.J.van Heerden, P.Zupranski Measurement of Gamow-Teller Strength for 176Yb → 176Lu and the Efficiency of a Solar Neutrino Detector NUCLEAR REACTIONS 13C, 176Yb(p, n), E=120, 160 MeV; measured missing mass, excitation energy spectra; deduced Gamow-Teller transition strengths. Application to solar neutrino detection discussed.
doi: 10.1103/PhysRevLett.85.4446
2000FU15 Phys.Rev.Lett. 85, 4442 (2000) M.Fujiwara, H.Akimune, A.M.van den Berg, M.Cribier, I.Daito, H.Ejiri, H.Fujimura, Y.Fujita, C.D.Goodman, K.Hara, M.N.Harakeh, F.Ihara, T.Ishikawa, J.Janecke, T.Kawabata, R.S.Raghavan, K.Schwarz, M.Tanaka, T.Yamanaka, M.Yosoi, R.G.T.Zegers Gamow-Teller Strengths of the Inverse Beta Transition 176Yb → 176Lu for Spectroscopy of Proton-Proton and Other Sub-MeV Solar Neutrinos NUCLEAR REACTIONS 176Yb(3He, t), E=450 MeV; measured triton spectra; deduced Gamow-Teller transition strengths. 176Lu deduced levels, IAS excitation strength. Application to solar neutrino detection discussed.
doi: 10.1103/PhysRevLett.85.4442
2000KH09 Nucl.Phys. A663-664, 565c (2000) A.Khoukaz, H.-H.Adam, J.T.Balewski, A.Budzanowski, C.Goodman, D.Grzonka, L.Jarczyk, M.Jochmann, K.Kilian, N.Lang, T.Lister, P.Moskal, W.Oelert, C.Quentmeier, R.Santo, G.Schepers, U.Seddik, T.Sefzick, S.Sewerin, J.Smyrski, A.Strzalkowski, M.Wolke, P.Wustner, D.Wyrwa Near Threshold Production of η, η' and Charged Kaon Pairs in Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, X), E ≈ threshold; measured η meson, kaon pair production σ.
doi: 10.1016/S0375-9474(99)00657-0
2000SE05 Nucl.Phys. A663-664, 473c (2000) S.Sewerin, J.T.Balewski, A.Budzanowski, C.Goodman, D.Grzonka, L.Jarczyk, M.Jochmann, A.Khoukaz, K.Kilian, M.Kohler, T.Lister, P.Moskal, W.Oelert, C.Quentmeier, R.Santo, G.Schepers, U.Seddik, T.Sefzick, J.Smyrski, A.Strzalkowski, M.Wolke, P.Wustner, W.Eyrich, M.Fritsch, J.Haidenbauer, C.Hanhart, F.Stinzing, C.Wilkin, and the COSY-11 Collaboration Near Threshold Hyperon-Production at COSY-11 in the Reactions pp → pK+Λ and pp → pK+Σ0 NUCLEAR REACTIONS 1H(p, K+X), E ≈ threshold; measured hyperon production associated invariant mass, σ.
doi: 10.1016/S0375-9474(99)00634-X
1999PA03 Phys.Rev. C59, 500 (1999) M.Palarczyk, J.Rapaport, C.Hautala, D.L.Prout, C.D.Goodman, I.J.van Heerden, J.Sowinski, G.Savopulos, X.Yang, H.M.Sages, R.Howes, R.Carr, M.Islam, E.Sugarbaker, D.C.Cooper, K.Lande, B.Luther, T.N.Taddeucci Measurement of Gamow-Teller Strength for 127I as a Solar Neutrino Detector NUCLEAR REACTIONS 127I(p, n), E=94, 159, 197 MeV; measured neutrons σ(E, θ=0°). 127Xe deduced IAS energy, Coulomb displacement energy, B(GT) vs excitation energy. 127I deduced solar neutrino capture σ.
doi: 10.1103/PhysRevC.59.500
1999RA22 Eur.Phys.J. A 6, 225 (1999) B.Ramstein, C.A.Mosbacher, D.Bachelier, I.Bergqvist, M.Boivin, J.L.Boyard, A.Brockstedt, L.Carlen, R.Dahl, P.Ekstrom, C.Ellegaard, C.Gaarde, T.Hennino, J.C.Jourdain, C.Goodman, J.S.Larsen, P.Radvanyi, M.Roy-Stephan Inclusive 2(3He, t) Reaction at 2 GeV NUCLEAR REACTIONS 2H(3He, t), E=2 GeV; measured σ(E, θ), energy transfer spectra; deduced Δ resonance contributions, final state interaction role. Coupled channels analysis.
doi: 10.1007/s100500050338
1999SE11 Phys.Rev.Lett. 83, 682 (1999) S.Sewerin, G.Schepers, J.T.Balewski, A.Budzanowski, W.Eyrich, M.Fritsch, C.Goodman, D.Grzonka, J.Haidenbauer, C.Hanhart, M.Hofmann, L.Jarczyk, M.Jochmann, A.Khoukaz, K.Kilian, M.Kohler, T.Lister, P.Moskal, W.Oelert, I.Pellmann, C.Quentmeier, R.Santo, U.Seddik, T.Sefzick, J.Smyrski, F.Stinzing, A.Strzalkowski, C.Wilkin, M.Wolke, P.Wustner, D.Wyrwa Comparison of Λ and Σ0 Production Near Threshold in Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, K+X), E ≈ threshold; measured Λ, Σ hyperon production associated missing mass spectra; deduced final state interaction role.
doi: 10.1103/PhysRevLett.83.682
1999VA04 Phys.Rev. C59, 1488 (1999) I.J.van Heerden, M.Palarczyk, X.Wang, J.Rapaport, D.L.Prout, C.D.Goodman, B.A.Luther, E.Sugarbaker, T.N.Taddeucci, D.Dehnhard, C.C.Foster, K.Hicks, L.Wang, X.Yang, J.M.O'Donnell, H.Ohnuma, B.K.Park, G.R.Burleson, S.Blanchard Zero-Degree Differential Cross Sections and DNN Values for the 17, 18O(p(pol), n(pol))17, 18F Reactions at Ep = 118 MeV NUCLEAR REACTIONS 17,18O(polarized p, n), E=118 MeV; measured neutron spectra, σ(θ=0°), polarization transfer coefficients. 17,18F levels deduced B(GT), B(F). Implications for solar neutrino detection discussed.
doi: 10.1103/PhysRevC.59.1488
1998BA24 Phys.Lett. 420, 211 (1998) J.T.Balewski, A.Budzanowski, H.Dombrowski, W.Eyrich, C.Goodman, D.Grzonka, J.Haidenbauer, C.Hanhart, J.Hauffe, L.Jarczyk, M.Jochmann, A.Khoukaz, K.Kilian, M.Kohler, A.Kozela, T.Lister, A.Metzger, P.Moskal, W.Oelert, C.Quentmeier, R.Santo, G.Schepers, U.Seddik, T.Sefzick, J.Smyrski, M.Sokolowski, F.Stinzing, A.Strzalkowski, C.Thomas, S.Wirth, M.Wolke, R.Woodward, P.Wustner, D.Wyrwa Total Cross Section of the Reaction pp → pK+ Λ Close to Threshold NUCLEAR REACTIONS 1H(p, pX), E at 2.3 GeV/c; measured total σ vs excess energy for pK+Λ final state; deduced reaction mechanism features.
doi: 10.1016/S0370-2693(97)01527-X
1998BA36 Eur.Phys.J. A 2, 99 (1998) J.T.Balewski, A.Budzanowski, C.Goodman, D.Grzonka, M.Hofmann, L.Jarczyk, A.Khoukaz, K.Kilian, T.Lister, P.Moskal, W.Oelert, I.A.Pellmann, C.Quentmeier, R.Santo, G.Schepers, T.Sefzick, S.Sewerin, J.Smyrski, A.Strzalkowski, C.Thomas, C.Wilkin, M.Wolke, P.Wustner, D.Wyrwa Low-Energy Λ-p Scattering Parameters from the pp → pK+Λ Reaction NUCLEAR REACTIONS 1H(p, K+X), E ≈ threshold; measured Λ-associated missing mass distributions; deduced Λ-p scattering parameters.
doi: 10.1007/s100500050095
1998MO07 Phys.Rev.Lett. 80, 3202 (1998) P.Moskal, J.T.Balewski, A.Budzanowski, H.Dombrowski, C.Goodman, D.Grzonka, J.Haidenbauer, C.Hanhart, L.Jarczyk, M.Jochmann, A.Khoukaz, K.Kilian, M.Kohler, A.Kozela, T.Lister, U.-G.Meissner, N.Nikolaev, W.Oelert, C.Quentmeier, R.Santo, G.Schepers, U.Seddik, T.Sefzick, J.Smyrski, M.Sokolowski, A.Strzalkowski, C.Thomas, M.Wolke, P.Wustner, D.Wyrwa η' Production in Proton-Proton Scattering Close to Threshold NUCLEAR REACTIONS 1H(p, pX), E at 3.2 GeV/c; measured η' production σ; deduced coupling constant.
doi: 10.1103/PhysRevLett.80.3202
1997BA89 Nucl.Phys. A626, 85c (1997) J.Balewski, S.Brauksiepe, A.Budzanowski, H.Dombrowski, C.Goodman, D.Grzonka, J.Haidenbauer, C.Hanhart, A.Hardt, L.Jarczyk, M.Jochmann, A.Khoukaz, K.Kilian, M.Kohler, A.Kozela, T.Lister, R.Maier, P.Moskal, W.Oelert, D.Prasuhn, C.Quentmeier, R.Santo, G.Schepers, U.Seddik, T.Sefzick, J.Smyrski, M.Sokolowski, A.Strzalkowski, M.Wolke, P.Wustner Threshold Measurements at the Internal Experimental Facility COSY-11 NUCLEAR REACTIONS 1H(p, 2pX), E not given; measured strangeness production associated missing mass spectra; 1H(p, pX), E at 2.345 GeV/c; measured K+Λ associated events yield.
doi: 10.1016/S0375-9474(97)00524-1
1996BA83 Phys.Lett. 388B, 859 (1996) J.T.Balewski, A.Budzanowski, H.Dombrowski, C.Goodman, D.Grzonka, J.Haidenbauer, C.Hanhart, L.Jarczyk, M.Jochmann, A.Khoukaz, K.Kilian, M.Kohler, A.Kozela, T.Lister, R.Maier, P.Moskal, W.Oelert, D.Prasuhn, C.Quentmeier, R.Santo, G.Schepers, U.Seddik, T.Sefzick, J.Smyrski, M.Sokolowski, A.Strzalkowski, M.Wolke, P.Wustner Λ-Hyperon Production via the pp → pK+Λ Rection 2 MeV Above Threshold NUCLEAR REACTIONS 1H(p, pX), E at 2.345 GeV/c; measured total σ for K+Λ production; deduced phenomenological parametrizations insufficiency.
doi: 10.1016/S0370-2693(96)01360-3
1996BB16 Acta Phys.Pol. B27, 2911 (1996) J.T.Balewski, R.Bilger, A.Budzanowski, H.Clement, K.H.Diart, H.Dombrowski, K.Fohl, C.Goodman, D.Grzonka, H.Gutschmidt, K.Heitlinger, L.Jarczyk, M.Jochmann, M.Karnadi, A.Khoukaz, K.Kilian, M.Kohler, A.Kozela, T.Lister, P.Moskal, R.Nellen, W.Oelert, C.Quentmeier, R.Santo, D.Schapler, G.Schepers, U.Seddik, T.Sefzick, J.Smyrski, M.Sokolowski, A.Strzalkowski, M.Wolke, G.J.Wagner, K.H.Watzlawik, P.Wustner, K.Zwoll Meson Production in p + p Interaction at Threshold
1996MI11 Phys.Lett. 379B, 67 (1996) R.G.Milner, C.Bloch, J.F.J.van den Brand, H.J.Bulten, D.DeSchepper, T.W.Donnelly, R.Ent, C.D.Goodman, J.-O.Hansen, W.W.Jacobs, C.E.Jones, W.Korsch, L.H.Kramer, K.Lee, M.Leuschner, W.Lorenzon, N.C.R.Makins, D.Marchlenski, H.O.Meyer, M.A.Miller, J.S.Neal, P.V.Pancella, S.F.Pate, W.K.Pitts, B.von Przewoski, T.Rinckel, P.U.Sauer, G.Savopulos, R.-W.Schulze, A.Smith, J.Sowinski, F.Sperisen, E.R.Sugarbaker, M.A.Titko, C.Tschalar, O.Unal, T.P.Welch, Z.-L.Zhou The Spin Dependent Momentum Distributions of the Neutron and Proton in 3He NUCLEAR REACTIONS 3He(polarized p, 2p), (polarized p, np), E=197 MeV; analyzed data. 3He deduced nucleon momentum distribution spin asymmetries. PWIA model, Faddeev calculation.
doi: 10.1016/0370-2693(96)00450-9
1996PR03 Phys.Rev.Lett. 76, 4488 (1996) D.L.Prout, S.DeLucia, D.Cooper, B.Luther, E.Sugarbaker, T.N.Taddeucci, L.J.Rybarcyk, J.Rapaport, B.K.Park, C.D.Goodman, G.Edwards, C.Glashausser, T.Sams, T.Udagawa, F.Osterfeld Spin Decomposition of the Δ Resonance Cross Section using the 12C(p(pol), n(pol)) Reaction at E(p) = 795 MeV NUCLEAR REACTIONS 12C(polarized p, n), E=795 MeV; measured polarization observables; deduced spin-longitudinal, spin-transverse, spin-independent partial σ, Δ-production related features.
doi: 10.1103/PhysRevLett.76.4488
1995BL25 Nucl.Instrum.Methods Phys.Res. A354, 437 (1995) C.Bloch, J.Doskow, C.D.Goodman, W.W.Jacobs, M.Leuschner, H.O.Meyer, B.von Przewoski, T.Rinckel, G.Savopulos, A.Smith, J.Sowinski, F.Sperisen, W.K.Pitts, D.DeSchepper, R.Ent, J.-O.Hansen, J.Kelsey, W.Korsch, L.H.Kramer, K.Lee, N.C.R.Makins, R.G.Milner, S.F.Pate, C.Tschalar, T.P.Welch, D.Marchlenski, E.Sugarbaker, W.Lorenzon, P.V.Pancella, J.F.J.van den Brand, H.J.Bulten, C.E.Jones, M.A.Miller, J.Neal, O.Unal, Z.-L.Zhou Spin-Dependent Scattering of Polarized Protons from a Polarized 3He Internal Gas Target NUCLEAR REACTIONS 3He(polarized p, p), E=197-414 MeV; measured (θp, E(3He)) correlation. 3He(p, 2p), E=197 MeV; measured E(recoil), missing momentum correlation, other features. Laser optically pumped polarized target, circulating proton beams.
doi: 10.1016/0168-9002(94)01057-9
1995MI05 Phys.Rev.Lett. 74, 502 (1995) M.A.Miller, K.Lee, A.Smith, J.-O.Hansen, C.Bloch, J.F.J.van den Brand, H.J.Bulten, D.DeSchepper, R.Ent, C.D.Goodman, W.W.Jacobs, C.E.Jones, W.Korsch, L.H.Kramer, M.Leuschner, W.Lorenzon, N.C.R.Makins, D.Marchlenski, H.O.Meyer, R.G.Milner, J.S.Neal, P.V.Pancella, S.F.Pate, W.K.Pitts, B.von Przewoski, T.Rinckel, G.Savopulos, J.Sowinski, F.Sperisen, E.R.Sugarbaker, C.Tschalar, O.Unal, T.P.Welch, Z.-L.Zhou Measurement of Quasielatic 3He(p(pol), pN) Scattering from Polarized 3He and the Three-Body Ground State Spin Structure NUCLEAR REACTIONS 3He(polarized p, 2p), (polarized p, np), E=197 MeV; measured analyzing power, spin correlations vs missing momentum, momentum transfer. 3He deduced nucleons polarizations at low missing momentum.
doi: 10.1103/PhysRevLett.74.502
1995PR04 Phys.Rev. C52, 228 (1995) D.L.Prout, C.Zafiratos, T.N.Taddeucci, J.Ullmann, R.C.Byrd, T.A.Carey, P.Lisowski, J.B.McClelland, L.J.Rybarcyk, W.Sailor, W.Amian, M.Braunstein, D.Lind, D.J.Mercer, D.Cooper, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, J.Rapaport, B.K.Park, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, W.Huang, D.Ciskowski, W.P.Alford Cross Sections and Analyzing Powers for Quasielastic Scattering at 795 and 495 MeV using the (p(pol), n) Reaction NUCLEAR REACTIONS 12C, Pb(polarized p, n), E=495, 795 MeV; measured σ(θ), analyzing power vs energy loss. Models comparison.
doi: 10.1103/PhysRevC.52.228
1995SA06 Phys.Rev. C51, 1945 (1995) T.Sams, C.Ellegaard, C.Gaarde, J.S.Larsen, J.L.Boyard, T.Hennino, J.C.Jourdain, B.Ramstein, M.Roy-Stephan, P.Radvanyi, A.Brockstedt, M.Osterlund, P.Zupranski, C.D.Goodman, M.Ichimura, V.F.Dmitriev Quasifree (d(pol), 2He) Data NUCLEAR REACTIONS 2,1H, 12C(polarized d, X), E=1.6, 2 GeV; measured σ(θ), tensor analyzing powers vs momentum transfer; deduced spin-isospin response in the quasifree region.
doi: 10.1103/PhysRevC.51.1945
1995WA05 Phys.Rev. C51, 1345 (1995) Y.Wang, X.Yang, J.Rapaport, C.D.Goodman, S.L.De Lucia, B.A.Luther, D.G.Marchlenski, B.K.Park, L.Rybarcyk, A.Smith, E.Sugarbaker, T.Taddeucci, L.Wang Study of the (1/2)-(g.s.) → (1/2)+1 Transition in the 13C(p, n)13N Reaction at Intermediate Energies NUCLEAR REACTIONS 13C(p, n), E=160, 186 MeV; measured σ(θ), σ(θ, En); deduced absolute σ for ΔJ(π)=0-, ΔJ(π)=1- transitions.
doi: 10.1103/PhysRevC.51.1345
1995YA12 Phys.Rev. C52, 2535 (1995) X.Yang, L.Wang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park Dipole Excitations in p-Shell Nuclei Via (p, n) Reactions NUCLEAR REACTIONS 6,7Li, 10,11B, 12,13C(p, n), E=186 MeV; measured σ(θ, En); deduced quasifree reaction contribution in giant resonance region, ΔL=1 transitions energy spectra.
doi: 10.1103/PhysRevC.52.2535
1994AU01 Phys.Rev. C49, 678 (1994) M.B.Aufderheide, S.D.Bloom, D.A.Resler, C.D.Goodman Comparison of Gamow-Teller Strength in 37Ar and 37K and 37Cl Neutrino Cross Sections NUCLEAR STRUCTURE 37Ar; analyzed Gamow-Teller transition strength; deduced 37Cl(ν, X) reaction σ for solar, supernova, μ+-decay neutrinos. 37K level deduced β--delayed proton emission suppression features. Shell model.
doi: 10.1103/PhysRevC.49.678
1994GO23 Nucl.Phys. A577, 3c (1994) Extracting GT Matrix Elements from (p, n) Cross Sections NUCLEAR REACTIONS 90Zr, 89Y, 93Nb(polarized p, n), E not given; compiled, reviewed neutron spectra, spin observable D(NN), data on other nuclei; deduced β-decay, (p, n) matrix elements correlation.
doi: 10.1016/0375-9474(94)90825-7
1994ME07 Phys.Rev. C49, 3104 (1994) D.J.Mercer, J.Rapaport, C.A.Whitten, Jr., D.Adams, R.Byrd, X.Y.Chen, A.Fazely, T.Gaussiran, E.Gulmez, C.Goodman, D.W.Huang, G.Igo, A.Ling, D.Marchlenski, D.Prout, L.Rybarcyk, E.Sugarbaker, T.N.Taddeucci Multipole Decomposition of the 16O(p, n)16F and 18O(p, n)18F Reactions at 494 MeV NUCLEAR REACTIONS 16,18O(p, n), E=494 MeV; measured σ(θ); deduced transition multipole components for ΔL=0, ΔL=1, ΔL ≥ 2. 18,16F deduced Gamow-Teller strength B(GT).
doi: 10.1103/PhysRevC.49.3104
1994PR08 Nucl.Phys. A577, 233c (1994) D.Prout, S.Delucia, E.Sugarbaker, B.Luther, D.Cooper, T.Taddeucci, L.Rybarcyk, J.McClelland, C.Goodman, B.Park, J.Rapaport, T.Sams, G.Edwards, C.Glashausser Spin-Longitudinal and Spin-Transverse Cross Section for Δ Production in the 12C(p(pol), n(pol)) Reaction NUCLEAR REACTIONS 2H, 12C(polarized p, n), E=795 MeV; measured spin observables; deduced spin-longitudinal, spin-transverse σ(θ) vs energy transfer.
doi: 10.1016/0375-9474(94)90861-3
1994TA24 Phys.Rev.Lett. 73, 3516 (1994) T.N.Taddeucci, B.A.Luther, L.J.Rybarcyk, R.C.Byrd, J.B.McClelland, D.L.Prout, S.DeLucia, D.A.Cooper, D.G.Marchlenski, E.Sugarbaker, B.K.Park, T.Sams, C.D.Goodman, J.Rapaport, M.Ichimura, K.Kawahigashi Momentum Dependence of the Nuclear Isovector Spin Responses from (p(pol), n(pol)) Reactions at 494 MeV NUCLEAR REACTIONS 2H, 12C, 40Ca(polarized p, n), E=494 MeV; measured polarization transfer coefficients; deduced longitudinal, transverse isovector spin responses.
doi: 10.1103/PhysRevLett.73.3516
1994WA22 Phys.Rev. C50, 2438 (1994) L.Wang, X.Yang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, J.Piekarewicz, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park (p, n) Quasifree Excitations in p-Shell Nuclei at 186 MeV NUCLEAR REACTIONS 6,7Li, 10,11B, 12,13C(p, n), (polarized p, n), E=186 MeV; measured σ(θ, En), polarization transfer coefficient, analyzing power vs θ. Quasifree model analysis.
doi: 10.1103/PhysRevC.50.2438
1993CH13 Phys.Rev. C47, 2159 (1993) X.Y.Chen, T.N.Taddeucci, J.B.McClelland, T.A.Carey, R.C.Byrd, L.J.Rybarcyk, W.C.Sailor, D.J.Mercer, D.L.Prout, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, J.Rapaport, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, W.Huang, Y.Wang, W.P.Alford Polarization Transfer in Quasifree (p(pol), n(pol) Reactions at 495 MeV NUCLEAR REACTIONS 2H, 12C, 40Ca(polarized p, n), E=495 MeV; measured σ(θ), analyzing power, polarization transfer coefficient vs energy loss; deduced response functions, residual interaction modifications.
doi: 10.1103/PhysRevC.47.2159
1993LE02 Phys.Rev.Lett. 70, 738 (1993) K.Lee, M.A.Miller, A.Smith, J.-O.Hansen, C.Bloch, J.F.J.van den Brand, H.J.Bulten, R.Ent, C.D.Goodman, W.W.Jacobs, C.E.Jones, W.Korsch, M.Leuschner, W.Lorenzon, D.Marchlenski, H.O.Meyer, R.G.Milner, J.S.Neal, P.V.Pancella, S.F.Pate, W.K.Pitts, B.von Przewoski, T.Rinckel, J.Sowinski, F.Sperisen, E.Sugarbaker, C.Tschalar, O.Unal, Z.-L.Zhou Measurement of Spin Observables Using a Storage Ring with Polarized Beam and Polarized Internal Gas Target NUCLEAR REACTIONS 3He(polarized p, p), E=45, 198 MeV; measured analyzing power, spin correlation parameter, spin observables vs θ. Laser pumped internal, polarized, gas target.
doi: 10.1103/PhysRevLett.70.738
1993ME06 Phys.Rev.Lett. 71, 684 (1993) D.J.Mercer, T.N.Taddeucci, L.J.Rybarcyk, X.Y.Chen, D.L.Prout, R.C.Byrd, J.B.McClelland, W.C.Sailor, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, J.Rapaport Polarization Transfer in (p(pol), n(pol)) Reactions at 318 and 494 MeV and the Effective Interaction NUCLEAR REACTIONS 2H, 12,14C(polarized p, n), E=318, 494 MeV; measured polarization transfer observable; deduced medium effects modification to effective interaction.
doi: 10.1103/PhysRevLett.71.684
1993WA06 Phys.Rev. C47, 2123 (1993) L.Wang, X.Yang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, R.A.Lindgren, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park 10B(p, n)10C Reaction at 186 MeV NUCLEAR REACTIONS 10B(p, n), (polarized p, n), E=186 MeV; measured σ(θn, En), analyzing power, polarization, polarization transfer. 10C deduced resonances, J, π, possible IAS character.
doi: 10.1103/PhysRevC.47.2123
1993YA11 Phys.Rev. C48, 1158 (1993) X.Yang, L.Wang, J.Rapaport, C.D.Goodman, C.Foster, Y.Wang, W.Unkelbach, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, J.L.Ullmann, A.G.Ling, B.K.Park, D.S.Sorenson, L.Rybarcyk, T.N.Taddeucci, C.R.Howell, W.Tornow Dipole and Spin-Dipole Resonances in Charge-Exchange Reactions on 12C NUCLEAR REACTIONS 12C(n, p), E=60-260 MeV; measured σ(θ, Ep); 12C(p, n), E=186 MeV; 12C(polarized p, n), E=160 MeV; measured σ(θ, En), polarization, spin observables, analyzing power; deduced dipole, spin-dipole resonances.
doi: 10.1103/PhysRevC.48.1158
1992AU05 Phys.Rev. C46, 2251 (1992) M.B.Aufderheide, S.D.Bloom, D.A.Resler, C.D.Goodman Gamow-Teller Strength in A = 37 Nuclei NUCLEAR STRUCTURE A=37; analyzed Gamow-Teller transition strength from 37Ca(β+) decay, 37Cl(p, n) reaction data; deduced branching ratios sum possible values range, relevance to solar, supernova ν σ of 37Cl.
doi: 10.1103/PhysRevC.46.2251
1992GO13 Phys.Rev.Lett. 69, 2445 (1992) C.D.Goodman, M.B.Aufderheide, S.D.Bloom, D.A.Resler Comment on ' Is the Weak Axial-Vector Current Renormalized in Nuclei ( Question ) ' NUCLEAR STRUCTURE 37K, 37Ar; analyzed Gamow-Teller transition strength data; deduced β-decay, (p, n) reaction probe consistency evidence.
doi: 10.1103/PhysRevLett.69.2445
1992MC09 Phys.Rev.Lett. 69, 582 (1992) J.B.McClelland, T.N.Taddeucci, X.Y.Chen, W.P.Alford, R.C.Byrd, T.A.Carey, S.DeLucia, C.D.Goodman, E.Gulmez, W.Huang, B.Luther, D.G.Marchlenski, D.J.Mercer, D.L.Prout, J.Rapaport, L.J.Rybarcyk, W.Sailor, E.Sugarbaker, Y.Wang, C.Whitten, Jr. Quasifree Polarization-Transfer Measurements in the (p(pol), n(pol)) Reaction at 495 MeV NUCLEAR REACTIONS 2H, C, Ca(polarized p, n), E=495 MeV; measured polarization transfer variables, complete set; deduced longitudinal to spin-transverse responses ratio. Distorted waves, RPA nuclear response.
doi: 10.1103/PhysRevLett.69.582
1991BR20 Nucl.Phys. A530, 571 (1991) A.Brockstedt, I.Bergqvist, L.Carlen, L.P.Ekstrom, B.Jakobsson, C.Ellegaard, C.Gaarde, J.S.Larsen, C.Goodman, M.Bedjidian, D.Contardo, J.Y.Grossiord, A.Guichard, M.Roy-Stephan, M.Boivin, T.Hasegawa, P.Radvanyi The (3He, t) Reaction at Intermediate Energies Spin-Isospin Multipole Transitions NUCLEAR REACTIONS 26Mg, 40,48Ca, 54Fe, 90Zr, 208Pb(3He, t), E=0.9-2 GeV; measured σ(θ). 26Al, 40,48Sc, 54Co, 90Nb, 208Bi deduced spin multipole, Gamow-Teller transition strength distributions. DWIA calculations, quasi-elastic peak, distortion effects.
doi: 10.1016/0375-9474(91)90770-7
1991TA13 Nucl.Phys. A527, 393c (1991) T.N.Taddeucci, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.D.Goodman, E.Gulmez, W.Huang, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker Cross Section and Analyzing Power for Quasifree (p, n) Reactions NUCLEAR REACTIONS 12C(polarized p, n), E=494, 795 MeV; measured σ(θ), analyzing power; deduced quasifree neutron knockout. Relativistic fermi gas model.
doi: 10.1016/0375-9474(91)90128-S
1990GO12 Phys.Rev. C42, 1150 (1990) C.D.Goodman, J.Rapaport, S.D.Bloom Comment on ' Testing ' the Gamow-Teller Sum Rule
doi: 10.1103/PhysRevC.42.1150
1990RA08 Phys.Rev. C41, 1920 (1990) J.Rapaport, C.C.Foster, C.D.Goodman, C.A.Goulding, T.N.Taddeucci, D.J.Horen, E.R.Sugarbaker, C.Gaarde, J.Larsen, J.A.Carr, F.Petrovich, M.J.Threapleton (p, n) Reaction on Li Isotopes for E(p) = 60-200 MeV NUCLEAR REACTIONS 7,6Li(p, n), (polarized p, n), E=60-200 MeV; measured σ(θ). 6Be deduced Gamow-Teller transition strength. 7Be deduced branching ratio, Gamow-Teller transition strength. DWIA analysis.
doi: 10.1103/PhysRevC.41.1920
1990SU12 Phys.Rev.Lett. 65, 551 (1990) E.Sugarbaker, D.Marchlenski, T.N.Taddeucci, L.J.Rybarcyk, J.B.McClelland, T.A.Carey, R.C.Byrd, C.D.Goodman, W.Huang, J.Rapaport, D.Mercer, D.Prout, W.P.Alford, E.Gulmez, C.A.Whitten, D.Ciskowski Isovector Effective Interactions from 14C(p, n)14N Studies between 500 and 800 MeV NUCLEAR REACTIONS 14C(p, n), E=494, 644, 795 MeV; measured σ(θ=0°); deduced effective nucleon interaction components.
doi: 10.1103/PhysRevLett.65.551
1990TA11 Phys.Rev. C41, 2548 (1990) T.N.Taddeucci, W.P.Alford, M.Barlett, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, C.A.Goulding, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker, C.A.Whitten, Jr. Zero-Degree Cross Sections for the 7Li(p, n)7Be(g.s.+0.43-MeV) Reaction in the Energy Range 80-795 MeV NUCLEAR REACTIONS 7Li(p, n), E=80-795 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.41.2548
1990TA15 Phys.Rev. C42, 935 (1990) T.N.Taddeucci, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, E.Sugarbaker, I.J.Van Heerden, C.A.Whitten, Jr. Gamow-Teller Transition Strengths from the 11B(p, n)11C Reaction in the Energy Range 160-795 MeV NUCLEAR REACTIONS 11B(p, n), E=160-795 MeV; measured σ(En, θ=0°). 11C levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.42.935
1989EL05 Phys.Lett. 231B, 365 (1989) C.Ellegaard, C.Gaarde, T.S.Jorgensen, J.S.Larsen, B.Million, C.Goodman, A.Brockstedt, P.Ekstrom, M.Osterlund, M.Bedjidian, D.Contardo, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, P.Radvanyi, P.Zupranski Spin Structure of the Δ Excitation NUCLEAR REACTIONS 1,2H, 12C(polarized d, 2p), E=1.6, 2 GeV; measured pp-coin spectra, tensor polarization response; deduced Δ excitation spin structure.
doi: 10.1016/0370-2693(89)90677-1
1988PL02 Phys.Rev.Lett. 61, 1465 (1988) S.Platchkov, A.Amroun, P.Bricault, J.M.Cavedon, P.K.A.de Witt Huberts, P.Dreux, B.Frois, C.D.Goodman, D.Goutte, J.Martino, V.Meot, G.A.Peterson, X.H.Phan, S.Raman, I.Sick Measurement of the 1f7/2-Neutron-Orbit Radius in 41Ca NUCLEAR REACTIONS 41Ca(e, e'), (e, e), E=275 MeV; measured σ(E(e)); deduced magnetic form factor. 41Ca deduced 1f7/2 neutron orbit radius.
doi: 10.1103/PhysRevLett.61.1465
1988WA07 Nucl.Phys. A480, 285 (1988) D.Wang, J.Rapaport, D.J.Horen, B.A.Brown, C.Gaarde, C.D.Goodman, E.Sugarbaker, T.N.Taddeucci The 52, 54Cr(p, n)52, 54Mn and 57, 58Fe(p, n)57, 58Co Reactions at E(p) = 120 MeV NUCLEAR REACTIONS, MECPD 52,54Cr, 57,58Fe(p, n), E=120 MeV; measured σ(θ). 52,54Mn, 57,58Co deduced Gamow-Teller resonances, transition strengths. Enriched targets. DWIA analysis.
doi: 10.1016/0375-9474(88)90398-3
1987BE25 Nucl.Phys. A469, 648 (1987) I.Bergqvist, A.Brockstedt, L.Carlen, L.P.Ekstrom, B.Jakobsson, C.Ellegaard, C.Gaarde, J.S.Larsen, C.Goodman, M.Bedjidian, D.Contardo, J.Y.Grossiord, A.Guichard, R.Haroutunian, J.R.Pizzi, D.Bachelier, J.l.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, M.Boivin, P.Radvanyi The (3He, t) Reaction at Intermediate Energies: Spin-isospin transitions to states in 12N and 13N NUCLEAR REACTIONS 12,13C(3He, t), E=0.6-2.3 GeV; measured σ(Et, θt), σ(θ); deduced isovector strength ratio. 12,13N deduced spin-isospin transitions. Magnetic spectrometer. DWIA calculations.
doi: 10.1016/0375-9474(87)90019-4
1987EL08 Phys.Rev.Lett. 59, 974 (1987) C.Ellegaard, C.Gaarde, T.S.Jorgensen, J.S.Larsen, C.Goodman, I.Bergqvist, A.Brockstedt, P.Ekstrom, M.Bedjidian, D.Contardo, J.Y.Grossiord, A.Guichard, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, P.Radvanyi, J.Tinsley Reaction (d(pol), 2He) at Intermediate Energies NUCLEAR REACTIONS 1H(d, 2p), E=0.65, 2 GeV; measured σ vs two-proton relative momentum. 1H(polarized d, 2p), E=2 GeV; measured σ(Ep, θp), tensor analyzing power. Drift chambers, tensor polarized beam.
doi: 10.1103/PhysRevLett.59.974
1987KR10 Phys.Lett. 189B, 299 (1987) D.Krofcheck, E.Sugarbaker, A.J.Wagner, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, C.Gaarde, D.J.Horen, T.Carey, T.N.Taddeucci Gamow-Teller Strength Distribution in 81Kr and the Consequences for a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 81Br(p, n), E=190, 200 MeV; measured σ(En). 81Kr transitions deduced Gamow-Teller transition strength distribution. Tof.
doi: 10.1016/0370-2693(87)91436-5
1987RA15 Phys.Rev. C36, 500 (1987) J.Rapaport, D.Wang, J.A.Carr, F.Petrovich, C.C.Foster, C.D.Goodman, C.Gaarde, J.Larsen, C.A.Goulding, T.N.Taddeucci, D.Horen, E.Sugarbaker (p(pol), n) Reaction on Carbon Isotopes at E(p) = 160 MeV NUCLEAR REACTIONS 12,13,14C(polarized p, n), E=160 MeV; measured σ(θ), σ(θ, En), analyzing power. 15N(polarized p, n), E=160 MeV; analyzed data. 12,13,14N, 15O levels deduced Gamow-Teller transition strength.
doi: 10.1103/PhysRevC.36.500
1987SA02 Phys.Rev. C35, 344 (1987) H.Sakai, T.A.Carey, J.B.McClelland, T.N.Taddeucci, R.C.Byrd, C.D.Goodman, D.Krofcheck, L.J.Rybarcyk, E.Sugarbaker, A.J.Wagner, J.Rapaport Cross Section and Transverse Polarization Transfer for the 2H(p, n)2p Reaction at 160 MeV NUCLEAR REACTIONS, MECPD 2H(p, n), E=160 MeV; measured σ(En, θ), transverse polarization coefficient. Plastic scintillators. Impulse approximation analysis.
doi: 10.1103/PhysRevC.35.344
1987TA13 Nucl.Phys. A469, 125 (1987) T.N.Taddeucci, C.A.Goulding, T.A.Carey, R.C.Byrd, C.D.Goodman, C.Gaarde, J.Larsen, D.Horen, J.Rapaport, E.Sugarbaker The (p, n) Reaction as a Probe of Beta Decay Strength NUCLEAR REACTIONS 12,14C, 42Ca, 28Si, 90Zr, 208Pb, 7Li, 54Fe(p, n), E=50-200 MeV; measured σ(Ep, θ=0°). 12,14N, 42Sc, 28P, 90Nb, 208Bi, 7Be, 54Co deduced reaction population, B(GT) proportionality.
doi: 10.1016/0375-9474(87)90089-3
1986CO03 Phys.Lett. 168B, 331 (1986) D.Contardo, M.Bedjidian, J.Y.Grossiord, A.Guichard, R.Haroutunian, J.R.Pizzi, C.Ellegaard, C.Gaarde, J.S.Larsen, C.Goodman, I.Bergqvist, A.Brockstedt, L.Carlen, P.Ekstrom, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, M.Boivin, P.Radvanyi Study of the Δ Isobar Excitation in Nuclei with the (3He, t) Reaction NUCLEAR REACTIONS 12C, 48Ca, 54Fe, 89Y, 159Tb, 208Pb(3He, t), E=2 GeV; measured σ(θ) vs triton momentum; deduced isobar excitation.
doi: 10.1016/0370-2693(86)91639-4
1986KI12 Phys.Lett. 175B, 279 (1986) N.S.P.King, P.W.Lisowski, G.L.Morgan, P.N.Craig, R.G.Jeppesen, D.A.Lind, J.R.Shepard, J.L.Ullmann, C.D.Zafiratos, C.D.Goodman, C.A.Goulding Observation of Fermi and Gamow-Teller Strength in the 800 MeV (p, n) Reaction NUCLEAR REACTIONS 6Li, 12,13C, 15N(p, n), E=800 MeV; measured σ(θ), σ(θ) vs neutron momentum. 12,13N, 15O, 6Be deduced Gamow-Teller, Fermi transition strengths.
doi: 10.1016/0370-2693(86)90856-7
1986TA05 Phys.Rev. C33, 746 (1986) T.N.Taddeucci, C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker Spin-Flip Decomposition of the Spectrum for 90Zr(p, n) at E(p) = 160 MeV NUCLEAR REACTIONS 90Zr(polarized p, n), E=160 MeV; measured σ(θ=0°), transverse polarization transfer. 90Nb deduced ΔL=0, ΔL=1 resonance excitations, transition strengths.
doi: 10.1103/PhysRevC.33.746
1985GO02 Phys.Rev.Lett. 54, 877 (1985); Erratum Phys.Rev.Lett. 54, 2060 (1985) C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker, T.N.Taddeucci Measurements of Gamow-Teller Strength Distributions in Masses 13 and 15 NUCLEAR REACTIONS 13C, 15N(polarized p, n), E=160 MeV; measured σ(θ), spin-flip probabilities. 13N, 15O deduced quenched Gamow-Teller transition strengths. Shell model comparison.
doi: 10.1103/PhysRevLett.54.877
1985KR10 Phys.Rev.Lett. 55, 1051 (1985) D.Krofcheck, E.Sugarbaker, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, I.J.Van Heerden, C.Gaarde, J.S.Larsen, D.J.Horen, T.N.Taddeucci Gamow-Teller Strength Function in 71Ge via the (p, n) Reaction at Medium Energies NUCLEAR REACTIONS 71Ga(p, n), E=120, 200 MeV; measured σ(En), σ(θ, En); deduced neutrino capture σ corrections in 71Ga detector. 71Ge deduced Gamow-Teller strength function, transition strength fragmentation.
doi: 10.1103/PhysRevLett.55.1051
1985RA11 Phys.Rev.Lett. 54, 2325 (1985) J.Rapaport, P.Welch, J.Bahcall, E.Sugarbaker, T.N.Taddeucci, C.D.Goodman, C.F.Foster, D.Horen, C.Gaarde, J.Larsen, T.Masterson Solar-Neutrino Detection: Experimental determination of Gamow-Teller strengths via the 98Mo and 115In(p, n) reactions NUCLEAR REACTIONS 98Mo, 115In(p, n), E=120, 200 MeV; measured σ(En, θ=0°); deduced target solar neutrino absorption σ. 98Tc, 115Sn deduced Gamow-Teller strengths.
doi: 10.1103/PhysRevLett.54.2325
1985TA23 Nucl.Instrum.Methods 241, 448 (1985) T.N.Taddeucci, C.D.Goodman, R.C.Byrd, T.A.Carey, D.J.Horen, J.Rapaport, E.Sugarbaker A Neutron Polarimeter for (p, n) Measurements at Intermediate Energies NUCLEAR REACTIONS 14C(polarized p, n), E=80, 120, 160 MeV; measured transverse polarization transfer, σ(En). Large volume, large acceptance neutron polarimeter, plastic scintillator.
doi: 10.1016/0168-9002(85)90597-2
1984GA11 Nucl.Phys. A422, 189 (1984) C.Gaarde, J.S.Larsen, H.Sagawa, N.Ohtsuka, J.Rapaport, T.N.Taddeucci, C.D.Goodman, C.C.Foster, C.A.Goulding, D.Horen, T.Masterson, E.Sugarbaker Spin-Dipole Strength in 12N NUCLEAR REACTIONS 12C(p, n), E=120, 160, 200 MeV; measured σ(θ). 12N deduced levels, J, π, analogs.
doi: 10.1016/0375-9474(84)90513-X
1984RA15 Nucl.Phys. A427, 332 (1984) J.Rapaport, R.Alarcon, B.A.Brown, C.Gaarde, J.Larsen, C.D.Goodman, C.C.Foster, D.Horen, T.Masterson, E.Sugarbaker, T.N.Taddeucci The 51V(p, n)51Cr Reaction at E(p) = 160 MeV NUCLEAR STRUCTURE 40,42,44,46,48Ca, 50Ti, 51V, 52Cr, 54Fe; calculated B(M1). 22O, 23F, 24Ne, 25Na, 26Mg, 27Al, 28Si; calculated Gamow-Teller transition strength. Shell model. NUCLEAR REACTIONS 51V(p, n), E=159.4 MeV; measured σ(θ), σ(En). 51Cr deduced levels, analogs, Gamow-Teller transition strengths. 50Ti, 51V(p, p'), (e, e'), (p, n), E not given; calculated Gamow-Teller transition strengths. Shell model.
doi: 10.1016/0375-9474(84)90089-7
1984RA22 Nucl.Phys. A431, 301 (1984) J.Rapaport, C.Gaarde, J.Larsen, C.Goulding, C.D.Goodman, C.Foster, D.J.Horen, T.Masterson, E.Sugarbaker, T.N.Taddeucci The 19F(p, n)19Ne and 39K(p, n)39Ca Reactions at Intermediate Energies and Quenching of the Gamow-Teller Strength NUCLEAR REACTIONS 19F, 39K(p, n), E=120, 160 MeV; measured σ(En), σ(θ). 19Ne, 39Ca levels deduced Gamow-Teller transition strength distribution. DWBA analysis.
doi: 10.1016/0375-9474(84)90177-5
1984TA07 Phys.Rev.Lett. 52, 1960 (1984) T.N.Taddeucci, T.A.Carey, C.Gaarde, J.Larsen, C.D.Goodman, D.J.Horen, T.Masterson, J.Rapaport, T.P.Welch, E.Sugarbaker Measurement of the Tranverse Spin-Transfer Coefficient D(NN)(0°) for (p(pol), n(pol)) Reactions at 160 MeV NUCLEAR REACTIONS 6,7Li, 12,13,14C, 90Zr(polarized p, n), E=160 MeV; measured transverse spin transfer coefficient D(NN)(θ=0°), polarized neutrons. 6,7Be, 12,13,14N, 90Nb deduced L=0 Gamow-Teller transition expected average value.
doi: 10.1103/PhysRevLett.52.1960
1983EL05 Phys.Rev.Lett. 50, 1745 (1983) C.Ellegaard, C.Gaarde, J.S.Larson, C.Goodman, I.Bergqvist, L.Carlen, P.Ekstrom, B.Jakobsson, J.Lyttkens, M.Bedjidian, M.Chamcham, J.Y.Grossiord, A.Guichard, M.Gusakow, R.Haroutunian, J.R.Pizzi, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, M.Boivin, P.Radvanyi (3He, t) Reaction at Intermediate Energies NUCLEAR REACTIONS C, 54Fe, 89Y(3He, t), E=0.6, 1.2, 2 GeV; measured σ(θ), σ(θ, Et); deduced spin-isospin excitation dominance, isobar resonance effects. DWIA, nucleon-nucleon data input.
doi: 10.1103/PhysRevLett.50.1745
1983RA30 Nucl.Phys. A410, 371 (1983) J.Rapaport, T.Taddeucci, T.P.Welch, C.Gaarde, J.Larsen, D.J.Horen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Giant Spin-Isospin Multipole Vibrations in 54,56Fe and 58,60Ni NUCLEAR REACTIONS 58Ni(p, n), E=120 MeV; 54,56Fe, 58,60Ni(p, n), E=160 MeV; measured σ(θ, En), θ < 6°, σ(θ). 58Cu, 54,56Co deduced L=0 transition strengths, Gamow-Teller state strengths. Shell model.
doi: 10.1016/0375-9474(83)90632-2
1983TA16 Phys.Rev. C28, 2511 (1983) T.N.Taddeucci, J.Rapaport, C.C.Foster, C.D.Goodman, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Spin Excitations in 40C(p, n) NUCLEAR REACTIONS 40Ca(p, n), E=59.3, 118.3, 159.3 MeV; measured σ(θ), σ(En). 40Sc level deduced Gamow-Teller transition strength. 42Ca(p, n), E=159.3 MeV; measured σ(θ). DWIA analyses.
doi: 10.1103/PhysRevC.28.2511
1982DO02 Phys.Rev.Lett. 48, 989 (1982) A.Doron, J.Alster, A.Erell, S.Gilad, M.A.Moinester, R.A.Anderson, H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, N.S.P.King, M.J.Leitch, J.P.Piffaretti, P.R.Bevington, E.Winkelmann, C.D.Goodman Energy Dependence of the Small-Angle Differential Cross Sections to Isobaric Analog States in 7Li(π+, π0)7Be and 13C(π+, π0)13N NUCLEAR REACTIONS 7Li, 13C(π+, π0), E=70, 100, 150, 165, 180 MeV; measured σ(θ), σ(E(π0)). 13N, 7Be deduced IAS excitation dependence on pion energy.
doi: 10.1103/PhysRevLett.48.989
1982DO10 Phys.Rev. C26, 189 (1982) A.Doron, J.Alster, A.Erell, M.A.Moinester, R.A.Anderson, H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, N.S.P.King, M.J.Leitch, J.P.Piffaretti, C.D.Goodman Angular Distributions of Single Pion Charge Exchange Reactions to Isobaric Analog States in Light Nuclei NUCLEAR REACTIONS 13C, 15N(π+, π0), E=164 MeV; measured σ(θ). 13N, 15O deduced IAS excitation. Enriched targets. Semiphenomenological isobar doorway, second-order coupled-channels calculations.
doi: 10.1103/PhysRevC.26.189
1982RA30 Phys.Lett. 119B, 61 (1982) J.Rapaport, T.Taddeucci, T.P.Welch, D.J.Horen, J.B.McGrory, C.Gaarde, J.Larsen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Gamow-Teller Resonances in A = 58 Nuclei NUCLEAR REACTIONS 58Ni(p, n), E=120, 160 MeV; measured σ(En, θ=0°). 58Cu deduced levels, isovector Gamow-Teller transition strength.
doi: 10.1016/0370-2693(82)90243-X
1982TA03 Phys.Rev. C25, 1094 (1982) T.N.Taddeucci, J.Rapaport, D.E.Bainum, C.D.Goodman, C.C.Foster, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Energy Dependence of the Ratio of Isovector Effective Interaction Strengths [J(στ)/J(τ)] from 0° (p, n) Cross Sections NUCLEAR REACTIONS 7Li, 13,14C, 26Mg, 37Cl, 42Ca(p, n), E=60-200 MeV; measured σ(θ=0°); deduced isovector effective interaction strength ratio. 7Be, 13,14N, 26Al, 37Ar, 42Sc levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.25.1094
1982TA06 Phys.Rev. C25, 2130 (1982) T.N.Taddeucci, J.Rapaport, C.D.Goodman Comment on ' Giant M1 States in Zr Isotopes within the Simple Shell Model ' NUCLEAR REACTIONS 90Zr(p, n), E=120, 200 MeV; 90Zr(p, p'), E=200 MeV; analyzed σ(θ); deduced optical model distortion energy dependence. 90Zr deduced M1 transition strength quenching factor. DWBA analysis.
doi: 10.1103/PhysRevC.25.2130
1981BL17 Phys.Lett. 107B, 336 (1981) S.D.Bloom, C.D.Goodman, S.M.Grimes, R.F.Hausman, Jr. Gamow-Teller Strength Function for 26Mg → 26Al NUCLEAR REACTIONS 26Mg(p, n), E=120 MeV; calculated Gamow-Teller strength function distribution. Shell model.
doi: 10.1016/0370-2693(81)90336-1
1981CO20 Phys.Rev. C24, 1834 (1981) J.R.Comfort, G.L.Moake, C.C.Foster, P.Schwandt, C.D.Goodman, J.Rapaport, W.G.Love Analyzing Powers for the 12C(p(pol), p')12C Reaction at 120 MeV and a Test of the Distorted-Wave Impulse Approximation NUCLEAR REACTIONS 12C(polarized p, p'), E=120 MeV; measured σ(E, θ), A(θ). DWIA analysis.
doi: 10.1103/PhysRevC.24.1834
1981FU04 Nucl.Phys. A356, 235 (1981) C.B.Fulmer, G.R.Satchler, E.E.Gross, F.E.Bertrand, C.D.Goodman, D.C.Hensley, J.R.Wu, N.M.Clarke, M.F.Steeden Elastic and Inelastic Scattering of 88 MeV 6Li Ions NUCLEAR REACTIONS 24,25,26Mg, 27Al, 40,48Ca, 59Co, 60Ni, 197Au, 206,208Pb(6Li, 6Li), 24,26Mg, 60Ni(6Li, 6Li'), E=88 MeV; measured σ(θ); deduced optical potentials. DWBA, coupled-channels calculations.
doi: 10.1016/0375-9474(81)90125-1
1981GA26 Nucl.Phys. A369, 258 (1981) C.Gaarde, J.Rapaport, T.N.Taddeucci, C.D.Goodman, C.C.Foster, D.E.Bainum, C.A.Goulding, M.B.Greenfield, D.J.Horen, E.Sugarbaker Excitation of Giant Spin-Isospin Multipole Vibrations NUCLEAR REACTIONS 40Ca, 90Zr, 112,124Sn, 208Pb, 169Tm(p, n), E=200 MeV; measured σ(En, θ). 40Sc, 90Nb, 112,124Sb, 169Yb, 208Bi deduced resonances, L, Gamow-Teller resonance characteristics, giant spin-isospin multipole vibrations. Enriched targets, time-compensated large volume detectors.
doi: 10.1016/0375-9474(81)90019-1
1981GO18 Phys.Lett. 107B, 406 (1981) C.D.Goodman, C.C.Foster, D.E.Bainum, S.D.Bloom, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, S.Grimes, J.Rapaport, T.N.Taddeucci, E.Sugarbaker Missing Gamow-Teller Strength in Mass 42 NUCLEAR REACTIONS 42Ca(p, n), E=160 MeV; measured σ(θ, En). 42Sc deduced Gamow-Teller transition strength distribution. Shell model.
doi: 10.1016/0370-2693(81)91217-X
1981HO03 Phys.Lett. 99B, 383 (1981) D.J.Horen, C.D.Goodman, D.E.Bainum, C.C.Foster, C.Gaarde, C.A.Goulding, M.B.Greenfield, J.Rapaport, T.N.Taddeucci, E.Sugarbaker, T.Masterson, S.M.Austin, A.Galonsky, W.Sterrenburg Energy Systematics of the Giant Gamow-Teller Resonance and a Charge-Exchange Dipole Spin-Flip Resonance NUCLEAR REACTIONS 90,92,94Zr, 112,116,124Sn, 169Tm, 208Pb(p, n), E=120, 160, 200 MeV; measured σ(En, θ). 90,92,94Nb, 112,116,124Sb, 169Yb, 208Bi deduced giant Gamow-Teller, charge exchange dipole spin-flip resonance energy systematics. Tof.
doi: 10.1016/0370-2693(81)90553-0
1981RA12 Phys.Rev. C24, 335 (1981) J.Rapaport, T.Taddeucci, C.Gaarde, C.D.Goodman, C.C.Foster, C.A.Goulding, D.Horen, E.Sugarbaker, T.G.Masterson, D.Lind 12C(p, n)12N Reaction at 120, 160, and 200 MeV NUCLEAR REACTIONS 12C(p, n), E=120, 160, 200 MeV; measured σ(En, θ); deduced energy independence of effective interaction spin-isospin term. Tof. Microscopic DWIA calculations.
doi: 10.1103/PhysRevC.24.335
1981RA19 Phys.Rev.Lett. 47, 1518 (1981) J.Rapaport, T.Taddeucci, P.Welch, C.Gaarde, J.Larsen, C.Goodman, C.C.Foster, C.A.Goulding, D.Horen, E.Sugarbaker, T.Masterson Empirical Evaluation of Gamow-Teller Strength Function for 37Cl → 37Ar and Its Implication in the Cross Section for Solar Neutrino Absorption by 37Cl NUCLEAR REACTIONS 37Cl(p, n), E=120 MeV; measured σ(En), σ(θ). 37Ar level deduced Gamow-Teller transition strengths, log ft. Tof.
doi: 10.1103/PhysRevLett.47.1518
1980BA16 Phys.Rev.Lett. 44, 1751 (1980) D.E.Bainum, J.Rapaport, C.D.Goodman, D.J.Horen, C.C.Foster, M.B.Greenfield, C.A.Goulding Observation of Giant Particle-Hole Resonances in 90Zr(p, n)90Nb NUCLEAR REACTIONS 90Zr(p, n), E=120 MeV; measured σ(En, θn). 90Nb deduced T=4, 5 components of Gamow-Teller strength, E1 resonance. Tof, macroscopic DWBA analysis.
doi: 10.1103/PhysRevLett.44.1751
1980GO07 Phys.Rev.Lett. 44, 1755 (1980) C.D.Goodman, C.A.Goulding, M.B.Greenfield, J.Rapaport, D.E.Bainum, C.C.Foster, W.G.Love, F.Petrovich Gamow-Teller Matrix Elements from 0°(p, n) Cross Sections NUCLEAR REACTIONS 7Li, 12,13C, 25,26Mg, 27Al, 28Si, 90Zr(p, n), E=120 MeV; measured σ(θ=0°). 7Be, 12,13N, 25,26Al, 27Si, 28P, 90Nb deduced Gamow-Teller matrix elements.
doi: 10.1103/PhysRevLett.44.1755
1980HO21 Phys.Lett. B95, 27 (1980) D.J.Horen, C.D.Goodman, C.C.Foster, C.A.Goulding, M.B.Greenfield, J.Rapaport, D.E.Bainum, E.Sugarbaker, T.G.Masterson, F.Petrovich, W.G.Love Search for Isobaric Analogues of M1 States and Giant Spinflip Resonance NUCLEAR REACTIONS 208Pb(p, n), E=120, 160 MeV; measured σ(θ, En). 209Bi deduced resonances, Γ, J, π, analog M1 states, giant spinflip resonance. Tof, enriched target.
doi: 10.1016/0370-2693(80)90391-3
1980WH03 Phys.Rev. C22, 1138 (1980) W.R.Wharton, C.D.Goodman, D.C.Hensley Gamow-Teller Sum Rules and the 14C(6Li, 6He)14N Reaction NUCLEAR REACTIONS 14C(6Li, 6He), E=62 MeV; measured σ(θ); 14N deduced Gamow-Teller sum rules. 14C level deduced configuration.
doi: 10.1103/PhysRevC.22.1138
1979GO16 Nucl.Phys. A331, 29 (1979) C.A.Goulding, M.B.Greenfield, C.C.Foster, T.E.Ward, J.Rapaport, D.E.Bainum, C.D.Goodman Comparison of the 12C(p, n)12N and 12C(p, p') Reactions at E = 62 and 120 MeV NUCLEAR REACTIONS 7Li(p, n), E=120 MeV; measured Eγ, Iγ, σ(θ); deduced production σ for 7Be. 12C(p, p'), E=62 MeV; measured σ(θ). 12C(p, n), E=62, 120 MeV; measured σ(θ).
doi: 10.1016/0375-9474(79)90298-7
1978GO04 Phys.Rev. C17, 493 (1978) C.D.Goodman, D.L.Hanson, D.C.Hensley, R.G.Stokstad Isospin Conservation in the Reactions 16O(p, t)14O(g.s.) And 16O(p, 3He)14N(2.31 MeV) NUCLEAR REACTIONS 16O(p, t), (p, 3He), E=27-30, 7 MeV; measured σ(E, θ). DWBA, Hauser-Feshbach analysis.
doi: 10.1103/PhysRevC.17.493
1976GO25 Phys.Lett. 64B, 417 (1976) C.D.Goodman, W.R.Wharton, D.C.Hensley The Reaction 14C(6Li, 6He)14N and the Distribution of Gamow-Teller Strength NUCLEAR REACTIONS 14C(6Li, 6He), E=62 MeV; measured σ(E(6He), θ). 14N levels deduced L, Gamow-Teller strength.
doi: 10.1016/0370-2693(76)90110-6
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
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
1974FI14 Phys.Rev. C10, 1560 (1974) H.W.Fielding, S.D.Schery, D.A.Lind, C.D.Zafiratos, C.D.Goodman Widths of Analog States in Heavy Elements from (p, n) Spectra NUCLEAR REACTIONS 197Au, 206,207,208Pb, 209Bi, 232Th(p, n), E=25.8 MeV; measured σ(En). 197Hg, 206,207,208Bi, 209Po, 232Pa IAR deduced level-widths.
doi: 10.1103/PhysRevC.10.1560
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
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
1973BE33 Phys.Rev.Lett. 31, 647 (1973) C.E.Bemis, Jr., R.J.Silva, D.C.Hensley, O.L.Keller, Jr., J.R.Tarrant, L.D.Hunt, P.F.Dittner, R.L.Hahn, C.D.Goodman X-Ray Identification of Element 104 RADIOACTIVITY 257Rf [from 249Cf(12C, 4n), E=73.0 MeV]; measured αx-coin, Eα. 214Ra measured T1/2. 253No levels deduced transitions, T1/2.
doi: 10.1103/PhysRevLett.31.647
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
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