NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = J.Rapaport Found 196 matches. Showing 1 to 100. [Next]2010CR03 Phys.Rev. C 82, 045211 (2010) C.Crawford, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.R.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, D.Hasell, P.Karpius, M.Kohl, H.Kolster, T.Lee, E.Lomon, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.Milner, J.Rapaport, R.Redwine, J.Seely, A.Shinozaki, A.Sindile, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart Role of mesons in the electromagnetic form factors of the nucleon
doi: 10.1103/PhysRevC.82.045211
2009FU03 Phys.Rev. C 79, 024314 (2009) H.Fujita, G.P.A.Berg, Y.Fujita, J.Rapaport, T.Adachi, N.T.Botha, H.Fujimura, K.Fujita, K.Hara, K.Hatanaka, J.Kamiya, T.Kawabata, K.Nakanishi, R.Neveling, N.Sakamoto, Y.Sakemi, Y.Shimbara, Y.Shimizu, F.D.Smit, M.Uchida, T.Wakasa, M.Yoshifuku, M.Yosoi, R.G.T.Zegers High resolution study of isovector negative parity states in the 16O(3He, t)16F reaction at 140 MeV/nucleon NUCLEAR REACTIONS 12C, 16O(3He, t), E=140 MeV/nucleon; measured triton spectra, σ, angular distributions. 16F; deduced levels, J, π, widths. 12N; deduced levels, J. Comparison with distorted wave Born approximation. 30Si(3He, t), E=140 MeV/nucleon; analyzed angular distribution data for IAS.
doi: 10.1103/PhysRevC.79.024314
2007MA46 Phys.Rev. C 76, 014004 (2007) Y.Maeda, H.Sakai, K.Fujita, M.B.Greenfield, K.Hatanaka, M.Hatano, J.Kamiya, T.Kawabata, H.Kuboki, H.Okamura, J.Rapaport, T.Saito, Y.Sakemi, M.Sasano, K.Sekiguchi, Y.Shimizu, K.Suda, Y.Tameshige, A.Tamii, T.Wakasa, K.Yako, J.Blomgren, P.Mermod, A.Ohrn, M.Osterlund, H.Witala, A.Deltuva, A.C.Fonseca, P.U.Sauer, W.Glockle, J.Golak, H.Kamada, A.Nogga, R.Skibinski Differential cross section and analyzing power measurements for (n-pol, d) elastic scattering at 248 MeV NUCLEAR REACTIONS 2H(n, n), E=248 MeV; measured En, σ and vector analyzing power.
doi: 10.1103/PhysRevC.76.014004
2007SO06 Phys.Rev. C 75, 034611 (2007) D.S.Sorenson, J.L.Ullmann, A.Ling, B.K.Park, R.C.Haight, N.S.P.King, R.A.Lindgren, H.Baghaei, E.J.Stephenson, F.P.Brady, J.L.Romero, J.Rapaport, B.L.Clausen, C.Wuest, F.Sammarruca Limitations of the distorted-wave impulse approximation in describing the energy dependence of the 10B(n, p)10Be(g.s.) reaction NUCLEAR REACTIONS 10B(n, p), E=70240 MeV; measured σ(E, θ). Comparison with zero- and finite-range DWIA predictions.
doi: 10.1103/PhysRevC.75.034611
2006SA38 Phys.Rev. C 74, 044003 (2006) M.Sarsour, T.Peterson, M.Planinic, S.E.Vigdor, C.Allgower, B.Bergenwall, J.Blomgren, T.Hossbach, W.W.Jacobs, C.Johansson, J.Klug, A.V.Klyachko, P.Nadel-Turonski, L.Nilsson, N.Olsson, S.Pomp, J.Rapaport, T.Rinckel, E.J.Stephenson, U.Tippawan, S.W.Wissink, Y.Zhou Measurement of the absolute differential cross section for np elastic scattering at 194 MeV NUCLEAR REACTIONS 1H(n, n), E=194 MeV; measured backscattering σ(θ). Comparison with previous results.
doi: 10.1103/PhysRevC.74.044003
2005SA06 Phys.Rev.Lett. 94, 082303 (2005) M.Sarsour, T.Peterson, M.Planinic, S.E.Vigdor, C.Allgower, B.Bergenwall, J.Blomgren, T.Hossbach, W.W.Jacobs, C.Johansson, J.Klug, A.V.Klyachko, P.Nadel-Turonski, L.Nilsson, N.Olsson, S.Pomp, J.Rapaport, T.Rinckel, E.J.Stephenson, U.Tippawan, S.W.Wissink, Y.Zhou Measurement of the Absolute np Scattering Differential Cross Section at 194 MeV NUCLEAR REACTIONS 1H(n, n), E=194 MeV; measured σ(θ). Tagged beam, comparisons with previous results and model predictions.
doi: 10.1103/PhysRevLett.94.082303
2005YA11 Phys.Lett. B 615, 193 (2005) K.Yako, H.Sakai, M.B.Greenfield, K.Hatanaka, M.Hatano, J.Kamiya, H.Kato, Y.Kitamura, Y.Maeda, C.L.Morris, H.Okamura, J.Rapaport, T.Saito, Y.Sakemi, K.Sekiguchi, Y.Shimizu, K.Suda, A.Tamii, N.Uchigashima, T.Wakasa Determination of the Gamow-Teller quenching factor from charge exchange reactions on 90Zr NUCLEAR REACTIONS 90Zr(n, p), E=293 MeV; measured σ(E, θ); 90Zr(p, n), E=295 MeV; analyzed σ(E, θ); deduced Gamow-Teller strengths, quenching factor.
doi: 10.1016/j.physletb.2005.04.032
2004OS02 Phys.Rev. C 70, 054613 (2004) J.H.Osborne, F.P.Brady, J.L.Romero, J.L.Ullmann, D.S.Sorenson, A.Ling, N.S.P.King, R.C.Haight, J.Rapaport, R.W.Finlay, E.Bauge, J.P.Delaroche, A.J.Koning Measurement of neutron elastic scattering cross sections for 12C, 40Ca, and 208Pb at energies from 65 to 225 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(n, n), E=65-225 MeV; measured σ(θ). Comparison with model predictions, previous results.
doi: 10.1103/PhysRevC.70.054613
2004PE18 Nucl.Instrum.Methods Phys.Res. A527, 432 (2004) T.Peterson, S.E.Vigdor, C.Allgower, B.Bergenwall, L.C.Bland, J.Blomgren, J.Doskow, T.Hossbach, W.W.Jacobs, C.Johansson, T.Kinashi, J.Klug, A.V.Klyachko, P.Nadel-Turonski, L.Nilsson, N.Olsson, M.Planinic, S.Pomp, J.Rapaport, T.Rinckel, E.J.Stephenson, U.Tippawan, S.W.Wissink, Y.Zhou Development of a tagged neutron facility at intermediate energies NUCLEAR REACTIONS 2H(p, 2p), E=200 MeV; measured proton spectra; deduced neutron spectrum, angular distribution. 1H(n, n), E ≈ 193 MeV; measured σ(θ). Tagged neutron beam facility.
doi: 10.1016/j.nima.2004.03.194
2003MB06 Mod.Phys.Lett. A 18, 298 (2003) Y.Maeda, H.Sakai, A.Tamii, S.Sakoda, H.Kato, M.Hatano, T.Saito, N.Uchigashima, H.Kuboki, K.Hatanaka, D.Hirooka, Y.Shimizu, Y.Kitamura, K.Fujita, N.Sakamoto, H.Okamura, K.Suda, T.Ikeda, K.Itoh, Y.Sakemi, T.Wakasa, J.Kamiya, K.Yako, K.Sekiguchi, Y.Sato, M.B.Greenfield, J.Rapaport, H.Kamada Measurement of differential cross sections and vector analyzing powers for the (n(pol))d reaction at 250 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=245 MeV; measured σ(θ), Ay(θ).
doi: 10.1142/S0217732303010387
2003ST16 Phys.Rev.Lett. 91, 142302 (2003) E.J.Stephenson, A.D.Bacher, C.E.Allgower, A.Gardestig, C.M.Lavelle, G.A.Miller, H.Nann, J.Olmsted, P.V.Pancella, M.A.Pickar, J.Rapaport, T.Rinckel, A.Smith, H.M.Spinka, U.van Kolck Observation of the Charge Symmetry Breaking d + d → 4He + π0 Reaction Near Threshold NUCLEAR REACTIONS 2H(d, π0), (d, 2γ), E=228.5, 231.8 MeV; measured missing mass spectra, pion production total σ; deduced charge symmetry breaking features.
doi: 10.1103/PhysRevLett.91.142302
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
2002RA51 Acta Phys.Hung.N.S. 16, 105 (2002) Spin Transfer Measurements in (p(pol), n(pol)) Reactions NUCLEAR REACTIONS 13C(polarized p, n), E=197 MeV; measured σ(E, θ), polarization transfer coefficients. 13N deduced level J, π.
doi: 10.1556/APH.16.2002.1-4.12
2002WA23 Phys.Rev. C66, 014606 (2002) X.Wang, J.Rapaport, M.Palarczyk, C.Hautala, X.Yang, D.L.Prout, B.Anderson, A.R.Baldwin, J.Olmsted, J.W.Watson, W.-M.Zhang, I.Van Heerden, E.J.Stephenson, R.Howes, S.Parks, E.Sugarbaker, B.A.Brown, F.Sammarruca Polarization Transfer Measurements for the 13C(p(pol), n(pol))13N Reaction at 197 MeV and Empirical Isovector Spin-Longitudinal Response for the (1/2)g.s.- → (1/2)1+ Transition NUCLEAR REACTIONS 13C(polarized p, n), E=197 MeV; measured excitation energy spectra, σ(E, θ), polarization transfer coefficients. 13N deduced transitions spin-transverse and spin-longitudinal components. Comparison with model predictions.
doi: 10.1103/PhysRevC.66.014606
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
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
2001SA33 Nucl.Phys. A689, 353c (2001) H.Sakai, Y.Maeda, K.Sekiguchi, W.Glockle, M.B.Greenfield, K.Hatanaka, M.Hatano, D.Hirooka, H.Kamada, J.Kamiya, H.Kato, T.Ohnishi, H.Okamura, J.Rapaport, T.Saito, N.Sakamoto, S.Sakoda, Y.Satou, K.Suda, A.Tamii, N.Uchigashima, T.Uesaka, T.Wakasa, H.Witala, K.Yako d(pol)p and n(pol)d Scatterings at Intermediate Energy and Three-Nucleon Force Effects NUCLEAR REACTIONS 1H(polarized d, d), E=270 MeV; 2H(polarized n, n), E=250 MeV; measured σ(θ), Ay(θ). Comparison with model predictions.
doi: 10.1016/S0375-9474(01)00853-3
2001WA05 Phys.Rev. C63, 024608 (2001) X.Wang, J.Rapaport, M.Palarczyk, C.Hautala, X.Yang, D.L.Prout, I.Van Heerden, R.Howes, S.Parks, E.Sugarbaker, B.A.Brown Zero Degree Polarization Transfer Measurements for the 13C(p(pol), n(pol))13N Reaction at 197 MeV and Empirical Gamow-Teller Strength Distribution NUCLEAR REACTIONS 13C(polarized p, n), E=197 MeV; measured σ(E, θ=0°), polarization transfer observables; deduced Gamow-Teller strength distribution. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.63.024608
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
2000HI06 Phys.Rev. C61, 054609 (2000) K.Hicks, V.Gladyshev, H.Baghaei, A.Caracappa, A.Cichocki, R.Deininger, R.Finlay, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Li, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, D.Willits, L.E.Wright The 16O(γ(pol), π-p) Reaction at Eγ ≈ 300 MeV NUCLEAR REACTIONS 16O(polarized γ, π-p), E=290-325 MeV; measured σ(E, θ1, θ2), spin asymmetries. Comparison with DWIA results.
doi: 10.1103/PhysRevC.61.054609
2000PE14 Nucl.Phys. A663-664, 1057c (2000) T.Peterson, L.C.Bland, J.Blomgren, W.W.Jacobs, T.Kinashi, A.Klyachko, P.Nadel-Turonski, L.Nilsson, N.Olsson, J.Rapaport, T.Rinckel, E.J.Stephenson, S.E.Vigdor, S.W.Wissink, Y.Zhou Development of a Tagged Neutron Facility for Neutron Scattering Experiments at Intermediate Energies
doi: 10.1016/S0375-9474(99)00769-1
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
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
1998AN09 Nucl.Phys. A631, 752c (1998) B.D.Anderson, D.L.Prout, M.Palarczyk, A.Ahmidouch, A.R.Baldwin, D.Cooper, C.C.Foster, W.Glockle, M.S.Islam, C.Hautala, K.Hicks, M.Khayat, B.Luther, R.Madey, D.M.Manley, I.Niculescu, J.Rapaport, G.Savopulos, J.Sowinski, E.R.Sugarbaker, R.Suleiman, I.Van Heerden, J.W.Watson, H.Witala, X.Yang, W.M.Zhang Measurement of a Complete Set of Spin Observables in the 2H(p, n)2p Reaction at 200 MeV NUCLEAR REACTIONS 2H(polarized p, n), E=200 MeV; measured σ(θ), spin observables. Three-body Fadeev calculations.
doi: 10.1016/S0375-9474(98)00104-3
1997HI01 Phys.Rev. C55, R12 (1997) K.Hicks, H.Baghaei, A.Caracappa, A.Cichocki, G.Davenport, R.Finlay, V.Gladyshev, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Lee, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, L.E.Wright Spin Asymmetries from 16O(γ(pol), pπ-) Near Δ Resonance Energies NUCLEAR REACTIONS 16O(polarized γ, pπ-), E=293 MeV; measured spin asymmetry vs θp, θ(π); deduced Δ-nucleus potential, δ lifetime dependences.
doi: 10.1103/PhysRevC.55.R12
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
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
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
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
1994RA23 Nucl.Phys. A577, 83c (1994) Charge-Exchange Spin-Dipole and Quasifree Excitations in p-Shell Nuclei NUCLEAR REACTIONS 6,7Li, 10,11B, 12,13C(polarized p, n), E=186 MeV; measured σ(θ, En), σ(θ), analyzing power, neutron polarization, spin observable vs θ; deduced quasifree excitation role in giant resonance region.
doi: 10.1016/0375-9474(94)90838-9
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
1993MA33 Nucl.Phys. A561, 387 (1993) A.Marcinkowski, J.Rapaport, R.W.Finlay, C.Brient, M.Herman, M.B.Chadwick Neutron Emission Cross Sections at Low Bombarding Energies and the Novelty in Multistep Compound Reaction Model NUCLEAR REACTIONS 165Ho, 181Ta(n, xn), E=6.7, 20 MeV; measured σ(E(n), θ); deduced reaction mechanism. Modified statistical multistep model analysis.
doi: 10.1016/0375-9474(93)90018-S
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
1993PA18 Phys.Rev. C48, 711 (1993) B.K.Park, J.Rapaport, G.Fink, J.L.Ullmann, A.G.Ling, D.S.Sorenson, F.P.Brady, J.L.Romero, C.R.Howell, W.Tornow, W.Unkelbach Energy Dependence of Multipole Strength Distributions in the 32S(n, p)32P Reaction NUCLEAR REACTIONS 32S(n, p), E=60-220 MeV; measured σ(θ, Ep), σ(θ); deduced Gamow-Teller transition strengths. Shell model, RPA comparison.
doi: 10.1103/PhysRevC.48.711
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
1993WA09 Phys.Rev. C47, 2677 (1993) Y.Wang, C.C.Foster, R.D.Polak, J.Rapaport, E.J.Stephenson Proton-90Zr Mean Field between -60 and + 185 MeV from a Dispersive Optical Model Analysis NUCLEAR REACTIONS 90Zr(polarized p, p), E=9.8-135 MeV; analyzedσ(θ), analyzing power data; deduced model parameters. 90Zr deduced proton single particle orbits occupation probabilities, spectroscopic factors. Dispersive optical model potential.
doi: 10.1103/PhysRevC.47.2677
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
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
1992PA06 Phys.Rev. C45, 1791 (1992) B.K.Park, J.Rapaport, J.L.Ullmann, A.G.Ling, D.S.Sorenson, F.P.Brady, J.L.Romero, C.R.Howell, W.Tornow, T.C.Ronnqvist Gamow-Teller and Dipole Strength Distribution in 40Ca(n, p)40K Reaction NUCLEAR REACTIONS 40Ca(n, p), E=60-260 MeV; measured σ(E, θ). 40K deduced Gamow-Teller strength, dipole, spin-dipole transition strength. DWIA analysis, compared with 1p-1h shell model predictions.
doi: 10.1103/PhysRevC.45.1791
1992RA20 Phys.Rev.Lett. 69, 2444 (1992) Comment on ' Is the Weak Axial-Vector Current Renormalized in Nuclei ( Question ) ' NUCLEAR STRUCTURE 37Ar, 37K; caluclated Gamow-Teller transition strength; deduced support for (p, n) reaction, β+ decay probes specific proportionality.
doi: 10.1103/PhysRevLett.69.2444
1992SO02 Phys.Rev. C45, R500 (1992) D.S.Sorenson, X.Aslanoglou, F.P.Brady, J.R.Drummond, R.C.Haight, C.R.Howell, N.S.P.King, A.Ling, P.W.Lisowski, B.K.Park, J.Rapaport, J.L.Romero, W.Tornow, J.L.Ullmann Energy Dependence of the Gamow-Teller Strength in p-Shell Nuclei Observed in the (n, p) Reaction NUCLEAR REACTIONS 6Li, 13,12C(n, p), E=60-260 MeV; measured σ(θ, E); deduced unit σ, effective interaction volume integrals.
doi: 10.1103/PhysRevC.45.R500
1992WA12 Phys.Rev. C45, 2891 (1992) Y.Wang, C.C.Foster, E.J.Stephenson, L.Yuan, J.Rapaport Dispersion Relation Analysis of d + 208Pb Elastic Scattering NUCLEAR REACTIONS 208Pb(polarized d, d), E=9-79.2 MeV; analyzed σ(θ), analyzing power data; deduced model parameters. Dispersive optical model.
doi: 10.1103/PhysRevC.45.2891
1991GL01 Phys.Rev. C43, 1664 (1991) C.W.Glover, C.C.Foster, P.Schwandt, J.R.Comfort, J.Rapaport, T.N.Taddeucci, D.Wang, G.J.Wagner, J.Seubert, A.W.Carpenter, J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton Scattering of Polarized Protons from 7Li at 200 MeV NUCLEAR REACTIONS 7Li(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ. 6,7Li deduced radial density shape differences. Single scattering model.
doi: 10.1103/PhysRevC.43.1664
1991HI05 Phys.Rev. C43, 2554 (1991) K.H.Hicks, A.Celler, O.Hausser, R.Henderson, K.P.Jackson, B.Pointon, J.Rapaport, M.Vetterli, S.Yen Multipole Strength in 16O(n, p)16N at 298 MeV NUCLEAR REACTIONS 16O(n, p), E=298 MeV; measured σ(Ep, θ). 16N deduced Gamow-Teller, spin-dipole transition strength functions.
doi: 10.1103/PhysRevC.43.2554
1991LI36 Phys.Rev. C44, 2794 (1991) A.Ling, X.Aslanoglou, F.P.Brady, R.W.Finlay, R.C.Haight, C.R.Howell, N.S.P.King, P.W.Lisowski, B.K.Park, J.Rapaport, J.L.Romero, D.S.Sorenson, W.Tornow, J.L.Ullmann Ground-State Gamow-Teller Strength in 64Ni(n, p)64Co Cross Sections at 90-240 MeV NUCLEAR REACTIONS 64Ni(n, p), E=90-240 MeV; measured σ(E, θ); deduced unit σ. DWIA analysis.
doi: 10.1103/PhysRevC.44.2794
1991MA32 Nucl.Phys. A530, 75 (1991) A.Marcinkowski, J.Rapaport, R.Finlay, X.Aslanoglou, D.Kielan Neutron Emission Cross Sections on 93Nb and 209Bi at 20 MeV Incident Energy NUCLEAR REACTIONS 93Nb, 209Bi(n, xn), E=20 MeV; measured σ(En, θ). Statistical multistep theory analysis.
doi: 10.1016/0375-9474(91)90756-V
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
1990GL04 Phys.Rev. C41, 2487 (1990) C.W.Glover, C.C.Foster, P.Schwandt, J.R.Comfort, J.Rapaport, T.N.Taddeucci, D.Wang, G.J.Wagner, J.Seubert, A.W.Carpenter, J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton Scattering of Polarized Protons from 6Li at 200 MeV NUCLEAR REACTIONS 6Li(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs (θ). Microscopic single scattering model with free, Pauli corrected effective nucleon-nucleon interactions.
doi: 10.1103/PhysRevC.41.2487
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
1990WA13 Nucl.Phys. A517, 301 (1990) Neutron Scattering from 90,91,92,94Zr NUCLEAR REACTIONS 90,91,92,94Zr(n, n), (n, n'), E=8, 10, 24 MeV; measured σ(θ); deduced optical model parameters, isoscalar, isovector potential depths. 90,92,94Zr levels deduced deformation lengths, transition matrix element ratios. Excited core model analysis for 91Zr, coupled-channels, microscopic calculations.
doi: 10.1016/0375-9474(90)90037-M
1989DE04 Phys.Rev. C39, 391 (1989) J.P.Delaroche, Y.Wang, J.Rapaport Neutron-90Zr Mean Field from a Dispersive Optical Model Analysis NUCLEAR REACTIONS 90Zr(n, n), E=8, 10, 24 MeV; measured σ(θ); deduced optical model neutron mean field, Hartree-Fock empirical parameters. Enriched target. Other data analyzed.
doi: 10.1103/PhysRevC.39.391
1989MA42 Nucl.Phys. A501, 1 (1989) A.Marcinkowski, R.W.Finlay, J.Rapaport, P.E.Hodgson, M.B.Chadwick Neutron Emission Cross Sections on 184W at 11.5 and 26 MeV and the Neutron-Nucleus Scattering Mechanism NUCLEAR REACTIONS 184W(n, xn), (n, n), E=11.5, 26 MeV; measured σ(En, θ). Statistical multistep theory analysis. Tof.
doi: 10.1016/0375-9474(89)90562-9
1989RA09 Phys.Rev. C39, 1929 (1989) J.Rapaport, P.W.Lisowski, J.L.Ullmann, R.C.Byrd, T.A.Carey, J.B.McClelland, L.J.Rybarcyk, T.N.Taddeucci, R.C.Haight, N.S.P.King, G.L.Morgan, D.A.Clark, D.E.Ciskowski, D.A.Lind, R.Smythe, C.D.Zafiratos, D.Prout, E.R.Sugarbaker, D.Marchlenski, W.P.Alford, W.G.Love Fermi and Gamow-Teller Strength in p-Shell Nuclei from (p, n) Reactions at 492 and 590 MeV NUCLEAR REACTIONS 7Li, 11B, 12,13,14C(p, n), E=492 MeV; 13C, 11B(p, n), E=590 MeV; measured σ(θ, E); deduced unit σ(ratio).
doi: 10.1103/PhysRevC.39.1929
1988HA25 Phys.Rev. C38, 525 (1988) L.F.Hansen, J.Rapaport, X.Wang, F.A.Barrios, F.Petrovich, A.W.Carpenter, M.J.Threapleton Proton and Neutron Transition Densities in 6,7Li from Low Energy Neutron and Proton Scattering NUCLEAR REACTIONS 6,7Li(n, n), (n, n'), E=24 MeV; measured σ(θ). 6,7Li deduced transition densities.
doi: 10.1103/PhysRevC.38.525
1988IS03 Phys.In Med.Biol. 33, 315 (1988) M.S.Islam, R.W.Finlay, J.S.Petler, J.Rapaport, R.Alarcon, J.Wierzbicki Neutron Scattering Cross Sections and Partial Kerma Values for Oxygen, Nitrogen and Calcium at 18 < En < 60 MeV NUCLEAR REACTIONS 14N, 16O, 40Ca(n, n), (n, n'), E=18-60 MeV; measured σ(θ); deduced optical model parameters, partial kerma factors. Previously acquired data included in analysis.
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
1988WA27 Z.Phys. A331, 305 (1988) Nuclear Scattering Analysis from 90,92,94Zr and Isospin Decomposition of Transition Matrix Elements for Low-Lying Collective Transitions NUCLEAR REACTIONS 90,92,94Zr(n, n'), E=8-24 MeV; measured σ(En), σ(θ). 90,92,94Zr level deduced deformation length, neutron, proton matrix element ratio. Proton data input.
1987AL02 Nucl.Phys. A462, 413 (1987) R.Alarcon, J.Rapaport, R.W.Finlay Nucleon Elastic Scattering from 40Ca between 11 and 48 MeV NUCLEAR REACTIONS Ca(n, n), E=19, 21.7, 25.5 MeV; measured σ(θ); 40Ca(n, n), (p, p), E=11-48 MeV; analyzed σ(θ). Optical model.
doi: 10.1016/0375-9474(87)90397-6
1987AL03 Nucl.Phys. A462, 445 (1987) Neutron Inelastic Scattering from 40Ca at 21.7 and 25.5 MeV NUCLEAR REACTIONS Ca(n, n'), E=21.7, 25.5 MeV; measured σ(θ), σ(En). 40Ca levels deduced deformation parameters, octupole moments, B(λ). Natural target. Coupled-channels analysis.
doi: 10.1016/0375-9474(87)90398-8
1987DO06 Nucl.Phys. A467, 511 (1987) The 26Mg(p, n)26Al and 23Na(α, n)26Al Reactions near Threshold NUCLEAR REACTIONS, ICPND 26Mg(p, n), E=5.3-7 MeV; 23Na(α, n), E=3.9-5.9 MeV; 26Mg(p, p'), 26Mg(p, α), E=5.3-6.1 MeV; measured σ(E), σ(E, E(n), θ), σ(E, E(p), θ), σ(E, E(α), θ); deduced thermonuclear reaction rate. 26Al deduced levels, resonance strengths, Γ, J, π, p, α-induced reaction rate. Enriched 26Mg target.
doi: 10.1016/0375-9474(87)90542-2
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
1987PO18 Can.J.Phys. 65, 687 (1987) D.Pocanic, K.Wang, C.J.Martoff, S.S.Hanna, R.C.Byrd, C.C.Foster, D.L.Friesel, J.Rapaport First (n, p) Measurements with the Indiana University Cyclotron Facility NUCLEAR REACTIONS 6Li(n, p), E=118 MeV; measured σ(Ep), σ(θp). Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13152. 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
1987RA32 Can.J.Phys. 65, 574 (1987) On the Quenching of Gamow-Teller Strength NUCLEAR REACTIONS 6,7Li(p, n), E=80, 120, 160, 200 MeV; 9Be(p, n), E=135 MeV; 11B(p, n), E=26, 160 MeV; 12,13,14C(p, n), E not given; 15N(polarized p, n), E=160 MeV; analyzed data; deduced Gamow-Teller transitions B(GT), quenching factor.
doi: 10.1139/p87-081
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
1987WA08 Nucl.Phys. A465, 483 (1987) X.Wang, Y.Wang, D.Wang, J.Rapaport Neutron Scattering and Neutron Emission Cross Sections on 27Al, 93Nb and 209Bi at 7 MeV NUCLEAR REACTIONS 27Al, 93Nb, 209Bi(n, xn), E=7 MeV; measured σ(θ) vs En. Compound nucleus, pre-equilibrium analyses.
doi: 10.1016/0375-9474(87)90360-5
1986AL21 Nucl.Phys. A458, 502 (1986) Neutron Elastic and Inelastic Scattering from 28Si, 32S and 34S NUCLEAR REACTIONS Si, S, 34S(n, n), (n, n'), E=21.7 MeV; 34S(n, n), (n, n'), E=25.5 MeV. 28Si levels deduced β2, β4, multipole moments, B(λ). 32,34S levels deduced β, B(λ). Coupled-channels analysis. Natural Si, S targets.
doi: 10.1016/0375-9474(86)90048-5
1986DE29 Phys.Rev. C34, 2005 (1986) J.P.Delaroche, Y.Wang, J.Rapaport Hadronic Excitation of the Second O+ State in 90Zr NUCLEAR REACTIONS 90Zr(p, p'), E=12.7, 18.8, 25, 40 MeV; 90Zr(n, n'), E=8 MeV; 90Zr(α, α'), E=65 MeV; calculated reaction mechanism. Coupled channels calculations.
doi: 10.1103/PhysRevC.34.2005
1986RA21 Radiat.Eff. 95, 223 (1986) Physics with Monoenergetic Neutrons below 100 MeV NUCLEAR REACTIONS 40Ca(n, n), E=21.7 MeV; 40Ca(p, p), E=30.3 MeV; 54Fe(n, n'), E=20, 22, 24, 26 MeV; 2H(d, n), E ≤ 90 MeV; 3H(d, n), E ≤ 30 MeV; 2,3H, 6,7Li(p, n), E ≤ 200 MeV; analyzed, calculated σ(θ), σ(E).
doi: 10.1080/00337578608208701
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
1986WA14 Nucl.Phys. A454, 359 (1986) The Optical Model Potential for Low-Energy Nucleons NUCLEAR STRUCTURE A=28-76; analyzed low energy proton optical potential parameters; deduced average Fermi energy role.
doi: 10.1016/0375-9474(86)90273-3
1985AL03 Phys.Rev. C31, 697 (1985) R.Alarcon, J.Rapaport, R.T.Kouzes, W.H.Moore, B.A.Brown Nucleon Scattering from 34S and the Relative Sign of Neutron and Proton Transition Matrix Elements for the (0 → 2+2) Transition NUCLEAR REACTIONS 34S(p, p'), E=29.8 MeV; measured σ(Ep), σ(θ). 34S(n, n'), E=21.7 MeV; measured σ(θ); deduced optical model parameters, absolute σ. 34S level deduced σ(θ), neutron to proton matrix element ratios. Coupled-channels analysis.
doi: 10.1103/PhysRevC.31.697
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
1984BA56 Phys.Rev.Lett. 53, 2078 (1984) A.J.Baltz, J.Weneser, B.A.Brown, J.Rapaport Specificity of the (p, n) Reaction at 35 MeV for Gamow-Teller Strength NUCLEAR REACTIONS 71Ga(p, n), E=35 MeV; calculated σ(θ); deduced no correspondence between σ(θ=0°), Gamow-Teller transition strength, inadequacy to estimate solar neutrino absorption.
doi: 10.1103/PhysRevLett.53.2078
1984DA22 Phys.Rev. C30, 1999 (1984) J.D'Auria, M.Dombsky, L.Moritz, T.Ruth, G.Sheffer, T.E.Ward, C.C.Foster, J.W.Watson, B.D.Anderson, J.Rapaport Activation Measurements of the 7Li(p, n)7Be Reaction from 60-480 MeV NUCLEAR REACTIONS, ICPND 7Li(p, n), E=60-480 MeV; measured reaction σ. Activation analysis. Comparison with theoretical analysis.
doi: 10.1103/PhysRevC.30.1999
1984FI12 Phys.Rev. C30, 796 (1984) R.W.Finlay, J.R.M.Annand, T.S.Cheema, J.Rapaport, F.S.Dietrich Energy Dependence of Neutron Scattering from 208Pb in the Energy Range 7-50 MeV NUCLEAR REACTIONS 208Pb(n, n), E=7, 20, 22, 24 MeV; 208Pb(n, n'), E=7, 20, 22 MeV; measured σ(E, θ); deduced optical model parameters. 208Pb level deduced octupole deformation parameter.
doi: 10.1103/PhysRevC.30.796
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
1984KU09 Nucl.Phys. A420, 237 (1984) J.P.Kurup, R.W.Finlay, J.Rapaport, J.P.Delaroche Strong coupling and isospin effects in neutron scattering from 76, 80Se NUCLEAR REACTIONS 76Se, 80Se(n, n), (n, n'), E=8, 10 MeV; measured σ(θ), σ(En); deduced optical model parameters. 80,76Se levels deduced deformation parameters. Tof. Coupled-channels analyses.
doi: 10.1016/0375-9474(84)90441-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
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
1983TA09 Nucl.Phys. A401, 237 (1983) R.C.Tailor, J.Rapaport, R.W.Finlay, G.Randers-Pehrson Neutron Scattering from 26Mg NUCLEAR REACTIONS 26Mg(n, n), (n, n'), E=24 MeV; measured σ(E, θ); deduced optical model parameters. 26Mg levels deduced deformation parameters, neutron, proton transition matrix elements ratio. Enriched target. DWBA, coupled-channels model analyses.
doi: 10.1016/0375-9474(83)90528-6
1983TA12 Phys.Rev. C28, 969 (1983) T.N.Taddeucci, J.Rapaport, C.C.Foster, J.R.Comfort 14N(p(pol), p')14N(2.31 MeV) Reaction at 159.4 MeV NUCLEAR REACTIONS 12C, 14N(polarized p, p), (polarized p, p'), E=159.4 MeV; measured σ(θ), analyzing power vs θ. Single-step DWBA, DWIA analyses.
doi: 10.1103/PhysRevC.28.969
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
1982FI08 Nucl.Instrum.Methods 198, 197 (1982) R.W.Finlay, C.E.Brient, D.E.Carter, A.Marcinkowski, S.Mellema, G.Randers-Pehrson, J.Rapaport The Ohio University Beam Swinger Facility NUCLEAR REACTIONS B(d, n), E=8 MeV; 12C(n, n), (n, n'), E=24 MeV; measured σ(En); 208Pb(n, n), (n, n'), E=7.2 MeV; measured σ(θ). Tof, beam swinger magnet.
doi: 10.1016/0167-5087(82)90256-3
1982GR26 Nucl.Instrum.Methods 203, 269 (1982) S.M.Grimes, P.Grabmayr, R.W.Finlay, S.L.Graham, G.Randers-Pehrson, J.Rapaport A Technique to Correct for Backgrounds Caused by Break-Up Neutrons from the D(d, n) Reaction NUCLEAR REACTIONS 2H, 3,4He(d, n), E=8 MeV; measured σ(En). 2H(d, n), E=8.03, 6.04 MeV; 3He(d, n), E=7.78, 8.28, 6.4, 6.15 MeV; measured breakup σ(θn=0°).
doi: 10.1016/0167-5087(82)90636-6
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