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NSR database version of April 11, 2024.

Search: Author = C.Goodman

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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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0864.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0863.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0792.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0809.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0443.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0428.


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
Citations: PlumX Metrics


1994GO23      Nucl.Phys. A577, 3c (1994)

C.D.Goodman

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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