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NSR database version of April 11, 2024.

Search: Author = C.D.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


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.


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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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0587.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0823.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0587.


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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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14204.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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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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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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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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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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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2624.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1972LE24      Phys.Rev. C6, 836 (1972)

L.Y.Lee, C.D.Goodman

Asymmetries in Gamma Scattering by Fe57

NUCLEAR REACTIONS 57Fe(γ, γ), E=14.4 keV; measured Iγ(θ, H) in Fe.

doi: 10.1103/PhysRevC.6.836
Citations: PlumX Metrics


1971DI03      Phys.Rev.Lett. 26, 1037 (1971)

P.F.Dittner, C.E.Bemis, Jr., D.C.Hensley, R.J.Silva, C.D.Goodman

Identification of the Atomic Number of Nobelium by an X-Ray Technique

RADIOACTIVITY 255No; measured αX-coin, αX-delay, Eα. 251Fm level deduced T1/2.

doi: 10.1103/PhysRevLett.26.1037
Citations: PlumX Metrics


1971KA21      Nucl.Phys. A172, 555 (1971)

D.G.Kamke, C.D.Goodman

States in 8Be Studied Through the Reaction 11B(p, α)8Be with 40 MeV Protons

NUCLEAR REACTIONS 11B(p, α), 11B(p, 3He), E=40 MeV; measured σ(Eα, θ(α)), σ(E(3He), θ(3He)). 8Be deduced level, level-width. 11B target.

doi: 10.1016/0375-9474(71)90043-1
Citations: PlumX Metrics


1971LE09      Phys.Rev. C3, 2027 (1971); Erratum Phys.Rev. C4, 284 (1971)

M.B.Lewis, C.D.Goodman, D.C.Hensley

Investigation of the 207Pb(α, d)209Bi Reaction

NUCLEAR REACTIONS 207Pb(α, d), E=42 MeV; measured σ(Ed, θ). 209Bi deduced levels, configurations.

doi: 10.1103/PhysRevC.3.2027
Citations: PlumX Metrics


1970GO07      Priv.Comm. (1970) to Be Published

C.D.Goodman, P.G.Roos, D.G.Kamke


1970LE06      Phys.Lett. To Be Published (1970)

M.B.Lewis, C.D.Goodman, D.Hensley

Investigation of the 207Pb(α, d)209Bi Reaction


1969EP01      Phys.Rev. 178, 1698 (1969)

M.Epstein, H.D.Holmgren, M.Jain, H.G.Pugh, P.G.Roos, N.S.Wall, C.D.Goodman, C.A.Ludemann

Study of the C12(p, pα)Be8 Reaction and Excited States of C12

NUCLEAR REACTIONS 12C(p, pα)8Be 12C(p, 2p), E=57 MeV; measured σ(Ep, Eα); deduced reaction mechanism. 12C deduced levels, J, π, proton decay, T.

doi: 10.1103/PhysRev.178.1698
Citations: PlumX Metrics


1969GO25      Bull.Am.Phys.Soc. 14, No.1, 121, KE4 (1969)

C.D.Goodman, P.G.Roos, D.G.Kamke

Excitation of T = 5 and T = 6 0+ States in 88Sr(3He, t)88Y


1967GO14      Phys.Rev. 156, 1249 (1967)

C.D.Goodman, J.D.Anderson, C.Wong

Quasi-Elastic (p, n) Scattering from Scandium and Titanium Isotopes

NUCLEAR STRUCTURE 47V, 46V, 48V, 49V, 45Ti, 56Co, 58Co, 52Mn, 55Fe, 27Si; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.156.1249
Citations: PlumX Metrics


1967GO33      Proc.Problem Symp.Nucl.Phys., Tbilisi, Vol.I, p.211 (1967)

C.D.Goodman

Experimental Evidence for Isobaric Spin in Direct Reaction Nuclear Spectroscopy

NUCLEAR REACTIONS 89Y(p, dγ), E not given; 90Zr(d, α), E not given; measured σ(Ed, Eγ), σ(Eα). 88Y levels deduced isobaric analog, configuration.


1966GO34      ORNL-3940, p.34 (1966)

C.D.Goodman, C.A.Ludemann, W.H.Kelly

Analog States Near N = 50

NUCLEAR REACTIONS 90Zr, 89Y(p, d), E = 36 MeV; measured Q, σ(Ed, θ). 88Y, 89Zr levels deduced L(n), isobaric analog.


1966LU08      Bull.Am.Phys.Soc. 11, No.1, 118, HA4 (1966)

C.A.Ludemann, C.D.Goodman, W.H.Kelly

Isobaric Analogs of Levels of 88Sr and 89Y

NUCLEAR REACTIONS 89Y, 90Zr(p, d), E=37 MeV; measured Q, σ(Ed, θ). 88Y, 89Zr isobaric analog, deduced Coulomb energy differences.


1965GO01      Bull.Am.Phys.Soc. 10, No.1, 27, BC13 (1965)

C.D.Goodman, W.H.Kelly, C.A.Ludemann

States in 87Y and 88Zr

NUCLEAR STRUCTURE 87Y, 88Zr; measured not abstracted; deduced nuclear properties.


1965GO16      ORNL-3800, p.12 (1965)

C.D.Goodman, C.A.Ludemann, W.H.Kelly

Shell-Model Studies for (p1/2)m (g9/2)n Configurations

NUCLEAR REACTIONS 89Y(p, d), E=19 MeV; measured σ(Ed, θ). 88Y deduced levels, J, π, L(n), S.


1965KE02      Bull.Am.Phys.Soc. 10, No.1, 121, KD1 (1965)

W.H.Kelly, C.A.Ludemann, C.D.Goodman

12C(p, d)11C Reaction at 36 MeV

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1965LU01      Bull.Am.Phys.Soc. 10, No.1, 122, KD5 (1965)

C.A.Ludemann, C.D.Goodman, W.H.Kelly

Levels in 88Y

NUCLEAR STRUCTURE 88Y; measured not abstracted; deduced nuclear properties.


1964GO02      Bull.Am.Phys.Soc. 9, No.1, 106, KC1 (1964)

C.D.Goodman

Three Spin 1/2- Levels in Zr89

NUCLEAR STRUCTURE 89Zr; measured not abstracted; deduced nuclear properties.


1964SW03      Bull.Am.Phys.Soc. 9, No.4, 483, JA3 (1964)

R.F.Sweet, J.B.Ball, C.D.Goodman, K.H.Bhatt

Measurement and Nuclear-Shell-Model Interpretation of the Low-Lying States of 92Nb

NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.


1963BA33      Phys.Rev. 130, 2341 (1963)

J.B.Ball, C.B.Fulmer, C.D.Goodman

(p, d), (p, t), and (p, α) Reactions to the Same Final States in Fe56 and in Zr90

NUCLEAR STRUCTURE 90Zr, 56Fe; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.130.2341
Citations: PlumX Metrics


1963BA78      Phys.Rev. 130, 2342 (1963)

J.B.Ball, C.B.Fulmer, C.D.Goodman

(p, d), (p, t), and (p, α) Reaction to the Same Final States in Fe56 and in Zr90

NUCLEAR REACTIONS 57Fe(p, d), 58Fe(p, t), 59Co(p, α), E=22.3 MeV; measured products, 56Fe, 2H, 3H, 4He; deduced σ(θ, E), σ(θ). Data were imported from EXFOR entry C1034.

doi: 10.1103/PhysRev.130.2342
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1034.


1963GO12      Phys.Rev.Letters 10, 247 (1963)

C.D.Goodman

Analogue States in Isobaric Nuclei

NUCLEAR STRUCTURE 89Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.10.247
Citations: PlumX Metrics


1963GO15      Ornl Annual Information Meeting p.88 (1963)

C.D.Goodman

Spectroscopic Factors for (p, d) and (p, t) Reactions on Zirconium Isotopes and the Relevance of Isotopic Spin

NUCLEAR STRUCTURE 89Zr; measured not abstracted; deduced nuclear properties.


1962BA01      Bull.Am.Phys.Soc. 7, No.1, 83, Y9 (1962)

J.B.Ball, C.D.Goodman, C.B.Fulmer

A Comparison of Cross-Sections for (p, d), (p, t) and (p, α) to the Same Final States

NUCLEAR STRUCTURE 90Zr, 56Fe; measured not abstracted; deduced nuclear properties.


1962FU02      Bull.Am.Phys.Soc. 7, No.1, 83, Y8 (1962)

C.B.Fulmer, J.B.Ball, C.D.Goodman

(p, t) Reactions in Zirconium Isotopes

NUCLEAR STRUCTURE 91Nb, 92Zr, 89Zr, 90Zr, 94Zr; measured not abstracted; deduced nuclear properties.


1962GO01      Bull.Am.Phys.Soc. 7, No.1, 82, Y7 (1962)

C.D.Goodman, C.B.Fulmer, J.B.Ball

NUCLEAR STRUCTURE 88Y, 95Zr, 90Zr, 92Nb, 91Zr, 93Zr; measured not abstracted; deduced nuclear properties.


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