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NSR database version of February 19, 2024.

Search: Author = B.D.Anderson

Found 80 matches.

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2014MO25      J.Phys.(London) G41, 105109 (2014)

P.Monaghan, R.Shneor, R.Subedi, B.D.Anderson, K.Aniol, J.Annand, J.Arrington, H.B.Benaoum, F.Benmokhtar, P.Bertin, W.Bertozzi, W.Boeglin, J.P.Chen, S.Choi, E.Chudakov, C.Ciofi degli Atti, E.Cisbani, W.Cosyn, B.Craver, C.W.de Jager, R.J.Feuerbach, E.Folts, S.Frullani, F.Garibaldi, O.Gayou, S.Gilad, R.Gilman, O.Glamazdin, J.Gomez, O.Hansen, D.W.Higinbotham, T.Holmstrom, H.Ibrahim, R.Igarashi, E.Jans, X.Jiang, L.Kaufman, A.Kelleher, A.Kolarkar, E.Kuchina, G.Kumbartzki, J.J.LeRose, R.Lindgren, N.Liyanage, D.J.Margaziotis, P.Markowitz, S.Marrone, M.Mazouz, D.Meekins, R.Michaels, B.Moffit, H.Morita, S.Nanda, C.F.Perdrisat, E.Piasetzky, M.Potokar, V.Punjabi, Y.Qiang, J.Reinhold, B.Reitz, G.Ron, G.Rosner, J.Ryckebusch, A.Saha, B.Sawatzky, J.Segal, A.Shahinyan, S.Sirca, K.Slifer, P.Solvignon, V.Sulkosky, N.Thompson, P.E.Ulmer, G.M.Urciuoli, E.Voutier, K.Wang, J.W.Watson, L.B.Weinstein, B.Wojtsekhowski, S.Wood, H.Yao, X.Zheng, L.Zhu

Measurement of the 12C(e, e'p)11B two-body breakup reaction at high missing momentum

NUCLEAR REACTIONS 12C(E, E'P), E200-400 MeV; measured reaction products, Ep, Ip; deduced σ(θ, E). Comparison with WS+Glauber calculations.

doi: 10.1088/0954-3899/41/10/105109
Citations: PlumX Metrics


2008AN15      Phys.Rev. C 78, 065803 (2008)

N.Anantaraman, S.M.Austin, B.A.Brown, G.M.Crawley, A.Galonsky, R.G.T.Zegers, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, J.W.Watson, C.C.Foster

Electron capture strength for 60, 62Ni and 58, 60, 62, 64Ni(p, n)58, 60, 62, 64Cu reactions at 134.3 MeV

NUCLEAR REACTIONS 58,60,62,64Ni(p, n), E=134.3 MeV; measured neutron spectra, angular distributions, σ; calculated B(GT), reaction rates. 58,60,62,64Cu; deduced levels. Comparison with (n, p) reactions, shell model calculations.

doi: 10.1103/PhysRevC.78.065803
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1743.


2006MA08      Nucl.Phys. A764, 261 (2006)

G.MacLachlan, A.Aghalaryan, A.Ahmidouch, B.D.Anderson, R.Asaturyan, O.Baker, A.R.Baldwin, D.Barkhuff, H.Breuer, R.Carlini, E.Christy, S.Churchwell, L.Cole, E.Crouse, S.Danagoulian, D.Day, T.Eden, M.Elaasar, R.Ent, M.Farkhondeh, H.Fenker, J.M.Finn, L.Gan, K.Garrow, P.Gueye, C.R.Howell, B.Hu, M.K.Jones, J.J.Kelly, C.Keppel, M.Khandaker, W.-Y.Kim, S.Kowalski, A.Lai, A.Lung, D.Mack, R.Madey, D.M.Manley, P.Markowitz, J.Mitchell, H.Mkrtchyan, A.K.Opper, B.Plaster, C.Perdrisat, V.Punjabi, B.Raue, T.Reichelt, J.Reinhold, J.Roche, Y.Sato, N.Savvinov, A.Yu.Semenov, I.A.Semenova, W.Seo, N.Simicevic, G.Smith, S.Taylor, S.Stepanyan, V.Tadevosyan, S.Tajima, L.Tang, W.Tireman, P.E.Ulmer, W.Vulcan, J.W.Watson, S.P.Wells, F.Wesselmann, S.Wood, C.Yan, C.Yan, S.Yang, L.Yuan, W.-M.Zhang, H.Zhu, X.Zhu

The ratio of proton electromagnetic form factors via recoil polarimetry at Q2=1.13 (GeV/c)2

NUCLEAR REACTIONS 1H(polarized e, e'p), E=2329 MeV; measured recoil proton spectra, polarization. 1H deduced ratio of electromagnetic form factors.

doi: 10.1016/j.nuclphysa.2005.09.012
Citations: PlumX Metrics


2003MA36      Eur.Phys.J. A 17, 323 (2003)

R.Madey, A.Yu.Semenov, S.Taylor, A.Aghalaryan, E.Crouse, G.MacLachlan, B.Plaster, S.Tajima, W.Tireman, C.Yan, A.Ahmidouch, B.D.Anderson, H.Arenhovel, R.Asaturyan, O.Baker, A.R.Baldwin, H.Breuer, R.Carlini, E.Christy, S.Churchwell, L.Cole, S.Danagoulian, D.Day, M.Elaasar, R.Ent, M.Farkhondeh, H.Fenker, J.M.Finn, L.Gan, K.Garrow, P.Gueye, C.Howell, B.Hu, M.K.Jones, J.J.Kelly, C.Keppel, M.Khandaker, W.-Y.Kim, S.Kowalski, A.Lung, D.Mack, D.M.Manley, P.Markowitz, J.Mitchell, H.Mkrtchyan, A.Opper, C.Perdrisat, V.Punjabi, B.Raue, T.Reichelt, J.Reinhold, J.Roche, Y.Sato, I.A.Semenova, W.Seo, N.Simicevic, G.Smith, S.Stepanyan, V.Tadevosyan, L.Tang, P.Ulmer, W.Vulcan, J.W.Watson, S.Wells, F.Wesselmann, S.Wood, C.Yan, S.Yang, L.Yuan, W.-M.Zhang, H.Zhu, X.Zhu

Neutron electric form factor up to Q2 = 1.47 (GeV/c)2

NUCLEAR REACTIONS 2H(polarized e, e'n), E=0.844-3.395 GeV; measured neutron spectra, polarization. 1n deduced form factors.

doi: 10.1140/epja/i2002-10169-6
Citations: PlumX Metrics


2000AN10      Nucl.Phys. A663-664, 545c (2000)

B.D.Anderson, O.Osadchy, J.Sowinski, A.R.Baldwin, W.Franklin, J.W.Watson, S.Wissink, M.Wolanski, G.Yang, W.Glockle, H.Witala

Cross-Section and Analyzing-Power Measurements for the 2H(n, pn)n Reaction at 189 MeV

NUCLEAR REACTIONS 2H(polarized n, n), (polarized n, np), E=189 MeV; measured Ay(θ). Comparison with p-d reaction.

doi: 10.1016/S0375-9474(99)00652-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13953.


1999HT01      Phys.Rev. C59, 336 (1999)

M.M.Htun, R.Madey, W.M.Zhang, M.Elaasar, D.Keane, B.D.Anderson, A.R.Baldwin, J.Jiang, A.Scott, Y.Shao, J.W.Watson, K.Frankel, L.Heilbronn, G.Krebs, M.A.McMahan, W.Rathbun, J.Schambach, G.D.Westfall, S.Yennello, C.Gale, J.Zhang

Neutrons from Multiplicity-Selected La-La and Nb-Nb Collisions at 400A MeV and La-La Collisions at 250A MeV

NUCLEAR REACTIONS La(La, nX), E=250, 400 MeV/nucleon; Nb(Nb, nX), E=250 MeV/nucleon; measured neutron emission σ(θ, φ) vs rapidity; deduced maximum azimuthal anisotropy ratio vs θ, neutron flow features. Comparison with BUU calculations.

doi: 10.1103/PhysRevC.59.336
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1998AN09      Nucl.Phys. A631, 752c (1998)

B.D.Anderson, D.L.Prout, M.Palarczyk, A.Ahmidouch, A.R.Baldwin, D.Cooper, C.C.Foster, W.Glockle, M.S.Islam, C.Hautala, K.Hicks, M.Khayat, B.Luther, R.Madey, D.M.Manley, I.Niculescu, J.Rapaport, G.Savopulos, J.Sowinski, E.R.Sugarbaker, R.Suleiman, I.Van Heerden, J.W.Watson, H.Witala, X.Yang, W.M.Zhang

Measurement of a Complete Set of Spin Observables in the 2H(p, n)2p Reaction at 200 MeV

NUCLEAR REACTIONS 2H(polarized p, n), E=200 MeV; measured σ(θ), spin observables. Three-body Fadeev calculations.

doi: 10.1016/S0375-9474(98)00104-3
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1998HE33      Phys.Rev. C58, 3451 (1998)

L.Heilbronn, R.Madey, M.Elaasar, M.Htun, K.Frankel, W.G.Gong, B.D.Anderson, A.R.Baldwin, J.Jiang, D.Keane, M.A.McMahan, W.H.Rathbun, A.Scott, Y.Shao, J.W.Watson, G.D.Westfall, S.Yennello, W.-M.Zhang

Neutron Yields from 435 MeV/nucleon Nb Stopping in Nb and 272 MeV/nucleon Nb Stopping in Nb and Al

NUCLEAR REACTIONS 93Nb(93Nb, nX), E=272, 435 MeV/nucleon; 27Al(93Nb, nX), E=272 MeV/nucleon; measured neutron stopping-target yields, multiplicity, σ(En, θ). Comparison to model calculations.

doi: 10.1103/PhysRevC.58.3451
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0897.


1997MA68      Phys.Rev. C56, 3210 (1997)

R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, W.Bertozzi, T.Chittrakarn, J.R.Comfort, J.M.Finn, C.C.Foster, C.Hyde-Wright, J.J.Kelly, C.Lebo, H.Orihara, W.Pairsuwan, J.W.Watson

0+ to 0- Transition in the 16O(p, n)16F Reaction at 79 MeV

NUCLEAR REACTIONS 16O(p, n), E=79 MeV; measured σ(θ, En), σ(θ). Comparison with DWIA calculations.

doi: 10.1103/PhysRevC.56.3210
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0813.


1997PL01      Phys.Rev. C56, 263 (1997)

M.R.Plumley, J.W.Watson, B.D.Anderson, A.R.Baldwin, C.C.Foster, R.Madey, P.J.Pella, E.Ramstrom, W.Unkelbach, Y.Wang

Spin Observables for the 208Pb(p, n)208Bi Reaction at 135 MeV

NUCLEAR REACTIONS 208Pb(polarized p, n), E=135.7 MeV; measured reaction σ(E, θ), analyzing power vs E(neutron), spin observables; deduced spin-flip probability. 48Ca(polarized p, n), E not given; analyzed reaction σ, spin-flip probability. Neutron polarimeter, DWIA-RPA calculations.

doi: 10.1103/PhysRevC.56.263
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1997VO01      Phys.Rev. C55, 532 (1997)

P.von Neumann-Cosel, A.Richter, Y.Fujita, B.D.Anderson

Enhancement of the Isovector M1 Strength in 28Si Due to Meson Exchange Currents

NUCLEAR REACTIONS 28Si(p, n), E=135 MeV; 28Si(3He, t), E=450 MeV; analyzed σ(θ) vs E. 28P deduced levels, J, π, Gamow-Teller transition strength, meson exchange current contributions to M1 strength.

doi: 10.1103/PhysRevC.55.532
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1996AN08      Phys.Rev. C54, 237 (1996)

B.D.Anderson, L.A.C.Garcia, D.J.Millener, D.M.Manley, A.R.Baldwin, A.Fazely, R.Madey, N.Tamimi, J.W.Watson, C.C.Foster

12C(p, n)12N Reaction at 135 MeV

NUCLEAR REACTIONS 12C(p, n), E=135 MeV; measured σ(θ) vs excitation energy. 12N deduced levels, Γ, J, π. DWBA analysis.

NUCLEAR STRUCTURE 12N; calculated levels, one-body density matrices, Coulomb energy shifts. 12N levels deduced J, π. Shell model.

doi: 10.1103/PhysRevC.54.237
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0441.


1996AN09      Phys.Rev. C54, 602 (1996)

B.D.Anderson, A.R.Baldwin, P.Baumann, B.A.Brown, F.Didierjean, C.C.Foster, L.A.C.Garcia, A.Huck, A.Knipper, R.Madey, D.M.Manley, G.Marguier, M.Ramdane, H.Ravn, C.Richard-Serre, G.Walter, J.W.Watson

Gamow-Teller Strength to 38K from 38Ar(p, n) Reaction and 38Ca(β+) Decay

NUCLEAR REACTIONS 38Ar(p, n), E=135 MeV; measured σ(θ). 38K levels deduced Gamow-Teller transition strength. Shell-model comparison.

RADIOACTIVITY 38Ca(β+); measured β-delayed Eγ, Iγ. 38K levels deduced β-decay branching ratios, Gamow-Teller transition strength. Shell-model comparison.

doi: 10.1103/PhysRevC.54.602
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0440.


1996AN16      Phys.Rev. C54, 1531 (1996)

B.D.Anderson, A.R.Baldwin, W.Bertozzi, T.N.Buti, A.Fazely, J.M.Finn, C.C.Foster, W.Glockle, J.Golak, M.A.Kovash, R.Kurmanov, R.Madey, B.Murdoch, P.C.Tandy, J.W.Watson, H.Witala

Cross-Section Measurements for the 2H(p, n)2p Reaction at 135 MeV

NUCLEAR REACTIONS 2H(p, nX), E=135 MeV; measured σ(E(x), θ). Compared with impulse approximation, 3-body Faddeev calculations.

doi: 10.1103/PhysRevC.54.1531
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0442.


1996WA09      Nucl.Phys. A599, 211c (1996)

J.W.Watson, B.D.Anderson, A.R.Baldwin, R.Madey, M.Plumley, D.Prout, C.C.Foster, P.J.Pella, S.N.Ershov, F.A.Gareev, E.L.Trykov

Spin Observables for the Isovector Spin-Dipole Resonance Seen in 40Ca(p(pol), n(pol))

NUCLEAR REACTIONS 40Ca(polarized p, n), E=135 MeV; measured polarization transfer coefficient, σ(θ) vs energy transfer. 40Sc deduced isovector spin-dipole resonances, J, π. DWIA, finite Fermi systems theory.

doi: 10.1016/0375-9474(96)00063-2
Citations: PlumX Metrics


1995AN18      Phys.Rev. C52, 2210 (1995)

B.D.Anderson, B.Wetmore, A.R.Baldwin, L.A.C.Garcia, D.M.Manley, R.Madey, J.W.Watson, W.M.Zhang, B.A.Brown, C.C.Foster, Y.Wang

Excitation of the 2.65 MeV State in the 20Ne(p, n)20Na Reaction at 135 MeV

NUCLEAR REACTIONS 20Ne(p, n), E=135 MeV; measured σ(θ, En); deduced σ(θ). 20Na levels deduced spectroscopic strength, J, π. Comparison with analog states, DWIA calculations.

doi: 10.1103/PhysRevC.52.2210
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0426.


1995AN35      Nucl.Instrum.Methods Phys.Res. B99, 326 (1995)

B.D.Anderson

Nuclear Structure Studies with (p, n) Reactions at Intermediate Energies

NUCLEAR REACTIONS 48Ca(p, n), E=135 MeV; analyzed σ(θ). 48Sc levels deduced renormalization factors. DWIA, large basis shell model wave functions.

doi: 10.1016/0168-583X(94)00659-8
Citations: PlumX Metrics


1995ZH33      Phys.Rev. C52, 2643 (1995)

W.M.Zhang, R.Madey, J.Schambach, M.Elaasar, D.Keane, B.D.Anderson, A.R.Baldwin, J.W.Watson, G.D.Westfall, G.Krebs, H.Weimann, J.Zhang, C.Gale

Neutrons from Multiplicity-Selected Au-Au Collisions at 150A, 250A, 400A, and 650A MeV

NUCLEAR REACTIONS 197Au(197Au, xn), E=150-650 MeV/nucleon; measured neutron triple differential σ at multiplicity-selected relativistic collisions; deduced collective flow variables. BUU calculations, momentum dependent interaction.

doi: 10.1103/PhysRevC.52.2643
Citations: PlumX Metrics


1994ED01      Phys.Rev. C50, R1749 (1994)

T.Eden, R.Madey, W.-M.Zhang, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, M.Farkhondeh, J.M.Finn, B.S.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, D.M.Manley, P.Markowitz, J.Mougey, B.Ni, T.Payerle, P.J.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney

Electric Form Factor of the Neutron from the 2H(e(pol), e'n(pol))1H Reaction at Q2 = 0.255 (GeV/c)2

NUCLEAR REACTIONS 2H(polarized e, e'n), E=868 MeV; measured neutron polarization. 1n deduced electric form factor.

doi: 10.1103/PhysRevC.50.R1749
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1994ED02      Nucl.Instrum.Methods Phys.Res. A338, 432 (1994)

T.Eden, R.Madey, W.-M.Zhang, B.D.Anderson, A.R.Baldwin, J.M.Cameron, J.M.Finn, C.C.Foster, J.J.Kelly, S.Kowalski, R.Lourie, P.Markowitz, B.Ni, P.J.Pella, J.Schambach, M.Spraker, E.Steinfelds, E.J.Stephenson, J.W.Watson

Performance of a Neutron Polarimeter to Measure the Electric Form Factor of the Neutron

NUCLEAR REACTIONS 14C(polarized p, n), E=138.4 MeV; measured neutron spectra, analyzing power; deduced method suitability for 1n electric form factor extriction studies.

doi: 10.1016/0168-9002(94)91327-7
Citations: PlumX Metrics


1994EL01      Phys.Rev. C49, R10 (1994)

M.Elaasar, R.Madey, W.M.Zhang, J.Schambach, D.Keane, B.D.Anderson, A.R.Baldwin, J.W.Watson, G.D.Westfall, G.Krebs, H.Wieman, C.Gale, K.Haglin

Maximum Azimuthal Anisotropy of Neutrons from Nb-Nb Collisions at 400 A MeV and the Nuclear Equation of State

NUCLEAR REACTIONS 93Nb(93Nb, xn), E=400 MeV/nucleon; measured triple differential σ. Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1103/PhysRevC.49.R10
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1994GA18      Phys.Rev. C50, 289 (1994)

L.A.C.Garcia, B.D.Anderson, D.M.Manley, A.R.Baldwin, R.Pourang, E.Steinfelds, J.W.Watson, R.A.Lindgren, B.L.Clausen, A.D.Bacher, C.C.Foster

Identification of 4- States in the 14C(p, n)14N Reaction at 135 MeV

NUCLEAR REACTIONS 14C(p, n), E=135 MeV; measured neutron spectra, σ(E(n), θ=135°), σ(θ) vs momentum. 14N deduced levels, J, π, T, isovector transition strengths.

doi: 10.1103/PhysRevC.50.289
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0131.


1994WA24      Nucl.Phys. A577, 79c (1994)

J.W.Watson, B.D.Anderson, A.R.Baldwin, C.C.Foster, D.Lamm, R.Madey, M.R.Plumley, P.J.Pella

The Spin-Dipole Resonance in (p(pol), n(pol)) on 16O and 40Ca

NUCLEAR REACTIONS 16O, 40,48Ca, 208Pb(polarized p, n), E=135 MeV; measured spin observable D(NN')(θ); analyzed σ(θ) vs excitation, 0° neutron spectra data. 16F, 40,48Sc, 208Bi deduced spin dipole resonance features.

doi: 10.1016/0375-9474(94)90837-0
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1993MA21      Phys.Rev. C48, R5 (1993)

P.Markowitz, J.M.Finn, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, T.Eden, M.Farkhondeh, B.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, R.Madey, D.M.Manley, J.Mougey, B.Ni, T.Payerle, P.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney, W.M.Zhang

Measurement of the Magnetic Form Factor of the Neutron

NUCLEAR REACTIONS 2H(e, e'n), E not given; measured en-coin. 1n deduced magnetic form factor. Associated particle technique.

doi: 10.1103/PhysRevC.48.R5
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1993PO05      Phys.Rev. C47, 2751 (1993)

R.Pourang, J.W.Watson, R.Abegg, M.Ahmad, W.P.Alford, B.D.Anderson, A.R.Baldwin, A.Celler, D.Frekers, O.Hausser, R.Helmer, R.Henderson, K.Hicks, R.Jeppesen, K.P.Jackson, N.S.P.King, R.Madey, C.A.Miller, M.Moinester, M.C.Vetterli, S.Yen

High-Spin Stretched States Excited in (n, p) Reactions at 300 MeV

NUCLEAR REACTIONS 12C, 28Si, 120Sn(n, p), E=300 MeV; measured spectra, σ(θ). 12B, 28Al, 120In deduced stretched states normalizations. DWIA analysis.

doi: 10.1103/PhysRevC.47.2751
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13962.


1992AN09      Phys.Rev. C46, 504 (1992)

B.D.Anderson, A.R.Baldwin, L.A.C.Garcia, R.Madey, D.M.Manley, R.Pourang, E.Steinfelds, J.W.Watson, J.D.Brown, E.R.Jacobsen, R.Sherr, B.A.Brown, C.C.Foster

Excitation of 6- and 7+ Stretched States in the 38Ar(p, n)38K Reaction at 135 MeV

NUCLEAR REACTIONS 38Ar(p, n), E=135 MeV; measured σ(θ, En), σ(θ). 38K deduced levels, possible J, π, configuration. Model comparison.

doi: 10.1103/PhysRevC.46.504
Citations: PlumX Metrics


1992BA33      Phys.Rev. C46, 258 (1992)

A.R.Baldwin, R.Madey, W.-M.Zhang, B.D.Anderson, D.Keane, J.Varga, J.W.Watson, G.D.Westfall, K.Frankel, C.Gale

Inclusive Neutron Cross Sections from Ne-Pb Collisions at 790 MeV/Nucleon

NUCLEAR REACTIONS Pb(Ne, nX), E=790 MeV/nucleon; measured inclusive neutron spectra. Comparison with four different nucleus-nucleus collision models.

doi: 10.1103/PhysRevC.46.258
Citations: PlumX Metrics


1992TA04      Phys.Rev. C45, 1005 (1992)

N.Tamimi, B.D.Anderson, A.R.Baldwin, T.Chittrakarn, M.Elaasar, R.Madey, D.M.Manley, M.Mostajaboddavati, J.W.Watson, W.-M.Zhang, J.A.Carr, C.C.Foster

Isovector Stretched-State Excitations in the 20Ne, 24Mg, 28Si, and 32S(p, n) Reactions at 136 MeV

NUCLEAR REACTIONS 20Ne, 24Mg, 28Si, 32S(p, n), E=136 MeV; measured σ(θ), σ(En). 20Na, 24Al, 28P, 32Cl deduced stretched states, spectroscopic strengths. DWIA, large basis shell model calculations.

doi: 10.1103/PhysRevC.45.1005
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1992ZH09      Phys.Rev. C45, 2819 (1992)

W.-M.Zhang, B.D.Anderson, A.R.Baldwin, T.Eden, D.M.Manley, R.Madey, E.Steinfelds, J.W.Watson, P.J.Pella, C.C.Foster

P - A in the 48Ca(p, n)48Sc Reaction at 135 MeV

NUCLEAR REACTIONS 48Ca(polarized p, n), E=135 MeV; measured P(θ), analyzing power vs θ; deduced non-local effects. 48Sc levels deduced (P-A) differences, configurations role. DWIA analysis.

doi: 10.1103/PhysRevC.45.2819
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1991AN01      Phys.Rev. C43, 50 (1991)

B.D.Anderson, N.Tamimi, A.R.Baldwin, M.Elaasar, R.Madey, D.M.Manley, M.Mostajaboddavati, J.W.Watson, W.M.Zhang, C.C.Foster

Gamow-Teller Strength in the (p, n) Reaction at 136 MeV on 20Ne, 24Mg, and 28Si

NUCLEAR REACTIONS 20Ne, 24Mg, 28Si(p, n), E=36 MeV; measured σ(θn, En), σ(θ). 20Na, 24Al, 28P levels deduced Gamow-Teller transition strength distribution.

doi: 10.1103/PhysRevC.43.50
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0137.


1991AN04      Phys.Rev. C43, 1630 (1991)

B.D.Anderson, M.Mostajaboddavati, C.Lebo, R.J.McCarthy, L.Garcia, J.W.Watson, R.Madey

Isobaric-Analog-State Transitions in the (p, n) Reaction at 135 MeV and Density-Dependent Impulse-Approximation Calculations

NUCLEAR REACTIONS 14C, 42Ca, 88Sr, 124Sn(p, n), E=135 MeV; 144Sm(p, n), E=136 MeV; measured neutron spectra. 88Sr, 124Sn, 128Te, 144Sm, 208Pb, 14C, 26Mg, 42,48Ca, 54Fe(p, n), E=135 MeV; measured σ(θ). 48Ca(polarized p, n), E=135 MeV; measured analyzing power vs θ; deduced normalization factors, IAS σ. Density-dependent DWIA analysis.

doi: 10.1103/PhysRevC.43.1630
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1991PO05      Phys.Rev. C44, 689 (1991)

R.Pourang, J.W.Watson, M.Ahmad, W.P.Alford, B.D.Anderson, A.R.Baldwin, A.Celler, M.Elaasar, C.C.Foster, R.Helmer, O.Hausser, K.P.Jackson, C.A.Miller, R.Madey, M.Moinester, M.Mostajaboddavati, N.Tamimi, S.Yen

Energy Dependence of Stretched States Excited in (p, n) Reactions

NUCLEAR REACTIONS 28Si, 88Sr(p, n), E=100-400 MeV; measured σ(θn, En), σ(θ). 28P, 88Y deduced stretched states features. Distorted wave impulse approximation.

doi: 10.1103/PhysRevC.44.689
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1990AN05      Phys.Rev. C41, 1470 (1990)

B.D.Anderson, M.Mostajaboddavati, A.R.Baldwin, M.Elaasar, R.Madey, D.M.Manley, R.J.McCarthy, N.Tamimi, J.W.Watson, W.M.Zhang, C.C.Foster

Excitation of Two-Particle-One-Hole High-Spin States in the 45Sc(p, n)45Ti Reaction at 136 MeV

NUCLEAR REACTIONS 45Sc(p, n), E=136 MeV; measured σ(θ, E). 45Ti levels deduced spectroscopic strength.

doi: 10.1103/PhysRevC.41.1470
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1990AN06      Phys.Rev. C41, 1474 (1990)

B.D.Anderson, C.Lebo, A.R.Baldwin, T.Chittrakarn, R.Madey, J.W.Watson, C.C.Foster

Gamow-Teller Strength in the 54Fe(p, n)54Co Reaction at 135 MeV

NUCLEAR REACTIONS 54Fe(p, n), E=135 MeV; measured σ(θ, E). 54Co levels deduced Gamow-Teller transition strength. Sum rule, shell model predictions.

doi: 10.1103/PhysRevC.41.1474
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1989FL01      Phys.Rev. C40, 1985 (1989)

B.S.Flanders, R.Madey, B.D.Anderson, A.R.Baldwin, J.W.Watson, C.C.Foster, H.V.Klapdor, K.Grotz

Gamow-Teller Strength in the 208Pb(p, n)208Bi Reaction at 134.4 MeV

NUCLEAR REACTIONS 208Pb(p, n), E=134.3 MeV; measured σ(En). 208Bi deduced Gamow-Teller transition strength distribution.

doi: 10.1103/PhysRevC.40.1985
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1989MA35      Phys.Rev. C40, 540 (1989)

R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, J.W.Watson, S.M.Austin, C.C.Foster, H.V.Klapdor, K.Grotz

Low-Lying Structures in the Gamow-Teller Strength Functions for the Double-Beta-Decaying Nuclei 76Ge, 82Se, 128Te, and 130Te

NUCLEAR REACTIONS 76Ge, 82Se, 128,130Te(p, n), E=134.4 MeV; measured neutron spectra at θ ≤ 8°. 76As, 82Br, 128,130I deduced Gamow-Teller transition strengths. Shell model comparison.

doi: 10.1103/PhysRevC.40.540
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1989WA17      Phys.Rev. C40, 570 (1989)

J.W.Watson, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.S.Flanders, C.Lebo, R.Madey, J.D.Brown, C.C.Foster, D.L.Friesel, H.Nann, E.J.Stephenson, P.B.Foot, G.G.Shute, B.M.Spicer

48Ca(d, n)49Sc Reaction at 79 MeV

NUCLEAR REACTIONS 48Ca(polarized d, n), E=79 MeV; measured σ(En), σ(θ), vector analyzing power; deduced model parameters. 49Sc levels deduced C2S. DWBA, Johnson-Soper adiabatic approximation analyses.

doi: 10.1103/PhysRevC.40.570
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1988LE17      Phys.Rev. C38, 1099 (1988)

C.Lebo, B.D.Anderson, T.Chittrakarn, A.R.Baldwin, R.Madey, J.W.Watson, C.C.Foster

Particle-Hole Stretched States Excited in the 26Mg(p, n)26Al Reaction at 134 MeV

NUCLEAR REACTIONS 26Mg(p, n), E=134.4 MeV; measured σ(θ), σ(En). 26Al levels deduced transition strengths. DWIA calculations, large basis shell-model wave functions.

doi: 10.1103/PhysRevC.38.1099
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1988WA25      Nucl.Instrum.Methods Phys.Res. A272, 750 (1988)

J.W.Watson, M.R.Plumley, P.J.Pella, B.D.Anderson, A.R.Baldwin, R.Madey

A High-Performance Polarimeter for Medium-Energy Neutrons

NUCLEAR REACTIONS 14C(polarized p, n), E=100 MeV; measured polarized neutron spectra. High performance polarimeter.

doi: 10.1016/0168-9002(88)90756-5
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1987AN13      Phys.Rev. C36, 2195 (1987)

B.D.Anderson, T.Chittrakarn, A.R.Baldwin, C.Lebo, R.Madey, P.C.Tandy, J.W.Watson, C.C.Foster, B.A.Brown, B.H.Wildenthal

Gamow-Teller and M1 Strength in the 32S(p, n)32Cl Reaction at 135 MeV

NUCLEAR REACTIONS, MECPD 32S(p, n), E=135 MeV; measured σ(E, θ), σ(θ). 32Cl deduced Gamow-Teller transition strength, M1 transition strength, DWIA analysis.

doi: 10.1103/PhysRevC.36.2195
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1987FO22      Aust.J.Phys. 40, 611 (1987)

P.B.Foot, G.G.Shute, B.M.Spicer, C.C.Foster, J.D.Brown, D.L.Friesel, H.Nann, J.W.Seubert, E.J.Stephenson, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, W.Pairsuwan, J.W.Watson

D State Effects in the 11B(d(pol), n)12C Reaction at 79 MeV

NUCLEAR REACTIONS 11B(polarized d, n), E=79 MeV; measured σ(θ), vector analyzing power vs θ; deduced 2H D-state effects role. DWBA analysis.


1987MA19      Phys.Rev. C35, 2011 (1987); Erratum Phys.Rev. C36, 1647 (1987)

R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, C.Lebo, J.W.Watson, S.M.Austin, A.Galonsky, B.H.Wildenthal, C.C.Foster

Gamow-Teller Strength in the 26Mg(p, n)26Al Reaction at 135 MeV and Its Fractionation into T=0, 1, and 2 Isospin Channels

NUCLEAR REACTIONS, MECPD 26Mg(p, n), E=134.4 MeV; measured σ(En); deduced σ(θ). 26Al deduced levels, J, π, T, Gamow-Teller transition strength distribution. Tof. DWIA.

doi: 10.1103/PhysRevC.35.2011
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1987WA31      Can.J.Phys. 65, 566 (1987)

J.W.Watson, B.D.Anderson, R.Madey

Studies of the (p, n) Reaction at Medium Energies

NUCLEAR REACTIONS, MECPD 40,48Ca(polarized p, n), E=134 MeV; measured σ(En, θn), analyzing power, polarization transfer coefficients.

doi: 10.1139/p87-080
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1986AN23      Phys.Rev. C34, 422 (1986)

B.D.Anderson, T.Chittrakarn, A.R.Baldwin, A.Fazely, C.Lebo, R.Madey, J.W.Watson, C.C.Foster

Analyzing-Power Measurements in the 48Ca(p, n)48Sc Reaction at 134 MeV

NUCLEAR REACTIONS 48Ca(polarized p, n), E=134 MeV; measured σ(θ), A(θ). 48Sc deduced state population sensitivity to configurations. DWIA calculations.

doi: 10.1103/PhysRevC.34.422
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1986CH19      Phys.Rev. C34, 80 (1986)

T.Chittrakarn, B.D.Anderson, A.R.Baldwin, C.Lebo, R.Madey, J.W.Watson, C.C.Foster

Particle-Hole Strength Excited in the 40Ca(p, n)40Sc Reaction at 134 MeV

NUCLEAR REACTIONS 40Ca(p, n), (polarized p, n), E=134 MeV; measured σ(θ), A(θ). 40Sc deduced levels, J, π. DWIA calculations.

doi: 10.1103/PhysRevC.34.80
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1986MA51      Phys.Rev. C34, 1342 (1986)

R.Madey, J.Varga, G.Fai, A.F.Barghouty, B.D.Anderson, A.R.Baldwin, R.Cecil, J.W.Watson, G.D.Westfall

Angular Distributions of Low-Energy Neutrons from 390-MeV/Nucleon Ne + Pb Collisions

NUCLEAR REACTIONS Pb(Ne, nX), E=390 MeV/nucleon; measured σ(θn). TOF, plastic scintillators. Three source model calculations.

doi: 10.1103/PhysRevC.34.1342
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1986WA28      Phys.Lett. 181B, 47 (1986)

J.W.Watson, P.J.Pella, B.D.Anderson, A.R.Baldwin, T.Chittrakarn, B.S.Flanders, R.Madey, C.C.Foster, I.J.van Heerden

Gamow-Teller and Spin-Dipole Strength in the 40,48Ca(p(pol), n(pol)) Reactions at 135 MeV

NUCLEAR REACTIONS, MECPD 40,48Ca(polarized p, n), E=135 MeV; measured σ(En, θ), spin flip probabilities, neutron polarization vs θ, polarization transfer coefficient. 48Ca deduced 1+ strength in continuum near giant Gamow-Teller resonance. 40Ca deduced dipole resonance spin-flip, nonspin-flip component relative width.

doi: 10.1016/0370-2693(86)91252-9
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1985AN06      Phys.Rev. C31, 1147 (1985)

B.D.Anderson, T.Chittrakarn, A.R.Baldwin, C.Lebo, R.Madey, R.J.McCarthy, J.W.Watson, B.A.Brown, C.C.Foster

Particle-Hole Strength Excited in the 48Ca(p, n)48Sc Reaction at 134 and 160 MeV: (πf7/2, νf7/2-1) Band

NUCLEAR REACTIONS 48Ca(p, n), E=134, 160 MeV; measured σ(E, θ), σ(θ). 48Sc deduced Gamow-Teller to Fermi transition strength, stretched transition excitation. DWIA analysis.

doi: 10.1103/PhysRevC.31.1147
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1985AN29      Phys.Rev. C 31, 1161 (1985)

B.D.Anderson, T.Chittrakarn, A.R.Baldwin, C.Lebo, R.Madey, P.C.Tandy, J.W.Watson, B.A.Brown, C.C.Foster

Particle-hole strength excited in the 48Ca(p, n)48Sc reaction at 134 and 160 MeV: Gamow-Teller strength

NUCLEAR REACTIONS 48Ca(p, n), E=134, 160 MeV; measured reaction products, En, In; deduced σ(θ, E), Gamow-Teller strength.

doi: 10.1103/PhysRevC.31.1161
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1985FA06      Nucl.Phys. A443, 29 (1985)

A.Fazely, R.Madey, B.D.Anderson, A.R.Baldwin, C.Lebo, P.C.Tandy, J.W.Watson, W.Bertozzi, T.Buti, M.Finn, C.Hyde-Wright, J.Kelly, M.A.Kovash, B.Murdock, B.Pugh, C.C.Foster

Cross Section and Analyzing Power for the Isovector ' Stretched ' 6- State in the 28Si(p, n)28P Reaction

NUCLEAR REACTIONS 28Si(p, n), E=135.2 MeV; 28Si(polarized p, n), E=133.5 MeV; measured σ(θ), A(θ). 28P deduced 6-, T=1 state population vs momentum transfer. DWIA calculations, analog 28Si(polarized p, p') reaction data input.

doi: 10.1016/0375-9474(85)90319-7
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1985FO05      Phys.Rev. C31, 1133 (1985)

P.B.Foot, G.G.Shute, B.M.Spicer, C.C.Foster, H.Nann, E.J.Stephenson, B.D.Anderson, A.R.Baldwin, B.S.Flanders, C.Lebo, R.Madey, J.W.Watson

11B(d, n)12C Reaction and the Adiabatic Approximation

NUCLEAR REACTIONS 11B(d, n), E=79 MeV; measured σ(θ); deduced deuteron optical model parameters. 12C levels deduced L, S. Adiabatic model, DWBA analysis.

doi: 10.1103/PhysRevC.31.1133
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1985MA44      Phys.Rev.Lett. 55, 1453 (1985)

R.Madey, J.Varga, A.R.Baldwin, B.D.Anderson, R.A.Cecil, G.Fai, P.C.Tandy, J.W.Watson

Inclusive Neutron Spectra at 0° from the Reactions Pb(Ne, n)X and NaF(Ne, n)X at 390 and 790 MeV per Nucleon

NUCLEAR REACTIONS Pb, Na, F(Ne, nX), E=390, 790 MeV/nucleon; measured inclusive σ(En, θ=0°); deduced projectile evaporation. Natural Pb, NaF targets.

doi: 10.1103/PhysRevLett.55.1453
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1985WA24      Phys.Rev.Lett. 55, 1369 (1985)

J.W.Watson, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, R.J.McCarthy, B.A.Brown, B.H.Wildenthal, C.C.Foster

Relationship between Gamow-Teller Transition Proabilities and (p, n) Cross Sections at Small Momentum Transfers

NUCLEAR REACTIONS 14C, 15N, 17,18O, 26Mg, 39K(p, n), E=135 MeV; measured σ(θ), σ(θn, En). 13C, 19F(p, n), E=160 MeV; analyzed σ(θ). 14N, 15O, 17,18F, 26Al, 39Ca levels deduced Gamow-Teller transitions. DWBA analysis, β-decay input.

doi: 10.1103/PhysRevLett.55.1369
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1984AN08      Phys.Rev.Lett. 52, 1872 (1984)

B.D.Anderson, C.Lebo, A.R.Baldwin, T.Chittrakarn, R.Madey, J.W.Watson, C.C.Foster

Concentrated Particle-Hole Strength Observed in 0(h-bar x Omega) Stretched-State Excitations

NUCLEAR REACTIONS 48Ca, 54Fe, 88Sr, 208Pb(p, n), E=134 MeV; measured σ(θ, En). 48Sc, 54Co, 88Y, 208Bi deduced stretched state excitation, particle-hole strength contribution. DWIA analysis.

doi: 10.1103/PhysRevLett.52.1872
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1984DA22      Phys.Rev. C30, 1999 (1984)

J.D'Auria, M.Dombsky, L.Moritz, T.Ruth, G.Sheffer, T.E.Ward, C.C.Foster, J.W.Watson, B.D.Anderson, J.Rapaport

Activation Measurements of the 7Li(p, n)7Be Reaction from 60-480 MeV

NUCLEAR REACTIONS, ICPND 7Li(p, n), E=60-480 MeV; measured reaction σ. Activation analysis. Comparison with theoretical analysis.

doi: 10.1103/PhysRevC.30.1999
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1983AN05      Phys.Rev. C27, 1387 (1983)

B.D.Anderson, A.Fazely, R.J.McCarthy, P.C.Tandy, J.W.Watson, R.Madey, W.Bertozzi, T.N.Buti, J.M.Finn, J.Kelly, M.A.Kovash, B.Pugh, B.H.Wildenthal, C.C.Foster

Gamow-Teller Strength in the 18O(p, n)18F Reaction at 135 MeV

NUCLEAR REACTIONS 18O(p, n), E=135.2 MeV; measured σ(En), σ(θ). 18F deduced levels, J, π, T, Gamow-Teller transition strength. DWIA analysis.

doi: 10.1103/PhysRevC.27.1387
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1983AN06      Phys.Lett. 123B, 383 (1983)

B.D.Anderson, J.W.Watson, C.Lebo, A.R.Baldwin, A.Fazely, R.Madey, C.C.Foster

Excitation of the 6- Particle-Hole State with the 40Ca(p, n)40Sc Reaction at 133.5 MeV

NUCLEAR REACTIONS 40Ca(p, n), E=133.5 MeV; measured σ(θ), σ(θ, En). 40Sc deduced level J, π, T, configuration. Tof. DWIA analysis.

doi: 10.1016/0370-2693(83)90977-2
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1983GR16      Phys.Lett. 126B, 417 (1983)

K.Grotz, H.V.Klapdor, J.Metzinger, R.Madey, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.Flanders, C.Lebo, J.W.Watson, C.C.Foster

The Gamow-Teller Strength Distribution in 208Bi - A Probe of the Charge Distribution in 208Pb ( Question )

NUCLEAR STRUCTURE 208Bi; calculated Gamow-Teller transition strength distribution. Two-quasiparticle formalism, comparison with (p, n) data.

NUCLEAR REACTIONS 208Pb(p, n), E=134.4 MeV; measured σ(θ). 208Pb deduced ground state correlation effects, single particle orbit occupation probabilities. Comparison with Gamow-Teller strength calculations.

doi: 10.1016/0370-2693(83)90353-2
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1983KA13      Phys.Rev. C28, 105 (1983)

A.M.Kalenda, B.D.Anderson, A.R.Baldwin, R.Madey, J.W.Watson, C.C.Chang, H.D.Holmgren, R.W.Koontz, J.R.Wu, H.Machner

Energy and Angular Distributions of Neutrons from 90 MeV Proton and 140 MeV Alpha-Particle Bombardment of Nuclei

NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, n), E=90 MeV; 27Al, 58Ni, 90Zr, 209Bi(α, n), E=140 MeV; measured σ(θ, En); deduced reaction mechanisms. Plane wave impulse approximation, quasifree scattering, preequilibrium exciton, intranuclear cascade, geometry dependent hybrid models, (p, p') data comparison.

doi: 10.1103/PhysRevC.28.105
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1983MA33      Phys.Rev. C28, 706 (1983)

R.Madey, B.D.Anderson, R.A.Cecil, P.C.Tandy, W.Schimmerling

Total Inclusive Neutron Cross Sections and Multiplicities in Nucleus-Nucleus Collisions at Intermediate Energies

NUCLEAR REACTIONS C, Al, Cu, U(Ne, nX), E=337 MeV/nucleon; analyzed inclusive σ, mean neutron multiplicity. Participant spectator model, one parameter formulae.

doi: 10.1103/PhysRevC.28.706
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1983WA29      Nucl.Instrum.Methods 215, 413 (1983)

J.W.Watson, B.D.Anderson, A.R.Baldwin, C.Lebo, B.Flanders, W.Pairsuwan, R.Madey, C.C.Foster

A Comparison of Methods for Determining Neutron Detector Efficiencies at Medium Energies

NUCLEAR REACTIONS 7Li, 12C(p, n), E=135, 160 MeV; measured σ(θ). Lithium activation method, comparison to other techniques, neutron detector efficiency determination.

doi: 10.1016/0167-5087(83)90472-6
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1982AN08      Phys.Rev. C26, 8 (1982)

B.D.Anderson, R.J.McCarthy, M.Ahmad, A.Fazely, A.M.Kalenda, J.N.Knudson, J.W.Watson, R.Madey, C.C.Foster

Comparison of 0°(p, n) Cross Sections and B(M1) Values for Separating Current and Spin Contributions to Isovector M1 Transitions

NUCLEAR REACTIONS 12C, 16O, 24,26Mg, 28Si, 48Ca(p, n), E=62-160 MeV; analyzed σ(θ=0°) vs E. 12N, 24,26Al, 16F, 28P, 48Sc level deduced σ/B(M1) spin, current contribution dependence. Inelastic electron scattering data input.

doi: 10.1103/PhysRevC.26.8
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1982FA06      Phys.Rev. C25, 1760 (1982); Erratum Phys.Rev. C26, 746 (1982)

A.Fazely, B.D.Anderson, M.Ahmad, A.R.Baldwin, A.M.Kalenda, R.J.McCarthy, J.W.Watson, R.Madey, W.Bertozzi, T.N.Buti, J.M.Finn, M.A.Kovash, B.Pugh, C.C.Foster

Spectroscopy of 16F from the 16O(p, n)16F Reaction at 99 and 135 MeV

NUCLEAR REACTIONS 16O(p, n), E=99.1, 135.2 MeV; measured σ(En) vs θ; deduced σ(θ). 16F levels deduced J, π, analog character. Tof. Shell model.

doi: 10.1103/PhysRevC.25.1760
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1982MA11      Phys.Rev. C25, 1715 (1982)

R.Madey, A.Fazely, B.D.Anderson, A.R.Baldwin, A.M.Kalenda, R.J.McCarthy, P.C.Tandy, J.W.Watson, W.Bertozzi, T.Buti, M.Finn, M.Kovash, B.Pugh, C.C.Foster

Analyzing Power for the 16O(p(pol), n)16F(4-, 6.37 MeV) Reaction at 134 MeV

NUCLEAR REACTIONS 16O(polarized p, n), E=134 MeV; measured σ(θ), σ(En), A(θ). 16F level deduced configuration. DWIA, effective nucleon-nucleon interaction.

doi: 10.1103/PhysRevC.25.1715
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1982MA22      Phys.Rev. C25, 3050 (1982)

R.Madey, T.Vilaithong, B.D.Anderson, J.N.Knudson, T.R.Witten, A.R.Baldwin, F.M.Waterman

Neutrons from Nuclear Capture of Negative Pions

NUCLEAR REACTIONS C, N, O, Al, Cu, Ta, Pb(π-, xn), E ≈ 0; measured σ(En), yields; deduced nuclear temperature. Tof. Intranuclear cascade, preequilibrium models.

doi: 10.1103/PhysRevC.25.3050
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1981AN01      Phys.Rev.Lett. 46, 226 (1981)

B.D.Anderson, A.R.Baldwin, A.M.Kalenda, R.Madey, J.W.Watson, C.C.Chang, H.D.Holmgren, R.W.Koontz, J.R.Wu

Proton and Neutron Inclusive Spectra and the Importance of the Single Nucleon-Nucleon Scattering Process

NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, pX), (p, nX), E=90 MeV; measured σ(En, θ), σ(Ep, θ); deduced nucleon-nucleon scattering mechanism dominance. PWIA, quasifree scattering calculation.

doi: 10.1103/PhysRevLett.46.226
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1981CE07      Phys.Rev. C 24, 2013 (1981)

R.A.Cecil, B.D.Anderson, A.R.Baldwin, R.Madey, W.Schimmerling, J.W.Kast, D.Ortendahl

Inclusive neutron production by 337 MeV/nucleon neon ions on carbon, aluminum, copper, and uranium

NUCLEAR REACTIONS C, Al, Cu, U(Ne, X)00-NN-1, E=337 MeV/nucleon; measured reaction products, En, In; deduced σ(θ, E). Comparison with available data.

doi: 10.1103/PhysRevC.24.2013
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1981WA08      Phys.Rev. C23, 2373 (1981)

J.W.Watson, M.Ahmad, B.D.Anderson, A.R.Baldwin, A.Fazely, P.C.Tandy, R.Madey, C.C.Foster

'Stretched' States Excited in the 48Ca(p, n)48Sc Reaction at 160 MeV

NUCLEAR REACTIONS 48Ca(p, n), E=160 MeV; measured σ(θ, En). 48Sc level deduced stretched configuration. DWIA analysis. Tof.

doi: 10.1103/PhysRevC.23.2373
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1980AN05      Nucl.Instrum.Methods 169, 153 (1980)

B.D.Anderson, J.N.Knudson, R.Madey, C.C.Foster

A Comparison of 12C(p, n)12N and 12C(p, p')12C* Cross-Section Measurements to Analog States as a Test of Monte-Carlo Calculated Efficiencies for Large-Volume Neutron Counters

NUCLEAR REACTIONS 12C(p, n), E=61.9, 119.8 MeV; measured σ. 12C level deduced isospin mixing. Tof, large-volume detector.

doi: 10.1016/0029-554X(80)90115-9
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1980AN19      Phys.Rev.Lett. 45, 699 (1980)

B.D.Anderson, J.N.Knudson, P.C.Tandy, J.W.Watson, R.Madey, C.C.Foster

Observation of a T(>) Gamow-Teller State in 48Ca(p, n)48Sc at 160 MeV

NUCLEAR REACTIONS 48Ca(p, n), E=160 MeV; measured σ(En, θ). 48Sc deduced level, isospin, Gamow-Teller transition strength, giant M1 analog. Shell model, tof.

doi: 10.1103/PhysRevLett.45.699
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1612.


1980CE01      Phys.Rev. C21, 2471 (1980)

R.A.Cecil, B.D.Anderson, A.R.Baldwin, R.Madey, A.Galonsky, P.Miller, L.Young, F.M.Waterman

Neutron Angular and Energy Distributions from 710-MeV Alphas Stopping In Water, Carbon, Steel, and Lead, and 640-MeV Alphas Stopping in Lead

NUCLEAR REACTIONS 2H, O, C, Fe(α, xn), E=710 MeV; Pb(α, xn), E=640, 710 MeV; measured σ(θn, En), stopped α; deduced total integrated neutron yield. Intranuclear cascade model.

doi: 10.1103/PhysRevC.21.2471
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0268.


1980KN02      Phys.Rev. C22, 1826 (1980)

J.N.Knudson, B.D.Anderson, P.C.Tandy, J.W.Watson, R.Madey, C.C.Foster

12C(p, n)12N Reaction at 99 MeV

NUCLEAR REACTIONS 12C(p, n), E=99.1 MeV; measured σ(En, θ). DWIA calculations, effective nucleon-nucleon interaction.

doi: 10.1103/PhysRevC.22.1826
Citations: PlumX Metrics


1979AN03      Phys.Rev. C19, 905 (1979)

B.D.Anderson, P.R.Bevington, F.H.Cverna, M.W.McNaughton, H.B.Willard, R.J.Barrett, N.S.P.King, D.J.Ernst

Proton Total Reaction Cross Section Measurements for 40,44,48Ca at 700 MeV

NUCLEAR REACTIONS 40,44,48Ca(p, X), E=700 MeV; measured total reaction σ; deduced matter radii differences.

doi: 10.1103/PhysRevC.19.905
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1863.


1979AN15      Phys.Rev. C20, 897 (1979)

B.D.Anderson, N.Jarmie, R.J.Barrett, E.D.Arthur

The 16O(d, p)17O Reaction to the Unbound 5.09-MeV State of 17O

NUCLEAR REACTIONS 16O(d, d), (d, p), E=12 MeV; measured σ(θ). 17O level deduced Γn. DWBA calculations for unbound states.

doi: 10.1103/PhysRevC.20.897
Citations: PlumX Metrics


1979SC21      Phys.Rev.Lett. 43, 1985 (1979)

W.Schimmerling, J.W.Kast, D.Ortendahl, R.Madey, R.A.Cecil, B.D.Anderson, A.R.Baldwin

Measurement of the Inclusive Neutron Production by Relativistic Neon Ions on Uranium

NUCLEAR REACTIONS U(20Ne, n), E=337 MeV/nucleon; measured σ. Firestreak model calculation.

doi: 10.1103/PhysRevLett.43.1985
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0290.


1976IN01      Phys.Rev. C13, 524 (1976)

P.D.Ingalls, J.S.Schweitzer, B.D.Anderson, M.Rios

14N(p, α)11C Cross Sections from 3.8 to 6.4 MeV

NUCLEAR REACTIONS 14N(p, α), E=3.8-6.4 MeV; measured σ(E). Inferred σ(E), astrophysical σ factor for inverse reaction. Sealed gas target.

doi: 10.1103/PhysRevC.13.524
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0178.


1976WI13      Phys.Rev. C14, 1545 (1976)

H.B.Willard, B.D.Anderson, H.W.Baer, R.J.Barrett, P.R.Bevington, A.N.Anderson, H.Willmes, N.Jarmie

Absolute Differential Cross Section Measurements for Proton-Proton Elastic Scattering at 647 and 800 MeV

NUCLEAR REACTIONS 1H(p, p), E=647, 800 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.14.1545
Citations: PlumX Metrics


1974AN19      Nucl.Phys. A233, 286 (1974)

B.D.Anderson, M.R.Dwarakanath, J.S.Schweitzer, A.V.Nero

A New Determination of the Partial Widths of the 16.11 MeV State in 12C

NUCLEAR REACTIONS 11B(d, n), E=6 MeV; measured σ(En, θ); 11B(p, γ), (p, α), E=163 keV; measured σ; 10B(3He, pγ), E=2.2 MeV; measured pγ-coin. 12C levels deduced p-width, γ-width, S.

doi: 10.1016/0375-9474(74)90456-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0359.


1974RI16      Nucl.Phys. A236, 523 (1974)

M.Rios, B.D.Anderson, J.S.Schweitzer

The 46Ti(p, γ)47V, 50Cr(p, γ)51Mn, 58Ni(α, γ)62Zn and 58Ni(α, p)61Cu Cross Sections

NUCLEAR REACTIONS 46Ti, 50Cr(p, γ), 58Ni(α, γ), (α, p); measured σ(E). Natural, enriched targets.

doi: 10.1016/0375-9474(74)90271-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1111.


1972AN21      Phys.Rev. C6, 1513 (1972)

B.D.Anderson, D.E.Velkley, H.B.Willard

16O(d, n) Polarizations and Cross Sections from 3 to 4 MeV

NUCLEAR REACTIONS 16O(d, n), E=3-4 MeV; measured σ(E;θ), P(E;θ). 17F levels deduced S.

doi: 10.1103/PhysRevC.6.1513
Citations: PlumX Metrics


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