NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = B.D.Anderson Found 80 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1995AN35 Nucl.Instrum.Methods Phys.Res. B99, 326 (1995) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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