NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = W.Benenson Found 130 matches. Showing 1 to 100. [Next]2004CL02 Phys.Rev.Lett. 92, 172502 (2004) R.R.C.Clement, D.Bazin, W.Benenson, B.A.Brown, A.L.Cole, M.W.Cooper, P.A.DeYoung, A.Estrade, M.A.Famiano, N.H.Frank, A.Gade, T.Glasmacher, P.T.Hosmer, W.G.Lynch, F.Montes, W.F.Mueller, G.F.Peaslee, P.Santi, H.Schatz, B.M.Sherrill, M.-J.van Goethem, M.S.Wallace New Approach for Measuring Properties of rp-Process Nuclei NUCLEAR REACTIONS H, C(34Ar, 33ArX), E=84 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following neutron removal. 33Ar deduced levels, J, π, spectroscopic factors. 32Cl(p, γ), E=low; calculated astrophysical reaction rates.
doi: 10.1103/PhysRevLett.92.172502
2003CL07 Nucl.Phys. A718, 617c (2003) R.R.C.Clement, W.Benenson, B.A.Brown, W.A.Richter, H.Schatz, B.M.Sherrill, A.Volya Sensitivities of rp-process calculations to nuclear mass uncertainties
doi: 10.1016/S0375-9474(03)00903-5
2001CA37 Phys.Rev. C64, 025802 (2001) J.A.Caggiano, D.Bazin, W.Benenson, B.Davids, R.Ibbotson, H.Scheit, B.M.Sherrill, M.Steiner, J.Yurkon, A.F.Zeller, B.Blank, M.Chartier, J.Greene, J.A.Nolen, Jr., A.H.Wuosmaa, M.Bhattacharya, A.Garcia, M.Wiescher Spectroscopy of 23Al and 27P using the (7Li, 8He) Reaction and the Implications for 22Na and 26Al Nucleosynthesis in Explosive Hydrogen Burning NUCLEAR REACTIONS 9Be, 10B, 24Mg, 28Si(7Li, 8He), E=50.1 MeV/nucleon; measured particle spectra. 23Al, 27P deduced level energies. 22Mg, 26Si(p, γ), E=low; deduced stellar reaction rates. ATOMIC MASSES 23Al, 27P; measured ground-state mass excess.
doi: 10.1103/PhysRevC.64.025802
1999CA48 Phys.Rev. C60, 064322 (1999) J.A.Caggiano, D.Bazin, W.Benenson, B.Davids, B.M.Sherrill, M.Steiner, J.Yurkon, A.F.Zeller, B.Blank Spectroscopy of the 10Li Nucleus NUCLEAR REACTIONS 9Be, 12C(9Be, 8B), (9Be, 11C), E=40.1 MeV/nucleon; measured particle spectra, σ(θ). 10Li deduced low-lying resonance energy, width. S800 spectrograph.
doi: 10.1103/PhysRevC.60.064322
1998BA28 Phys.Rev. C57, 2156 (1998) D.Bazin, W.Benenson, B.A.Brown, J.Brown, B.Davids, M.Fauerbach, P.G.Hansen, P.Mantica, D.J.Morrissey, C.F.Powell, B.M.Sherrill, M.Steiner Probing the Halo Structure of 19,17,15C and 14B NUCLEAR REACTIONS Ta, Be(15C, n14C), (17C, n16C), (19C, n18C), (14B, n13B), E ≈ 85 MeV/nucleon; measured core fragments parallel momenta; deduced breakup σ, role of core excitations. 15,17,19C, 14B deduced neutron halo features. Secondary beams from 18O, 40Ar fragmentation.
doi: 10.1103/PhysRevC.57.2156
1997PA12 Phys.Rev.Lett. 78, 1022 (1997) R.Pak, W.Benenson, O.Bjarki, J.A.Brown, S.A.Hannuschke, R.A.Lacey, B.-A.Li, A.Nadasen, E.Norbeck, P.Pogodin, D.E.Russ, M.Steiner, N.T.B.Stone, A.M.Vander Molen, G.D.Westfall, L.B.Yang, S.J.Yennello Isospin Dependence of Collective Transverse Flow in Nuclear Collisions NUCLEAR REACTIONS 58Fe(58Mn, X), E=56.6 MeV/nucleon; 58Ni, 58Fe(58Ni, X), (58Fe, X), E=55 MeV/nucleon; measured collective transverse flow; deduced flow variables, nucleon-nucleon collisions elementary aspects models dependence. Transport models.
doi: 10.1103/PhysRevLett.78.1022
1997PA13 Phys.Rev.Lett. 78, 1026 (1997) R.Pak, B.-A.Li, W.Benenson, O.Bjarki, J.A.Brown, S.A.Hannuschke, R.A.Lacey, D.J.Magestro, A.Nadasen, E.Norbeck, D.E.Russ, M.Steiner, N.T.B.Stone, A.M.Vander Molen, G.D.Westfall, L.B.Yang, S.J.Yennello Isospin Dependence of the Balance Energy NUCLEAR REACTIONS 58Fe(58Fe, X), 58Ni(58Ni, X), E ≤ 105 MeV/nucleon; measured transverse flow vs E; deduced balance energy isospin dependence related features. Transport model.
doi: 10.1103/PhysRevLett.78.1026
1996BR30 Phys.Rev. C54, R2105 (1996) J.A.Brown, D.Bazin, W.Benenson, J.Caggiano, M.Fauerbach, M.Hellstrom, J.H.Kelley, R.A.Kryger, R.Pfaff, B.M.Sherrill, M.Steiner, D.J.Morrissey, C.F.Powell Measurement of the 1H(6He, 6Li)n Reaction in Inverse Kinematics NUCLEAR REACTIONS 1H(6He, 6Li), 6He(p, n), E=93 MeV/nucleon; measured σ(θ); deduced B(GT) and ratio of transitions to the ground state and isobaric analog state in 6Li. 6Li levels deduced transition ratios.
doi: 10.1103/PhysRevC.54.R2105
1996FA01 Phys.Rev. C53, 647 (1996) M.Fauerbach, D.J.Morrissey, W.Benenson, B.A.Brown, M.Hellstrom, J.H.Kelley, R.A.Kryger, R.Pfaff, C.F.Powell, B.M.Sherrill New Search for 26O NUCLEAR REACTIONS, ICPND 9Be(40Ar, X)17O/18O/19O/20O/21O/22O/23O/24O, E=90 MeV/nucleon; measured residuals relative production σ for O and P, Si, Al, Mg, Na, Ne, F, N.C.B isotopes; deduced 26O particle unstable characteristics.
doi: 10.1103/PhysRevC.53.647
1996PF01 Phys.Rev. C53, 1753 (1996) R.Pfaff, D.J.Morrissey, W.Benenson, M.Fauerbach, M.Hellstrom, C.F.Powell, B.M.Sherrill, M.Steiner, J.A.Winger Fragmentation of 78Kr Projectiles NUCLEAR REACTIONS, ICPND 58Ni(78Kr, X), E=75 MeV/nucleon; measured fragment mass distribution for Zn, Sr, Ga, Ge, As, Se, Br, Kr, Rb isotopes, production σ vs mass. 69Br deduced particle instability. Other data, intranuclear cascade model comparisons, projectile fragmentation.
doi: 10.1103/PhysRevC.53.1753
1996ST05 Phys.Rev.Lett. 76, 26 (1996) M.Steiner, S.M.Austin, D.Bazin, W.Benenson, C.A.Bertulani, J.A.Brown, M.Fauerbach, M.Hellstrom, E.Kashy, J.H.Kelley, R.A.Kryger, T.Kubo, N.A.Orr, R.Pfaff, B.M.Sherrill, M.Thoennessen, S.J.Yennello, B.M.Young, P.D.Zecher, D.J.Morrissey, C.F.Powell First Study of Heavy-Ion Mirror Charge Exchange NUCLEAR REACTIONS 13C(13N, 13C), E=57, 105 MeV/nucleon; measured σ(θ), spectra; deduced Gamow-Teller to Fermi-transition unit σ(ratio).
doi: 10.1103/PhysRevLett.76.26
1995BE30 Nucl.Phys. A588, 11c (1995) Structure of 10Li and 11Li NUCLEAR STRUCTURE 10,11Li; compiled, reviewed data; deduced mass related features. 10Li deduced possible levels Γ, neutron separation energy features. Data on 14C(11B, 10Be), (11B, 11Li), 11B(7Li, 8B) considered.
doi: 10.1016/0375-9474(95)00092-F
1994YE01 Phys.Lett. 321B, 15 (1994) S.J.Yennello, B.Young, J.Lee, J.A.Winger, J.S.Winfield, G.D.Westfall, A.Vander Molen, B.M.Sherrill, J.Shea, E.Norbeck, D.J.Morrissey, T.Li, E.Gualtieri, D.Craig, W.Benenson, D.Bazin The use of Radioactive Nuclear Beams to Study the Equilibration of the N/Z Degree of Freedom in Intermediate-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 58Ni, 58Fe(40Ca, X), (40Ar, X), E=53 MeV/nucleon; 9Be(40Ar, X), E=80 MeV/nucleon; measured fragment spectra, isotope production ratio for fragment Z ≤ 5; deduced target, beam N/Z dependence.
doi: 10.1016/0370-2693(94)90321-2
1994YO01 Phys.Rev. C49, 279 (1994) B.M.Young, W.Benenson, J.H.Kelley, N.A.Orr, R.Pfaff, B.M.Sherrill, M.Steiner, M.Thoennessen, J.S.Winfield, J.A.Winger, S.J.Yennello, A.Zeller Low-Lying Structure of 10Li in the Reaction 11B(7Li, 8B)10Li NUCLEAR REACTIONS 11B(7Li, 8B), E=130 MeV; measured momentum spectra; deduced Q. 10Li deduced neutron separation energy, levels, Γ, possible, J.
doi: 10.1103/PhysRevC.49.279
1993CH10 Phys.Rev. C47, 1462 (1993) Y.Chen, E.Kashy, D.Bazin, W.Benenson, D.J.Morrissey, N.A.Orr, B.M.Sherrill, J.A.Winger, B.Young, J.Yurkon Half-Life of 32Si RADIOACTIVITY 32Si(β-) [from 9Be(40Ar, X), E=65 MeV/nucleon]; measured specific activity; deduced T1/2. Two independent measurements.
doi: 10.1103/PhysRevC.47.1462
1993LU01 Phys.Rev. C47, 1211 (1993) S.J.Luke, R.Vandenbosch, W.Benenson, J.Clayton, K.Joh, D.Krofcheck, T.K.Murakami, J.D.Stevenson High Energy γ Rays from 14N + (nat)Ag at 35 MeV/nucleon NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; measured σ(θ, Eγ), high energy γ(θ). Nucleon exchange transport model, diffuse momentum distribution.
doi: 10.1103/PhysRevC.47.1211
1993MI15 Phys.Lett. 314B, 7 (1993) J.Miller, G.F.Krebs, J.Panetta, L.S.Schroeder, P.N.Kirk, Z.-F.Wang, W.Bauer, W.Benenson, D.Cebra, M.Cronqvist, B.-A.Li, R.Pfaff, T.Reposeur, J.Stevenson, A.Vander Molen, G.Westfall, J.S.Winfield, B.Young, T.Murakami, T.Suzuki, I.Tanihata Mass Dependence of Pion Production in Heavy Ion Collisions Near, But Below Threshold NUCLEAR REACTIONS 139La(139La, X), 197Au(197Au, X), E=183, 236 MeV/nucleon; measured π- inclusive production σ vs E(π), charged particle multiplicity, beam energy; deduced pion production mechanism.
doi: 10.1016/0370-2693(93)91314-D
1993PF01 Z.Phys. A347, 67 (1993) R.Pfaff, B.M.Young, W.Benenson, J.Clayton, D.J.Morrissey, N.A.Orr, T.Reposeur, M.Thoennessen, J.A.Winger Target Isotope Effect in High Energy Photon Production at E/A = 10 MeV NUCLEAR REACTIONS, ICPND 112,124Sn(12C, X), E=10 MeV/nucleon; measured Eγ, Iγ, photon yield vs Eγ; deduced σ ratio. Neutron-Proton bremsstrahlung model.
doi: 10.1007/BF01301279
1993WI03 Phys.Lett. 299B, 214 (1993) J.A.Winger, D.P.Bazin, W.Benenson, G.M.Crawley, D.J.Morrissey, N.A.Orr, R.Pfaff, B.M.Sherrill, M.Steiner, M.Thoennessen, S.J.Yennello, B.M.Young Halflife Measurements of the rp-Process Nuclei 61Ga, 63Ge, and 65As RADIOACTIVITY 61,62Ga, 63,64Ge, 65,66As(β+)[from 58Ni(78Kr, X), E=75 MeV/nucleon]; measured TOF, Ie, Ee summed decay spectra; deduced T1/2, implications to rp-process.
doi: 10.1016/0370-2693(93)90250-L
1993WI18 Phys.Rev. C48, 3097 (1993) J.A.Winger, D.P.Bazin, W.Benenson, G.M.Crawley, D.J.Morrissey, N.A.Orr, R.Pfaff, B.M.Sherrill, M.Thoennessen, S.J.Yennello, B.M.Young Half-Life Measurements for 61Ga, 63Ge, and 65As and Their Importance in the rp Process RADIOACTIVITY 61,62Ga, 63Ge, 65,66As(β+) [from 58Ni(84Kr, X), E=75 MeV/nucleon]; measured β-decay summed spectra. 66As, 62,61Ga, 63Ge deduced T1/2. 65As deduced T1/2, proton partial T1/2, Q(β), mass excess, proton separation energy. Implications to rp-process. NUCLEAR REACTIONS 58Ni(84Kr, X), E=75 MeV/nucleon; measured β-decay summed spectra; deduced evidence for 66Se.
doi: 10.1103/PhysRevC.48.3097
1993YO03 Phys.Lett. 311B, 22 (1993) B.M.Young, D.Bazin, W.Benenson, J.H.Kelley, D.J.Morrissey, N.A.Orr, R.Ronningen, B.M.Sherrill, M.Steiner, M.Thoennessen, J.A.Winger, S.J.Yennello, I.Tanihata, X.X.Bai, N.Inabe, T.Kubo, C.-B.Moon, S.Shimoura, T.Suzuki, R.N.Boyd, K.Subotic Strong Isomer Production in Fragmentation Reactions NUCLEAR REACTIONS, ICPND 9Be(27Al, X)26mAl/26Al, E=100 MeV/nucleon; 9Be(28Si, X)26mAl/26Al, E=80 MeV/nucleon; 12C(40Ar, X)26mAl/26Al, E=65 MeV/nucleon; measured isomer production yields following projectile fragmentation. Activation technique.
doi: 10.1016/0370-2693(93)90527-O
1993YO07 Phys.Rev.Lett. 71, 4124 (1993) B.M.Young, W.Benenson, M.Fauerbach, J.H.Kelley, R.Pfaff, B.M.Sherrill, M.Steiner, J.S.Winfield, T.Kubo, M.Hellstrom, N.A.Orr, J.Stetson, J.A.Winger, S.J.Yennello Mass of 11Li from the 14C(11B, 11Li)14O Reaction NUCLEAR REACTIONS 14C(11B, 11Li), E=32 MeV/nucleon; measured momentum spectra, Q. 11Li deduced two-neutron separation energy, mass.
doi: 10.1103/PhysRevLett.71.4124
1992CL02 Phys.Rev. C45, 1810 (1992) J.Clayton, W.Benenson, M.Cronqvist, R.Fox, D.Krofcheck, R.Pfaff, T.Reposeur, J.D.Stevenson, J.S.Winfield, B.Young, M.F.Mohar, C.Bloch, D.E.Fields Proton-Deuteron Bremsstrahlung at 145 and 195 MeV NUCLEAR REACTIONS 2H(p, γ), E=145, 195 MeV; measured Eγ, Iγ, σ(θ, Eγ); deduced n-p bremsstrahlung σ. BaF detectors.
doi: 10.1103/PhysRevC.45.1810
1992CL03 Phys.Rev. C45, 1815 (1992) J.Clayton, W.Benenson, M.Cronqvist, R.Fox, D.Krofcheck, R.Pfaff, T.Reposeur, J.D.Stevenson, J.S.Winfield, B.Young, M.F.Mohar, C.Bloch, D.E.Fields High Energy Gamma Ray Production in Proton-Induced Reactions at 104, 145, and 195 MeV NUCLEAR REACTIONS C, Zn, Pb(p, γ), E=104, 145, 195 MeV; measured Eγ, σ(θ, Eγ); deduced reaction mechanism, proton-neutron collision associated γ-emission probability.
doi: 10.1103/PhysRevC.45.1815
1992RE01 Phys.Lett. 276B, 418 (1992) T.Reposeur, J.Clayton, W.Benenson, M.Cronqvist, S.Hannuschke, S.Howden, J.Karn, D.Krofcheck, A.Nadasen, C.Ogilvie, R.Pfaff, J.D.Stevenson, A.Vander Molen, G.D.Westfall, K.Wilson, J.S.Winfield, B.Young, M.F.Mohar, D.J.Morrissey Impact Parameter Dependence of High Energy Gamma Ray Production in Heavy-Ion Collisions NUCLEAR REACTIONS 51V(40Ar, X), E=65 MeV/nucleon; measured σ(fragment θ, Eγ), (fragment)γ-coin; deduced impact parameter dependence. Multi-detector array.
doi: 10.1016/0370-2693(92)91660-2
1992YE04 Phys.Rev. C46, 2620 (1992) S.J.Yennello, J.A.Winger, T.Antaya, W.Benenson, M.F.Mohar, D.J.Morrissey, N.A.Orr, B.M.Sherrill New Nuclei Near the Proton Drip Line Around Z = 40 NUCLEAR REACTIONS 58Ni(92Mo, X), E=70 MeV/nucleon; measured fragment mass, charge; deduced evidence for 78Y, 82Nb, 85Mo, 86Tc, 89,90Ru. A1200 beam analysis device.
doi: 10.1103/PhysRevC.46.2620
1991MO10 Phys.Rev.Lett. 66, 1571 (1991) M.F.Mohar, D.Bazin, W.Benenson, D.J.Morrissey, N.A.Orr, B.M.Sherrill, D.Swan, J.A.Winger, A.C.Mueller, D.Guillemaud-Mueller Identification of New Nuclei Near the Proton-Drip Line for 31 ≤ Z ≤ 38 NUCLEAR REACTIONS 58Ni(78Kr, X), E=65 MeV/nucleon; measured fragment spectra; deduced evidence for 65As, 61Ga, 62,63Ge, 69Br, 75Sr. Implications for r-process.
doi: 10.1103/PhysRevLett.66.1571
1990CL04 Phys.Rev. C42, 1009 (1990) J.Clayton, J.Stevenson, W.Benenson, D.Krofcheck, D.J.Morrissey, T.K.Murakami, J.S.Winfield Search for Photons from the Decay of the Delta Resonance in Heavy-Ion Collisions NUCLEAR REACTIONS Zn(14N, X), E=75 MeV/nucleon; measured σ(Eγ, θγ); deduced no Δ-resonance decay related photons.
doi: 10.1103/PhysRevC.42.1009
1990CL07 Phys.Lett. 251B, 23 (1990) G.Claesson, G.Krebs, J.Miller, G.Roche, L.S.Schroeder, W.Benenson, J.van der Plicht, J.S.Winfield, G.Landaud, J.-F.Gilot, C.Hartnack, H.Stocker Proton Emission in La + La Collisions at E/A = 138 and 246 MeV NUCLEAR REACTIONS 139La(139La, pX), E=138, 246 MeV/nucleon; measured proton multiplicities, differential σ; deduced nuclear matter flow features.
doi: 10.1016/0370-2693(90)90225-U
1990FO04 Phys.Rev. C41, 2689 (1990) S.Fortier, S.Gales, S.M.Austin, W.Benenson, G.M.Crawley, C.Djalali, J.S.Winfield, G.Yoo One-Nucleon-Transfer Reactions Induced by 20Ne at 500 and 600 MeV NUCLEAR REACTIONS 90Zr, 208Pb(20Ne, 19Ne), (20Ne, 21Ne), (20Ne, 21Na), E=500, 600 MeV; measured σ(fragment E, θ) vs excitation. 91Zr, 209Pb deduced structure characteristics. DWBA analysis. Enriched targets.
doi: 10.1103/PhysRevC.41.2689
1990LE08 Phys.Rev. C41, 1562 (1990) J.H.Lee, W.Benenson, D.J.Morrissey Statistical Equilibrium in the 40Ar + 12C System at E/A = 8 MeV NUCLEAR REACTIONS 12C(40Ar, X), E=320 MeV; measured fragment isotopic distribution. Statistical equilibrium models.
doi: 10.1103/PhysRevC.41.1562
1990LE10 Phys.Rev. C41, 2406 (1990) J.H.Lee, W.Benenson, C.Bloch, Y.Chen, R.J.Radtke, E.Kashy, M.F.Mohar, D.J.Morrissey, R.Blue, R.M.Ronningen New Test of the Excited State Population Method for Measurements of Nuclear Temperatures NUCLEAR REACTIONS 12C(40Ar, X), E=8, 10, 12 MeV/nucleon; measured fragment excited state production for X=7Li, 7Be, 10B, γ(fragment)-coin; deduced nuclear temperatures.
doi: 10.1103/PhysRevC.41.2406
1990WI03 Phys.Rev. C41, R1881 (1990) W.K.Wilson, W.Benenson, D.A.Cebra, J.Clayton, S.Howden, J.Karn, T.Li, C.A.Ogilvie, A.Vander Molen, G.D.Westfall, J.S.Winfield, B.Young, A.Nadasen Azimuthal Asymmetry in Ar + V Collisions from E/A = 35 to 85 MeV NUCLEAR REACTIONS 51V(40Ar, X), E=35-85 MeV/nucleon; measured σ(fragment θ); deduced asymmetry mechanism.
doi: 10.1103/PhysRevC.41.R1881
1989CE02 Phys.Lett. 227B, 336 (1989) D.A.Cebra, W.Benenson, Y.Chen, E.Kashy, A.Pradhan, A.Vander Molen, G.D.Westfall, W.K.Wilson, D.J.Morrissey, R.S.Tickle, R.Korteling, R.L.Helmer Two-Particle Correlations from 500 MeV p + Ag and Be NUCLEAR REACTIONS Ag, Be(p, 2pX), (p, 2dX), (p, dαX), (p, pdX), (p, pαX), (p, 2tX), E=500 MeV; measured light (particle)(particle)-correlations; deduced reaction mechanism.
doi: 10.1016/0370-2693(89)90940-4
1989CL05 Phys.Rev. C40, 1207 (1989) J.Clayton, J.Stevenson, W.Benenson, Y.Chen, E.Kashy, A.R.Lampis, M.Samuel, C.L.Tam, M.F.Mohar, D.J.Morrissey, T.K.Murakami, B.Sherrill, J.S.Winfield High Energy Gamma-Ray Production in the Heavy-Ion Reaction 136Xe + Sn at E/A = 89 and 124 MeV NUCLEAR REACTIONS Sm(136Xe, X), E=89, 124 MeV/nucleon; measured σ(Eγ, θγ); deduced high energy γ-emission mechanism.
doi: 10.1103/PhysRevC.40.1207
1989MU11 Phys.Rev. C40, 2079 (1989) T.K.Murakami, W.Benenson, Y.Chen, J.Clayton, E.Kashy, J.Stevenson, C.L.Tam, K.Hanold, M.Mohar High-Energy Gamma Rays from Reactions Induced by E/A = 15 MeV Heavy-Ion Beams NUCLEAR REACTIONS Zr(86Kr, X), (40Ar, X), Ca(40Ar, X), E=15 MeV/nucleon; measured σ(Eγ, θγ), γ-multiplicity; deduced γ-emission source velocity.
doi: 10.1103/PhysRevC.40.2079
1989TA10 Phys.Rev. C39, 1371 (1989) C.L.Tam, J.Stevenson, W.Benenson, J.Clayton, Y.Chen, E.Kashy, A.R.Lampis, D.J.Morrissey, M.Samuel, T.K.Murakami, J.S.Winfield Mass Dependence of High-Energy Gamma-Ray Production in Heavy-Ion Reactions NUCLEAR REACTIONS Li, Pb(7Li, X), Mg(20Ne, X), Pb, Ca(40Ar, X), E=30 MeV/nucleon; measured σ(E(γ), θ(γ)); deduced reaction mechanism, γ production σ.
doi: 10.1103/PhysRevC.39.1371
1988BL09 Phys.Rev. C37, 2469 (1988) C.Bloch, W.Benenson, A.I.Galonsky, E.Kashy, J.Heltsley, L.Heilbronn, M.Lowe, R.J.Radtke, B.Remington, J.Kassagi, D.J.Morrissey Neutrons in Coincidence with Intermediate Mass Fragments at Large Angles from 14N + Ag Reactions at E/A = 20 and 35 MeV NUCLEAR REACTIONS Ag(14N, X), E=20, 35 MeV/nucleon; measured neutron spectra shapes, multiplicities σ(fragment θ, E) for X=6,7Li, 7,9Be, 10,11B; deduced model parameters. Moving source.
doi: 10.1103/PhysRevC.37.2469
1988LA20 Phys.Rev. C38, 1961 (1988) A.R.Lampis, J.Stevenson, W.Benenson, J.Clayton, D.Cebra, Y.Chen, D.Fox, E.Kashy, D.J.Morrissey, M.Samuel, R.Smith, C.L.Tam, G.D.Westfall, K.Wilson, J.S.Winfield Correlations between High-Energy Gamma Rays and Light Fragments in Heavy Ion Collisions NUCLEAR REACTIONS Zn(14N, pγ), (14N, dγ), (14N, tγ), E=40 MeV/nucleon; measured (particle)γ-coin, σ(Ep, θp, θγ).
doi: 10.1103/PhysRevC.38.1961
1988MI03 Phys.Rev. C37, 766 (1988) D.Mikolas, B.A.Brown, W.Benenson, L.H.Harwood, E.Kashy, J.A.Nolen, Jr., B.Sherrill, J.Stevenson, J.S.Winfield, Z.Q.Xie, R.Sherr Branching Ratios of 9C to Low Lying States in 9B RADIOACTIVITY 9C(β+) [from Ni(12C, X), E=35 MeV/nucleon]; measured β-delayed Ep, Ip, β-delayed Eα, Iα, βαp-coin; deduced log ft. 9B levels deduced Iβ, Gamow-Teller transition strengths, comparison with other data. NUCLEAR STRUCTURE 9B, 9Be, 9C; calculated levels, Gamow-Teller transition strengths, particle decay spectroscopic factors, particle decay reduced widths. Input from 9Be(p, n) reaction.
doi: 10.1103/PhysRevC.37.766
1988MO18 Phys.Rev. C38, 737 (1988) M.F.Mohar, E.Adamides, W.Benenson, C.Bloch, B.A.Brown, J.Clayton, E.Kashy, M.Lowe, J.A.Nolen, Jr., W.E.Ormand, J.van der Plicht, B.Sherrill, J.Stevenson, J.S.Winfield Mass of 39Sc via the 40Ca(7Li, 8He) Reaction NUCLEAR REACTIONS 40Ca(7Li, 8He), E=27.24 MeV/nucleon; measured σ(E(8He)); deduced Q, mass equation parameters. 39Sc deduced mass excess. Isobaric multiplet mass equation, isospin-nonconserving Hamiltonian.
doi: 10.1103/PhysRevC.38.737
1988TA22 Phys.Rev. C38, 2526 (1988) C.L.Tam, J.Stevenson, W.Benenson, J.Clayton, Y.Chen, E.Kashy, A.R.Lampis, D.J.Morrissey, M.Samuel, T.K.Murakami, J.S.Winfield High-Energy Gamma-Ray Production in Light-Ion Induced Reactions NUCLEAR REACTIONS C, Zn, Pb(p, X), E=53 MeV/nucleon; C, Zn, Pb(α, X), E=25, 53 MeV/nucleon; measured σ(θγ, Eγ); deduced γ-production mechanism.
doi: 10.1103/PhysRevC.38.2526
1987BL13 Phys.Rev. C36, 203 (1987) C.Bloch, W.Benenson, A.I.Galonsky, E.Kashy, J.Heltsley, L.Heilbronn, M.Lowe, B.Remington, D.J.Morrissey, J.Kasagi Neutron Decay of Excited Nuclear States in Heavy Ion Collisions NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured (fragment)n-coin, yields for X=7,8Li. 7,8Li levels deduced neutron decay characteristics, nuclear temperature.
doi: 10.1103/PhysRevC.36.203
1987FO16 Phys.Rev. C36, 1830 (1987) S.Fortier, S.Gales, S.M.Austin, W.Benenson, G.M.Crawley, C.Djalali, J.H.Lee, J.van der Plicht, J.S.Winfield Search for High Excitation Energy Structures in 90Zr and 208Pb, via 20Ne Inelastic Scattering NUCLEAR REACTIONS 90Zr, 208Pb(20Ne, 20Ne'), E=500, 600 MeV; measured σ(E(20Ne')); deduced structure, excitation mechanism.
doi: 10.1103/PhysRevC.36.1830
1987MI09 Phys.Rev.Lett. 58, 2408 (1987) J.Miller, J.Bercovitz, G.Claesson, G.Krebs, G.Roche, L.S.Schroeder, W.Benenson, J.van der Plicht, J.S.Winfield, G.Landaud, J.-F.Gilot Subthreshold Pion Production with Associated Multiplicity Selection in the Reaction 139La + 139La → π± + X NUCLEAR REACTIONS 139La(139La, π+X), (139La, π-X), E=138, 183, 246 MeV/nucleon; measured σ(Eπ, θπ) vs fragment E, multiplicity distributions; deduced pion yield target, projectile mass dependences. Multi-wire proportional chamber, scintillation hodoscope, multiplicity array.
doi: 10.1103/PhysRevLett.58.2408
1986BL12 Phys.Rev. C34, 850 (1986) C.Bloch, W.Benenson, E.Kashy, D.J.Morrissey, R.A.Blue, R.M.Ronningen, H.Utsunomiya Effect of 8Be Decay on Nuclear Temperature Measurements NUCLEAR REACTIONS Ag(14N, X)6Li/7Li/7Be/9Be/10Be/10B/11B, E=280, 350, 490 MeV; measured inclusive residual fragment spectra, 7Li, 8Be yields relative to 6Li, γ-multiplicity; deduced nuclear temperatures.
doi: 10.1103/PhysRevC.34.850
1986KR07 Phys.Lett. 171B, 37 (1986) G.F.Krebs, J.-F.Gilot, P.N.Kirk, G.Claesson, J.Miller, H.G.Pugh, L.S.Schroeder, G.Roche, J.Vicente, K.Beard, W.Benenson, J.Van der Plicht, B.Sherrill, J.W.Harris Subthreshold Negative Pions and Energetic Protons Produced at θ(cm) = 90° in 246 MeV/nucleon 139La + 139La Collisions NUCLEAR REACTIONS 139La(139La, π-X), (139La, pX), E=246 MeV/nucleon; measured inclusive pion, proton production σ; deduced reaction mechanism. Phase space, intranuclear cascade models.
doi: 10.1016/0370-2693(86)90993-7
1986MO13 Phys.Rev. C34, 761 (1986) D.J.Morrissey, C.Bloch, W.Benenson, E.Kashy, R.A.Blue, R.M.Ronningen, R.Aryaeinejad Thermal Population of Nuclear Excited States NUCLEAR REACTIONS 12C(14N, X)7Be/10B, E=6.25-25 MeV/nucelon; measured σ(fragment θ), (fragment)γ-coin, Eγ, Iγ, γ-multiplicity. 7Be, 10B deduced bound state population. 26Al deduced equilibrium characteristics.
doi: 10.1103/PhysRevC.34.761
1986ST07 Phys.Rev.Lett. 57, 555 (1986) J.Stevenson, K.B.Beard, W.Benenson, J.Clayton, E.Kashy, A.Lampis, D.J.Morrissey, M.Samuel, R.J.Smith, C.L.Tam, J.S.Winfield High-Energy Gamma-Ray Emission in Heavy-Ion Collisions NUCLEAR REACTIONS Pb, Zn, C(14N, X), E=20, 30, 40 MeV/nucleon; measured Eγ, Iγ, γ(θ); deduced model parameters. Individual neutron-proton collision induced bremsstrahlung.
doi: 10.1103/PhysRevLett.57.555
1985BE33 Phys.Rev. C32, 1111 (1985) K.B.Beard, W.Benenson, C.Bloch, E.Kashy, J.Stevenson, D.J.Morrissey, J.van der Plicht, B.Sherrill, J.S.Winfield Observation of High Energy Gamma Rays in Intermediate Energy Nucleus-Nucleus Collisions NUCLEAR REACTIONS Cu(14N, γ), E=40 MeV/nucleon; measured σ(Eγ, θ); deduced temperature parameter, e+, e-, pair production limits.
doi: 10.1103/PhysRevC.32.1111
1985BE50 Phys.Lett. 162B, 87 (1985) W.Benenson, K.Beard, C.Bloch, B.Sherrill, B.A.Brown, A.D.Panagiotou, J.van der Plicht, J.S.Winfield, C.E.Thorn The Masses of 51Ca and 47Ar NUCLEAR REACTIONS 48Ca(14C, 15O), (14C, 11C), E=100 MeV; measured σ(E(15O)), σ(E(11C)). 47Ar, 51Ca deduced masses.
doi: 10.1016/0370-2693(85)91066-4
1985FR13 Phys.Rev. C32, 975 (1985) K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.L.Murphy, J.O.Rasmussen, J.P.Sullivan, E.Yoo, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert Pion Production Near Mid-Rapidity in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS C, Ca, U(40Ar, X), E=1050 MeV/nucleon; 9Be, 23Na, 19F(20Ne, X), E=655 MeV/nucleon; measured σ(θ(π+), E(π+)), σ(θ(π-), E(π-)); deduced ratio. Coulomb effect calculation comparison.
doi: 10.1103/PhysRevC.32.975
1985MO17 Phys.Rev. C32, 877 (1985) D.J.Morrissey, W.Benenson, E.Kashy, C.Bloch, M.Lowe, R.A.Blue, R.M.Ronningen, B.Sherrill, H.Utsunomiya, I.Kelson Nuclear Temperatures in the Reactions of 14N with Ag at 35 MeV/nucleon NUCLEAR REACTIONS Ag(14N, X), E=490 MeV; measured particle spectra for X=6,7,8Li, 7,9,10Be, yield vs Q, γ-multiplicity, (particle)γ-coin. 6,7,8Li, 7Be levels deduced effective nuclear temperatures.
doi: 10.1103/PhysRevC.32.877
1985MO24 Nucl.Phys. A447, 603c (1985) D.J.Morrissey, W.Benenson, E.Kashy, C.Bloch, M.Lowe, B.Sherrill, R.A.Blue, R.M.Ronningen, H.Utsunomiya Results from a New Temperature Measurement in Nuclear Reactions NUCLEAR REACTIONS 12C(14N, X), E=8 MeV/nucleon; measured inclusive fragment spectra for X=Li, Be, B. 7Li, 7Be deduced excited state population fraction. Ag(14N, X), E=490 MeV; measured inclusive fragment spectra for X=Li, Be; deduced temperature for 6,8Li, 7Be fragments.
doi: 10.1016/0375-9474(86)90636-6
1985SH03 Phys.Rev. C31, 875 (1985) B.Sherrill, K.Beard, W.Benenson, C.Bloch, B.A.Brown, E.Kashy, J.A.Nolen, Jr., A.D.Panagiotou, J.van der Plicht, J.S.Winfield Mass of 57Cu NUCLEAR STRUCTURE A=39-59; calculated Coulomb displacement energies; deduced rp-process rate for 56Ni(p, γ) reaction. Mass excess input. NUCLEAR REACTIONS 58Ni(7Li, 8He), E=173.6 MeV; measured Q, σ(θ). 57Cu deduced levels, mass excess.
doi: 10.1103/PhysRevC.31.875
1984MO29 Phys.Lett. 148B, 423 (1984) D.J.Morrissey, W.Benenson, E.Kashy, B.Sherrill, A.D.Panagiotou, R.A.Blue, R.M.Ronningen, J.van der Plicht, H.Utsunomiya Excited State Production and Temperature Measurement in a Heavy Ion Reaction NUCLEAR REACTIONS Ag(14N, X), E=490 MeV; measured fragment spectra for X=6,7Li, 7Be; deduced fragment excited state population, effective temperature inconsistency.
doi: 10.1016/0370-2693(84)90730-5
1983SH31 Phys.Rev. C28, 1712 (1983) B.Sherrill, K.Beard, W.Benenson, B.A.Brown, E.Kashy, W.E.Ormand, H.Nann, J.J.Kehayias, A.D.Bacher, T.E.Ward Mass of 59Zn NUCLEAR STRUCTURE A=41-59; analyzed Coulomb energy systematics. New data on 59Zn input. RADIOACTIVITY 59Zn(β+); calculated ft. Latest mass measurement input. NUCLEAR REACTIONS 58Ni(p, π-), E=190 MeV; measured σ(E(π)), σ(θ), Q. 40Ca(p, π-), E=190 MeV; measured σ(reaction) upper limit. 59Zn deduced mass.
doi: 10.1103/PhysRevC.28.1712
1982CR01 Phys.Lett. 109B, 8 (1982) G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski Pairing Model Predictions for (p, t) Experiments on the Cadmium Isotopes NUCLEAR REACTIONS 110,112,114,116Cd(p, t), E=42 MeV; measured σ(Et). 106Cd(p, t), E=42 MeV; measured σ(Et), Q. 110,112,114,116,106Cd deduced two-particle pickup from deep orbits. 104Cd deduced mass excess. Split-pole spectrograph, position sensitive proportional counter. Pairing model.
doi: 10.1016/0370-2693(82)90450-6
1982FR05 Phys.Rev. C25, 1102 (1982) K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.Murphy, J.O.Rasmussen, J.P.Sullivan, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert Pions Produced near the Center-of-Mass Velocity in Heavy-Ion Collisions NUCLEAR REACTIONS C, Ca, U(40Ar, π+), (40Ar, π-), E=1.05 GeV/nucleon; measured σ(E, θ).
doi: 10.1103/PhysRevC.25.1102
1982SU01 Phys.Rev. C25, 1499 (1982) J.P.Sullivan, J.A.Bistirlich, H.R.Bowman, R.Bossingham, T.Buttke, K.M.Crowe, K.A.Frankel, C.J.Martoff, J.Miller, D.L.Murphy, J.O.Rasmussen, W.A.Zajc, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr. Strong Coulomb Effects on Pions Produced in Heavy Ion Collisions NUCLEAR REACTIONS C, Na, F, Cu, U(20Ne, π+), (20Ne, π-), E=280-480 MeV/nucleon; C, K, Cl(40Ar, π+), (40Ar, π-), E=535 MeV/nucleon; measured σ(Eπ, θπ); deduced Coulomb effects, projectile fragment charges.
doi: 10.1103/PhysRevC.25.1499
1982ZW02 Nucl.Phys. A389, 301 (1982) B.Zwieglinski, W.Benenson, G.M.Crawley, S.Gales, D.Weber Study of 11B at High Excitations with the 9Be(3He, p)11B and 9Be(α, d)11B Reactions NUCLEAR REACTIONS 9Be(3He, p), E=38 MeV; 9Be(α, d), E=48 MeV; measured σ(E(p), θ), σ(E(d)). 11B deduced levels, widths, isospin purity, L, normalization factors. DWBA analysis, shell-model form factors. Natural targets.
doi: 10.1016/0375-9474(82)90521-8
1981CR01 Phys.Rev. C23, 589 (1981) G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski Hole States in the Tin Isotopes Observed by the (p, t) Reaction NUCLEAR REACTIONS 112,116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ); 117,119Sn(p, d), E=42 MeV; measured σ(Ed). 110,114,116,118,120,122Sn deduced broad resonances, Γ. DWBA analysis. Enriched targets.
doi: 10.1103/PhysRevC.23.589
1981DE17 Phys.Lett. 101B, 147 (1981) P.Decowski, H.P.Morsch, W.Benenson Low-Lying Isoscalar Dipole Excitations in 208Pb NUCLEAR REACTIONS 208Pb(α, α'), E=48 MeV; measured σ(Eα, θ). 208Pb deduced T=0, dipole states, Γ, EWSR. Microscopic DWBA analysis, nuclear diffuseness dipole oscillation.
doi: 10.1016/0370-2693(81)90661-4
1980CR02 Phys.Rev. C22, 316 (1980) G.M.Crawley, S.Gales, D.Weber, B.Zwieglinski, W.Benenson, D.Friesel, A.Bacher, B.M.Spicer Deep Hole States Observed in (p, t) Reactions NUCLEAR REACTIONS 120,122,124Sn(p, t), E=89 MeV; measured σ(Et, θ). 118,120,122Sn deduced levels, Γ. DWBA, enriched targets.
doi: 10.1103/PhysRevC.22.316
1980PA02 Phys.Rev. C21, 462 (1980) R.C.Pardo, L.W.Robinson, W.Benenson, E.Kashy, R.M.Ronningen Mass and Excited States of the Nucleus 89Mo NUCLEAR REACTIONS 92Mo(3He, 6He), E=70 MeV; measured σ(E(6He)), Q. 89Mo deduced mass excess, levels, J, π.
doi: 10.1103/PhysRevC.21.462
1979BE31 Phys.Rev.Lett. 43, 683 (1979) W.Benenson, G.Bertsch, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., H.Bowman, J.G.Ingersoll, J.O.Rasmussen, J.Sullivan, M.Koike, M.Sasao, J.Peter, T.E.Ward Low-Energy Pion Production at 0° with Heavy Ions from 125 to 400 MeV/Nucleon NUCLEAR REACTIONS Na, F, Cu, U(20Ne, π+), (20Ne, π-), E=125-400 MeV/nucleon; measured σ(0°), σ(π+)/σ(π-); discussed reaction mechanisms.
doi: 10.1103/PhysRevLett.43.683
1979WE02 Nucl.Phys. A313, 385 (1979) D.J.Weber, G.M.Crawley, W.Benenson, E.Kashy, H.Nann Study of 60Zn and 61Zn NUCLEAR REACTIONS 58Ni(12C, 10Be), 58Ni(12C, 9Be), E=77 MeV; measured σ(E(10Be), θ), σ(E(9Be), θ). 60Zn, 61Zn deduced levels. 64Zn(3He, 6He), E=70 MeV; measured σ; deduced Q. 61Zn deduced mass excess, levels. Enriched targets. Atomic mass 61Zn.
doi: 10.1016/0375-9474(79)90508-6
1979ZW01 Nucl.Phys. A315, 124 (1979) B.Zwieglinski, W.Benenson, R.G.H.Robertson, W.R.Coker Study of the 10Be(d, p)11Be Reaction at 25 MeV NUCLEAR REACTIONS 10Be(d, p), E=25 MeV; measured σ(θ). 11Be levels deduced S, DWBA analysis. Comparison with shell model. Reactor-produced 10Be target.
doi: 10.1016/0375-9474(79)90637-7
1978BE26 Phys.Rev. C17, 1939 (1978) W.Benenson, E.Kashy, A.G.Ledebuhr, R.C.Pardo, R.G.H.Robertson, L.W.Robinson T = 3/2 Levels in 15F and 15O NUCLEAR REACTIONS 20Ne(3He, 8Li), E=74.5 MeV; 17O(p, t), E=45 MeV; measured σ; deduced Q. 15F deduced mass excess, levels, Γ. 15O deduced analog level, Γ, proton branching.
doi: 10.1103/PhysRevC.17.1939
1978DE18 Nucl.Phys. A302, 186 (1978) P.Decowski, W.Benenson, B.A.Brown, H.Nann Levels of 52Fe Studied with the (p, t) Reaction NUCLEAR REACTIONS 54Fe(p, t), E=45 MeV; measured σ(Et, θ). 52Fe deduced levels, L, J, π. Enriched target, magnetic spectrograph. Shell model calculation.
doi: 10.1016/0375-9474(78)90294-4
1978MO04 Nucl.Phys. A297, 317 (1978) H.P.Morsch, P.Decowski, W.Benenson Fine Structure in the Giant Resonance Region and the Collective Dipole Spin-Flip Excitation in 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=40, 45 MeV; 208Pb(α, α'), E=48 MeV; measured σ(θ). 208Pb deduced strengths for J=1, 2, 3 transitions in the region 6-12 MeV excitation, B(M2).
doi: 10.1016/0375-9474(78)90279-8
1978PA11 Phys.Rev. C18, 1249 (1978) R.C.Pardo, E.Kashy, W.Benenson, L.W.Robinson Mass Measurement of Proton-Rich, Medium-Weight Nuclei by the (3He, 6He) Reaction NUCLEAR REACTIONS 70Ge, 90Zr, 106Cd, 112Sn, 144Sm(3He, 6He), E=70 MeV; measured yields; deduced Q. 67Ge, 87Zr, 103Cd, 109Sn, 141Sm deduced mass excess, levels.
doi: 10.1103/PhysRevC.18.1249
1978RO01 Phys.Rev. C17, 4 (1978) R.G.H.Robertson, E.Kashy, W.Benenson, A.Ledebuhr Mass of 6He NUCLEAR REACTIONS 7Li, 19F(d, 3He), E=20.8 MeV; measured σ; deduced Q. 6He deduced mass excess.
doi: 10.1103/PhysRevC.17.4
1977BE13 Phys.Rev. C15, 1187 (1977) W.Benenson, D.Mueller, E.Kashy, H.Nann, L.W.Robinson Mass of 27P and 31Cl NUCLEAR REACTIONS 32S, 36Ar(3He, 8Li), 29Si(p, t); measured spectra; deduced Q. 31Cl deduced mass excess. 27P deduced mass excess, lowest T=3/2 level.
doi: 10.1103/PhysRevC.15.1187
1977CR04 Phys.Rev.Lett. 39, 1451 (1977) G.M.Crawley, W.Benenson, D.Weber, B.Zwieglinski Observation of Hole States at High Excitation in (p, t) Reactions NUCLEAR REACTIONS 106Cd, 104Pd, 116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ). 114,116,118,120,122Sn deduced enhancements, widths.
doi: 10.1103/PhysRevLett.39.1451
1977MU03 Phys.Rev. C15, 1282 (1977) D.Mueller, E.Kashy, W.Benenson Coulomb Displacement Energies of the A = 4n + 3, T + 1/2 Mirror Nuclei in the 1f7/2 Shell NUCLEAR REACTIONS 46Ti, 50Cr, 54Fe, 58Ni(3He, 6He), E=70 MeV; measured σ(θ); deduced Q. 43Ti, 47Cr, 51Fe, 55Ni deduced mass excess, Coulomb displacement energies.
doi: 10.1103/PhysRevC.15.1282
1977NA19 Phys.Rev. C16, 1684 (1977) H.Nann, W.Benenson, E.Kashy, H.P.Morsch, D.Mueller Levels of 16F NUCLEAR REACTIONS 19F(3He, 6He), E=70 MeV; 16O(3He, t), E=35 MeV; measured spectra. 16F deduced levels.
doi: 10.1103/PhysRevC.16.1684
1977PA27 Phys.Lett. 71B, 301(1977) R.Pardo, R.G.Markham, W.Benenson, A.I.Galonsky, E.Kashy Excitation of Giant Resonance in 90Zr by Inelastic 6Li Scattering NUCLEAR REACTIONS 90Zr(6Li, 6Li'), E=74 MeV; measured σ(θ). 90Zr deduced giant resonance, width.
doi: 10.1016/0370-2693(77)90221-0
1976BE08 Phys.Rev. C13, 1479 (1976) W.Benenson, A.Guichard, E.Kashy, D.Mueller, H.Nann Mass of 35K NUCLEAR REACTIONS 40Ca(3He, 8Li), E=75.8, 73.7 MeV; measured σ; deduced Q. 35K deduced mass excess, levels.
doi: 10.1103/PhysRevC.13.1479
1976GU03 Phys.Rev. C13, 540 (1976) A.Guichard, W.Benenson, R.G.Markham, H.Nann 48Ti(p, 3He)46Sc Reaction NUCLEAR REACTIONS 48Ti(p, 3He), E=40.2 MeV; measured σ(E(3He), θ). 46Sc deduced levels, L, J, π.
doi: 10.1103/PhysRevC.13.540
1976KA24 Phys.Rev. C14, 1773 (1976) E.Kashy, W.Benenson, D.Mueller, H.Nann, L.Robinson Observation of Highly Neutron-Rich 43Cl and 59Mn NUCLEAR REACTIONS 48Ca, 64Ni(3He, 8B), E=74 MeV; measured σ(E(8B), θ); deduced Q. 43Cl, 59Mn deduced mass excess.
doi: 10.1103/PhysRevC.14.1773
1976MO07 Phys.Lett. 61B, 167 (1976) A.Moalem, W.Benenson, G.M.Crawley, T.L.Khoo Decay Modes of the Giant Resonance Region in 40Ca NUCLEAR REACTIONS 40Ca(3He, 3He'), E=70 MeV; measured p3He'(θ), 3He'α(θ). 40Ca resonance deduced Γp/Γα.
doi: 10.1016/0370-2693(76)90617-1
1976MO18 Phys.Rev.Lett. 37, 263 (1976) H.P.Morsch, P.Decowski, W.Benenson Monopole Excitation in the Giant-Resonance Region of 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=45 MeV; 208Pb(3He, 3He'), E=70 MeV; measured σ(θ). 208Pb deduced resonances, L.
doi: 10.1103/PhysRevLett.37.263
1976RO04 Phys.Rev. C13, 1018 (1976) R.G.H.Robertson, W.Benenson, E.Kashy, D.Mueller Measurement of the Mass of 8C by the 14N(3He, 9Li) Reaction NUCLEAR REACTIONS 14N(3He, 9Li), E=76 MeV; measured σ(θ), Q. 8C deduced mass excess, Γ.
doi: 10.1103/PhysRevC.13.1018
1975BE38 Phys.Lett. 58B, 46 (1975) W.Benenson, A.Guichard, E.Kashy, D.Mueller, H.Nann, L.W.Robinson Mass Measurements of 19Na and 23Al Using the (3He, 8Li) Reaction NUCLEAR REACTIONS 24Mg, 28Si(3He, 8Li), E=76.8 MeV; measured σ(E(8Li)); deduced Q. 19Na, 23Al deduced mass excess. 19Na deduced level.
doi: 10.1016/0370-2693(75)90723-6
1975BE56 Nukleonika 20, 775 (1975) Exotic Nuclei with Z > N NUCLEAR STRUCTURE 41,42,43,44V, 42,43,44,45,46Cr, 44,45,46,47,48Mn, 45,46,47,48,49,50Fe, 48,49,50,51,52Co, 48,49,50,51,52,53,54Ni; calculated mass excess, binding energies. Isobaric multiplet mass equation. Review paper.
1975GU05 Phys.Rev. C11, 2027 (1975) A.Guichard, W.Benenson, H.Nann Spectroscopy of 52Mn from the 54Fe(p, 3He) Reaction at 40.2 MeV NUCLEAR REACTIONS 54Fe(p, 3He), E=40.2 MeV; measured σ(E(3He), θ). 52Mn deduced levels, L.
doi: 10.1103/PhysRevC.11.2027
1975GU13 Phys.Rev. C12, 806 (1975) A.Guichard, W.Benenson, H.Nann Study of 48V with the 50Cr(p, 3He) Reaction at 44.7 MeV NUCLEAR REACTIONS 50Cr(p, 3He), E=44.7 MeV; measured σ(E(3He), θ). 48V deduced levels, L, J, π.
doi: 10.1103/PhysRevC.12.806
1975GU18 Phys.Rev. C12, 1762 (1975) A.Guichard, W.Benenson, H.Nann Level Structure of 54Mn from the 56Fe(p, 3He) Reaction at 40.2 MeV NUCLEAR REACTIONS 56Fe(p, 3He), E=40.2 MeV; measured σ(E(3He), θ). 54Mn deduced levels, L, J, π.
doi: 10.1103/PhysRevC.12.1762
1975GU19 Phys.Rev. C12, 1780 (1975) A.Guichard, W.Benenson, R.G.Markham, H.Nann 52Cr(p, 3He)50V Reaction NUCLEAR REACTIONS 52Cr(p, 3He), E=40.2 MeV; measured σ(E(3He), θ). 50V deduced levels, L, J, π.
doi: 10.1103/PhysRevC.12.1780
1975KA18 Phys.Rev. C11, 1959 (1975) E.Kashy, W.Benenson, D.Mueller, R.G.H.Robertson, D.R.Goosman Mass of 9Li NUCLEAR REACTIONS 10Be(d, 3He), E=23.92 MeV; measured σ(E(3He)). 9Li deduced mass excess.
doi: 10.1103/PhysRevC.11.1959
1975MU09 Phys.Rev. C12, 51 (1975) D.Mueller, E.Kashy, W.Benenson, H.Nann Masses of T(z) = -1/2 Nuclei in the 1f7/2 Shell NUCLEAR REACTIONS 27Al, 50Cr, 54Fe, 58Ni(p, 6He), E=46 MeV; 27Al, 46Ti, 50Cr, 54Fe, 58Ni(3He, 6He), E=70 MeV; measured σ. 43Ti, 45V, 47Cr, 49Mn, 51Fe, 53Co, 55Ni deduced mass excess. Z=21-28 calculated mass of proton rich nuclei.
doi: 10.1103/PhysRevC.12.51
1974BE20 Phys.Rev. C9, 2130 (1974) W.Benenson, E.Kashy, D.H.Kong-A-Siou, A.Moalem, H.Nann T = 3/2 States in Mass-11 Nuclei NUCLEAR REACTIONS 14N(3He, 6He), E=70 MeV; 13C(p, t), E=46.7 MeV; 13C(p, 3He), E=40 MeV; measured σ(E(6He), Et, E(3He)). 11N, 11C, 11B deduced levels.
doi: 10.1103/PhysRevC.9.2130
1974BE66 Phys.Rev. C10, 2633 (1974) First Excited A = 9 Isospin Quartet NUCLEAR REACTIONS 12C(3He, 6He), E=74 MeV; measured σ(E(6He)). 11B(p, t), E=46.5 MeV; measured σ(Et). 9B, 9C deduced levels, new mass quartet, mass excesses.
doi: 10.1103/PhysRevC.10.2633
1974HA02 Phys.Rev. C9, 252 (1974) J.C.Hardy, H.Schmeing, W.Benenson, G.M.Crawley, E.Kashy, H.Nann Fermi Beta Decay: The Masses of 22Mg, 26Si, 30S, and 34Ar NUCLEAR REACTIONS 24Mg, 28Si, 32S, 36Ar(p, t), E=40.2 MeV; measured Q values. 22Mg, 26Si, 30S, 34Ar deduced masses, ft values, mirror asymmetries for A=26, 34.
doi: 10.1103/PhysRevC.9.252
1974KA15 Phys.Rev. C9, 2102 (1974) E.Kashy, W.Benenson, J.A.Nolen, Jr. A = 9 Isospin Quartet NUCLEAR REACTIONS 11B(p, t), (p, 3He), E=42 MeV; 10,11B(p, p'), E=35 MeV; measured σ(Et, E(3He), Ep'), Q. 9,10,11B, 9Be deduced levels.
doi: 10.1103/PhysRevC.9.2102
1974MO26 Nucl.Phys. A236, 307 (1974) A.Moalem, W.Benenson, G.M.Crawley A Study of the Nuclear Continuum in 16O by Inelastic 3He Scattering NUCLEAR REACTIONS 16O(3He, 3He'), E=71 MeV; measured σ(E(3He'), θ). 16O resonances deduced E2 strength.
doi: 10.1016/0375-9474(74)90256-5
1974NA07 Phys.Rev. C9, 1848 (1974) H.Nann, W.Benenson, E.Kashy, P.Turek Isobaric Mass Quartets in A = 33 Nuclei NUCLEAR REACTIONS 36Ar(3He, 6He), E=70 MeV; measured Q, σ(E(6He)). 33Ar deduced levels.
doi: 10.1103/PhysRevC.9.1848
1974NA14 Phys.Rev. C10, 1001 (1974) H.Nann, W.Benenson, W.A.Lanford, B.H.Wildenthal (p, 3He) and (p, t) Reactions on 29Si NUCLEAR REACTIONS 29Si(p, t), (p, 3He), E=40.1 MeV; measured σ(Et, θ), σ(E(3He), θ). 27Si, 27Al deduced levels, J, π, L, t. Enriched targets.
doi: 10.1103/PhysRevC.10.1001
1974NA19 Phys.Rev. C10, 1880 (1974) Levels of 56Ni NUCLEAR REACTIONS 58Ni(p, t), Ep=40.0, 45.5 MeV; measured σ(Et, θ); enriched target. 56Ni deduced levels, L, J, π.
doi: 10.1103/PhysRevC.10.1880
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