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NSR database version of February 19, 2024.

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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0970.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1399.


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
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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
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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
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1995BE30      Nucl.Phys. A588, 11c (1995)

W.Benenson

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1342.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1098.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1975BE56      Nukleonika 20, 775 (1975)

W.Benenson

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0248.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2668.


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
Citations: PlumX Metrics


1974BE66      Phys.Rev. C10, 2633 (1974)

W.Benenson, E.Kashy

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1974NA19      Phys.Rev. C10, 1880 (1974)

H.Nann, W.Benenson

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
Citations: PlumX Metrics


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