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NSR database version of April 11, 2024.

Search: Author = R.Sherr

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2013FO04      Phys.Rev. C 87, 014306 (2013); Pub.Note Phys.Rev. C 87, 019903 (2013)

H.T.Fortune, R.Sherr

Continuum three-body decays of 9Be(5/2-)

NUCLEAR STRUCTURE 9Be; calculated and analyzed α+5He and n+8Be widths for the 5/2- state at 2.43 MeV in 9Be. Discussed three-body decay mechanisms. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.014306
Citations: PlumX Metrics

2013FO05      Phys.Rev. C 87, 014316 (2013)

H.T.Fortune, R.Sherr

Excited states of 19Mg

NUCLEAR STRUCTURE 19Mg; calculated levels, J, π using a potential model and mirror symmetry arguments. Comparison with levels in 19N, and with experimental data. Systematics of T=2 states in 20O and 20Mg, and T=5/2 states in 19Mg and 19N.

doi: 10.1103/PhysRevC.87.014316
Citations: PlumX Metrics

2013FO07      Nucl.Phys. A898, 78 (2013)

H.T.Fortune, R.Sherr

Update on 9B(1/2+)

NUCLEAR REACTIONS 9Be(6Li, 6He), E=32 MeV; reanalyzed earlier σ(E). 9B deduced (1/2)+ energy, J, π. Corrected results of earlier papers.

doi: 10.1016/j.nuclphysa.2012.12.120
Citations: PlumX Metrics

2013FO09      Eur.Phys.J. A 49, 26 (2013)

H.T.Fortune, R.Sherr

Matter radii of 17-24O

NUCLEAR STRUCTURE 17,18,19,20,21,22,23,24O;calculated nuclear matter radius, radius of valence neutron orbit using potential model with binding energies taken from experiment. Radii compared with data and other calculations.

doi: 10.1140/epja/i2013-13026-7
Citations: PlumX Metrics

2013FO10      J.Phys.(London) G40, 055102 (2013)

H.T.Fortune, R.Sherr

Update on 12O(g.s.) width for simultaneous 2p decay

RADIOACTIVITY 12O(2p); analyzed available data. 12O; deduced decay width, mass excess. Comparison with available data.

doi: 10.1088/0954-3899/40/5/055102
Citations: PlumX Metrics

2013FO12      Phys.Rev. C 87, 044315 (2013)

H.T.Fortune, R.Sherr

Mass of 18Mg(g.s.)

NUCLEAR STRUCTURE 18Mg; calculated binding energy of the ground state, Ep, E2p, 18C - 18Mg energy difference. Potential model with spectroscopic factors from combination of weak coupling and shell-model calculation.

doi: 10.1103/PhysRevC.87.044315
Citations: PlumX Metrics

2013FO16      Phys.Rev. C 87, 054315 (2013)

H.T.Fortune, R.Sherr

Comparison of 1n and 2n prescriptions for matter radii

NUCLEAR STRUCTURE 17N; calculated ground state matter radius with 16N states (1n approach), and 15N (2n approach) used as cores. 16N; calculated matter radii for four states with 15N g.s. core. Shell model calculations.

doi: 10.1103/PhysRevC.87.054315
Citations: PlumX Metrics

2013FO18      Phys.Rev. C 87, 057308 (2013)

H.T.Fortune, R.Sherr

Connection between separation energy and matter radius: Application to 34Na

NUCLEAR STRUCTURE 31,32,33Na; deduced matter radii from relationship between matter radius and S(n) values. 34Na; deduced matter radius for 2p and 1f configurations as a function of S(n).

doi: 10.1103/PhysRevC.87.057308
Citations: PlumX Metrics

2013FO26      Phys.Rev. C 88, 034326 (2013)

H.T.Fortune, R.Sherr

Potential-model estimate of the mass of 11O(g.s.)

NUCLEAR STRUCTURE 11O; calculated ground state energy using a simple potential model, mirror symmetry and known 11Li structure; comparison with isobaric multiplet mass equation (IMME) result.

doi: 10.1103/PhysRevC.88.034326
Citations: PlumX Metrics

2013SH19      Phys.Rev. C 87, 054333 (2013)

R.Sherr, H.T.Fortune

Energies within the A=10 isospin quintet

NUCLEAR STRUCTURE 10Be, 10B, 10C, 10N; calculated levels, J, π of T=2 states, and mass excess using a potential model. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.054333
Citations: PlumX Metrics

2012FO04      Phys.Rev. C 85, 027303 (2012)

H.T.Fortune, R.Sherr

Binding energy of 22C

NUCLEAR STRUCTURE 22C; analyzed S(2n) binding energy using a recent experimental value of matter radius Rm. Comparison with several other calculations.

doi: 10.1103/PhysRevC.85.027303
Citations: PlumX Metrics

2012FO05      Phys.Rev. C 85, 027305 (2012)

H.T.Fortune, R.Sherr

Widths and spectroscopic factors in 21O

NUCLEAR REACTIONS 2H(20O, p)21O, E not given; analyzed levels, J, π, single-particle widths, branching ratios, spectroscopic factors using relationship between width and spectroscopic factor.

doi: 10.1103/PhysRevC.85.027305
Citations: PlumX Metrics

2012FO10      Phys.Rev. C 85, 051302 (2012)

H.T.Fortune, R.Sherr

Reexamining 18Na and 19Mg

NUCLEAR STRUCTURE 18Na; calculated proton resonance energies, excitation energies, J, π, widths and spectroscopic factors. Comparison with experimental values. 19Mg; deduced mass excess of ground-state using data for core states in 18Na. Shell-model calculations.

doi: 10.1103/PhysRevC.85.051302
Citations: PlumX Metrics

2012FO11      Phys.Rev. C 85, 051303 (2012)

H.T.Fortune, R.Sherr

Consistent description of 11Be and 12Be and of the 11Be(d, p)12Be reaction

NUCLEAR STRUCTURE 11,12Be; analyzed shell-model wave functions and their validity from spectroscopic factors obtained in experimental results from various reactions.

NUCLEAR REACTIONS 11Be(d, p)12Be; analyzed spectroscopic factors from various experiments and compared with shell-model calculations. Discussed discrepancy in spectroscopic factor obtained from 11Be(d, p) reaction in inverse kinematics.

doi: 10.1103/PhysRevC.85.051303
Citations: PlumX Metrics

2012FO13      Phys.Rev. C 85, 054304 (2012)

H.T.Fortune, R.Sherr, B.A.Brown

Lowest 2+, T=2 states in 20Mg and 20F

NUCLEAR STRUCTURE 20Mg, 20F; calculated energies of ground and 2+ states in 20Mg and lowest T=2, 2+ in 20F in a potential model using shell-model spectroscopic factors for 20O to 19O. Comparison with experimental data. Disagreement of the energy of 2+, T=2 state in 20F with the IMME.

doi: 10.1103/PhysRevC.85.054304
Citations: PlumX Metrics

2012FO18      Eur.Phys.J. A 48, 103 (2012)

H.T.Fortune, R.Sherr

Matter radii and wave function admixtures in 2n halo nuclei

NUCLEAR STRUCTURE 11Li, 14Be, 17,19B halo nuclei; calculated nuclear matter radius, core radius, s2 parentage, 19B 2n-binding energy using potential model. Compared with data; 11Li also with other calculations.

doi: 10.1140/epja/i2012-12103-9
Citations: PlumX Metrics

2012FO22      Phys.Rev. C 86, 034301 (2012)

H.T.Fortune, R.Sherr

Predictions for the first two positive-parity states of 13F

NUCLEAR STRUCTURE 13F; calculated levels, J, π, widths using a potential model, structure information for ground states of 12O and 12Be, and mirror states in 13Be states.

doi: 10.1103/PhysRevC.86.034301
Citations: PlumX Metrics

2012FO27      Phys.Rev. C 86, 064322 (2012)

H.T.Fortune, R.Sherr

Matter radii of 29-35Mg

NUCLEAR STRUCTURE 29,30,31,32,33,34,35Mg; calculated matter radii for ground states for different configurations. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.064322
Citations: PlumX Metrics

2011FO04      Phys.Rev. C 83, 044313 (2011)

H.T.Fortune, R.Sherr

Structure of 2+, T = 2 states in A = 12 nuclei

NUCLEAR STRUCTURE 12Be, 12O; calculated level energies, wavefunctions, and widths for decay of 12O 2+ state to 11N using local single-particle energies and global two-body residual interaction matrix elements. Mirror states.

NUCLEAR REACTIONS 11Be(d, p)12Be; calculated Spectroscopic factors. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.044313
Citations: PlumX Metrics

2011FO05      Phys.Rev. C 83, 057301 (2011)

H.T.Fortune, R.Sherr

Update on energy and width of 19Mg(g.s.)

NUCLEAR STRUCTURE 19Mg; analyzed energy and width of the ground state from its 2p decay mode using shell-model.

doi: 10.1103/PhysRevC.83.057301
Citations: PlumX Metrics

2011FO07      Phys.Rev. C 83, 054314 (2011)

H.T.Fortune, R.Sherr

Neutron widths and configuration mixing in 11Be

NUCLEAR STRUCTURE 11Be; analyzed J, π, neutron widths; deduced J, π, configuration mixings.

doi: 10.1103/PhysRevC.83.054314
Citations: PlumX Metrics

2011FO10      Phys.Rev. C 84, 024304 (2011)

H.T.Fortune, R.Sherr

(sd)2 states or superclusters in 10Be

NUCLEAR STRUCTURE 10Be; analyzed energies, α-widths, spectroscopic factors, cluster states and decay to 6He+α and 9Be+n. Comparison with level systematics of 10B, 12Be, 14,16C. Woods-Saxon potential. Discussed (sd)2 states and superclusters.

doi: 10.1103/PhysRevC.84.024304
Citations: PlumX Metrics

2011FO12      Phys.Rev. C 84, 047301 (2011)

H.T.Fortune, R.Sherr

Update on the 18Ne 7.37-MeV state and its mirror in 18O

NUCLEAR STRUCTURE 18Ne; analyzed J, π, configuration of 7.37 MeV state in connection with possible mirror state in 18O at 7.796 MeV.

doi: 10.1103/PhysRevC.84.047301
Citations: PlumX Metrics

2011FO18      Eur.Phys.J. A 47, 154 (2011)

H.T.Fortune, R.Sherr

New calculations of matter radii for neutron-rich C nuclei

NUCLEAR STRUCTURE 14,15,16,17,18,19,20C; calculated nuclear matter radii using updated information on nuclear structure. Results compared with data and other calculations.

doi: 10.1140/epja/i2011-11154-8
Citations: PlumX Metrics

2011SH17      Phys.Lett. B 699, 281 (2011)

R.Sherr, H.T.Fortune

Low-lying resonances in 14F and 14B

NUCLEAR STRUCTURE 14F, 14B; calculated energies, widths, spectroscopic factors of low-lying resonances. Simple potential model, comparison with experimental data.

doi: 10.1016/j.physletb.2011.04.018
Citations: PlumX Metrics

2010FO06      Phys.Rev. C 82, 027310 (2010)

H.T.Fortune, R.Sherr

Coulomb energies in 16Ne and low-lying levels of 17Na

NUCLEAR STRUCTURE 16Ne, 17Na; calculated levels, J, π, widths, and spectroscopic factors in core plus two-nucleon space using experimental 16C energies and known wave functions.

doi: 10.1103/PhysRevC.82.027310
Citations: PlumX Metrics

2010FO07      Phys.Rev. C 82, 034312 (2010)

H.T.Fortune, A.Lacaze, R.Sherr

Update on α-particle and nucleon widths in 19F and 19Ne

NUCLEAR REACTIONS 15N(6Li, d)19F, E=22 MeV; 15N(7Li, t)19F, E=15, 20, 28 MeV; analyzed α widths. 19F, 19Ne; analyzed widths; deduced updated α widths and level half-lives.

doi: 10.1103/PhysRevC.82.034312
Citations: PlumX Metrics

2010FO08      Phys.Rev. C 82, 034325 (2010)

H.T.Fortune, R.Sherr

Energy and width of the excited 0+ state in 12O

NUCLEAR STRUCTURE 12O; calculated and analyzed energy and width of the excited 0+ state using shell model. Reviewed existing experimental data.

doi: 10.1103/PhysRevC.82.034325
Citations: PlumX Metrics

2010FO11      Phys.Rev. C 82, 064302 (2010)

H.T.Fortune, R.Sherr

Neutron decays of 13Be* to the 02+ state of 12Be

NUCLEAR REACTIONS 1H(14Be, 13Be), E not given; analyzed neutron decay of 13Be resonances to 12Be+n. 13Be; estimated energies, widths and spectroscopic factors of 1/2- and 5/2+ resonances; deduced decay to excited states in 12Be.

doi: 10.1103/PhysRevC.82.064302
Citations: PlumX Metrics

2007FO07      Phys.Rev. C 76, 014313 (2007)

H.T.Fortune, R.Sherr

Two-proton decay energy and width of 19Mg(g.s.)

RADIOACTIVITY 19Mg(2p); calculated two proton separation energy using the shell model.

doi: 10.1103/PhysRevC.76.014313
Citations: PlumX Metrics

2006FO03      Phys.Rev. C 73, 024302 (2006)

H.T.Fortune, R.Sherr

Proton and alpha spectroscopic factors for states at 6.4-7.5 MeV in 19Ne

NUCLEAR STRUCTURE 19Ne; calculated levels single-particle alpha and proton widths; deduced spectroscopic factors, J, π.

doi: 10.1103/PhysRevC.73.024302
Citations: PlumX Metrics

2006FO07      Phys.Rev. C 73, 064302 (2006)

H.T.Fortune, R.Sherr

Constraints on energy of 9B(1/2+) and 10C(02+)

NUCLEAR STRUCTURE 10Be, 10B; analyzed level energies, configurations. 9B, 10C; deduced constraints on excited states energies.

doi: 10.1103/PhysRevC.73.064302
Citations: PlumX Metrics

2006FO08      Phys.Rev. C 73, 064310 (2006)

H.T.Fortune, R.Sherr, B.A.Brown

Coulomb energies in 17Ne and the ground state mass of 18Na

NUCLEAR STRUCTURE 17N, 17Ne; calculated Coulomb energies. 18Na; calculated mass excess.

doi: 10.1103/PhysRevC.73.064310
Citations: PlumX Metrics

2006FO11      Phys.Rev. C 74, 024301 (2006)

H.T.Fortune, R.Sherr

Excited 0+, T = 2 states in 12Be, 12C, and 12O

NUCLEAR STRUCTURE 12Be, 12O; calculated 0+ states energies, energy splitting, wave functions.

NUCLEAR REACTIONS 10Be(t, p), 14C(p, t), E not given; calculated cross-section ratios.

doi: 10.1103/PhysRevC.74.024301
Citations: PlumX Metrics

2006SH10      Phys.Rev. C 73, 037310 (2006)


Energies of analog levels

NUCLEAR STRUCTURE 13C, 13N; calculated Coulomb displacement energy. Woods-Saxon potential, different prescriptions for resonant energy compared.

doi: 10.1103/PhysRevC.73.037310
Citations: PlumX Metrics

2005FO10      Phys.Rev. C 72, 024319 (2005)

H.T.Fortune, R.Sherr

Energy shifts and configuration mixing in the A = 15 quartet

NUCLEAR STRUCTURE 15N, 15O, 15F; calculated level energies, widths, configuration mixing features.

doi: 10.1103/PhysRevC.72.024319
Citations: PlumX Metrics

2005FO13      Phys.Rev. C 72, 034304 (2005)

H.T.Fortune, R.Sherr

18Na: Mass excess and low-lying states

NUCLEAR STRUCTURE 19O, 18N, 19Na; analyzed levels, J, π, mass excesses. 18Na analyzed proton decay data; deduced mass excess, excited state energy. Weak coupling and simple potential-model calculations.

doi: 10.1103/PhysRevC.72.034304
Citations: PlumX Metrics

2004SH45      Phys.Rev. C 70, 054312 (2004)

R.Sherr, H.T.Fortune

Low-lying levels of 9B

NUCLEAR STRUCTURE 9B; calculated level energies, widths. Comparison with data.

doi: 10.1103/PhysRevC.70.054312
Citations: PlumX Metrics

2003FO11      Phys.Rev. C 68, 024301 (2003)

H.T.Fortune, R.Sherr

Configuration of 13B(g.s.)

NUCLEAR STRUCTURE 14Be, 13,14B; analyzed β-delayed neutron decay data; deduced ground-state configuration features.

doi: 10.1103/PhysRevC.68.024301
Citations: PlumX Metrics

2003FO13      Phys.Rev. C 68, 034307 (2003)

H.T.Fortune, R.Sherr

Properties of states at 7-8 MeV in 18Ne

NUCLEAR STRUCTURE 18Ne; calculated level energies, widths. Comparison with data. Astrophysical implications discussed.

doi: 10.1103/PhysRevC.68.034307
Citations: PlumX Metrics

2003FO14      Phys.Rev. C 68, 034309 (2003); Comment Phys.Rev. C 71, 059801 (2005)

H.T.Fortune, R.Sherr

Width of 12O(g.s.)

RADIOACTIVITY 12O(p), (2p); calculated widths for sequential and simultaneous two-proton decay.

doi: 10.1103/PhysRevC.68.034309
Citations: PlumX Metrics

2003FO16      Phys.Rev. C 68, 035802 (2003)

H.T.Fortune, R.Sherr, B.A.Brown

22Mg and the 21Na(p, γ) reaction rate

NUCLEAR STRUCTURE 22Mg, 22Na; calculated levels, J, π, spectroscopic factors, mirror relationships. Shell model and Coulomb-energy calculations, implications for 21Na+p reaction rate discussed.

doi: 10.1103/PhysRevC.68.035802
Citations: PlumX Metrics

2002FO09      Phys.Rev. C65, 067301 (2002)

H.T.Fortune, R.Sherr

2p3/2 Strength in 40, 41Sc and 39Ca(p, γ) Reaction Rate

NUCLEAR STRUCTURE 40,41Ca, 40,41Sc; calculated level energies, spectroscopic factors, configurations. 40Sc levels calculated proton widths. Implication for astrophysical reaction rate discussed.

doi: 10.1103/PhysRevC.65.067301
Citations: PlumX Metrics

2002FO11      Phys.Rev. C66, 017301 (2002)

H.T.Fortune, R.Sherr

Structure of 16Ne Ground State

NUCLEAR STRUCTURE 16N, 16O, 16F, 16Ne; analyzed Coulomb energies; deduced ground-state configurations. 8C, 12O, 16,17,18Ne, 20Mg; analyzed ground-state configurations, mass dependence.

doi: 10.1103/PhysRevC.66.017301
Citations: PlumX Metrics

2001FO05      Phys.Lett. 503B, 70 (2001)

H.T.Fortune, R.Sherr

Structure of 17Ne Ground State

NUCLEAR STRUCTURE 17Ne; analyzed data; deduced ground-state configuration.

doi: 10.1016/S0370-2693(00)01371-X
Citations: PlumX Metrics

2001SH39      Phys.Rev. C64, 064307 (2001)

R.Sherr, H.T.Fortune

Energies and Widths of T = 3/2 States in A = 11 Nuclei

NUCLEAR STRUCTURE 11B, 11C, 11N; calculated T=3/2 states energies, widths. Isobaric multiplet mass equation, comparison with data.

doi: 10.1103/PhysRevC.64.064307
Citations: PlumX Metrics

2000FO01      Phys.Rev. C61, 024313 (2000)

H.T.Fortune, R.Sherr

Properties of 19Ne(7.07 MeV) and Its Mirror in 19F

NUCLEAR STRUCTURE 19Ne; analyzed l=0 resonance energy, width, related data. 19F; calculated mirror resonance energy.

doi: 10.1103/PhysRevC.61.024313
Citations: PlumX Metrics

2000FO08      Phys.Rev. C61, 057303 (2000)

H.T.Fortune, R.Sherr, B.A.Brown

ωγ for 19Ne(p, γ)20Na(2.64 MeV)

NUCLEAR REACTIONS 19Ne(p, γ), E not given; analyzed data, isospin nonconserving effects; deduced resonance features. Astrophysical implications discussed.

NUCLEAR STRUCTURE 20F, 20Na; calculated resonance T1/2, spectroscopic factors. Isospin-nonconserving interaction parameters.

doi: 10.1103/PhysRevC.61.057303
Citations: PlumX Metrics

2000FO19      Phys.Rev.Lett. 84, 1635 (2000)

H.T.Fortune, R.Sherr

Comment on "Stellar Reactions with Short-Lived Nuclei: 17F(p, α)14O"

NUCLEAR REACTIONS 1H(17F, α), E not given; analyzed available data. 18,19Ne, 18O; deduced energy levels, J, π, resonances.

doi: 10.1103/PhysRevLett.84.1635
Citations: PlumX Metrics

1999SH32      Eur.Phys.J. A 5, 371 (1999)

R.Sherr, H.T.Fortune, B.A.Brown

No Tetra-Proton Cluster in 20Mg

NUCLEAR STRUCTURE 20O, 20F, 20Ne, 20Na, 20Mg; calculated excitation energies of lowest 0+ state. 20O, 20Mg; calculated matter radii. 20Mg deduced no support for tetra-proton cluster.

doi: 10.1007/s100500050299
Citations: PlumX Metrics

1999SH43      Phys.Rev. C60, 064323 (1999)

R.Sherr, H.T.Fortune

Structure of 12Be and 12O Ground States

NUCLEAR STRUCTURE 12B, 12C, 12O; calculated level energies, ground-state features. 12Be, 12O deduced ground-state configurations. Shell model, comparisons with data.

doi: 10.1103/PhysRevC.60.064323
Citations: PlumX Metrics

1998SH35      Phys.Rev. C58, 3292 (1998)

R.Sherr, H.T.Fortune

Coulomb Energies in 18Ne

NUCLEAR STRUCTURE 18O, 18Ne; calculated levels excitation energies. 18Ne deduced degenerate level.

doi: 10.1103/PhysRevC.58.3292
Citations: PlumX Metrics

1996BR04      Nucl.Phys. A597, 66 (1996)

B.A.Brown, A.Csoto, R.Sherr

Coulomb Displacement Energy and the Low-Energy Astrophysical S17 Factor for the 7Be(p, γ)8B Reaction

NUCLEAR REACTIONS, ICPND 7Be(p, γ), E=low; calculated astrophysical S-factor. Shell model, solar neutrinos.

NUCLEAR STRUCTURE 8B; calculated quadrupole moment. Shell model.

doi: 10.1016/0375-9474(95)00417-3
Citations: PlumX Metrics

1996SH13      Phys.Rev. C54, 1177 (1996)


Simple Model of Neutron ' Halo Nuclei '

NUCLEAR STRUCTURE 4,6,8He, 6,7,8,9,11Li, 7,9,10,11,12,14Be, 10,11,12,13,14,15,17B, 12,13,14,15,16,17,18,19,20,22C; calculated rms matter radii. Single-particle potential model approach.

doi: 10.1103/PhysRevC.54.1177
Citations: PlumX Metrics

1993BR12      Phys.Rev. C48, 1456 (1993)

B.A.Brown, A.E.Champagne, H.T.Fortune, R.Sherr

Nature of the 20Na 2646-keV Level and the Stellar Reaction Rate for 19Ne(p, γ)20Na

NUCLEAR STRUCTURE 20F, 20Na; calculated M1 decay associated B(λ), T1/2. 20Na levels deduced J, π, Γp, Γγ, γ-strength function. All data relevant to this included in analysis.

NUCLEAR REACTIONS 19Ne(p, γ), E=stellar; calculated reaction rate. All data relevant to this included in analysis.

doi: 10.1103/PhysRevC.48.1456
Citations: PlumX Metrics

1993CH18      Nucl.Phys. A556, 123 (1993)

A.E.Champagne, B.A.Brown, R.Sherr

The 26Al(p, γ)27Si Reaction at Low Stellar Temperature

NUCLEAR STRUCTURE 27Si, 27Al; calculated levels. 27Si deduced resonances near 26Al+p threshold.

NUCLEAR REACTIONS 26Al(p, γ), E ≈ threshold; calculated reaction rate vs temperature. Shell model.

doi: 10.1016/0375-9474(93)90242-P
Citations: PlumX Metrics

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

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

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

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

doi: 10.1103/PhysRevC.46.504
Citations: PlumX Metrics

1988BU18      Phys.Rev. C38, 2078 (1988)

M.Burlein, H.T.Fortune, P.H.Kutt, R.Gilman, R.Sherr, J.D.Brown

Energies and Widths of States in 9B

NUCLEAR REACTIONS 9Be(6Li, 6He), E=32 MeV; measured σ(θ, E(6He)). 9B deduced levels, Γ.

doi: 10.1103/PhysRevC.38.2078
Citations: PlumX Metrics

1988CA22      Phys.Rev. C38, 2550 (1988)

M.Carchidi, M.Burlein, H.T.Fortune, G.P.Gilfoyle, R.Gilman, J.Gorres, P.Kutt, S.Saini, J.W.Sweet, R.T.Kouzes, R.Sherr

70Zn(p, t)68Zn Reaction at E(p) = 35 MeV

NUCLEAR REACTIONS 70Zn(p, t), E=35 MeV; measured σ(Et), σ(θ). 68Zn deduced levels, J, π, L.

doi: 10.1103/PhysRevC.38.2550
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1985SH24      Phys.Rev. C32, 1809 (1985)

R.Sherr, G.Bertsch

Coulomb Energy Systematics and the Missing J(π) = (1/2)+ State in 9B

NUCLEAR STRUCTURE 13,11C, 11B, 9B, 9Be, 13,15N, 15,17O, 17F; calculated Coulomb displacement energies. 9B deduced level Γ.

doi: 10.1103/PhysRevC.32.1809
Citations: PlumX Metrics

1984SH20      Phys.Lett. 146B, 25 (1984)

R.Sherr, R.T.Kouzes, B.A.Brown, H.Nann

Excitation of High-Spin States in 49Ti by the (p, π-) and (d, α) Reactions

NUCLEAR REACTIONS 51V(d, α), E=28 MeV; measured σ(Eα), σ(θ). 49Ti deduced levels, L-transfer, J, π. Microscopic DWBA analysis, (p, π-) data input.

doi: 10.1016/0370-2693(84)90635-X
Citations: PlumX Metrics

1979BR10      Nucl.Phys. A322, 61 (1979)

B.A.Brown, R.Sherr

Charge-Dependent Two-Body Interactions Deduced from Displacement Energies in the 1f7/2 Shell

NUCLEAR STRUCTURE 40,41,42,43,44,46,48Ca, 41,45Sc, 46,47,48,49,50Ti, 51V, 50,52Cr, 54Fe; calculated rms charge radii. Harmonic oscillator, Woods-Saxon wave functions 1f7/2 shell model.

COMPILATION A=21-25; Sc-Ca, Ti-Sc, V-Ti, Ca-V, Mn-Cr; compiled, revised expexperimental displacement energies; deduced charge-dependent two-body interations.

doi: 10.1016/0375-9474(79)90333-6
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1978KO27      Nucl.Phys. A309, 329 (1978)

R.T.Kouzes, P.Kutt, D.Mueller, R.Sherr

Experimental Displacement Energies of Isobaric Analog States in the 1f7/2 Shell

NUCLEAR REACTIONS 46,48,50Ti, 52Cr, 54Fe(p, t), 46,50Ti(p, d), 46,48,50Ti, 52Cr, 54Fe(p, 3He), E ≈ 42-46 MeV; measured particle spectra; deduced Q. 44,46,48Sc, 44,45,46,48,49Ti, 50V, 50Cr, 52Mn, 52Fe deduced analog states. 44,46,48Sc-44,46,48Ca, 44,45,46,48,49Ti-44,45,46,48,49Sc, 50V-50Ti, 50Cr-50V, 52Mn-52Cr, 52Fe-52Mn deduced displacement energies of IAS in 1f7/2 shell.

doi: 10.1016/0375-9474(78)90485-2
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1977KO14      Nucl.Phys. A286, 253 (1977)

R.Kouzes, J.Lind, W.H.Moore, R.G.H.Robertson, R.Sherr

Investigation of the (3He, 8He) Reaction on 58Ni and 64Ni

NUCLEAR REACTIONS 58,64Ni(3He, 8He), E=75.3 MeV; measured σ.

doi: 10.1016/0375-9474(77)90406-7
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1977SH13      Phys.Rev. C16, 1159 (1977)


Charge-Dependent and A-Dependent Effects in Isotope Shifts of Coulomb Displacement Energies

NUCLEAR STRUCTURE 33,34,35,36Cl, 33,34,35,36S, 37Cl, 34,35,36,37,38Ar, 35,36,37,38,39K, 36,37,38,39,41,42,43,44,45,46,47,48Ca, 41,42,43,44,45,46,47,48,49Sc, 42,43,44,45,46,47,48,49,50Ti, 45,46,47,48,49,50,51V, 46,47,48,49,51,52,50Cr, 49,50,51,52,53Mn, 50,51,52,53,54Fe, 53,54,55Co, 54,55Ni, 17,18,19,20O, 17,18,19,20,21F, 18,19,20,21,22,23,24Ne, 19,20,21,22,23,24,25Na, 20,21,22,23,24,25,26Mg, 23,24,25,26,27Al, 24,25,26,27Si; calculated Coulomb displacement energies.

doi: 10.1103/PhysRevC.16.1159
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1976DE24      Nucl.Phys. A265, 220 (1976)

R.M.del Vecchio, R.T.Kouzes, R.Sherr

Experimental Study of (f7/2)7+ States in s-d Shell Nuclei

NUCLEAR REACTIONS 24,26Mg, 28,30Si(α, d), E=40 MeV; 32,34S, 42Ca(α, d), E=34.8 MeV; 36,38,40Ar(α, d), E=34 MeV; 24Mg, 28Si, 32S(3He, p), E=24.5 MeV; measured σ(θ). 26,28Al, 30,32P, 34,36Cl, 38,40,42K, 44Sc deduced levels, L, J, π. DWBA analysis. Resolution 40-110 keV. Enriched targets.

doi: 10.1016/0375-9474(76)90351-1
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1975SH10      Phys.Lett. 56B, 212 (1975)

R.Sherr, I.Talmi

Systematic Effects of Charge Independence Breaking on Energies of Analog States

NUCLEAR STRUCTURE 33,34,35,36Cl, 34,35,36,37Ar, 35,36,37,38K, 36,37,38,39Ca; calculated IAS energy differences.

doi: 10.1016/0370-2693(75)90377-9
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1975SH20      Phys.Rev. C12, 1671 (1975)

R.Sherr, G.Bertsch

Coulomb Displacement Energies of Excited States

NUCLEAR STRUCTURE A=13-45; calculated coulomb displacement energies of particle-hole states. Bansal-French-Zamick model.

doi: 10.1103/PhysRevC.12.1671
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1974SH21      Phys.Lett. 52B, 401 (1974)

R.Sherr, R.Kouzes, R.Del Vecchio

Systematics of Energies of Particle-Hole States in the 2s-1d and 1f7/2 Shells

NUCLEAR STRUCTURE A=40-55; analyzed systematics of particle-hole states.

doi: 10.1016/0370-2693(74)90110-5
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1973DA02      Phys.Rev. C7, 150 (1973)

W.W.Daehnick, R.Sherr

Investigation of 46K and 46Ca with (p, 3He) and (p, t) Reactions at 42 MeV

NUCLEAR REACTIONS 48Ca(p, t), (p, 3He), E=41.65 MeV; measured σ(θ). 46K, 46Ca deduced levels, J, π, L.

doi: 10.1103/PhysRevC.7.150
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1971SH16      Ann.Phys.(N.Y.) 66, 548 (1971)

R.Sherr, T.S.Bhatia, D.Cline, J.J.Schwartz

Measurements and Models of the Level Structure of 42Sc

NUCLEAR REACTIONS 42Ca(3He, t), E=26 MeV; measured σ(Et, θ). 42Sc deduced levels, J, π, T.

doi: 10.1016/0003-4916(71)90070-4
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1970DZ01      Nucl.Phys. A142, 488 (1970)

T.G.Dzubay, R.Sherr, F.D.Becchetti, Jr., D.Dehnhard

Isospin Mixing for Bound Analog States in 56Co and 58Co

NUCLEAR REACTIONS 54,56,58Fe(3He, t), E=24.6 MeV; measured σ(Et, θ). 56,58Co deduced analog states, J, π, isospin mixing.

doi: 10.1016/0375-9474(70)90807-9
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1970HI06      Phys.Rev.Lett. 25, 829 (1970)

R.A.Hinrichs, R.Sherr, G.M.Crawley, I.Proctor

Anomalous L = 1 Shapes of Angular Distribution for (3He, t) Transitions to 0+ Antianalog States in 64,66Ga and 40K

NUCLEAR REACTIONS 40Ar, 64,66Zn(3He, t), E=35 MeV; measured σ(θ). 40K, 64,66Ga deduced transitions, antianalog states.

doi: 10.1103/PhysRevLett.25.829
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1967SC28      Phys.Rev.Letters 19, 1482 (1967);Erratum Phys.Rev.Letters 20, 175 (1968)

J.J.Schwartz, D.Cline, H.E.Gove, R.Sherr, T.S.Bhatia, R.H.Siemssen

Complete (f7/2)2 Spectrum of Sc42

NUCLEAR STRUCTURE 42Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.19.1482
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1967SH03      Phys.Letters 24B, 321 (1967)


Coulomb Displacement Energies in the 1f7/2 Shell

doi: 10.1016/0370-2693(67)90232-8
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1966SH02      Phys.Letters 20, 392 (1966)

R.Sherr, A.G.Blair, D.D.Armstrong

Isotope Shift in Coulomb Displacement Energy

NUCLEAR REACTIONS 46,48,50Ti, 50,52,54Cr, 54,56,58Fe, 58,60,62,64Ni(3He, t), E=22 MeV; measured σ(Et). 46,48,50V, 50,52,54Mn, 54,56,58Co, 58,60,62,64Cu levels deduced isobaric analogs. Ti-V, Cr-Mn, Fe-Co, Ni-Cu isotopes deduced Coulomb displacement energies.

doi: 10.1016/0031-9163(66)90756-6
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1965SH06      Phys.Rev. 139, B1272 (1965)

R.Sherr, B.F.Bayman, E.Rost, M.E.Rickey, C.G.Hoot

Excitation of Isobaric Analog States in Medium-Weight Nuclei by the (p, d) Reaction at 28 MeV

NUCLEAR STRUCTURE 61Ni, 55Fe, 52Cr, 51Cr, 53Fe, 57Fe, 57Ni, 59Ni, 49Cr, 49Ti, 47Ti; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B1272
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1964DA03      Phys.Rev. 133, B934 (1964)

W.W.Daehnick, R.Sherr

Energy Dependence of Elastic and Inelastic Scattering from C12 for Protons Between 14 and 19 MeV

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

doi: 10.1103/PhysRev.133.B934
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1964NO02      Bull.Am.Phys.Soc. 9, No.4, 440, FA9 (1964)

J.A.Nolen, Jr., R.Sherr

27Al(p, α)24Mg and 25Mg(p, d)24Mg Reactions

NUCLEAR STRUCTURE 24Mg; measured not abstracted; deduced nuclear properties.

1964SH08      Bull.Am.Phys.Soc. 9, No.4, 458, GA13 (1964)

R.Sherr, M.E.Rickey, C.G.Hoot

Excitation of Analog States in the (p, d) Reaction. I. Angular Distributions and Coulomb Energies

NUCLEAR STRUCTURE 57Ni, 57Fe, 59Ni, 61Ni, 49Ti, 47Ti, 53Fe, 51Cr, 55Fe; measured not abstracted; deduced nuclear properties.

1964SH12      Phys.Rev.Letters 12, 420 (1964)

R.Sherr, E.Rost, M.E.Rickey

J Dependence of the Angular Distributions from (p, d) Reaction at 28 Mev

NUCLEAR STRUCTURE 59Ni, 57Fe, 57Ni, 55Fe, 61Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.12.420
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1962SH29      Proc.Conf.Direct Interactions and Nucl.Reaction Mechanisms, Padua, Italy, E.Clementel, C.Villi, Eds., Gordon and Breach, New York, p.1025 (1962)


(p, α) Reactions in the f7/2 Proton Shell at 18 MeV

NUCLEAR REACTIONS 45Sc, 51V, 55Mn, 59Co, 48Ti, 54,56,58Fe, 58,60Ni(p, α), E=17-18 MeV; measured σ(Eα, θ). 42Ca, 48Ti, 52Cr, 56Fe, 45Sc, 51,53,55Mn, 55,57Co deduced levels, S.

1961BA41      Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press, New York, p.553 (1961)

B.F.Bayman, F.P.Brady, R.Sherr

(p, α) Reaction and Seniority in the f7/2 Shell

NUCLEAR STRUCTURE 45Sc, 51V, 48Ti, 58Ni, 59Co, 60Ni, 55Mn, 56Fe, 53Mn; measured not abstracted; deduced nuclear properties.

1961DA03      Bull.Am.Phys.Soc. 6, No.1, 25, I5 (1961)

W.Daehnick, M.Garrell, R.Wood, R.Sherr

Energy Dependence of the Differential Cross Section for C12(p, p)C12

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

1961SH20      Phys.Rev. 124, 1928 (1961)

R.Sherr, F.P.Brady

Spectra of (p, d) and (p, p') Reactions and the Evaporation Model

NUCLEAR STRUCTURE 53Mn, 55Co, 56Fe, 57Co, 48Ti, 100Ru; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.124.1928
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1960BR08      Bull.Am.Phys.Soc. 5, No.4, 249, I10 (1960)

F.P.Brady, R.Sherr

Level Densities in Medium Heavy Nuclei from (p, α) Reactions

NUCLEAR STRUCTURE 56Fe, 55Co, 53Mn, 57Co, 48Ti, 100Ru; measured not abstracted; deduced nuclear properties.

1960DA06      Bull.Am.Phys.Soc. 5, No.4, 246, HA6 (1960)

W.W.Daehnick, R.Sherr, M.K.Banerjee

N14(p, n)O14 Differential Cross Section at 14.8 MeV

NUCLEAR STRUCTURE 14O; measured not abstracted; deduced nuclear properties.

1960HI01      Bull.Am.Phys.Soc. 5, No.4, 249, I11 (1960)

H.Hill, R.Sherr

Ni(p, α) and Ni(p, p') Reactions at Small Angles with 17.6-MeV Protons

NUCLEAR STRUCTURE 57Co, 60Ni, 58Ni, 55Co; measured not abstracted; deduced nuclear properties.

1959SU58      Bull.Am.Phys.Soc. 4, No.4, 278, U9 (1959)

D.C.Sutton, H.A.Hill, R.Sherr

Decay of Cu58 and Isomeric States in Co54 and Mn50

1958YO14      Bull.Am.Phys.Soc. 3, No.3, 200, P13 (1958)

H.Yoshiki, R.Sherr

Angular Correlation in the Inelastic Scattering of Protons by Mg24

1957BL77      Bull.Am.Phys.Soc. 2, No.6, 303, E1 (1957)

W.Blanpied, R.Sherr

Proton-Induced Reactions in Rhodium-103

1955HO68      Phys.Rev. 100, 1409 (1955)

W.F.Hornyak, R.Sherr

Inelastic Scattering of 19-Mev Protons by O16

NUCLEAR REACTIONS 16O(p, p'), E=19 MeV; measured reaction products, Ep, Ip; deduced energy levels, J, π, σ(θ).

doi: 10.1103/PhysRev.100.1409
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1955SH84      Phys.Rev. 100, 945 (1955)

R.Sherr, J.B.Gerhart, H.Horie, W.F.Hornyak

Decay Rates of C14, N14*, and O14

doi: 10.1103/PhysRev.100.945
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1954GE61      Phys.Rev. 94, 917 (1954)

J.B.Gerhart, B.C.Carlson, R.Sherr

Annihilation of Positrons in Flight

doi: 10.1103/PhysRev.94.917
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1954LI48      Phys.Rev. 96, 389 (1954)

C.W.Li, R.Sherr

Inelastic Scattering of Alpha Particles by Lithium

doi: 10.1103/PhysRev.96.389
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1954SH29      Phys.Rev. 94, 1076 (1954)

R.Sherr, C.W.Li, R.F.Christy

Low Excited States of F19. III. Coulomb Excitation by α Particles

doi: 10.1103/PhysRev.94.1076
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1954SH31      Phys.Rev. 93, 1076 (1954)

R.Sherr, R.H.Miller

Electron Capture in the Decay of Na22

RADIOACTIVITY 22Na(EC), (β+); measured decay products, Eβ, Iβ, Eγ, Iγ; deduced the ratio of electron capture to positron emission, fluorescent yield.

doi: 10.1103/PhysRev.93.1076
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1953HO06      Phys.Rev. 90, 388A (1953)

J.Horton, R.Sherr

Alpha-Gamma Angular Correlation in ThC

doi: 10.1103/PhysRev.90.388A
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1953SH38      Phys.Rev. 91, 909 (1953)

R.Sherr, J.B.Gerhart

Experimental Evidence for the Fermi Interaction in the β Decay of O14 and C10

doi: 10.1103/PhysRev.91.909
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