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NSR database version of May 24, 2024.

Search: Author = M.G.Herman

Found 12 matches.

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1990BU05      Phys.Rev. C41, 1530 (1990)

R.Butsch, M.Thoennessen, D.R.Chakrabarty, M.G.Herman, P.Paul

Nuclear Deformation in Excited Pb Isotopes from Giant Dipole γ-Ray-Fission Angular Correlations

NUCLEAR REACTIONS 181Ta(19F, X), (19F, F), E=105, 141 MeV; measured Eγ, Iγ, fission (fragment)γ-coin. 200Pb deduced GDR energy, width, deformation parameter. Statistical model analysis.

doi: 10.1103/PhysRevC.41.1530
Citations: PlumX Metrics

1990SZ05      Phys.Rev. C41, 2164 (1990)

E.M.Szanto, R.Liguori Neto, M.C.S.Figueira, A.Szanto de Toledo, M.G.Herman, N.G.Nicolis, P.M.Stwertka, T.M.Cormier

Search for Valence Proton Effects in Sub-Barrier Fusion Reactions

NUCLEAR REACTIONS, ICPND 50Ti, 51V, 52,54Cr, 54Fe(35Cl, X), E(cm) ≈ 50-80 MeV; measured fusion, residual production σ(E); deduced valence proton effects role.

doi: 10.1103/PhysRevC.41.2164
Citations: PlumX Metrics

1989VO10      Phys.Rev. C40, R2441 (1989)

R.J.Vojtech, R.Butsch, V.M.Datar, M.G.Herman, R.L.McGrath, P.Paul, M.Thoennessen

High Energy Photon Production in Low Energy 12C + 112,124Sn Collisions

NUCLEAR REACTIONS 112,124Sn(12C, X), E=7.5, 10.5 MeV/nucleon; measured γ yield, σ(θγ, Eγ); deduced source velocity, γ yield isotopic dependence. Statistical model calculations.

doi: 10.1103/PhysRevC.40.R2441
Citations: PlumX Metrics

1988CH11      Phys.Rev. C37, 1437 (1988)

D.R.Chakrabarty, M.Thoennessen, S.Sen, P.Paul, R.Butsch, M.G.Herman

Giant Dipole Resonances in Excited Er Isotopes

NUCLEAR REACTIONS 141Pr(19F, X), E=94.1, 96.5, 111.1, 129 MeV; measured γ spectra. 160Er deduced GDR energies, widths, deformation parameters, shape evolution. Statistical model analysis.

doi: 10.1103/PhysRevC.37.1437
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1988HE09      Phys.Lett. 203B, 29 (1988)

M.G.Herman, T.M.Cormier, M.Satteson

Statistical Origin of the Highest-Energy Fusion-Induced Gamma Rays

NUCLEAR REACTIONS 54Fe(35Cl, X), E=95-150 MeV; measured γ-multiplicities, γ-spectra; deduced GDR statistical decay of mass=85, 86, 87 nuclei.

doi: 10.1016/0370-2693(88)91564-X
Citations: PlumX Metrics

1988TH01      Phys.Rev. C37, 1762 (1988)

M.Thoennessen, D.R.Chakrabarty, R.Butsch, M.G.Herman, P.Paul, S.Sen

Onset of Deformation in Pb Isotopes at High Excitation Energies

NUCLEAR REACTIONS 181Ta(19F, X), E=93, 105 MeV; measured Eγ, Iγ. 200Pb deduced GDR, width, deformation parameter, shape transition. Statistical model.

doi: 10.1103/PhysRevC.37.1762
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1987TH07      Phys.Rev.Lett. 59, 2860 (1987)

M.Thoennessen, D.R.Chakrabarty, M.G.Herman, R.Butsch, P.Paul

Giant Dipole Resonance in Highly Excited Thorium: Evidence for strong fission hindrance

NUCLEAR REACTIONS 208Pb(16O, X), E=100, 120, 140 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ), yield ratios. 224Th deduced giant dipole resonance, level density parameters, fission hindrance factors.

doi: 10.1103/PhysRevLett.59.2860
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1986NI07      Phys.Lett. 178B, 339 (1986)

N.G.Nicolis, T.M.Cormier, P.M.Stwertka, M.G.Herman

Angular-Momentum Limitations in the High-Spin Gamma-Decay of Medium-Mass Evaporation Residues

NUCLEAR REACTIONS, ICPND 54Fe(28Si, X)80Sr/79Sr/78Sr/79Rb/76Kr/78Kr/74Kr, E=75-145 MeV; measured γ-ray multiplicity, evaporation residue σ(E). NaI γ-ray multiplicity filter. Statistical model calculations.

doi: 10.1016/0370-2693(86)91390-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0359.

1985ST06      Phys.Rev.Lett. 54, 1635 (1985)

P.M.Stwertka, T.M.Cormier, M.G.Herman, N.G.Nicolis

High-Spin Evolution of Quasicontinuum γ Radiation in 156Er

NUCLEAR REACTIONS 128Te(32S, 4n), E=135-156 MeV; measured Eγ, Iγ, γ-multiplicity, γ(θ). 156Er deduced spin, energy correlated high J transitions.

doi: 10.1103/PhysRevLett.54.1635
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1985ST21      Phys.Lett. 161B, 70 (1985)

P.M.Stwertka, T.M.Cormier, N.G.Nicolis, M.G.Herman

The Onset of Collectivity in Nuclei near the N = 82, Z = 64 Double Closed Shell

NUCLEAR REACTIONS 122,124Sn(28Si, xn), E=120-126 MeV; measured quasicontinuum Eγ, Iγ, γ-multiplicities. 145,146,147,148Gd deduced spin-energy correlated rotational transitions, collective behavior J dependence.

doi: 10.1016/0370-2693(85)90611-2
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1984CO27      Phys.Rev. C30, 2092 (1984)

M.M.Coimbra, N.Carlin Filho, A.Szanto de Toledo, P.M.Stwertka, M.G.Herman, N.G.Nicolis, T.M.Cormier

Use of Energy-Averaged Cross Sections for Nuclear Spectroscopy: 26Mg states in the continuum

NUCLEAR REACTIONS 12C(18O, α), E=46-50 MeV: measured σ(Eα), σ(θ); deduced energy averaged σ. 26Mg deduced continuum states.

doi: 10.1103/PhysRevC.30.2092
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0219.

1983CO13      Nucl.Instrum.Methods 212, 185 (1983)

T.M.Cormier, M.G.Herman, B.S.Lin, P.M.Stwertka

Performance of a Recoil Mass Spectrometer

NUCLEAR REACTIONS 58Ni(35Cl, X), E=120 MeV; 120Sn(35Cl, X), E=138 MeV; measured σ(evaporation residue) vs mass. Recoil mass spectrometer.

doi: 10.1016/0167-5087(83)90690-7
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