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NSR database version of April 11, 2024.

Search: Author = J.H.Heisenberg

Found 21 matches.

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2000MI02      Phys.Rev.Lett. 84, 1403 (2000)

B.Mihaila, J.H.Heisenberg

Microscopic Calculation of the Inclusive Electron Scattering Structure Function in 16O

NUCLEAR STRUCTURE 16O; calculated charge form factor, longitudinal structure function for electron scattering. Comparison with data.

doi: 10.1103/PhysRevLett.84.1403
Citations: PlumX Metrics

2000MI13      Phys.Rev. C61, 054309 (2000)

B.Mihaila, J.H.Heisenberg

Ground State Correlations and Mean Field in 16O. II. Effects of a Three-Nucleon Interaction

NUCLEAR STRUCTURE 16O; calculated ground-state wave function, charge form factor, charge density, longitudinal response for electron scattering. Coupled-cluster expansion.

doi: 10.1103/PhysRevC.61.054309
Citations: PlumX Metrics

1999HE06      Phys.Rev. C59, 1440 (1999)

J.H.Heisenberg, B.Mihaila

Ground State Correlations and Mean Field in 16O

NUCLEAR STRUCTURE 16O; calculated binding energy, charge density, two-body density. Coupled cluster expansion.

doi: 10.1103/PhysRevC.59.1440
Citations: PlumX Metrics

1999MI35      Phys.Rev. C60, 054303 (1999)

B.Mihaila, J.H.Heisenberg

Center-of-Mass Corrections Reexamined: A many-body expansion approach

NUCLEAR STRUCTURE 4He, 16O; calculated charge form factors, radii. Many-body expansion approach to center-of-mass correction.

doi: 10.1103/PhysRevC.60.054303
Citations: PlumX Metrics

1993KE03      Phys.Rev. C47, 2146 (1993)

J.J.Kelly, B.S.Flanders, F.W.Hersman, J.H.Heisenberg, J.Calarco, J.P.Connelly, T.E.Milliman, A.Scott, F.T.Baker, V.Penumetcha, W.P.Jones, G.T.Emery, A.D.Bacher, C.Olmer, M.A.Grimm, M.L.Whiten

Neutron Transition Densities from 88Sr(p, p') at E(p) = 200 MeV

NUCLEAR REACTIONS 88Sr(polarized p, p'), (polarized p, p), E=200 MeV; measured σ(θ), analyzing power vs θ. 88Sr levels deduced neutron transition densities. Shell model comparison.

doi: 10.1103/PhysRevC.47.2146
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0155.

1993WI08      Phys.Rev. C47, 2539 (1993)

J.E.Wise, J.R.Calarco, J.P.Connelly, S.A.Fayans, F.W.Hersman, J.H.Heisenberg, R.S.Hicks, W.Kim, T.E.Milliman, R.A.Miskimen, G.A.Peterson, A.P.Platonov, E.E.Saperstein, R.P.Singhal

Ground-State Magnetization Density of 89Y

NUCLEAR REACTIONS 89Y(e, e), E=71-262 MeV; measured σ(θ), θ=180°. 89Y deduced ground state M1 form factor. Fourier-Bessel analysis.

doi: 10.1103/PhysRevC.47.2539
Citations: PlumX Metrics

1992CO14      Phys.Rev. C45, 2711 (1992)

J.P.Connelly, D.J.DeAngelis, J.H.Heisenberg, F.W.Hersman, W.Kim, M.Leuschner, T.E.Milliman, J.Wise, C.N.Papanicolas

High Resolution Electron Scattering from High Spin States in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E=100-300 MeV; measured σ(E(e')), form factors. 208Pb deduced high spin states quenching, 12- state transition strength fragmentation. Independent particle model, DWBA.

doi: 10.1103/PhysRevC.45.2711
Citations: PlumX Metrics

1992KI10      Phys.Rev. C45, 2290 (1992)

W.Kim, B.L.Miller, J.R.Calarco, L.S.Cardman, J.P.Connelly, S.A.Fayans, B.Frois, D.Goutte, J.H.Heisenberg, F.W.Hersman, V.Meot, T.E.Milliman, P.Mueller, C.N.Papanicolas, A.P.Platonov, V.Yu.Ponomarev, J.E.Wise

Interplay between Single-Particle and Collective Degrees of Freedom in the Excitation of the Low-Lying States in 140Ce

NUCLEAR REACTIONS 140Ce(e, e'), E=190 MeV; measured σ(E(e')), θ=45°. 140Ce levels deduced form factors, transition charge densities, B(λ), configurations. Quasiparticle-phonon model, self-consistent finite Fermi system theory.

doi: 10.1103/PhysRevC.45.2290
Citations: PlumX Metrics

1992KI20      Phys.Rev. C46, 1656 (1992)

W.Kim, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, T.E.Milliman, J.E.Wise, C.N.Papanicolas, S.A.Fayans, A.P.Platonov

Ground-State Charge Distribution and Transition Charge Densities of the Low-Lying States in 86Sr

NUCLEAR REACTIONS 86Sr(e, e'), (e, e), E=100-370 MeV; measured form factors. 86Sr levels deduced B(λ), transition charge densities.

doi: 10.1103/PhysRevC.46.1656
Citations: PlumX Metrics

1992WI06      Phys.Rev. C45, 2701 (1992)

J.E.Wise, J.P.Connelly, F.W.Hersman, J.H.Heisenberg, W.Kim, M.Leuschner, S.A.Fayans, A.P.Platonov, E.E.Saperstein, V.Yu.Ponomarev

Transition Densities of Collective Excitations in 118Sn

NUCLEAR REACTIONS 118Sn(e, e), (e, e'), E=252, 376 MeV; measured σ(θ, E(e')). 118Sn levels deduced transition charge densities, B(λ). Finite Fermi system, quasiparticle-phonon approach.

doi: 10.1103/PhysRevC.45.2701
Citations: PlumX Metrics

1991KI13      Phys.Rev. C44, 2400 (1991)

W.Kim, J.R.Calarco, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, T.E.Milliman, J.E.WIse, B.L.Miller, C.N.Papanicolas, V.Yu.Ponomarev, E.E.Saperstein, A.P.Platonov

Properties of Low-Lying States in 142Ce via High Resolution Electron Scattering

NUCLEAR REACTIONS 142Ce(e, e'), E=100-370 MeV; measured reaction products, Eβ, Iβ; deduced σ(E(e'), θ=45°), form factors, B(E2). 142Ce levels deduced charge densities. Quasiparticle-phonon approach, finite Fermi system.

doi: 10.1103/PhysRevC.44.2400
Citations: PlumX Metrics

1991RI08      Phys.Rev. C44, R939 (1991)

D.E.J.Riedeman, H.P.Blok, M.N.Harakeh, J.H.Heisenberg, K.Heyde, C.W.de Jager, H.de Vries, L.de Vries

Study of the Proton 2p3/2 → 2p1/2 Transition in 65Cu 71Ga

NUCLEAR REACTIONS 65Cu(e, e'), E=82-443 MeV; 71Ge(e, e'), E=132-358 MeV; measured σ(θ, E(e')). 65Cu, 71Ga level deduced transition charge, current densities, B(E2). Particle vibration coupling model.

doi: 10.1103/PhysRevC.44.R939
Citations: PlumX Metrics

1990CO25      Phys.Rev. C42, 1948 (1990)

J.P.Connelly, T.E.Milliman, J.H.Heisenberg, F.W.Hersman, J.E.Wise, C.N.Papanicolas

Proton Core Polarization in Low-Lying States of 86Sr

NUCLEAR REACTIONS 92Mo(e, e'), E=200 MeV; 86Sr(e, e'), E=190 MeV; measured σ(θ). 92Mo, 86Sr levels deduced transition charge densities.

doi: 10.1103/PhysRevC.42.1948
Citations: PlumX Metrics

1990MI07      Phys.Rev. C41, 2586 (1990)

T.E.Milliman, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, J.E.Wise, C.N.Papanicolas

Electron Scattering from 92Mo

NUCLEAR REACTIONS 92Mo(e, e'), E=189.6 MeV; measured σ(θ), σ(E(e')). 92Mo levels deduced J, π, transition charge, current densities. Other data analyzed.

doi: 10.1103/PhysRevC.41.2586
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0223.

1990WI13      Phys.Rev. C42, 1077 (1990)

J.E.Wise, F.W.Hersman, J.H.Heisenberg, T.E.Milliman, J.P.Connelly, J.R.Calarco, C.N.Papanicolas

Single-Particle Excitations in 89Y

NUCLEAR REACTIONS 89Y(e, e'), E=370.9, 622.8 MeV; measured σ(θ), form factors. 89Y deduced transition charge, current densities. DWBA analysis, shell model.

NUCLEAR STRUCTURE 89Y; calculated levels, transition charge, current densities. Shell model.

doi: 10.1103/PhysRevC.42.1077
Citations: PlumX Metrics

1988MI05      Phys.Rev. C37, 895 (1988)

B.L.Miller, L.S.Cardman, C.N.Papanicolas, T.E.Milliman, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, J.E.Wise, B.Frois, D.Goutte, V.Meot

Electroexcitation of High-Multipolarity Transitions in 140Ce

NUCLEAR REACTIONS 140Ce(e, e'), E=100-370 MeV; measured σ(E(e')), σ(θ). 140Ce deduced level, J, π, configuration, γ-multipolarity, quenching factor.

doi: 10.1103/PhysRevC.37.895
Citations: PlumX Metrics

1987PA14      Phys.Rev.Lett. 58, 2296 (1987)

C.N.Papanicolas, L.S.Cardman, J.H.Heisenberg, O.Schwentker, T.E.Milliman, F.W.Hersman, R.S.Hicks, G.A.Peterson, J.S.McCarthy, J.Wise, B.Frois

Magnetic Form Factors of 205Tl and 207Pb: Establishing the limits of mean-field theory

NUCLEAR REACTIONS 205Tl, 207Pb(e, e), E not given; measured magnetic form factors, σ. 205Tl, 207Pb deduced quenching mechanism, ground state magnetization densities. Independent particle model calculations.

doi: 10.1103/PhysRevLett.58.2296
Citations: PlumX Metrics

1985MI15      Phys.Rev. C32, 805 (1985)

T.E.Milliman, J.H.Heisenberg, F.W.Hersman, J.P.Connelly, C.N.Papanicolas, J.E.Wise, H.P.Blok, L.T.van der Bijl

Determination of the π1g9/2 Orbit Size in 88Sr, 90Zr, and 92Mo from Inelastic Electron Scattering

NUCLEAR STRUCTURE 88Sr, 90Zr, 92Mo; calculated spectroscopic amplitudes for 8+ transitions, rms radii of 1g9/2 proton orbit. Shell model, electron scattering data input.

NUCLEAR REACTIONS 88Sr, 90Zr, 92Mo(e, e'), E=100-370 MeV; measured σ(E, θ) vs momentum transfer for 8+ states. 88Sr, 90Zr, 92Mo deduced point proton density. Shell model.

doi: 10.1103/PhysRevC.32.805
Citations: PlumX Metrics

1971HE07      Nucl.Phys. A164, 340 (1971)

J.H.Heisenberg, J.S.McCarthy, I.Sick, M.R.Yearian

Charge Distribution of the Even Nd Isotopes

NUCLEAR REACTIONS 142,144,146,148,150Nd(e, e), E=129.5, 199.4, 299.2, 499.7 MeV; measured σ. 142,144,146,148,150Nd deduced nuclear charge distributions. Enriched targets.

doi: 10.1016/0375-9474(71)90218-1
Citations: PlumX Metrics

1970HE18      Phys.Lett. 32B, 249 (1970)

J.H.Heisenberg, I.Sick

Transition Density of the Octupole Vibration in 208Pb Determined by Electron Scattering

NUCLEAR REACTIONS 208Pb(e, e'), E=500 MeV; calculated σ(Ee'). 208Pb calculated transition density of octupole vibration.

doi: 10.1016/0370-2693(70)90519-8
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1969MO39      Phys.Rev. 179, 1176 (1969)

L.G.Moretto, R.C.Gatti, S.G.Thompson, J.T.Routti, J.H.Heisenberg, L.M.Middleman, M.R.Yearian, R.Hofstadter

Electron- and Bremsstrahlung-Induced Fission of Heavy and Medium-Heavy Nuclei

NUCLEAR REACTIONS 154Sm(γ, f), 209Bi(γ, f), E=49.8-421 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry L0090.

doi: 10.1103/PhysRev.179.1176
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0090.

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