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NSR database version of April 25, 2024.

Search: Author = J.H.Heisenberg

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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
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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
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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 2p_3/2 → 2p_1/2 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
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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
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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 π1g_9/2 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 1g_9/2 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
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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 ^{142,144,146,148,150}Nd(e, e), E=129.5, 199.4, 299.2, 499.7 MeV; measured σ. ^{142,144,146,148,150}Nd 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0090.