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Search: Author = J.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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1987CA02      Phys.Rev.Lett. 58, 195 (1987)

J.M.Cavedon, B.Frois, D.Goutte, M.Huet, Ph.Leconte, X.H.Phan, S.K.Platchkov, C.N.Papanicolas, S.E.Williamson, W.Boeglin, I.Sick, J.Heisenberg

Measurement of Charge-Density Differences in the Interior of Pb Isotopes

NUCLEAR REACTIONS 204,206,207,208Pb(e, e), E=502 MeV; measured σ(θ). 204,206,207,208Pb deduced ground state charge densities. Enriched targets. Theoretical calculations.

doi: 10.1103/PhysRevLett.58.195
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1987CO30      Phys.Lett. 197B, 489 (1987)

G.Co, J.Heisenberg

Coulomb Distortion Effects in Deep-Inelastic Electron Scattering

NUCLEAR REACTIONS 12C, 40Ca(e, e'), E not given; calculated Rosenbluth plots. 12C, 40Ca deduced longitudinal, transverse response functions.

doi: 10.1016/0370-2693(87)91039-2
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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
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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
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1985WI06      Phys.Rev. C31, 1699 (1985)

J.E.Wise, J.S.McCarthy, R.Altemus, B.E.Norum, R.R.Whitney, J.Heisenberg, J.Dawson, O.Schwentker

Inelastic Electron Scattering from 48Ca

NUCLEAR REACTIONS 48Ca(e, e'), E=149.6-288.8 MeV; measured form factor, σ(E(e')); deduced σ(θ). 48Ca levels deduced transition charge, current densities. RPA calculation.

doi: 10.1103/PhysRevC.31.1699
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1984HE02      Phys.Rev. C29, 97 (1984)

J.Heisenberg, J.Dawson, T.Milliman, O.Schwentker, J.Lichtenstadt, C.N.Papanicolas, J.Wise, J.S.McCarthy, N.Hintz, H.P.Blok

Excitation of Positive-Parity States in Electron Scattering from 90Zr

NUCLEAR REACTIONS 90Zr(e, e'), E=70-368 MeV; measured σ(θ), σ(E(e')); deduced g9/2 proton orbit radius. 90Zr levels deduced charge distribution, transition charge densities, M7 transition current density. DWBA analysis.

doi: 10.1103/PhysRevC.29.97
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1984PA02      Phys.Rev.Lett. 52, 247 (1984)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, J.S.McCarthy, D.Goutte, J.M.Cavedon, B.Frois, M.Huet, P.Leconte, Phan Xuan Ho, S.Platchkov, I.Sick

Effective Charge of Neutron Quasiparticle Pairs in 206Pb and 204Pb

NUCLEAR REACTIONS 204,206,208Pb(e, e'), E=52-502 MeV; measured σ. 204,206,208Pb levels deduced transition charge densities, B(λ).

doi: 10.1103/PhysRevLett.52.247
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1984VA16      J.Phys.(Paris), Colloq.C4, 465 (1984); See 1984Va42

L.T.van der Bijl, H.Blok, H.P.Blok, R.Ent, J.Heisenberg, O.Schwentker, A.Richter, P.K.A.de Witt Huberts

Electro-Excitation of the 1+ State at 3.486 MeV in 88Sr


1984VA21      Nucl.Phys. A423, 365 (1984)

L.T.Van Der Bijl, H.Blok, H.P.Blok, R.Ent, J.Heisenberg, O.Schwentker, A.Richter, P.K.A.De Witt Huberts

Electro-Excitation of the 1+ State at E(x) = 3.486 MeV in 88Sr

NUCLEAR REACTIONS 88Sr(e, e'), E=23.7-261.6 MeV; measured σ(θ), σ(E(e')); deduced form factor, core, isobar-hole polarization effects.

doi: 10.1016/0375-9474(84)90029-0
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1984VA42      J.Phys.(Paris), Colloq.C-4, 465 (1984)

L.T.van der Bijl, H.Blok, H.P.Blok, R.Ent, J.Heisenberg, O.Schwentker, A.Richter, P.K.A.de Witt Huberts

Electro-Excitation of the 1+ State at 3, 486 MeV in 88Sr

NUCLEAR REACTIONS 88Sr(e, e'), E=81.4, 209.5 MeV; measured σ(Ee', θe'), form factor. 88Sr transition deduced B(M1) reduction. Enriched target. Theoretical analyses.


1983FR09      Phys.Lett. 122B, 347 (1983)

B.Frois, S.Turck-Chieze, J.B.Bellicard, M.Huet, P.Leconte, X.-H.Phan, I.Sick, J.Heisenberg, M.Girod, K.Kumar, B.Grammaticos

The Effects of Triaxial Deformations in the Structure of the 2+1 Transition Charge Density in 58Ni

NUCLEAR REACTIONS 58Ni(e, e'), E=700 MeV; measured σ(θ). 58Ni level deduced transition charge density. Triaxial rotor, Davidov-Filippov model.

doi: 10.1016/0370-2693(83)91579-4
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1983SC01      Phys.Rev.Lett. 50, 15 (1983)

O.Schwentker, J.Dawson, J.Robb, J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, J.Wise, J.S.McCarthy, L.T.van der Bijl, H.P.Blok

E2 Transition Densities and Proton Shell Structure in 88Sr, 89Y, and 90Zr

NUCLEAR REACTIONS 88Sr, 89Y, 90Zr(e, e'), E not given; measured σ(θ). 89Y, 90Zr levels deduced E2 transition charge densities. 88Sr levels deduced spectroscopic amplitudes, E2 transition charge densities. Fourier-Bessel expansion, RPA, broken pair calculations.

doi: 10.1103/PhysRevLett.50.15
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1982HE03      Phys.Rev. C25, 2292 (1982)

J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, J.S.McCarthy

Excitation of Low Lying Natural Parity Levels in 208Pb by Inelastic Electron Scattering

NUCLEAR REACTIONS 208Pb(e, e'), E=50-335 MeV; measured σ(E(e'), θ). 208Pb levels deduced transition charge, current densities. DWBA analysis.

doi: 10.1103/PhysRevC.25.2292
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1982PA05      Phys.Lett. 108B, 279 (1982)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, J.S.McCarthy, D.Goutte, J.M.Cavedon, B.Frois, M.Huet, P.Leconte, Phan Xuan Ho, S.Platchkov, I.Sick

Transition Charge Densities for the Lowest E5 Transitions in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E not given; measured σ(θ) vs momentum transfer. 208Pb levels deduced transition charge densities.

doi: 10.1016/0370-2693(82)91192-3
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1982SC08      Phys.Lett. 112B, 40 (1982)

O.Schwentker, J.Dawson, S.McCaffrey, J.Robb, J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, J.Wise, J.S.McCarthy, N.Hintz, H.P.Blok

Measurement of the Effective E5 Single-Particle Transition Densities in 89Y and 90Zr

NUCLEAR REACTIONS 89Y, 90Zr(e, e'), E not given; measured σ(θ) vs momentum transfer. 89Y, 90Zr level deduced effective E5 transition charge, current densities, configuration.

doi: 10.1016/0370-2693(82)90901-7
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1981PA04      Phys.Lett. 99B, 96 (1981)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, J.S.McCarthy

High Multipolarity Electroexcitations in 207Pb and 206Pb

NUCLEAR REACTIONS 206,207Pb(e, e'), E not given; measured σ(θ(e')), form factors. 206,207Pb deduced levels, E10 transition strength distribution.

doi: 10.1016/0370-2693(81)90958-8
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1980GO12      Phys.Rev.Lett. 45, 1618 (1980)

D.Goutte, J.B.Bellicard, J.M.Cavedon, B.Frois, M.Huet, P.Leconte, Phan Xuan Ho, S.Platchkov, J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, I.Sick

Determination of the Charge Density of the Octupole Vibration in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E=502 MeV; measured σ(θ). 208Pb level deduced transition charge density.

doi: 10.1103/PhysRevLett.45.1618
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1980LI04      Phys.Rev.Lett. 44, 858 (1980)

J.Lichtenstadt, C.N.Papanicolas, C.P.Sargent, J.Heisenberg, J.S.McCarthy

Investigation of Natural-Parity High-Spin States in 208Pb by (e, e') Reactions

NUCLEAR REACTIONS 208Pb(e, e'), E=70-335 MeV; measured reduced σ(θ). 208Pb deduced high-spin states, parity, configuration. DWBA analysis, Hartree-Fock wave functions.

doi: 10.1103/PhysRevLett.44.858
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1980PA09      Phys.Rev.Lett. 45, 106 (1980)

C.N.Papanicolas, J.Lichtenstadt, C.P.Sargent, J.Heisenberg, J.S.McCarthy

Suppression of the Transverse Scattering Amplitude in 207Pb

NUCLEAR REACTIONS 207Pb(e, e'), E not given; measured longitudinal, transverse form factors, σ(θ). 207Pb levels deduced transverse amplitude quenching.

doi: 10.1103/PhysRevLett.45.106
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1979LI13      Phys.Rev. C20, 497 (1979)

J.Lichtenstadt, J.Heisenberg, C.N.Papanicolas, C.P.Sargent, A.N.Courtemanche, J.S.McCarthy

High-Spin States of Jπ = 12-, 14- in 208Pb Studied by (e, e')

NUCLEAR REACTIONS 208Pb(e, e'), E=50-335 MeV; measured σ(E). 208Pb deduced levels, J, π. DWBA, Hartree-Fock single-particle wave functions.

doi: 10.1103/PhysRevC.20.497
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1978CR05      Phys.Rev. C18, 2432 (1978)

C.Creswell, A.Hirsch, W.Bertozzi, J.Heisenberg, S.Kowalski, C.P.Sargent, W.Turchinetz, A.Dieperink

Indication for a Kπ = 0- Octupole Band in 150Nd from Electron Scattering

NUCLEAR REACTIONS 150Nd(e, e'), E not given; measured form factors. Compared with calculations based on small amplitude octupole vibration. 150Nd deduced 0- octupole band.

doi: 10.1103/PhysRevC.18.2432
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1978HI02      Phys.Rev.Lett. 40, 632 (1978)

A.Hirsch, C.Creswell, W.Bertozzi, J.Heisenberg, M.V.Hynes, S.Kowalski, H.Miska, B.Norum, F.N.Rad, C.P.Sargent, T.Sasanuma, W.Turchinetz

Electron Scattering from the Octupole Band in 238U

NUCLEAR REACTIONS 238U(e, e'), E=90-300 MeV; measured σ(E). 238U levels deduced B(λ).

doi: 10.1103/PhysRevLett.40.632
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1978LI05      Phys.Rev.Lett. 40, 1127 (1978)

J.Lichtenstadt, J.Heisenberg, C.N.Papanicolas, C.P.Sargent, A.N.Courtemanche, J.S.McCarthy

Observation of 12- Magnetic Spin States in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E=50-335 MeV; measured σ(E). 208Pb deduced levels, J, π.

doi: 10.1103/PhysRevLett.40.1127
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1978PA10      Phys.Rev.Lett. 41, 537 (1978)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, A.N.Courtemanche, J.S.McCarthy

Electron Scattering on 207Pb and the Induced Charge of the Neutron

NUCLEAR REACTIONS 207Pb(e, e'), E=50-320 MeV; measured σ(E). 207Pb levels deduced effective charges.

doi: 10.1103/PhysRevLett.41.537
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1978RA02      Phys.Rev.Lett. 40, 368 (1978)

F.N.Rad, T.Sasanuma, W.Bertozzi, J.Heisenberg, M.V.Hynes, S.Kowalski, H.Miska, B.Norum, C.P.Sargent, W.Turchinetz, C.F.Williamson

Electroexcitation of the Ground-State Rotational Band in 181Ta

NUCLEAR REACTIONS 181Ta(e, e), (e, e'), E ≤ 400 MeV; measured yields. 181Ta levels deduced form factors.

doi: 10.1103/PhysRevLett.40.368
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1978WI01      Phys.Rev.Lett. 40, 1702 (1978)

C.F.Williamson, F.N.Rad, S.Kowalski, J.Heisenberg, H.Crannell, J.T.O'Brien, H.C.Lee

Electroexcitation of the Ground-State Rotational Band in 19F

NUCLEAR REACTIONS 19F(e, e'), E=400 MeV; measured momentum transfer distribution. 19F level deduced J, π.

doi: 10.1103/PhysRevLett.40.1702
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1976CO08      Phys.Rev. C13, 1083 (1976)

T.Cooper, W.Bertozzi, J.Heisenberg, S.Kowalski, W.Turchinetz, C.Williamson, L.Cardman, S.Fivozinsky, J.Lightbody, Jr., S.Penner

Shapes of Deformed Nuclei as Determined by Electron Scattering: 152Sm, 154Sm, 166Er, 176Yb, 232Th, and 238U

NUCLEAR REACTIONS 152,154Sm, 166Er, 176Yb, 232Th, 238U(e, e'); measured σ(Ee'). 152,154Sm, 166Er, 176Yb, 232Th, 238U deduced shape parameters.

doi: 10.1103/PhysRevC.13.1083
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1973HA13      Phys.Rev. C7, 1396 (1973)

P.L.Hallowell, W.Bertozzi, J.Heisenberg, S.Kowalski, X.Maruyama, C.P.Sargent, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Electron Scattering from 19F and 40Ca

NUCLEAR REACTIONS 19F, 40Ca(e, e), (e, e'), E=120 MeV; measured σ(Ee), form factors; 19F, 40Ca deduced levels, charge radius, deformation parameters.

doi: 10.1103/PhysRevC.7.1396
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1973HE28      Proc.Int.Conf.Nuclear Physics, Munich, J.de Boer, H.J.Mang, Eds., North-Holland Publ.Co., Amsterdam, Vol.1, p.629 (1973)

J.Heisenberg, W.Bertozzi, T.Cooper, N.Ensslin, P.L.Hallowell, S.Kowalski, W.Turchinetz, C.F.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Deformed Charge Distributions of Some Rotational Heavy Nuclei

NUCLEAR REACTIONS 166Er, 176Yb, 232Th, 238U(e, e), E=35-110 MeV; measured σ(θ). 166Er, 176Yb, 232Th, 238U deduced charge distribution.


1972BE26      Phys.Rev.Lett. 28, 1711 (1972)

W.Bertozzi, T.Cooper, N.Ensslin, J.Heisenberg, S.Kowalski, M.Mills, W.Turchinetz, C.Williamson, S.P.Fivozinsky, J.W.Lightbody, Jr., S.Penner

Deformation Parameters of 152Sm by Electron Scattering

NUCLEAR REACTIONS 152Sm(e, e'), E=50-105 MeV; measured σ(Ee'). 152Sm deduced nuclear charge distribution, deformation parameters β(L).

doi: 10.1103/PhysRevLett.28.1711
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1972BE83      Phys.Lett. 41B, 408 (1972)

W.Bertozzi, J.Friar, J.Heisenberg, J.W.Negele

Contributions of Neutrons to Elastic Electron Scattering from Nuclei

NUCLEAR REACTIONS 40,48Ca(e, e), E not given; analyzed σ(θ); deduced charge form factors, rms charge radius.

doi: 10.1016/0370-2693(72)90662-4
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1972HE17      Phys.Rev. C6, 381 (1972)

J.Heisenberg, R.Hofstadter, J.S.McCarthy, R.Herman, B.C.Clark, D.G.Ravenhall

Electron-Scattering Determination of Isotopic Differences in the Charge Distributions of Ti46,48,50

NUCLEAR REACTIONS 46,48,50Ti(e, e), E=200, 300 MeV; measured σ(θ). 46,48,50Ti deduced rms radii.

doi: 10.1103/PhysRevC.6.381
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


1971HE08      Nucl.Phys. A164, 353 (1971)

J.Heisenberg, J.S.McCarthy, I.Sick

Inelastic Electron Scattering from Several Ca, Ti and Fe Isotopes

NUCLEAR REACTIONS 40,42,44Ca, 46,48,50Ti, 56Fe(e, e'), E=198, 250, 300 MeV; measured σ(E, θ). 40,42,44Ca, 46,48,50Ti, 56Fe deduced nuclear transition charge density, B(λ). Enriched targets.

doi: 10.1016/0375-9474(71)90219-3
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1970FI10      Phys.Lett. 32B, 460 (1970)

J.R.Ficenec, W.P.Trower, J.Heisenberg, I.Sick

Elastic Electron-Nickel Scattering

NUCLEAR REACTIONS 58,60,61,62,64Ni(e, e), E=300 MeV; measured σ(θ). 58,60,61,62,64Ni deduced nuclear charge distributions.

doi: 10.1016/0370-2693(70)90383-7
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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1970HE24      Nucl.Phys. A157, 435 (1970)

J.Heisenberg, J.S.McCarthy, I.Sick

Elastic Electron Scattering from 13C

NUCLEAR REACTIONS 13C(e, e), E=120, 170, 200, 250, 350, 500, 750 MeV; measured σ(E;θ). 13C deduced nuclear charge distribution. Enriched target.

doi: 10.1016/0375-9474(70)90224-1
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1969HE17      Phys.Rev.Letters 23, 1402 (1969)

J.Heisenberg, R.Hofstadter, J.S.McCarthy, I.Sick, B.C.Clark, R.Herman, D.G.Ravenhall

Elastic Electron Scattering by Pb208 and New Information About the Nuclear Charge Distribution

NUCLEAR REACTIONS 208Pb(e, e), E = 248, 502 MeV; measured σ(θ). 208Pb deduced nuclear charge distribution.

doi: 10.1103/PhysRevLett.23.1402
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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.


1966HE13      Thesis, Univ.Hamburg (1966)

J.Heisenberg

Untersuchungen am Np237 mit magnetisch gestorter α-γ Winkelkorrelation

RADIOACTIVITY 241Am; measured αγ(θ, H, t). 237Np level deduced g.


1964KO13      Perturbed Angular Correlations, E.Karlsson, E.Matthias, K.Siegbahn, Ed., North-Holland Publishing Co., p.200 (1964)

H.J.Korner, E.Gerdau, J.Heisenberg, J.Braunsfurth

Measurement of the g(R)-Factor of the 2+ Rotational Level in W184

NUCLEAR STRUCTURE 184Re; measured not abstracted; deduced nuclear properties.


1964KO15      Compt.Rend.Congr.Intern.Phys.Nucl., Paris, P.Gugenberger, Ed., Centre National de la Recherche Scientifique, Paris, Vol.II, p.481 (1964)

H.J.Korner, K.Auerbach, J.Braunsfurth, U.Ortabasi, J.Heisenberg

g-Factor Measurements on the First Excited States of Pd106, Pr143, Hg198 and Pb207

NUCLEAR STRUCTURE 143Ce; measured not abstracted; deduced nuclear properties.


1963GE09      Z.Physik 174, 389 (1963)

E.Gerdau, W.Krull, L.Mayer, J.Braunsfurth, J.Heisenberg, P.Steiner, E.Bodenstedt

Winkelkorrelationsmessungen an > 30 y Holmium 166 und Bestimmung des g(R) Faktors des 4+ Rotationsniveaus von Erbium 166

NUCLEAR STRUCTURE 166Ho; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01378614
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1963GE12      Physik.Verhandl. 14, 116 (1963)

E.Gerdau, W.Krull, L.Mayer, J.Braunsfurth, J.Heisenberg, P.Steiner, E.Bodenstedt

Der g(R)-Faktor des 4+ Rotationsniveaus von Er166 und andere Winkelkorrelations-Messungen

NUCLEAR STRUCTURE 166Er, 166Ho; measured not abstracted; deduced nuclear properties.


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