NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Heisenberg Found 60 matches. 2000MI02 Phys.Rev.Lett. 84, 1403 (2000) 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
2000MI13 Phys.Rev. C61, 054309 (2000) 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
1999HE06 Phys.Rev. C59, 1440 (1999) 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
1999MI35 Phys.Rev. C60, 054303 (1999) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
1987CO30 Phys.Lett. 197B, 489 (1987) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1970HE18 Phys.Lett. 32B, 249 (1970) 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
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
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
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
1966HE13 Thesis, Univ.Hamburg (1966) 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
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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