NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = J.E.Wise Found 22 matches. 1998MO09 Phys.Lett. 419B, 25 (1998) C.L.Morris, J.D.Zumbro, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Reidel, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, J.Ouyang, R.J.Peterson, J.E.Wise Evidence for Δ+ Components in Nuclei NUCLEAR REACTIONS 12,13C, 90Zr, 208Pb(π+, π+p), (π+, π-p), E=500 MeV; measured σ(DCX)/σ(NCX); deduced nuclear wave function Δ+ components.
doi: 10.1016/S0370-2693(97)01453-6
1996MI13 Phys.Lett. 382B, 29 (1996) R.Michael, M.B.Barakat, S.Bart, R.E.Chrien, B.C.Clark, D.J.Ernst, S.Hama, K.H.Hicks, W.Hinton, E.V.Hungerford, M.G.Jiang, T.Kishimoto, C.M.Kormanyos, L.J.Kurth, L.Lee, B.Mayes, R.J.Peterson, L.Pinsky, R.Sawafta, R.Sutter, L.Tang, J.E.Wise K+ Elastic Scattering from C and 6Li at 715 MeV/c NUCLEAR REACTIONS 12C, 6Li(K+, K+), E at 715 MeV/c; measured σ(θ). Parameter-free impluse approximation.
doi: 10.1016/0370-2693(96)00664-8
1995DE23 Phys.Rev. C52, 61 (1995) D.J.DeAngelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Multipole Strength in 12C from the (e, e'α) Reaction for Momentum Transfers up to 0.61 fm -1 NUCLEAR REACTIONS 12C(e, e'p), (e, e'α), E=124.1, 183.4 MeV; measured σ(θ(e'), θ(α)), σ(θ(e'), θ(p)) vs energy transfer. 12C deduced B(E2), EWSR strength.
doi: 10.1103/PhysRevC.52.61
1995KO01 Phys.Rev. C51, 669 (1995) C.M.Kormanyos, R.J.Peterson, J.R.Shepard, J.E.Wise, S.Bart, R.E.Chrien, L.Lee, B.L.Clausen, J.Piekarewicz, M.B.Barakat, E.V.Hungerford, R.A.Michael, K.H.Hicks, T.Kishimoto Quasielastic K+ Scattering NUCLEAR REACTIONS 2H, Ca, C, Pb(K+, K+), (K+, K+p), E at 705 MeV/c; measured σ(θ, E); deduced quasielastic scattering. RPA theory.
doi: 10.1103/PhysRevC.51.669
1993CL07 Phys.Rev. C48, 1632 (1993) B.L.Clausen, R.J.Peterson, C.Kormanyos, J.E.Wise, A.B.Kurepin, Y.K.Gavrilov High Resolution 162 MeV Pion Scattering to 6- Stretched States in 26Mg NUCLEAR REACTIONS 26Mg(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ), pion spectra. 26Mg deduced matrix elements, stretched states isospin composition.
doi: 10.1103/PhysRevC.48.1632
1993DE10 Phys.Rev.Lett. 70, 2872 (1993) D.De Angelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Isoscalar E2 Strength in 12C from the (e, e'α) Reaction NUCLEAR REACTIONS 12C(e, e'α), E=124.1-183.4 MeV; measured σ(θ(e), θ(α)) vs energy transfer. 12C deduced GQR associated EWSR, B(E2).
doi: 10.1103/PhysRevLett.70.2872
1993KO40 Phys.Rev.Lett. 71, 2571 (1993) C.M.Kormanyos, R.J.Peterson, J.R.Shepard, J.E.Wise, S.Bart, R.E.Chrien, L.Lee, B.L.Clausen, J.Piekarewicz, M.B.Barakat, R.A.Michael, T.Kishimoto K+-Nucleus Quasielastic Scattering NUCLEAR REACTIONS C, Ca, Pb, 2H(K+, X), E at 705 MeV/c; measured σ(θ) vs energy transfer; deduced participating nucleons effective number.
doi: 10.1103/PhysRevLett.71.2571
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
1993WI15 Phys.Rev. C48, 1840 (1993) J.E.Wise, M.R.Braunstein, S.Hoibraten, M.D.Kohler, B.J.Kriss, J.Ouyang, R.J.Peterson, J.A.McGill, C.L.Morris, S.J.Seestrom, R.M.Whitton, J.D.Zumbro, C.M.Edwards, A.L.Williams Quasifree Pion Scattering at 500 MeV NUCLEAR REACTIONS C(π+, π+), (π-, π-), E=500 MeV; measured σ(θ) vs energy loss, σ(θ). Ca, Zr, Pb(π+, π+), (π-, π-), E=500 MeV; measured σ(θ); deduced surface single nucleon knockout evidence.
doi: 10.1103/PhysRevC.48.1840
1993ZU01 Phys.Rev.Lett. 71, 1796 (1993) J.D.Zumbro, C.L.Morris, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Edwards, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, R.J.Peterson, J.Ouyang, J.E.Wise, W.R.Gibbs Inclusive Scattering of 500-MeV Pions from Carbon NUCLEAR REACTIONS C(π+, π+X), (π-, π-X), E=500 MeV; measured inclusive σ(θ, E(π)); deduced comparison with (e, e'X).
doi: 10.1103/PhysRevLett.71.1796
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
1991PO06 Nucl.Phys. A527, 372c (1991) M.Potokar, J.R.Calarco, J.E.Wise, N.Zimmermann, H.Weyand, H.J.Emrich, J.P.Fritsch, A.Grasmuck, R.Neuhausen, S.Schardt Separation of the Longitudinal and Transverse Amplitudes for the Giant Dipole Resonances of 12C and 16O from Measurement of the (e, e'p0) Angular Correlations NUCLEAR REACTIONS 12C, 16O(e, e'p), E not given; measured σ(θ(e'), θ(p)) vs energy transfer. 12C, 16O deduced GDR amplitudes features.
doi: 10.1016/0375-9474(91)90126-Q
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
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
1980AL04 Phys.Rev.Lett. 44, 965 (1980) R.Altemus, A.Cafolla, D.Day, J.S.McCarthy, R.R.Whitney, J.E.Wise Longitudinal and Transverse Inelastic Electron Scattering from 56Fe NUCLEAR REACTIONS 56Fe(e, e'), E ≈ 100-369 MeV; measured σ; deduced longitudinal, transverse response functions.
doi: 10.1103/PhysRevLett.44.965
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