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NSR database version of April 11, 2024.

Search: Author = J.E.Wise

Found 22 matches.

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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

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
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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
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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
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

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
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
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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
Citations: PlumX Metrics

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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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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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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