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NSR database version of April 11, 2024.

Search: Author = J.P.Connelly

Found 19 matches.

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1998CO06      Phys.Rev. C57, 1569 (1998)

J.P.Connelly, B.L.Berman, W.J.Briscoe, K.S.Dhuga, A.Mokhtari, D.Zubanov, H.P.Blok, R.Ent, J.H.Mitchell, L.Lapikas

Trinucleon Cluster Knockout from 6Li

NUCLEAR REACTIONS 6Li(e, e'3He), E=484.5 MeV; 6Li(e, e't), E=456, 524 MeV; measured σ(E, θ) momentum transfer dependence; deduced two-step processes.

doi: 10.1103/PhysRevC.57.1569
Citations: PlumX Metrics

1995PE01      Phys.Rev. C51, 1014 (1995)

M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, S.Raman

Low-Multipolarity Magnetic Transitions in 40Ca Excited by 180° Electron Scattering

NUCLEAR REACTIONS Ca, S(e, e'), E=28.4-56.5 MeV; measured σ(θ); deduced σ. 40Ca levels deduced B(λ). Model comparison.

doi: 10.1103/PhysRevC.51.1014
Citations: PlumX Metrics

1994PE08      Phys.Rev. C49, 3000 (1994)

M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, R.Lindgren, S.Raman

Low-Multipolarity Magnetic Transitions in 30Si, 32S, and 34S Studied by 180° Electron Scattering

NUCLEAR REACTIONS 30Si, 32,34S(e, e'), E=28.4-63.4 MeV; measured spectra, σ. 32,34S, 30Si deduced M1, M2 transition strength fragmentation features.

doi: 10.1103/PhysRevC.49.3000
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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1992CO03      Phys.Lett. 277B, 383 (1992)

J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, S.Raman, J.R.Deininger, S.E.Williamson

Magnetic Dipole Strength in 46Ca Observed with 180° Electron Scattering

NUCLEAR REACTIONS 46Ca(e, e'), E=32.9-63.1 MeV; measured σ(E(e')), θ=180°; deduced σ(θ). 46Ca level deduced reduced transition rate, transition radius, B(λ).

doi: 10.1016/0370-2693(92)91798-E
Citations: PlumX Metrics

1992CO07      Phys.Rev. C45, 2494 (1992)

J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, J.R.Deininger, S.E.Williamson

Low-Momentum-Tranfer 180° Electron Scattering from the 3.68 MeV (3/2)- and the 3.85 MeV (5/2)+ States in 13C

NUCLEAR REACTIONS 13C(e, e'), E=28.5-56.5 MeV; measured σ(E(e')), σ(θ), transverse form factors. 13C levels deduced B(λ).

doi: 10.1103/PhysRevC.45.2494
Citations: PlumX Metrics

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

1992OB01      Nucl.Instrum.Methods Phys.Res. A312, 531 (1992)

J.T.O'Brien, D.I.Sober, L.W.Fagg, H.Crannell, M.Petraitis, J.P.Connelly, J.R.Deininger, S.E.Williamson

Design and Testing of Apparatus for 180° Electron Scattering at Low Momentum-Transfer

NUCLEAR REACTIONS 28Si, 13C(e, e), E=53 MeV; measured electron spectra, before, after focal plane corrections. Low momentum transfer, 180° electron scattering appartus design and testing.

doi: 10.1016/0168-9002(92)90201-E
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

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
Citations: PlumX Metrics

1990HA09      Phys.Rev. C41, 1619 (1990)

K.Hansen, J.-O.Adler, K.I.Blomqvist, D.Nilsson, A.Sandell, B.Schroder, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, J.R.Calarco, J.P.Connelly, F.W.Hersman, W.Kim, M.Leuschner

Electrofission in the Quasifree and Delta Regions

NUCLEAR REACTIONS 233,238U(e, e'F), E=720-830 MeV; measured σ(E, θ), fission probability; deduced mean nuclear excitation energy. Parallel plate avalanche detector.

doi: 10.1103/PhysRevC.41.1619
Citations: PlumX Metrics

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
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

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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