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NSR database version of May 10, 2024.

Search: Author = T.Milliman

Found 15 matches.

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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
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

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

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

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

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
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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1984RE02      Phys.Lett. 137B, 32 (1984)

W.Reuter, E.B.Shera, M.V.Hoehn, F.W.Hersman, T.Milliman, J.M.Finn, C.Hyde-Wright, R.Lourie, B.Pugh, W.Bertozzi

Nuclear Charge Densities in the Transition Region: 192Os

NUCLEAR REACTIONS 192Os(e, e), (e, e'), E=150, 250, 360 MeV; measured σ(E(e)). 192Os levels deduced transition densities, B(E2), rms radii, quadrupole moment. Muonic atom data input.

doi: 10.1016/0370-2693(84)91100-6
Citations: PlumX Metrics

1984RE10      Phys.Rev. C30, 1465 (1984)

W.Reuter, E.B.Shera, M.V.Hoehn, F.W.Hersman, T.Milliman, J.M.Finn, C.Hyde-Wright, R.Lourie, B.Pugh, W.Bertozzi

Ground-State and Transition Charge Densities in 192Os

NUCLEAR STRUCTURE 192Os, 194Pt; calculated proton densities, rms radius, quadrupole moment. 186Os; calculated rms radius, quadrupole moment. Hartree-Fock theory, other model comparisons.

NUCLEAR REACTIONS 192Os(e, e), (e, e'), E=150, 250, 355, 364 MeV; measured σ(θ), σ(E(e)). 192Os levels deduced B(λ), transition radii, charge density. Hartree-Fock calculations.

doi: 10.1103/PhysRevC.30.1465
Citations: PlumX Metrics

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Note: The following list of authors and aliases matches the search parameter T.Milliman: , T.E.MILLIMAN