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NSR database version of May 22, 2024.

Search: Author = P.J.Ellis

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2005EL05      Phys.Rev. C 71, 034301 (2005)

P.J.Ellis, T.Engeland, M.Hjorth-Jensen, M.P.Kartamyshev, E.Osnes

Model calculation of effective three-body forces

doi: 10.1103/PhysRevC.71.034301
Citations: PlumX Metrics

2005ST17      Phys.Rep. 411, 325 (2005)

A.W.Steiner, M.Prakash, J.M.Lattimer, P.J.Ellis

Isospin asymmetry in nuclear and neutron stars

doi: 10.1016/j.physrep.2005.02.004
Citations: PlumX Metrics

2004MA49      Phys.Rev. C 69, 065206 (2004)

A.T.Martell, P.J.Ellis

Properties of the ω meson at finite temperature and density

doi: 10.1103/PhysRevC.69.065206
Citations: PlumX Metrics

2004MO31      Phys.Rev. C 70, 015204 (2004)

A.Mocsy, I.N.Mishustin, P.J.Ellis

Role of fluctuations in the linear σ model with quarks

doi: 10.1103/PhysRevC.70.015204
Citations: PlumX Metrics

2003SH11      Phys.Rev. C 67, 048801 (2003)

I.A.Shovkovy, P.J.Ellis

Optically opaque color-flavor locked phase inside compact stars

doi: 10.1103/PhysRevC.67.048801
Citations: PlumX Metrics

2003TO01      Phys.Rev. C 67, 015208 (2003)

K.Torikoshi, P.J.Ellis

Low energy pion-nucleon scattering in the heavy baryon and infrared schemes

doi: 10.1103/PhysRevC.67.015208
Citations: PlumX Metrics

2002HU11      Phys.Rev. C66, 014903 (2002)

P.Huovinen, M.Belkacem, P.J.Ellis, J.I.Kapusta

Dileptons and Photons from Coarse-Grained Microscopic Dynamics and Hydrodynamics Compared to Experimental Data

NUCLEAR REACTIONS Au, Pb(Pb, X), E=158 GeV/nucleon; calculated dilepton and photon spectra. Relativistic hydrodynamics, comparison with data.

doi: 10.1103/PhysRevC.66.014903
Citations: PlumX Metrics

2002SH29      Phys.Rev. C66, 015802 (2002)

I.A.Shovkovy, P.J.Ellis

Thermal Conductivity of Dense Quark Matter and Cooling of Stars

doi: 10.1103/PhysRevC.66.015802
Citations: PlumX Metrics

2001EL07      Phys.Rev. C64, 035202 (2001)

V.L.Eletsky, M.Belkacem, P.J.Ellis, J.I.Kapusta

Properties of ρ and ω Mesons at Finite Temperature and Density as Inferred from Experiment

doi: 10.1103/PhysRevC.64.035202
Citations: PlumX Metrics

2000CA09      Phys.Rev. C61, 045206 (2000)

G.W.Carter, O.Scavenius, I.N.Mishustin, P.J.Ellis

Effective Model for Hot Gluodynamics

doi: 10.1103/PhysRevC.61.045206
Citations: PlumX Metrics

2000CS04      Phys.Rev. C61, 054901 (2000)

L.P.Csernai, P.J.Ellis, S.Jeon, J.I.Kapusta

Dynamical Evolution of the Scalar Condensate in Heavy Ion Collisions

doi: 10.1103/PhysRevC.61.054901
Citations: PlumX Metrics

2000EL01      Phys.Rev. C61, 015205 (2000)

P.J.Ellis, K.Torikoshi

Baryon Masses in Chiral Perturbation Theory with Infrared Regularization

doi: 10.1103/PhysRevC.61.015205
Citations: PlumX Metrics

2000PO17      Phys.Rev. C62, 035803 (2000)

J.A.Pons, S.Reddy, P.J.Ellis, M.Prakash, J.M.Lattimer

Kaon Condensation in Proto-Neutron Star Matter

doi: 10.1103/PhysRevC.62.035803
Citations: PlumX Metrics

1999SH22      Phys.Rev. C59, 2931 (1999)

I.A.Shushpanov, J.I.Kapusta, P.J.Ellis

Low-Energy Theorems for QCD at Finite Temperature and Chemical Potential

doi: 10.1103/PhysRevC.59.2931
Citations: PlumX Metrics

1998CA04      Nucl.Phys. A628, 325 (1998)

G.W.Carter, P.J.Ellis

An Effective Lagrangian with Broken Scale and Chiral Symmetry IV: Nucleons and mesons at finite temperature

doi: 10.1016/S0375-9474(97)00640-4
Citations: PlumX Metrics

1998EL09      Phys.Rev. C57, 3356 (1998)

P.J.Ellis, H.-B.Tang

Pion-Nucleon Scattering in a New Approach to Chiral Perturbation Theory

doi: 10.1103/PhysRevC.57.3356
Citations: PlumX Metrics

1997CA18      Nucl.Phys. A618, 317 (1997)

G.W.Carter, P.J.Ellis, S.Rudaz

An Effective Lagrangian with Broken Scale and Chiral Symmetry III. Mesons at Finite Temperature

doi: 10.1016/S0375-9474(97)00048-1
Citations: PlumX Metrics

1997EL15      Phys.Rev. C56, 3363 (1997)

P.J.Ellis, H.-B.Tang

Pion-Nucleon Scattering at Low Energies

doi: 10.1103/PhysRevC.56.3363
Citations: PlumX Metrics

1996CA23      Nucl.Phys. A603, 367 (1996); Erratum Nucl.Phys. A608, 514 (1996)

G.Carter, P.J.Ellis, S.Rudaz

An Effective Lagrangian with Broken Scale and Chiral Symmetry II: Pion phenomenology

doi: 10.1016/0375-9474(96)80007-E
Citations: PlumX Metrics

1996TA16      Phys.Lett. 387B, 9 (1996)

H.-B.Tang, P.J.Ellis

Redundance of Δ-Isobar Parameters in Effective Field Theories

doi: 10.1016/0370-2693(96)00862-3
Citations: PlumX Metrics

1995BO09      Nucl.Phys. A583, 623c (1995)

I.Bombaci, M.Prakash, M.Prakash, P.J.Ellis, J.M.Lattimer, G.E.Brown

Newborn Hot Neutron Stars

doi: 10.1016/0375-9474(94)00736-7
Citations: PlumX Metrics

1995EL05      Phys.Lett. 349B, 11 (1995)

P.J.Ellis, R.Knorren, M.Prakash

Kaon Condensation in Neutron Star Matter with Hyperons

doi: 10.1016/0370-2693(95)00231-9
Citations: PlumX Metrics

1995EL12      Phys.Lett. 361B, 5 (1995)

P.J.Ellis, S.B.Parendo, M.Prakash

Role of Hyperon Negative Energy Sea in Nuclear Matter

doi: 10.1016/0370-2693(95)01161-I
Citations: PlumX Metrics

1995KN05      Phys.Rev. C52, 3470 (1995)

R.Knorren, M.Prakash, P.J.Ellis

Strangeness in Hadronic Stellar Matter

doi: 10.1103/PhysRevC.52.3470
Citations: PlumX Metrics

1994EL07      Nucl.Phys. A573, 216 (1994)

P.J.Ellis, T.Engeland, M.Hjorth-Jensen, A.Holt, E.Osnes

Convergence Properties of the Effective Interaction

NUCLEAR STRUCTURE 18O; calculated level energy vs starting energy. Folded diagram, Lee-Suzuki models comparison.

doi: 10.1016/0375-9474(94)90168-6
Citations: PlumX Metrics

1994HE13      Nucl.Phys. A571, 713 (1994)

E.K.Heide, S.Rudaz, P.J.Ellis

An Effective Lagrangian with Broken Scale and Chiral Symmetry Applied to Nuclear Matter and Finite Nuclei

NUCLEAR STRUCTURE 40Ca, 208Pb, 16O; calculated charge density. Mean field approximation, chiral lagrangian.

doi: 10.1016/0375-9474(94)90717-X
Citations: PlumX Metrics

1994PR06      Nucl.Phys. A575, 583 (1994)

M.Prakash, P.J.Ellis, E.K.Heide, S.Rudaz

Neutron Stars and Nuclei in the Modified Relativistic Hartree Approximation

NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated binding energy per nucleon, charge density, charge radius with fitted m(σ). Modified relativistic Hartree approximation. Neutron rich matter studied.

doi: 10.1016/0375-9474(94)90376-X
Citations: PlumX Metrics

1994TZ01      Nucl.Phys. A580, 277 (1994)

S.Y.T.Tzeng, P.J.Ellis, T.T.S.Kuo, E.Osnes

Finite-Temperature Many-Body Theory with the Lipkin Model

doi: 10.1016/0375-9474(94)90774-9
Citations: PlumX Metrics

1991MA33      Nucl.Phys. A530, 251 (1991)

H.A.Mavromatis, P.J.Ellis, H.Muther

Super-RPA Ground-State Correlations

NUCLEAR STRUCTURE 16O; calculated ground state correlation energies. New RPA approach.

doi: 10.1016/0375-9474(91)90802-D
Citations: PlumX Metrics

1988HA14      Phys.Rev. C37, 1554 (1988)

A.C.Hayes, S.Chakravarti, D.Dehnhard, P.J.Ellis, D.B.Holtkamp, L.-P.Lung, S.J.Seestrom-Morris, H.Baer, C.L.Morris, S.J.Greene, C.J.Harvey

Structure of the Low-Lying 2+ States in 14C from Inelastic Pion Scattering

NUCLEAR STRUCTURE 14C, 14N, 14O; calculated levels, B(λ). Shell model.

NUCLEAR REACTIONS 14C(π, π'), E=164 MeV; analyzed σ(θ). 14C level deduced isovector component quenching.

doi: 10.1103/PhysRevC.37.1554
Citations: PlumX Metrics

1986EL02      Phys.Rev. C34, 348 (1986)

P.J.Ellis, Q.K.K.Liu, S.Chakravarti

Spin-Flip Probability in the 12C(13C, 13C')12C(*)(2+) Reaction

NUCLEAR REACTIONS 12C(13C, 13C'), E=87 MeV; calculated σ(θ); deduced spin-flip probability, model parameters. 12C level population probability.

doi: 10.1103/PhysRevC.34.348
Citations: PlumX Metrics

1986EL04      Nucl.Phys. A458, 269 (1986)

P.J.Ellis, Z.El-Itaoui, M.A.Franey, B.A.Mughrabi

Inelastic Excitation and the Nucleon Optical Potential

NUCLEAR REACTIONS 40Ca(p, p), (p, p'), (n, n), 208Pb(p, p), (n, n), E=30 MeV; calculated σ(θ). Approximate polarization potentials, optical model, coupled channels calculations.

doi: 10.1016/0375-9474(86)90357-X
Citations: PlumX Metrics

1985EL07      Nucl.Phys. A441, 511 (1985)

Z.El-Itaoui, P.J.Ellis, B.A.Mughrabi

The Contribution of Nuclear Inelastic Excitation to the Optical Potential for Heavy Ions

NUCLEAR REACTIONS 40Ca(13C, 13C), (13C, 13C'), E=68 MeV; calculated σ(θ). 208Pb(16O, 16O), E=104 MeV; calculated imaginary, potential parameters; deduced nuclear inelastic excitation role. Plane wave approximation, analytical polarization potential expressions.

doi: 10.1016/0375-9474(85)90160-5
Citations: PlumX Metrics

1984BL17      Phys.Rev. C30, 1989 (1984)

C.L.Blilie, D.Dehnhard, M.A.Franey, D.H.Gay, D.B.Holtkamp, S.J.Seestrom-Morris, P.J.Ellis, C.L.Morris, D.J.Millener

Isospin Structure of Transitions in 17O from Inelastic Pion Scattering at 164 MeV

NUCLEAR REACTIONS 16,17O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 17O deduced M4, E2 transition strength distribution. Microscopic DWIA calculations.

doi: 10.1103/PhysRevC.30.1989
Citations: PlumX Metrics

1984LI14      Phys.Lett. 143B, 60 (1984)

Q.K.K.Liu, P.J.Ellis, S.Chakravarti

Spin Flip in the 24Mg(13C, 13C')24Mg(*)(2+) Inelastic Reaction

NUCLEAR REACTIONS 24Mg(13C, 13C'), E=35 MeV; calculated spin-flip probability vs θ; deduced projectile, 25Mg intermediate state excitation role. DWBA, coupled reaction channels formalisms.

doi: 10.1016/0370-2693(84)90804-9
Citations: PlumX Metrics

1984MU01      Phys.Rev. C29, 29 (1984)

B.A.Mughrabi, Z.El Itaoui, P.J.Ellis, Y.C.Tang

Coupled-Channel and Spin-Orbit Effects in Proton - 6Li Scattering

NUCLEAR REACTIONS 6Li(p, p), (p, p'), E=14.5, 25.9, 45.4, 49.75 MeV; analyzed σ(θ), polarization vs θ. 6Li(p, p), E=1-5.5 MeV; calculated phase shifts vs E. Coupled-channels method, spin-orbit nucleon-nucleon potential.

doi: 10.1103/PhysRevC.29.29
Citations: PlumX Metrics

1983CH01      Phys.Rev. C27, 143 (1983)

S.Chakravarti, P.J.Ellis, B.F.Bayman, Q.K.K.Liu

Inelastic Excitation and Spin Flip in Heavy Ion Reactions

NUCLEAR REACTIONS 24Mg(13C, 13C'), E=35 MeV; analyzed σ(θ), projectile, target polarization, spin-flip probability vs θ. Coupled-channels method.

doi: 10.1103/PhysRevC.27.143
Citations: PlumX Metrics

1981FR02      Phys.Rev. C23, 787 (1981)

M.A.Franey, P.J.Ellis

Coulomb and Nuclear Inelastic Excitations and the Optical Potential for Heavy Ions

NUCLEAR REACTIONS 152Sm(16O, 16O), E=72 MeV; 40Ca(13C, 13C'), E=68 MeV; analyzed σ(θ); deduced optical potential. Coupled-channels analysis.

doi: 10.1103/PhysRevC.23.787
Citations: PlumX Metrics

1980GO01      Nucl.Phys. A334, 229 (1980)

F.L.Goodin, P.J.Ellis

Study of Effective Operators in the 16O Region

NUCLEAR STRUCTURE 18O, 18F; calculated levels, effective operators. Hartree-Fock basis, self-consistent coupled equations, doubly-partitioned G-matrix.

doi: 10.1016/0375-9474(80)90066-4
Citations: PlumX Metrics

1980LI13      Phys.Rev. C22, 540 (1980)

Q.K.K.Liu, P.J.Ellis

Spin-Flip Systematics and Spin-Orbit Potentials in Heavy-Ion Inelastic Scattering

NUCLEAR REACTIONS 24Mg(13C, 13C'), E=35 MeV; analyzed σ(θ). 24Mg level deduced spin-flip probability. Coupled channel calculation.

doi: 10.1103/PhysRevC.22.540
Citations: PlumX Metrics

1980MU13      Phys.Rev. C22, 2354 (1980)

B.Mughrabi, P.J.Ellis

g-Shell Admixtures and the 19F(3He, d)20Ne*(4+)Reaction

NUCLEAR REACTIONS 19F(3He, d), E=10-23 MeV; analyzed σ(θ); deduced reaction mechanism. 20Ne level deduced g-shell admixtures. CCBA, source method.

NUCLEAR STRUCTURE 2H; calculated electromagnetic form factors, D-state probability, magnetic moment. Bethe-Salpeter equation, one boson exchange.

doi: 10.1103/PhysRevC.22.2354
Citations: PlumX Metrics

1979EL01      Phys.Rev. C19, 536 (1979)

P.J.Ellis, M.Strayer, M.F.Werby

Two-Step Process (p, 3He)(3He, t) in the 48Ca(p, t)46Ca Reaction

NUCLEAR REACTIONS 48Ca(p, t), E=41.7 MeV; calculated two-step (p, 3He)(3He, t) contribution to σ(θ).

doi: 10.1103/PhysRevC.19.536
Citations: PlumX Metrics

1978BA26      Nucl.Phys. A301, 141 (1978)

B.F.Bayman, A.Dudek-Ellis, P.J.Ellis

Spin-Dependent Effects in Heavy-Ion Reactions

NUCLEAR REACTIONS 40Ca(13C, 14N), (13C, 12C), E=60, 68 MeV; calculated σ(θ). DWBA calculations.

doi: 10.1016/0375-9474(78)90134-3
Citations: PlumX Metrics

1978DU07      Phys.Rev. C18, 158 (1978)

A.Dudek-Ellis, V.Shkolnik, J.L.Artz, D.Dehnhard, P.J.Ellis, H.P.Morsch

30Si(16O, 16O')30Si* Reaction at 60 MeV

NUCLEAR REACTIONS 30Si(16O, 16O), (16O, 16O'), E=60 MeV; measured σ(θ). Coupled channels analysis.

doi: 10.1103/PhysRevC.18.158
Citations: PlumX Metrics

1978EL08      Nucl.Phys. A302, 257 (1978)


On Polarization in Heavy Ion Reactions

NUCLEAR REACTIONS 29Si(19F, 16O), 40Ca(13C, 14N); calculated polarization parameters.

doi: 10.1016/0375-9474(78)90298-1
Citations: PlumX Metrics

1977KU04      Phys.Rev.Lett. 38, 817 (1977)

S.Kubono, D.Dehnhard, D.A.Lewis, T.K.Li, J.L.Artz, D.J.Weber, P.J.Ellis, A.Dudek-Ellis

j Dependence of the (19F, 16O) Reaction and Spin-Orbit Forces in the Heavy-Ion Optical Potential

NUCLEAR REACTIONS 28,30Si(19F, 16O), E=60 MeV; measured σ(θ).

doi: 10.1103/PhysRevLett.38.817
Citations: PlumX Metrics

1976BR37      Nucl.Phys. A273, 69 (1976)

A.S.Broad, D.A.Lewis, W.S.Gray, P.J.Ellis, A.Dudek-Ellis

Inelastic Processes and Form Factors in the 162,164Dy(3He, d) Reactions at 46.5 MeV

NUCLEAR REACTIONS 162,164Dy(3He, d), E=46.5 MeV; calculated σ(Ed, θ). 163,165Ho levels deduced form factors. CCBA, DWBA analysis.

doi: 10.1016/0375-9474(76)90301-8
Citations: PlumX Metrics

1976EN03      Phys.Rev.Lett. 36, 994 (1976)

T.Engeland, P.J.Ellis

Comment on the Quadrupole Moment of the First-Excited 2+ State of 18O

NUCLEAR MOMENTS 18O; analyzed data on first 2+ level quadrupole moment.

doi: 10.1103/PhysRevLett.36.994
Citations: PlumX Metrics

1976FI01      Nucl.Phys. A258, 317 (1976)

M.A.Firestone, J.Janecke, A.Dudek-Ellis, P.J.Ellis, T.Engeland

The 16O(d, 3He)15N Reaction at 29 Mev: Reaction Mechanism and Nuclear Structure

NUCLEAR REACTIONS 16O(d, 3He), E=29 MeV; measured σ(E(3He), θ). 15N deduced levels, J, π, S. Coupled channels, DWBA analysis.

doi: 10.1016/0375-9474(76)90009-9
Citations: PlumX Metrics

1976LI01      Phys.Rev. C13, 55 (1976)

T.K.Li, D.Dehnhard, R.E.Brown, P.J.Ellis

Investigation of the (d, 5/2)2 and (d5/2s1/2) Two-Particle Configurations in 18O Using the 17O(d, p)18O Reaction at 18 MeV

NUCLEAR REACTIONS 17O(d, d), E=18.0 MeV; measured σ(θ); deduced optical model parameters. 17O(d, p), E=18.0 MeV; measured σ(Ep, θ). 18O levels deduced L, S. Enriched target.

doi: 10.1103/PhysRevC.13.55
Citations: PlumX Metrics

1976MO28      Phys.Lett. 64B, 386 (1976)

H.P.Morsch, P.J.Ellis

On the Role of Indirect Processes in the Inelastic Excitation of Low Lying 0+ States

NUCLEAR REACTIONS 24Mg, 28Si(α, α'), E=23.5 MeV; 46Ti(3He, 3He), E=29 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(76)90102-7
Citations: PlumX Metrics

1974AN36      Phys.Rep. 12, 201 (1974)

N.Anyas-Weiss, J.C.Cornell, P.S.Fisher, P.N.Hudson, A.Menchaca-Rocha, D.J.Millener, A.D.Panagiotou, D.K.Scott, D.Strottman, D.M.Brink, B.Buck, P.J.Ellis, T.Engeland

Nuclear structure of light nuclei using the selectivity of high energy transfer reactions with heavy ions

NUCLEAR REACTIONS 12C, 16O, 40Ca(12C, 11B), (12C, 11C), (12C, 10B), (12C, 10Be), (12C, 10C), (12C, 9Be), E=114 MeV; 12,13C(11B, 9Li), E=114 MeV; 13C(11B, 10B), E=114 MeV; measured particle spectra, σ(E, θ). 13,14C, 13,14,15N, 14,15O deduced levels, J, π, spectroscopic amplitudes.

doi: 10.1016/0370-1573(74)90045-3
Citations: PlumX Metrics

1974EL01      Phys.Lett. 49B, 23 (1974)

P.J.Ellis, E.Osnes

Monopole Core Polarization in a Hartree-Fock Basis

NUCLEAR STRUCTURE 16O; calculated particle-hole states, monopole core polarization.

doi: 10.1016/0370-2693(74)90571-1
Citations: PlumX Metrics

1974EL05      Phys.Lett. 52B, 31 (1974)

P.J.Ellis, E.Osnes

On Possible Collective Effects in the Positive Parity Particle-Hole States of 16O

NUCLEAR STRUCTURE 16O; calculated levels.

doi: 10.1016/0370-2693(74)90710-2
Citations: PlumX Metrics

1974VE03      Nucl.Phys. A223, 207 (1974)

T.Vertse, A.Dudek-Ellis, P.J.Ellis, T.A.Belote, D.Roaf

Inelastic Processes in the 19F(3He, d)20Ne Reaction

NUCLEAR REACTIONS 19F(3He, d), (3He, 3He'), (3He, 3He), E=16.00 MeV; measured σ(Ed, θ), σ(E(3He), θ). 20Ne levels deduced effect of inelastic processes on S.

doi: 10.1016/0375-9474(74)90287-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0792.

1973EL07      Part.Nucl. 5, 1 (1973); Erratum Part.Nucl. 6, 95 (1973)

P.J.Ellis, A.Dudek

Inelastic Effects in Direct Reactions; 20Ne(d, 3He)19F

NUCLEAR REACTIONS 20Ne(d, 3He), E=51.7 MeV; 20Ne(d, d'), E=52 MeV; calculated σ(θ). 19F level deduced L.

1972EL13      Phys.Lett. 41B, 97 (1972)

P.J.Ellis, E.Osnes

RPA Renormalisation of the Effective Interaction in a Hartree-Fock Basis

doi: 10.1016/0370-2693(72)90435-2
Citations: PlumX Metrics

1972EL14      Nucl.Phys. A196, 161 (1972)

P.J.Ellis, A.D.Jackson, E.Osnes

On the Number-Conserving Sets

doi: 10.1016/0375-9474(72)90958-X
Citations: PlumX Metrics

1972EL17      Phys.Lett. 42B, 335 (1972)

P.J.Ellis, E.Osnes

RPA Calculation of the Effective Charge in a Hartree-Fock Basis

doi: 10.1016/0370-2693(72)90501-1
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1972EN03      Nucl.Phys. A181, 368 (1972)

T.Engeland, P.J.Ellis

The Weak Coupling Model Applied to the Nuclei with A = 16-19. (II). Gamma Transitions and Spectroscopic Factors

NUCLEAR STRUCTURE 16O, 17O, 18O, 17,18,19F, 18,19Ne; calculated γ-transition rates, level-width, S, B(λ). Weak coupling model.

doi: 10.1016/0375-9474(72)90490-3
Citations: PlumX Metrics

1972SC21      Phys.Rev.Lett. 28, 1659 (1972)

D.K.Scott, P.N.Hudson, P.S.Fisher, C.U.Cardinal, N.Anyas-Weiss, A.D.Panagiotou, P.J.Ellis

Selective Excitation of One-, Two-, and Three-Nucleon Configurations in Transfer Reactions Induced by Heavy Ions

NUCLEAR REACTIONS 12C, 16O, 40Ca(12C, 12C), (12C, 11C), (12C, 11B), (12C, 10C), (12C, 10B), (12C, 10Be), (12C, 9Be), E=114 MeV; measured charged particle spectra.

doi: 10.1103/PhysRevLett.28.1659
Citations: PlumX Metrics

1971EL07      Nucl.Phys. A175, 309 (1971)

P.J.Ellis, H.A.Mavromatis

Hartree-Fock Contributions to the Effective Charge and Interaction in the sd Shell

NUCLEAR STRUCTURE 18O, 18F; calculated levels. 2nd-order perturbation theory diagrams for the effective charge.

doi: 10.1016/0375-9474(71)90285-5
Citations: PlumX Metrics

1970EL08      Nucl.Phys. A152, 547 (1970)

P.J.Ellis, S.Siegel

Higher-Order Bubble Corrections to Two-Body Matrix Elements in the 1s 0d Shell

NUCLEAR STRUCTURE 18O, 18F, 17O, 18Ne; calculated levels, B(E2). 17O; calculated quadrupole moment.

doi: 10.1016/0375-9474(70)90931-0
Citations: PlumX Metrics

1970EL14      Nucl.Phys. A155, 625 (1970)


RPA Ground State Correlations from Perturbation Theory

NUCLEAR STRUCTURE 16O; calculated ground-state correlations. RPA.

doi: 10.1016/0375-9474(70)90917-6
Citations: PlumX Metrics

1970EL23      Nucl.Phys. A144, 161 (1970)

P.J.Ellis, T.Engeland

The weak coupling model applied to the nuclei with A = 16–19: (I). Energy levels

NUCLEAR STRUCTURE 16,17,18O, 18,19F; calculated energy levels, J, π; deduced particle-hole states by coupling in J and T eigenfunctions resulting from diagonalization of (sd)n1 and pn2, positive parity levels.

doi: 10.1016/0375-9474(70)90499-9
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1970GR02      Nucl.Phys. A140, 494 (1970)

W.S.Gray, P.J.Ellis, T.Wei, R.M.Polichar, J.Janecke

Study of the Structure of 36S and 38Ar

NUCLEAR REACTIONS 37Cl, 39K(d, 3He), E=28.9 MeV; measured Q, σ (E(3He), θ). 36S, 38Ar deduced levels, L(p), J, π, S. Enriched 37Cl target.

doi: 10.1016/0375-9474(70)90576-2
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1969EL05      Ann.Phys.(N.Y.) 55, 61 (1969)

P.J.Ellis, L.Zamick

Comparison of Various Approximations for the Ground State of 16O

NUCLEAR STRUCTURE 16O; calculated ground-state energy. 2p-2h correlations.

doi: 10.1016/0003-4916(69)90306-6
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1967EN01      Phys.Letters 25B, 57 (1967)

T.Engeland, P.J.Ellis

Calculation of Particle-Hole States in the 2s-1d Shell

doi: 10.1016/0370-2693(67)90175-X
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1965EL06      Proc.Phys.Soc.(London) 86, 422 (1965)

P.J.Ellis, D.Wilmore

The 3.92 to 1.98 MeV Transition in 18O

NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1088/0370-1328/86/2/122
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