NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = P.J.Ellis Found 69 matches. 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
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
2004MA49 Phys.Rev. C 69, 065206 (2004) Properties of the ω meson at finite temperature and density
doi: 10.1103/PhysRevC.69.065206
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
2003SH11 Phys.Rev. C 67, 048801 (2003) Optically opaque color-flavor locked phase inside compact stars
doi: 10.1103/PhysRevC.67.048801
2003TO01 Phys.Rev. C 67, 015208 (2003) Low energy pion-nucleon scattering in the heavy baryon and infrared schemes
doi: 10.1103/PhysRevC.67.015208
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
2002SH29 Phys.Rev. C66, 015802 (2002) Thermal Conductivity of Dense Quark Matter and Cooling of Stars
doi: 10.1103/PhysRevC.66.015802
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
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
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
2000EL01 Phys.Rev. C61, 015205 (2000) Baryon Masses in Chiral Perturbation Theory with Infrared Regularization
doi: 10.1103/PhysRevC.61.015205
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
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
1998CA04 Nucl.Phys. A628, 325 (1998) An Effective Lagrangian with Broken Scale and Chiral Symmetry IV: Nucleons and mesons at finite temperature
doi: 10.1016/S0375-9474(97)00640-4
1998EL09 Phys.Rev. C57, 3356 (1998) Pion-Nucleon Scattering in a New Approach to Chiral Perturbation Theory
doi: 10.1103/PhysRevC.57.3356
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
1997EL15 Phys.Rev. C56, 3363 (1997) Pion-Nucleon Scattering at Low Energies
doi: 10.1103/PhysRevC.56.3363
1996CA23 Nucl.Phys. A603, 367 (1996); Erratum Nucl.Phys. A608, 514 (1996) An Effective Lagrangian with Broken Scale and Chiral Symmetry II: Pion phenomenology
doi: 10.1016/0375-9474(96)80007-E
1996TA16 Phys.Lett. 387B, 9 (1996) Redundance of Δ-Isobar Parameters in Effective Field Theories
doi: 10.1016/0370-2693(96)00862-3
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
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
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
1995KN05 Phys.Rev. C52, 3470 (1995) R.Knorren, M.Prakash, P.J.Ellis Strangeness in Hadronic Stellar Matter
doi: 10.1103/PhysRevC.52.3470
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
1994HE13 Nucl.Phys. A571, 713 (1994) 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
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
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
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
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
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
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
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
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
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
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
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
1981FR02 Phys.Rev. C23, 787 (1981) 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
1980GO01 Nucl.Phys. A334, 229 (1980) 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
1980LI13 Phys.Rev. C22, 540 (1980) 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
1980MU13 Phys.Rev. C22, 2354 (1980) 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
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
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
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
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
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
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
1976EN03 Phys.Rev.Lett. 36, 994 (1976) 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
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
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
1976MO28 Phys.Lett. 64B, 386 (1976) 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
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
1974EL01 Phys.Lett. 49B, 23 (1974) 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
1974EL05 Phys.Lett. 52B, 31 (1974) 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
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
1973EL07 Part.Nucl. 5, 1 (1973); Erratum Part.Nucl. 6, 95 (1973) 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) RPA Renormalisation of the Effective Interaction in a Hartree-Fock Basis
doi: 10.1016/0370-2693(72)90435-2
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
1972EL17 Phys.Lett. 42B, 335 (1972) RPA Calculation of the Effective Charge in a Hartree-Fock Basis
doi: 10.1016/0370-2693(72)90501-1
1972EN03 Nucl.Phys. A181, 368 (1972) 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
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
1971EL07 Nucl.Phys. A175, 309 (1971) 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
1970EL08 Nucl.Phys. A152, 547 (1970) 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
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
1970EL23 Nucl.Phys. A144, 161 (1970) 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
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
1969EL05 Ann.Phys.(N.Y.) 55, 61 (1969) 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
1967EN01 Phys.Letters 25B, 57 (1967) Calculation of Particle-Hole States in the 2s-1d Shell
doi: 10.1016/0370-2693(67)90175-X
1965EL06 Proc.Phys.Soc.(London) 86, 422 (1965) 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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