NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = B.D.Serot Found 36 matches. 2012SE04 Phys.Rev. C 86, 015501 (2012) Neutrino production of photons and pions from nucleons in a chiral effective field theory for nuclei
doi: 10.1103/PhysRevC.86.015501
2012ZH38 Phys.Rev. C 86, 035502 (2012) Incoherent neutrino production of photons and pions in a chiral effective field theory for nuclei NUCLEAR REACTIONS 12C(e, e'), E=620, 680, 730 MeV; calculated differential σ(E, θ). 12C(ν, X), (ν-bar, X), E=250-600 MeV; calculated incoherent pion and photon production σ(E). Lorentz-covariant effective field theory (EFT). Comparison with experimental data. Relevance to background analysis in neutrino-oscillation experiments such as MiniBooNE collaboration. 12C; calculated proton and neutron densities with G1 and G2 parameter sets.
doi: 10.1103/PhysRevC.86.035502
2012ZH39 Phys.Rev. C 86, 035504 (2012) Coherent neutrino production of photons and pions in a chiral effective field theory for nuclei NUCLEAR REACTIONS 12C(γ, γ'), E=173, 235, 290 MeV; calculated differential σ(E, θ). 12C(ν, X), (ν-bar, X), E=250-600 MeV; calculated coherent pion and photon production σ(E). Lorentz-covariant effective field theory (EFT). Comparison with experimental data. Relevance to background analysis in neutrino-oscillation experiments such as MiniBooNE collaboration. 12C; calculated proton and neutron densities with G1 and G2 parameter sets.
doi: 10.1103/PhysRevC.86.035504
2010SE01 Phys.Rev. C 81, 034305 (2010) Field-theoretic parametrization of low-energy nucleon form factors
doi: 10.1103/PhysRevC.81.034305
2007HU21 Nucl.Phys. A794, 187 (2007) Two-loop corrections for nuclear matter in a covariant effective field theory
doi: 10.1016/j.nuclphysa.2007.08.005
2007MC05 Nucl.Phys. A794, 166 (2007) Loop corrections and naturalness in a chiral effective field theory
doi: 10.1016/j.nuclphysa.2007.08.008
2007SE15 Ann.Phys.(New York) 322, 2811 (2007) Electromagnetic interactions in a chiral effective lagrangian for nuclei
doi: 10.1016/j.aop.2007.04.003
2002AN29 Phys.Rev. C 66, 055502 (2002) S.M.Ananyan, B.D.Serot, J.Di.Walecka Axial-vector current in nuclear many-body physics
doi: 10.1103/PhysRevC.66.055502
2000FU02 Nucl.Phys. A663-664, 513c (2000) Effective Field Theory and Nuclear Mean-Field Models
doi: 10.1016/S0375-9474(99)00644-2
2000FU04 Nucl.Phys. A671, 447 (2000) Parameter Counting in Relativistic Mean-Field Models NUCLEAR STRUCTURE 16O, 208Pb; calculated energy contributions from relativistic mean field model terms; deduced parameter constraints, related features.
doi: 10.1016/S0375-9474(99)00839-8
2000FU07 Nucl.Phys. A673, 298 (2000) Large Lorentz Scalar and Vector Potentials in Nuclei
doi: 10.1016/S0375-9474(00)00146-9
1998FU04 Nucl.Phys. A632, 607 (1998) R.J.Furnstahl, J.J.Rusnak, B.D.Serot The Nuclear Spin-Orbit Force in Chiral Effective Field Theories NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; analyzed spin-orbit splitting; deduced role of tensor couplings of vector mesons.
doi: 10.1016/S0375-9474(98)00004-9
1997AL12 Phys.Rev. C55, 2704 (1997) Sudakov Form Factor in a Massive Vector Field Theory
doi: 10.1103/PhysRevC.55.2704
1997FU03 Nucl.Phys. A615, 441 (1997); Erratum Nucl.Phys. A640, 505 (1998) R.J.Furnstahl, B.D.Serot, H.-B.Tang A Chiral Effective Lagrangian for Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 88Sr, 208Pb; calculated binding energies, charge densities, form factors. Quantum chromodynamics approach, chiral effective hadronic lagrangian.
doi: 10.1016/S0375-9474(96)00472-1
1997FU05 Nucl.Phys. A618, 446 (1997) R.J.Furnstahl, B.D.Serot, H.-B.Tang Vacuum Nucleon Loops and Naturalness
doi: 10.1016/S0375-9474(97)00062-6
1997SE16 Int.J.Mod.Phys. E6, 515 (1997) Recent Progress in Quantum Hadrodynamics
doi: 10.1142/S0218301397000299
1996FU02 Nucl.Phys. A598, 539 (1996) R.J.Furnstahl, B.D.Serot, H.-B.Tang Analysis of Chiral Mean-Field Models for Nuclei NUCLEAR STRUCTURE 208Pb; calculated charge density, form factors. Chiral mean-field models.
doi: 10.1016/0375-9474(95)00488-2
1996MU07 Nucl.Phys. A606, 508 (1996) Relativistic Mean-Field Theory and the High-Density Nuclear Equation of State
doi: 10.1016/0375-9474(96)00187-X
1995FU06 Phys.Rev. C52, 1368 (1995) R.J.Furnstahl, J.-B.Tang, B.D.Serot Vacuum Contributions in a Chiral Effective Lagrangian for Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated rms charge radii, charge density, binding energy systematics. Relativistic hadronic model.
doi: 10.1103/PhysRevC.52.1368
1995MU16 Phys.Rev. C52, 2072 (1995) Phase Transitions in Warm, Asymmetric Nuclear Matter
doi: 10.1103/PhysRevC.52.2072
1995SE01 Phys.Rev. C51, 969 (1995) Two-Loop Calculations with Vertex Corrections in the Walecka Model
doi: 10.1103/PhysRevC.51.969
1993FU03 Phys.Rev. C47, 2338 (1993) Finite Nuclei in Relativistic Models with a Light Chiral Scalar Meson NUCLEAR STRUCTURE 40Ca, 208Pb; calculated charge density. 208Pb; calculated proton single-particle spectrum. Different mean field models, light chiral scalar meson.
doi: 10.1103/PhysRevC.47.2338
1993FU08 Phys.Lett. 316B, 12 (1993) Finite Nuclei in a Relativistic Model with Broken Chiral and Scale Invariance NUCLEAR STRUCTURE 208Pb; calculated charge density, proton single particle spectra. Relativistic hadronic model, broken chiral, scale invariances.
doi: 10.1016/0370-2693(93)90649-3
1988HA08 Phys.Rev. C37, 1111 (1988) S.Hama, B.C.Clark, R.E.Kozack, S.Shim, E.D.Cooper, R.L.Mercer, B.D.Serot Dirac Optical Potentials Constrained by a Dirac-Hartree Approach to Nuclear Structure NUCLEAR REACTIONS 16O, 48,40Ca, 90Zr, 208Pb(p, p), (polarized p, p), E=800 MeV; calculated σ(θ), polarization observables. Relativistic treatment.
doi: 10.1103/PhysRevC.37.1111
1987CO32 Phys.Rev. C36, 2170 (1987) E.D.Cooper, B.C.Clark, R.Kozack, S.Shim, S.Hama, J.I.Johansson, H.S.Sherif, R.L.Mercer, B.D.Serot Global Optical Potentials for Elastic p + 40Ca Scattering using the Dirac Equation NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=400 MeV; calculated σ(θ), analyzing power, spin rotation function vs θ; deduced global model parameters. Relativistic optical model.
doi: 10.1103/PhysRevC.36.2170
1987FU06 Nucl.Phys. A468, 539 (1987) Nuclear Currents in a Relativistic Mean-Field Theory NUCLEAR STRUCTURE 15N, 15,17O, 17F, 39K, 39,41Ca, 41Sc, 89Y, 91Zr, 209Bi, 207Pb; calculated μ. 22Na, 26Al, 30P, 34Cl, 54Co, 78Y, 82Nb; calculated isoscalar μ. Relativistic mean field theory. NUCLEAR REACTIONS 17O, 209Bi(e, e), E=175-500 MeV; calculated transverse form factors. Relativistic mean field theory.
doi: 10.1016/0375-9474(87)90182-5
1985FU13 Acta Phys.Pol. B16, 875 (1985) Nuclear Giant Resonances in a Relativistic Mean-Field Theory NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated isoscalar Coulomb, transverse form factors. Relativistic mean field theory. NUCLEAR STRUCTURE 40,48Ca, 90Zr, 208Pb; calculated isoscalar, isovector collective mode energies. A=40-240; analyzed isovector dipole, quadrupole, isoscalar quadrupole, octupole, monopole giant resonance systematics. Relativistic mean field theory.
1984CL05 Phys.Rev. C30, 314 (1984) B.C.Clark, S.Hama, E.Sugarbaker, M.A.Franey, R.L.Mercer, L.Ray, G.W.Hoffmann, B.D.Serot Relativistic Description of (p, n) Reactions to the Isobaric Analog State NUCLEAR REACTIONS 90Zr(polarized p, p), (polarized p, n), E=160, 500 MeV; calculated σ(θ), analyzing power vs θ, spin rotation function vs θ; deduced proton-nucleus optical potential parameters. Lane model, relativistic generalization.
doi: 10.1103/PhysRevC.30.314
1984CL11 Phys.Rev.Lett. 53, 1423 (1984) B.C.Clark, S.Hama, J.A.McNeil, R.L.Mercer, L.Ray, B.D.Serot, D.A.Sparrow, K.Stricker-Bauer Relative Impulse-Approximation Calculation of p(bar)-Nucleus Elastic Scattering NUCLEAR REACTIONS 12C(p-bar, p-bar), (polarized p-bar, p-bar), E=46.8 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Relativistic impulse approximation.
doi: 10.1103/PhysRevLett.53.1423
1984HO12 Phys.Lett. 140B, 181 (1984) Relativistic Hartree Theory of Finite Nuclei: The role of the quantum vacuum NUCLEAR STRUCTURE 208Pb; calculated total point baryon, scalar densities. Relativistic Hartree calculations.
doi: 10.1016/0370-2693(84)90916-X
1983CL04 Phys.Rev.Lett. 50, 1644 (1983) B.C.Clark, S.Hama, R.L.Mercer, L.Ray, B.D.Serot Dirac-Equation Impulse Approximation for Intermediate-Energy Nucleon-Nucleus Scattering NUCLEAR REACTIONS 40Ca, 208Pb(polarized p, p), E=497, 800 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ.
doi: 10.1103/PhysRevLett.50.1644
1983CL05 Phys.Rev. C28, 1421 (1983) B.C.Clark, S.Hama, R.L.Mercer, L.Ray, G.W.Hoffmann, B.D.Serot Energy Dependence of the Relativistic Impulse Approximation for Proton-Nucleus Elastic Scattering NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=181-1040 MeV; calculated σ(θ), analyzing power, spin rotation power vs θ. Relativistic, nonrelativistic impulse approximation.
doi: 10.1103/PhysRevC.28.1421
1981HO25 Nucl.Phys. A368, 503 (1981) Self-Consistent Hartree Description of Finite Nuclei in a Relativistic Quantum Field Theory NUCLEAR STRUCTURE 16O, 40Ca, 208Pb, 90Zr; calculated radii, nucleon binding energy, charge density distribution; 40,48Ca; calculated isotope shift. Self-consistent, relativistic Hartree-Fock equations.
doi: 10.1016/0375-9474(81)90770-3
1981SE17 Phys.Lett. 107B, 263 (1981) Elastic Electron-Nucleus Scattering in a Relativistic Theory of Nuclear Structure NUCLEAR REACTIONS 209Bi(e, e), E not given; calculated transverse form factor. Relativistic structure theory.
doi: 10.1016/0370-2693(81)90826-1
1979SE06 Nucl.Phys. A322, 408 (1979) Semileptonic Weak and Electromagnetic Interactions with Nuclei: Parity Violations in Electron Scattering and Abnormal-Parity Admixtures in Nuclear States NUCLEAR REACTIONS 12C, 13C(polarized e, e'), E at 30, 200 MeV/c, 1 GeV/c; calculated σ(θ); deduced one-body transition densities.
doi: 10.1016/0375-9474(79)90435-4
1979SE09 Phys.Lett. 87B, 172 (1979) Properties of Finite Nuclei in a Relativistic Quantum Field Theory NUCLEAR STRUCTURE 40Ca, 208Pb; calculated mass formula parameter, p-densities. Renormalizable relativistic quantum field theory.
doi: 10.1016/0370-2693(79)90957-2
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