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NSR database version of April 27, 2024.

Search: Author = B.D.Serot

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2012SE04      Phys.Rev. C 86, 015501 (2012)

B.D.Serot, X.Zhang

Neutrino production of photons and pions from nucleons in a chiral effective field theory for nuclei

doi: 10.1103/PhysRevC.86.015501
Citations: PlumX Metrics

2012ZH38      Phys.Rev. C 86, 035502 (2012)

X.Zhang, B.D.Serot

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
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2012ZH39      Phys.Rev. C 86, 035504 (2012)

X.Zhang, B.D.Serot

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
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2010SE01      Phys.Rev. C 81, 034305 (2010)

B.D.Serot

Field-theoretic parametrization of low-energy nucleon form factors

doi: 10.1103/PhysRevC.81.034305
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2007HU21      Nucl.Phys. A794, 187 (2007)

Y.Hu, J.McIntire, B.D.Serot

Two-loop corrections for nuclear matter in a covariant effective field theory

doi: 10.1016/j.nuclphysa.2007.08.005
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2007MC05      Nucl.Phys. A794, 166 (2007)

J.McIntire, Y.Hu, B.D.Serot

Loop corrections and naturalness in a chiral effective field theory

doi: 10.1016/j.nuclphysa.2007.08.008
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2007SE15      Ann.Phys.(New York) 322, 2811 (2007)

B.D.Serot

Electromagnetic interactions in a chiral effective lagrangian for nuclei

doi: 10.1016/j.aop.2007.04.003
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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
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2000FU02      Nucl.Phys. A663-664, 513c (2000)

R.J.Furnstahl, B.D.Serot

Effective Field Theory and Nuclear Mean-Field Models

doi: 10.1016/S0375-9474(99)00644-2
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2000FU04      Nucl.Phys. A671, 447 (2000)

R.J.Furnstahl, B.D.Serot

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
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2000FU07      Nucl.Phys. A673, 298 (2000)

R.J.Furnstahl, B.D.Serot

Large Lorentz Scalar and Vector Potentials in Nuclei

doi: 10.1016/S0375-9474(00)00146-9
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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
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1997AL12      Phys.Rev. C55, 2704 (1997)

M.P.Allendes, B.D.Serot

Sudakov Form Factor in a Massive Vector Field Theory

doi: 10.1103/PhysRevC.55.2704
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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
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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
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1997SE16      Int.J.Mod.Phys. E6, 515 (1997)

B.D.Serot, J.D.Walecka

Recent Progress in Quantum Hadrodynamics

doi: 10.1142/S0218301397000299
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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
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1996MU07      Nucl.Phys. A606, 508 (1996)

H.Muller, B.D.Serot

Relativistic Mean-Field Theory and the High-Density Nuclear Equation of State

doi: 10.1016/0375-9474(96)00187-X
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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
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1995MU16      Phys.Rev. C52, 2072 (1995)

H.Muller, B.D.Serot

Phase Transitions in Warm, Asymmetric Nuclear Matter

doi: 10.1103/PhysRevC.52.2072
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1995SE01      Phys.Rev. C51, 969 (1995)

B.D.Serot, H.-B.Tang

Two-Loop Calculations with Vertex Corrections in the Walecka Model

doi: 10.1103/PhysRevC.51.969
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1993FU03      Phys.Rev. C47, 2338 (1993)

R.J.Furnstahl, B.D.Serot

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
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1993FU08      Phys.Lett. 316B, 12 (1993)

R.J.Furnstahl, B.D.Serot

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
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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
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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
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1987FU06      Nucl.Phys. A468, 539 (1987)

R.J.Furnstahl, B.D.Serot

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
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1985FU13      Acta Phys.Pol. B16, 875 (1985)

R.J.Furnstahl, B.D.Serot

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
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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
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1984HO12      Phys.Lett. 140B, 181 (1984)

C.J.Horowitz, B.D.Serot

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
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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
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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
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1981HO25      Nucl.Phys. A368, 503 (1981)

C.J.Horowitz, B.D.Serot

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
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1981SE17      Phys.Lett. 107B, 263 (1981)

B.D.Serot

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
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1979SE06      Nucl.Phys. A322, 408 (1979)

B.D.Serot

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
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1979SE09      Phys.Lett. 87B, 172 (1979)

B.D.Serot, J.D.Walecka

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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