NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.L.Friar Found 107 matches. Showing 1 to 100. [Next]2018HA38 Phys.Rev. C 98, 065505 (2018) Effect of Siegert's theorem on low-energy neutrino-nucleus interactions NUCLEAR REACTIONS 16O(ν, X), E=25-150 MeV; 12C(ν, e-), E=30-75 MeV electron neutrinos; calculated σ(E), and differential σ(θ) using Siegert's theorem; discussed importance of conserving the vector current in calculating low-energy neutrino-nucleus interactions. 12C(μ-, ν)12B, E not given; calculated capture rates to low lying states of 12B, with and without using Siegert's theorem, and compared with experimental values.
doi: 10.1103/PhysRevC.98.065505
2016WA21 Phys.Rev. C 94, 034314 (2016) X.B.Wang, J.L.Friar, A.C.Hayes Nuclear Zemach moments and finite-size corrections to allowed β decay RADIOACTIVITY 14C, 25Na, 35S, 45Ca, 61Cr, 64Co, 100,104Nb, 121Sn(β-); calculated charge density distribution of 120Sn, radial wave functions of the neutron in the parent nuclei and the proton in the daughter nuclei, single-density moments, and Zeemach moments from convoluted densities for allowed ground-state-to-ground-state β- decays. Hartree-Fock model using a Skyrme-like energy density functional. Discussed role of finite-size correction in β- decay in determining the expected antineutrino spectra from reactors.
doi: 10.1103/PhysRevC.94.034314
2014HA12 Phys.Rev.Lett. 112, 202501 (2014) A.C.Hayes, J.L.Friar, G.T.Garvey, G.Jungman, G.Jonkmans Systematic Uncertainties in the Analysis of the Reactor Neutrino Anomaly
doi: 10.1103/PhysRevLett.112.202501
2013FR12 Phys.Rev. C 88, 034003 (2013) Nuclear polarization corrections to μ-d atoms in zero-range approximation
doi: 10.1103/PhysRevC.88.034003
2009ST11 Phys.Rev. C 79, 064001 (2009) I.Stetcu, S.Quaglioni, J.L.Friar, A.C.Hayes, P.Navratil Electric dipole polarizabilities of hydrogen and helium isotopes NUCLEAR STRUCTURE 3H, He, 4He; calculated electric dipole polarizability using the Schrodinger equation. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064001
2008HA32 Phys.Rev. C 78, 024311 (2008) A.C.Hayes, J.L.Friar, P.Moller Splitting sensitivity of the ground and 7.6 eV isomeric states of 229Th NUCLEAR STRUCTURE 229Th; calculated quasiparticle energies, energy deformations, splittings of g.s. and 7.6 eV isomeric state. Finite-rays microscopic-macroscopic model.
doi: 10.1103/PhysRevC.78.024311
2008ST14 Phys.Lett. B 665, 168 (2008) I.Stetcu, C.-P.Liu, J.L.Friar, A.C.Hayes, P.Navratil Nuclear electric dipole moment of 3He NUCLEAR STRUCTURE 3He; calculated electric dipole moment.
doi: 10.1016/j.physletb.2008.06.019
2007HA37 Phys.Lett. B 650, 229 (2007) Sensitivity of nuclear transition frequencies to temporal variation of the fine structure constant or the strong interaction
doi: 10.1016/j.physletb.2007.05.021
2005FR02 Phys.Rev. C 71, 024003 (2005) J.L.Friar, G.L.Payne, U.van Kolck Charge-symmetry-breaking three-nucleon forces NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference, role of charge-symmetry-breaking three-nucleon forces.
doi: 10.1103/PhysRevC.71.024003
2005FR20 Phys.Lett. B 618, 68 (2005) The nuclear physics of hyperfine structure in hydrogenic atoms NUCLEAR MOMENTS 2,3H, 3He; calculated hfs, nuclear corrections.
doi: 10.1016/j.physletb.2005.05.015
2005FR22 Phys.Rev. C 72, 014002 (2005) Nuclear corrections to hyperfine structure in light hydrogenic atoms NUCLEAR MOMENTS 2,3H, 3He; calculated hfs, nuclear corrections.
doi: 10.1103/PhysRevC.72.014002
2005FR23 Phys.Rev. C 72, 014004 (2005) Deuteron dipole polarizabilities and sum rules NUCLEAR STRUCTURE 2H; calculated scalar, vector, and tensor components of dipole polarizability, sum rules.
doi: 10.1103/PhysRevC.72.014004
2004FR02 Phys.Lett. B 579, 285 (2004) Zemach moments for hydrogen and deuterium NUCLEAR MOMENTS 1,2H; analyzed electron scattering data; deduced Zemach moments, hfs.
doi: 10.1016/j.physletb.2003.11.018
2004FR29 Phys.Rev. C 70, 044001 (2004) J.L.Friar, U.van Kolck, M.C.M.Rentmeester, R.G.E.Timmermans Nucleon-mass difference in chiral perturbation theory and nuclear forces
doi: 10.1103/PhysRevC.70.044001
2003FR20 Phys.Rev. C 68, 024003 (2003) J.L.Friar, U.van Kolck, G.L.Payne, S.A.Coon Charge-symmetry breaking and the two-pion-exchange two-nucleon interaction NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference, charge-symmetry breaking effects. Effective field theory.
doi: 10.1103/PhysRevC.68.024003
2003FR35 Few-Body Systems 33, 233 (2003) Configuration-Space-Faddeev Born Approximations NUCLEAR REACTIONS 2H(p, p), E=1, 3 MeV; 2H(n, n), E=3 MeV; calculated σ(θ), analyzing powers vs partial wave. Comparison of Fadeev and Schrodinger forms of the Born approximation.
doi: 10.1007/s00601-003-0016-0
2002FR21 Can.J.Phys. 80, 1337 (2002) The structure of light nuclei and its effect on precise atomic measurements
doi: 10.1139/p02-105
2001CH85 Few-Body Systems 31, 13 (2001) C.R.Chen, J.L.Friar, G.L.Payne Low-Energy Proton-Deuteron Scattering in Configuration Space NUCLEAR REACTIONS 2H(p, p), E=1, 2, 3 MeV; calculated elastic scattering matrix elements.
doi: 10.1007/s006010170002
2001FR08 Nucl.Phys. A684, 200c (2001) Three-Nucleon Forces for the New Millennium
doi: 10.1016/S0375-9474(01)00415-8
2001HU13 Few-Body Systems 30, 95 (2001) D.Huber, J.L.Friar, A.Nogga, H.Witala, U.van Kolck Novel Three-Nucleon-Force Terms in the Three-Nucleon System NUCLEAR REACTIONS 2H(polarized n, n), E=3, 10, 50 MeV; calculated Ay(θ). Three-nucleon force, comparisons with data.
2001KI11 Phys.Rev. C63, 064004 (2001) A.Kievsky, J.L.Friar, G.L.Payne, S.Rosati, M.Viviani Phase Shifts and Mixing Parameters for Low-Energy Proton-Deuteron Scattering NUCLEAR REACTIONS 2H(p, p), E=1, 2, 3 MeV; calculated phase shifts, mixing parameters. AV14 two-body potential.
doi: 10.1103/PhysRevC.63.064004
2000EN04 Phys.Rev. C61, 035502 (2000) Nuclear Octupole Correlations and the Enhancement of Atomic Time-Reversal Violation
doi: 10.1103/PhysRevC.61.035502
2000FR04 Acta Phys.Pol. B31, 749 (2000) J.L.Friar, D.Huber, H.Witala, G.L.Payne Quartet n-d Scattering Lengths NUCLEAR REACTIONS 2H(n, X), E not given; calculated quartet scattering lengths. Several potentials compared.
2000PA07 Phys.Rev. C61, 024005 (2000) G.L.Payne, W.Glockle, J.L.Friar Boundary Conditions for Three-Body Scattering in Configuration Space
doi: 10.1103/PhysRevC.61.024005
1999FR02 Phys.Rev. C59, 53 (1999) J.L.Friar, D.Huber, U.van Kolck Chiral Symmetry and Three-Nucleon Forces
doi: 10.1103/PhysRevC.59.53
1999FR25 Phys.Rev. C60, 034002 (1999) Equivalence of Nonstatic Two-Pion-Exchange Nucleon-Nucleon Potentials
doi: 10.1103/PhysRevC.60.034002
1999FR26 Phys.Rev. C60, 034006 (1999) Charge-Independence Breaking in the Two-Pion-Exchange Nucleon-Nucleon Force
doi: 10.1103/PhysRevC.60.034006
1999RE10 Phys.Rev.Lett. 82, 4992 (1999) M.C.M.Rentmeester, R.G.E.Timmermans, J.L.Friar, J.J.de Swart Chiral Two-Pion Exchange and Proton-Proton Partial-Wave Analysis
doi: 10.1103/PhysRevLett.82.4992
1998HU16 Phys.Rev. C58, 674 (1998) Ay Puzzle and the Nuclear Force
doi: 10.1103/PhysRevC.58.674
1998VA10 Phys.Rev.Lett. 80, 4386 (1998) U.van Kolck, M.C.M.Rentmeester, J.L.Friar, T.Goldman, J.J.de Swart Electromagnetic Corrections to the One-Pion-Exchange Potential
doi: 10.1103/PhysRevLett.80.4386
1997BE30 Phys.Rev. C56, 583 (1997) C.J.Benesh, A.C.Hayes, J.L.Friar Reply to ' Comment on ' Quantum-Mechanical Equivalent-Photon Spectrum for Heavy Ion Physics ' '
doi: 10.1103/PhysRevC.56.583
1997FR07 Phys.Rev. C55, 2764 (1997) Nuclear Polarizabilities and Logarithmic Sum Rules NUCLEAR STRUCTURE 2H; calculated electric polarizability, mean-excitation energy; deduced correction to atomic deuterium frequency shift. Comparison of several potentials.
doi: 10.1103/PhysRevC.55.2764
1997FR09 Phys.Rev. C56, 619 (1997) Higher-Order Nuclear-Polarizability Corrections in Atomic Hydrogen NUCLEAR STRUCTURE 2H; calculated nucleus polarizability corrections. Hydrogenic atomic S-states, analytic approach.
doi: 10.1103/PhysRevC.56.619
1997FR25 Phys.Rev. A56, 4579 (1997) J.L.Friar, J.Martorell, D.W.L.Sprung Nuclear Sizes and the Isotope Shift
doi: 10.1103/PhysRevA.56.4579
1997FR26 Few-Body Systems 22, 161 (1997) Dimensional Power Counting in Nuclei
doi: 10.1007/s006010050059
1996BE44 Phys.Rev. C54, 1404 (1996) C.J.Benesh, A.C.Hayes, J.L.Friar Quantum-Mechnical Equivalent-Photon Spectrum for Heavy-Ion Physics NUCLEAR REACTIONS 41Ca, 17O(197Au, 197Au'), E not given; calculated target dipole excitation σ. 197Au(12C, X), (20Ne, X), E=2.1 GeV/nucleon; 197Au(56Fe, X), (40Ar, X), E=1.9 GeV/nucleon; 197Au(20Ne, X), E=1.7 GeV/nucleon; 197Au(197Au, X), (209Bi, X), (86Kr, X), E=1 GeV/nucleon; 197Au(238U, X), E=0.96 GeV/nucleon; calculated single-neutron removal σ. Semi-classical, fully quantum mechanically derived photon spectrum approaches.
doi: 10.1103/PhysRevC.54.1404
1996CO07 Phys.Rev. C53, 2661 (1996) T.D.Cohen, J.L.Friar, G.A.Miller, U.van Kolck pp → ppπ0 Reaction Near Threshold: A chiral power counting approach NUCLEAR REACTIONS 1H(p, X), E ≈ threshold; calculated amplitude characteristics for different mechanisms in pp → ppπ0 reaction. Power-counting scheme.
doi: 10.1103/PhysRevC.53.2661
1996FR02 Phys.Rev. C53, 588 (1996) Leading-Order Nuclear π-γ Exchange Force
doi: 10.1103/PhysRevC.53.588
1996FR05 Phys.Rev. C53, 3085 (1996) J.L.Friar, D.G.Madland, B.W.Lynn QCD Scales in Finite Nuclei
doi: 10.1103/PhysRevC.53.3085
1996VA08 Phys.Lett. 371B, 169 (1996) U.van Kolck, J.L.Friar, T.Goldman Phenomenological Aspects of Isospin Violation in the Nuclear Force
doi: 10.1016/0370-2693(96)00009-3
1995FO14 Phys.Rev. C52, 568 (1995) J.L.Forest, V.R.Pandharipande, J.L.Friar Relativistic Nuclear Hamiltonians
doi: 10.1103/PhysRevC.52.568
1995FR11 Phys.Rev. C51, 2356 (1995) J.L.Friar, G.L.Payne, W.Glockle, D.Huber, H.Witala Benchmark Solutions for n-d Breakup Amplitudes NUCLEAR REACTIONS 2H(n, X), E=14.1, 42 MeV; calculated breakup σ(θ1, θ2) vs arc length. 2H(n, n), E=14.1, 42 MeV; calculated phase shifts. S-wave potential model.
doi: 10.1103/PhysRevC.51.2356
1995FR25 Few-Body Systems 19, 203 (1995) Assessment of Triton Potential Energy NUCLEAR STRUCTURE 3H; calculated different contributions to potential energy; deduced nucleon-nucleon separation regions role.
doi: 10.1007/s006010050027
1994BE32 Phys.Rev. C50, 3167 (1994) Simultaneous Projectile-Target Excitation in Heavy Ion Collisions NUCLEAR REACTIONS 197Au(12C, X), E=relativistic; calculated dipole-dipole excitation σ, relativistic energies. Simultaneous target, projectile excitation.
doi: 10.1103/PhysRevC.50.3167
1994FR04 Phys.Rev. C49, 1272 (1994) Non-Adiabatic Contributions to Static Two-Pion-Exchange Nuclear Potentials
doi: 10.1103/PhysRevC.49.1272
1994RA39 Few-Body Systems 17, 71 (1994) A.S.Raskin, E.L.Tomusiak, J.L.Friar Gauge-Invariant Nuclear Pion-Photoproduction Amplitude with Binding-Induced Contributions
doi: 10.1007/BF01074446
1993BE32 Phys.Rev. C48, 1285 (1993) Electromagnetic Dissociation of Nuclei in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(12C, X), (20Ne, X), (40Ar, X), (56Fe, X), (139La, X), (238U, X), E not given; calculated single neutron removal σ. Quantum theory, Goldhaber-Teller model transition densities.
doi: 10.1103/PhysRevC.48.1285
1993FR11 Phys.Lett. 311B, 4 (1993) J.L.Friar, G.L.Payne, V.G.J.Stoks, J.J.de Swart Triton Calculations with the New Nijmegen Potentials NUCLEAR STRUCTURE 3H; calculated binding energy. Nijmegen potentials.
doi: 10.1016/0370-2693(93)90523-K
1993FR18 Czech.J.Phys. B43, 259 (1993) Three-Nucleon Forces and the Three-Nucleon Systems NUCLEAR REACTIONS 2H(polarized n, n), E=22.7 MeV; compiled, reviewed tensor analyzing power data, analyses. 2H(p, p), E ≈ 0; compiled, reviewed E0 matrix element vs 3He binding energy. Muon catalyzed p-d fusion.
doi: 10.1007/BF01589847
1991CH16 Phys.Rev. C44, 50 (1991) C.R.Chen, G.L.Payne, J.L.Friar, B.F.Gibson Nd Zero-Energy Scattering NUCLEAR REACTIONS 2H(p, p), (n, n), E=low; calculated scattering lengths. Three-body models.
doi: 10.1103/PhysRevC.44.50
1991FR03 Phys.Rev.Lett. 66, 1827 (1991) J.L.Friar, B.F.Gibson, H.C.Jean, G.L.Payne Nuclear Transition Rates in μ-Catalyzed p-d Fusion NUCLEAR REACTIONS 2H(p, γ), E not given; calculated M1 radiative capture transition rates. Quartet, doublet initial states, μ-catalyzed fusion.
doi: 10.1103/PhysRevLett.66.1827
1990FR12 Phys.Rev. C42, 1211 (1990) J.L.Friar, B.F.Gibson, G.L.Payne n-p Mass Difference and Charge-Symmetry Breaking in the Trinucleons NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference; deduced n-p mass difference role.
doi: 10.1103/PhysRevC.42.1211
1990FR13 Phys.Rev. C42, 1838 (1990) J.L.Friar, B.F.Gibson, G.Berthold, W.Glockle, Th.Cornelius, H.Witala, J.Haidenbauer, Y.Koike, G.L.Payne, J.A.Tjon, W.M.Kloet Benchmark Solutions for a Model Three-Nucleon Scattering Problem NUCLEAR REACTIONS 2H(n, n), E=4-42 MeV; calculated s-wave scattering parameters. Three-nucleon problem, single model interaction.
doi: 10.1103/PhysRevC.42.1838
1990FR14 Phys.Rev. C42, 2310 (1990) J.L.Friar, B.F.Gibson, G.L.Payne, A.M.Bernstein, T.E.Chupp Neutron Polarization in Polarized 3He Targets NUCLEAR STRUCTURE 3He; calculated neutron, proton density matrix parameter; deduced neutron polarization to be 87% of 3He target polarization.
doi: 10.1103/PhysRevC.42.2310
1990FR18 Phys.Lett. 247B, 197 (1990) J.L.Friar, B.F.Gibson, G.L.Payne, C.R.Chen Neutron-Deuteron Zero-Energy Scattering NUCLEAR REACTIONS 2H(n, n), (p, p), E ≈ 0; calculated scattering lengths. Configuration space Faddeev-type scattering.
doi: 10.1016/0370-2693(90)90880-F
1990FR19 Phys.Lett. 251B, 11 (1990) J.L.Friar, B.F.Gibson, G.L.Payne Thermal n-d Radiative Capture NUCLEAR REACTIONS 2H(n, γ), E=thermal; calculated capture σ vs triton binding energy. Configuration space Faddeev equations.
doi: 10.1016/0370-2693(90)90223-S
1990HA10 Phys.Rev. C41, 1727 (1990) A.C.Hayes, J.L.Friar, D.Strottman Two-Photon Decay of the First Excited 0+ State in 16O NUCLEAR STRUCTURE 16O; calculated 2γ decay rate, matrix elements, GDR resonances, B(λ). Shell model, large SU(3) basis.
doi: 10.1103/PhysRevC.41.1727
1989CH10 Phys.Rev. C39, 1261 (1989) C.R.Chen, G.L.Payne, J.L.Friar, B.F.Gibson Low-Energy Nucleon-Deuteron Scattering NUCLEAR REACTIONS 2H(p, p), (n, n), E(cm)=0.001-1 MeV; calculated phase shifts, effective range function vs E. Faddeev formalism.
doi: 10.1103/PhysRevC.39.1261
1988FR11 Phys.Rev. C37, 2852 (1988) J.L.Friar, B.F.Gibson, G.L.Payne, E.L.Tomusiak, M.Kimura Trinucleon Magnetic Moments: 34-Channel results NUCLEAR STRUCTURE 3H, 3He; calculated μ. Configuration space Faddeev wave functions, one-body, meson exchange currents.
doi: 10.1103/PhysRevC.37.2852
1988FR12 Phys.Rev. C37, 2859 (1988) J.L.Friar, B.F.Gibson, D.R.Lehman, G.L.Payne Trinucleon Asymptotic Normalization Constants: Comparison of 3He and 3H NUCLEAR STRUCTURE 3H, 3He; calculated asymptotic normalization constants. Configuration space Faddeev calculation.
doi: 10.1103/PhysRevC.37.2859
1988FR13 Phys.Rev. C37, 2869 (1988) J.L.Friar, B.F.Gibson, G.L.Payne 3H and 3He Solutions for Momentum-Dependent Potentials NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, rms radii, asymptotic normalization constants, charge densities. Configuration space Faddeev equations.
doi: 10.1103/PhysRevC.37.2869
1988LE01 Phys.Rev. C37, 336 (1988) D.R.Lehman, L.C.Maximon, J.L.Friar Coulomb Effects in Asymptotic Normalization Constants: A soluble model NUCLEAR STRUCTURE 3H, 3He; calculated asymptotic normalization constant.
doi: 10.1103/PhysRevC.37.336
1987FR01 Nucl.Phys. A463, 315c (1987) Three-Nucleon Forces and Trinucleon Observables NUCLEAR REACTIONS 2H(n, n), (p, p), E=5-12 MeV; analyzed doublet scattering lengths. NUCLEAR STRUCTURE 3H, 3He; analyzed rms radii, Coulomb energies, charge densities, form factors.
doi: 10.1016/0375-9474(87)90674-9
1987FR02 Phys.Rev. C35, 1502 (1987) J.L.Friar, B.F.Gibson, G.L.Payne Coulomb Effects in the 3He Ground State NUCLEAR STRUCTURE 3H, 3He; calculated rms charge radii vs binding energy, nucleon density. 3He; calculated Coulomb energy, first-, second-order shifts. Hyperspherical approximation.
doi: 10.1103/PhysRevC.35.1502
1987FR12 Phys.Rev. C36, 1138 (1987) J.L.Friar, B.F.Gibson, G.L.Payne Variational Bounds for the Triton NUCLEAR STRUCTURE 3H; calculated binding energy; deduced convergence criteria. Faddeev formalism, different potentials.
doi: 10.1103/PhysRevC.36.1138
1987FR13 Phys.Rev. C36, 1140 (1987) J.L.Friar, B.F.Gibson, G.L.Payne Charge Dependence in the Triton NUCLEAR STRUCTURE 3H; calculated binding energy; deduced nuclear charge dependence role.
doi: 10.1103/PhysRevC.36.1140
1986CH02 Phys.Rev. C33, 401 (1986) C.R.Chen, G.L.Payne, J.L.Friar, B.F.Gibson Nucleon-Deuteron Doublet Scattering Lengths with Three-Nucleon Potentials NUCLEAR REACTIONS 2H(n, n), (p, p), E=low; calculated doublet scattering. Three-nucleon potential, Faddeev equations.
doi: 10.1103/PhysRevC.33.401
1986CH13 Phys.Rev. C33, 1740 (1986) C.R.Chen, G.L.Payne, J.L.Friar, B.F.Gibson Faddeev Calculations of the 2π-3N Force contribution to the 3H Binding Energy NUCLEAR STRUCTURE 3H; calculated binding energy. Faddeev calculations, 2π-3N force.
doi: 10.1103/PhysRevC.33.1740
1986FR15 Phys.Rev. C34, 1463 (1986) J.L.Friar, B.F.Gibson, G.L.Payne, C.R.Chen Trinucleon Charge Densities and Three-Nucleon Forces NUCLEAR STRUCTURE 3H, 3He; calculated charge densities, form factors. Impulse approximation, three-body force models.
doi: 10.1103/PhysRevC.34.1463
1986FR19 Phys.Rev. C34, 2029 (1986) Gauge-Invariant Nuclear Compton Amplitude Manifesting Low-Energy Theorems NUCLEAR REACTIONS 2H(γ, p), E ≈ 4-132 MeV; calculated photodisintegration σ(θ) vs E. Extended Seigert theorem.
doi: 10.1103/PhysRevC.34.2029
1985CH17 Phys.Rev. C31, 2266 (1985) C.R.Chen, G.L.Payne, J.L.Friar, B.F.Gibson Convergence of Faddeev Partial-Wave Series for Triton Ground State NUCLEAR STRUCTURE 3H, 3He; calculated Coulomb energies, charge radii, wave function component probability percentages.
doi: 10.1103/PhysRevC.31.2266
1985CH22 Phys.Rev.Lett. 55, 374 (1985) C.R.Chen, G.L.Payne, J.L.Friar, B.F.Gibson Faddeev Calculation of Three-Nucleon Force Contribution to Triton Binding Energy NUCLEAR STRUCTURE 3H; calculated binding energy, rms charge radius. 3He; calculated rms charge radius. Faddeev calculations, three-nucleon force contribution.
doi: 10.1103/PhysRevLett.55.374
1985FR08 Phys.Rev. C31, 2027 (1985) Current Conservation and the Transverse Electric Multipole Field NUCLEAR REACTIONS 12C(e, e'), E not given; calculated longitudinal, transverse form factors.
doi: 10.1103/PhysRevC.31.2027
1985FR12 Phys.Lett. 161B, 241 (1985) J.L.Friar, B.F.Gibson, C.R.Chen, G.L.Payne Scaling Relations for Triton Ground-State Observables NUCLEAR STRUCTURE 3H; calculated Coulomb energies, rms charge radii, binding energy. Faddeev equations, different two-, three-body potentials.
doi: 10.1016/0370-2693(85)90753-1
1985TO21 Phys.Rev. C32, 2075 (1985) E.L.Tomusiak, M.Kimura, J.L.Friar, B.F.Gibson, G.L.Payne, J.Dubach Trinucleon Magnetic Moments NUCLEAR STRUCTURE 3H, 3He; calculated μ, magnetic form factors; deduced dominant charge exchange effects. Various potential models, configuration space Faddeev equations.
doi: 10.1103/PhysRevC.32.2075
1984FR02 Phys.Rev. C29, 232 (1984) Deuteron Electric Polarizability NUCLEAR STRUCTURE 2H; calculated electric polarizability; deduced zero-range approximation upper limit.
doi: 10.1103/PhysRevC.29.232
1984FR07 Phys.Rev. C30, 441 (1984); Erratum Phys.Rev. C31, 287 (1985) J.L.Friar, B.F.Gibson, G.L.Payne Deuteron Forward Photodisintegration NUCLEAR REACTIONS 2H(γ, p), E ≈ 5-140 MeV; calculated photodisintegration σ(θ) vs E. Meson exchange, relativistic corrections, spin-orbit dipole operator.
doi: 10.1103/PhysRevC.30.441
1984FR09 Phys.Rev. C30, 1084 (1984) J.L.Friar, B.F.Gibson, G.L.Payne One-Pion-Exchange Potential Deuteron NUCLEAR REACTIONS 2H(γ, p), E=4-124 MeV; calculated photodisintegration σ(E). Nonrelativistic impulse approximation, deuteron observables from one pion exchange potential. NUCLEAR STRUCTURE 3H; calculated binding energy correction. 2H; calculated binding energy, D-state probability, rms radius, quadrupole moment. One pion exchange potential.
doi: 10.1103/PhysRevC.30.1084
1984FR11 Phys.Rev. C30, 1121 (1984) J.L.Friar, B.F.Gibson, G.L.Payne, C.R.Chen Configuration Space Faddeev Continuum Calculations: N-d s-wave scattering lengths with tensor-force interactions NUCLEAR REACTIONS 2H(p, p), (n, n), E ≈ 0 MeV; calculated s-wave scattering length. Faddeev continuum calculations, tensor interactions.
doi: 10.1103/PhysRevC.30.1121
1984FR16 Ann.Rev.Nucl.Part.Sci. 34, 403 (1984) J.L.Friar, B.F.Gibson, G.L.Payne Recent Progress in Understanding Trinucleon Properties
doi: 10.1146/annurev.ns.34.120184.002155
1984PA17 Phys.Rev. C30, 1132 (1984) G.L.Payne, W.H.Klink, W.N.Polyzou, J.L.Friar, B.F.Gibson Noncompact-Kernel Integral Equation for Three-Body Scattering: nd quartet equation and numerical results NUCLEAR REACTIONS 2H(n, n), E < breakup; calculated s-wave scattering lengths, mesh parameters. Integral equation approach.
doi: 10.1103/PhysRevC.30.1132
1984WA03 Phys.Rev. C29, 956 (1984) Approximate Dirac Scattering Amplitudes: Eikonal expansion NUCLEAR REACTIONS 40Ca(polarized p, p), E=300, 500, 800 MeV; calculated σ(θ), analyzing power, spin rotation vs θ. Dirac scattering amplitudes, eikonal expansions.
doi: 10.1103/PhysRevC.29.956
1984WI12 Phys.Lett. 143B, 273 (1984) R.B.Wiringa, J.L.Friar, B.F.Gibson, G.L.Payne, C.R.Chen Faddeev Monte-Carlo Calculations of Trinucleon Binding Energy with Three-Body Potentials NUCLEAR STRUCTURE 3H, 3He; calculated binding energy, charge rms radii. Configuration space Faddeev wave functions, Monte Carlo integrations.
doi: 10.1016/0370-2693(84)91464-3
1983FR05 Phys.Rev. C27, 1364 (1983) J.L.Friar, S.Fallieros, E.L.Tomusiak, D.Skopik, E.G.Fuller Electric Polarizability of the Deuteron NUCLEAR STRUCTURE 2H; analyzed photoabsorption data; deduced electric polarizability. Dispersion relation, Compton scattering effects.
doi: 10.1103/PhysRevC.27.1364
1983FR12 Phys.Lett. 124B, 287 (1983) J.L.Friar, B.F.Gibson, G.L.Payne The Proton-Deuteron Scattering Lengths NUCLEAR REACTIONS 2H(p, p), (n, n), E ≈ 0; calculated scattering lengths. Configuration space Faddeev calculations.
doi: 10.1016/0370-2693(83)91455-7
1983FR19 Z.Phys. A312, 169 (1983) J.L.Friar, B.F.Gibson, G.L.Payne Configuration Space Faddeev Calculations VI. Triton Wave Function NUCLEAR STRUCTURE 3H; calculated ground state wave function; deduced two-body force tensor component, potential short repulsion roles. Faddeev calculations, configuration space.
doi: 10.1007/BF01412160
1983FR21 Phys.Rev. C28, 983 (1983) J.L.Friar, B.F.Gibson, G.L.Payne Configuration Space Faddeev Continuum Calculations: p-d s-wave scattering length NUCLEAR REACTIONS 2H(p, p), E=0 MeV; calculated s-wave scattering lengths. Configuration space Faddeev calculations.
doi: 10.1103/PhysRevC.28.983
1982FR07 Phys.Rev. C25, 1616 (1982) J.L.Friar, B.F.Gibson, D.R.Lehman, G.L.Payne Trinucleon Asymptotic Normalization Constants Including Coulomb Effects NUCLEAR STRUCTURE 3H, 3He; calculated asymptotic normalization constant. Faddeev calculations, Coulomb effects.
doi: 10.1103/PhysRevC.25.1616
1982PA21 Phys.Rev. C26, 1385 (1982) G.L.Payne, J.L.Friar, B.F.Gibson Configuration Space Faddeev Continuum Calculations. I. n-d Scattering Length NUCLEAR REACTIONS 2H(n, n), E ≈ 0 MeV; calculated scattering length. Configuration space Faddeev calculations.
doi: 10.1103/PhysRevC.26.1385
1981FR15 Phys.Rev. C24, 665 (1981) J.L.Friar, B.F.Gibson, E.L.Tomusiak, G.L.Payne Configuration Space Faddeev Calculations. IV. Trinucleon Charge Density NUCLEAR STRUCTURE 3He, 3H; calculated charge densities. Faddeev calculations, several potential models.
doi: 10.1103/PhysRevC.24.665
1981TO13 Phys.Rev. C24, 2351 (1981) E.L.Tomusiak, J.L.Friar, B.F.Gibson, J.Dubach. G.L.Payne Threshold 3He(γ, π+)3H NUCLEAR REACTIONS 3He(γ, π+), E=threshold; calculated σ. Impulse approximation, realistic wave functions.
doi: 10.1103/PhysRevC.24.2351
1980PA12 Phys.Rev. C22, 823 (1980) G.L.Payne, J.L.Friar, B.F.Gibson, I.R.Afnan Configuration Space Faddeev Calculations. I. Triton Ground State Properties NUCLEAR STRUCTURE 3H; calculated binding energy, wave function, rms radius. Faddeev equations.
doi: 10.1103/PhysRevC.22.823
1980PA13 Phys.Rev. C22, 832 (1980) G.L.Payne, J.L.Friar, B.F.Gibson Configuration Space Faddeev Calculations. II. Trinucleon Coulomb Energy NUCLEAR STRUCTURE 3He; calculated Coulomb energy. Faddeev calculations.
doi: 10.1103/PhysRevC.22.832
1978FR07 Phys.Rev. C17, 1456 (1978) Charge Asymmetry in 3He-3H and the Neutron-Proton Mass Difference NUCLEAR STRUCTURE 3He, 3H; calculated charge asymmetry, n-p mass difference.
doi: 10.1103/PhysRevC.17.1456
1978FR09 Phys.Rev. C17, 1752 (1978) Nonlocal Contributions to the p-omega Mixing Charge-Symmetry-Breaking Force NUCLEAR STRUCTURE 3He, 3H; calculated mass difference, charge-symmetry breaking, meson mixing.
doi: 10.1103/PhysRevC.17.1752
1978FR17 Phys.Rev. C18, 908 (1978) Coulomb Energies in S-Shell Nuclei and Hypernuclei NUCLEAR STRUCTURE 3H, 3,4He; calculated Coulomb separation energy, hypernuclear separation energy.
doi: 10.1103/PhysRevC.18.908
1977FR16 Phys.Rev. C16, 1540 (1977) Nuclear Polarization Corrections in μ-4He Atoms NUCLEAR STRUCTURE, Mesic-Atoms 4He; calculated nuclear polarization corrections in muonic atom.
doi: 10.1103/PhysRevC.16.1540
1975FR05 Nucl.Phys. A240, 301 (1975) The Determination of the Nuclear Charge Distribution of 12C from Elastic Electron Scattering NUCLEAR STRUCTURE 12C, 208Pb; calculated density distributions.
doi: 10.1016/0375-9474(75)90333-4
1974FR12 Ann.Phys.(New York) 87, 289 (1974) Dispersion Corrections to Elastic Electron Scattering by 12C and 16O II. On the Use of the Closure Approximation NUCLEAR REACTIONS 12C(e, e'), E=374.5, 747.2 MeV; 16O(e, e'), E=750 MeV; calculated correction factors.
doi: 10.1016/0003-4916(74)90038-4
1973FR05 Phys.Lett. 43B, 108 (1973) Relativistic Corrections to Electron Scattering by the Deuteron and Triton
doi: 10.1016/0370-2693(73)90421-8
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