NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = R.J.McCarthy Found 30 matches. 1994BA24 Nucl.Phys. A570, 23c (1994) B.R.Barrett, D.C.Zheng, L.Jaqua, J.P.Vary, R.J.McCarthy Realistic Microscopic Calculations for the Light Nuclei A = 2 to 7 NUCLEAR STRUCTURE 4,5He, 6,7Li; calculated levels. Realistic microscopic calculation.
doi: 10.1016/0375-9474(94)90266-6
1994ZH07 Phys.Rev. C49, 1999 (1994) D.C.Zheng, B.R.Barrett, J.P.Vary, R.J.McCarthy Simple Approximation for the Starting-Energy-Independent Two-Body Effective Interaction with Applications to 6Li NUCLEAR STRUCTURE 6Li; calculated levels. Exact, approximate effective interactions, Lee-Suzuki iteration method.
doi: 10.1103/PhysRevC.49.1999
1993ZH15 Phys.Rev. C48, 1083 (1993) D.C.Zheng, B.R.Barrett, L.Jaqua, J.P.Vary, R.J.McCarthy Microscopic Calculations of the Spectra of Light Nuclei NUCLEAR STRUCTURE 4,5He, 6,7Li; calculated ground state energies, levels. Large shell model space, realistic interactions, G-matricies.
doi: 10.1103/PhysRevC.48.1083
1991AN04 Phys.Rev. C43, 1630 (1991) B.D.Anderson, M.Mostajaboddavati, C.Lebo, R.J.McCarthy, L.Garcia, J.W.Watson, R.Madey Isobaric-Analog-State Transitions in the (p, n) Reaction at 135 MeV and Density-Dependent Impulse-Approximation Calculations NUCLEAR REACTIONS 14C, 42Ca, 88Sr, 124Sn(p, n), E=135 MeV; 144Sm(p, n), E=136 MeV; measured neutron spectra. 88Sr, 124Sn, 128Te, 144Sm, 208Pb, 14C, 26Mg, 42,48Ca, 54Fe(p, n), E=135 MeV; measured σ(θ). 48Ca(polarized p, n), E=135 MeV; measured analyzing power vs θ; deduced normalization factors, IAS σ. Density-dependent DWIA analysis.
doi: 10.1103/PhysRevC.43.1630
1990AN05 Phys.Rev. C41, 1470 (1990) B.D.Anderson, M.Mostajaboddavati, A.R.Baldwin, M.Elaasar, R.Madey, D.M.Manley, R.J.McCarthy, N.Tamimi, J.W.Watson, W.M.Zhang, C.C.Foster Excitation of Two-Particle-One-Hole High-Spin States in the 45Sc(p, n)45Ti Reaction at 136 MeV NUCLEAR REACTIONS 45Sc(p, n), E=136 MeV; measured σ(θ, E). 45Ti levels deduced spectroscopic strength.
doi: 10.1103/PhysRevC.41.1470
1985AN06 Phys.Rev. C31, 1147 (1985) B.D.Anderson, T.Chittrakarn, A.R.Baldwin, C.Lebo, R.Madey, R.J.McCarthy, J.W.Watson, B.A.Brown, C.C.Foster Particle-Hole Strength Excited in the 48Ca(p, n)48Sc Reaction at 134 and 160 MeV: (πf7/2, νf7/2-1) Band NUCLEAR REACTIONS 48Ca(p, n), E=134, 160 MeV; measured σ(E, θ), σ(θ). 48Sc deduced Gamow-Teller to Fermi transition strength, stretched transition excitation. DWIA analysis.
doi: 10.1103/PhysRevC.31.1147
1985WA24 Phys.Rev.Lett. 55, 1369 (1985) J.W.Watson, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, R.J.McCarthy, B.A.Brown, B.H.Wildenthal, C.C.Foster Relationship between Gamow-Teller Transition Proabilities and (p, n) Cross Sections at Small Momentum Transfers NUCLEAR REACTIONS 14C, 15N, 17,18O, 26Mg, 39K(p, n), E=135 MeV; measured σ(θ), σ(θn, En). 13C, 19F(p, n), E=160 MeV; analyzed σ(θ). 14N, 15O, 17,18F, 26Al, 39Ca levels deduced Gamow-Teller transitions. DWBA analysis, β-decay input.
doi: 10.1103/PhysRevLett.55.1369
1983AN05 Phys.Rev. C27, 1387 (1983) B.D.Anderson, A.Fazely, R.J.McCarthy, P.C.Tandy, J.W.Watson, R.Madey, W.Bertozzi, T.N.Buti, J.M.Finn, J.Kelly, M.A.Kovash, B.Pugh, B.H.Wildenthal, C.C.Foster Gamow-Teller Strength in the 18O(p, n)18F Reaction at 135 MeV NUCLEAR REACTIONS 18O(p, n), E=135.2 MeV; measured σ(En), σ(θ). 18F deduced levels, J, π, T, Gamow-Teller transition strength. DWIA analysis.
doi: 10.1103/PhysRevC.27.1387
1982AN08 Phys.Rev. C26, 8 (1982) B.D.Anderson, R.J.McCarthy, M.Ahmad, A.Fazely, A.M.Kalenda, J.N.Knudson, J.W.Watson, R.Madey, C.C.Foster Comparison of 0°(p, n) Cross Sections and B(M1) Values for Separating Current and Spin Contributions to Isovector M1 Transitions NUCLEAR REACTIONS 12C, 16O, 24,26Mg, 28Si, 48Ca(p, n), E=62-160 MeV; analyzed σ(θ=0°) vs E. 12N, 24,26Al, 16F, 28P, 48Sc level deduced σ/B(M1) spin, current contribution dependence. Inelastic electron scattering data input.
doi: 10.1103/PhysRevC.26.8
1982CO03 Phys.Rev. C25, 756 (1982) S.A.Coon, R.J.McCarthy, J.P.Vary Three-Body Force Effects in the 17O Magnetic Form Factor NUCLEAR REACTIONS 17O(e, e), E not given; calculated magnetic form factor; deduced three-body force, two-pion exchange effects.
doi: 10.1103/PhysRevC.25.756
1982FA06 Phys.Rev. C25, 1760 (1982); Erratum Phys.Rev. C26, 746 (1982) A.Fazely, B.D.Anderson, M.Ahmad, A.R.Baldwin, A.M.Kalenda, R.J.McCarthy, J.W.Watson, R.Madey, W.Bertozzi, T.N.Buti, J.M.Finn, M.A.Kovash, B.Pugh, C.C.Foster Spectroscopy of 16F from the 16O(p, n)16F Reaction at 99 and 135 MeV NUCLEAR REACTIONS 16O(p, n), E=99.1, 135.2 MeV; measured σ(En) vs θ; deduced σ(θ). 16F levels deduced J, π, analog character. Tof. Shell model.
doi: 10.1103/PhysRevC.25.1760
1982MA11 Phys.Rev. C25, 1715 (1982) R.Madey, A.Fazely, B.D.Anderson, A.R.Baldwin, A.M.Kalenda, R.J.McCarthy, P.C.Tandy, J.W.Watson, W.Bertozzi, T.Buti, M.Finn, M.Kovash, B.Pugh, C.C.Foster Analyzing Power for the 16O(p(pol), n)16F(4-, 6.37 MeV) Reaction at 134 MeV NUCLEAR REACTIONS 16O(polarized p, n), E=134 MeV; measured σ(θ), σ(En), A(θ). 16F level deduced configuration. DWIA, effective nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.25.1715
1982MC01 Phys.Rev. C25, 73 (1982) Higher Order Effects on the Magnetic Form Factor of 17O NUCLEAR REACTIONS 17O(e, e), E not given; calculated magnetic form factor. Self-consistent method, effective operator, higher order terms.
doi: 10.1103/PhysRevC.25.73
1980PE05 Phys.Rev. C21, 1718 (1980) F.Petrovich, W.G.Love, R.J.McCarthy Separation of Current and Spin Contributions to Isovector M1 Excitations by Means of the (e, e') and (p, n) Reactions NUCLEAR REACTIONS 12C, 24Mg, 28Si(p, n), E=62 MeV; calculated σ(θ), B(M1), transition radii. 12C, 24Mg, 28Si(e, e'), E not given; calculated orbital current densities. 12C, 24Mg, 28Si deduced current, spin contributions to T=1, M1 excitations. g-matrix, shell model, distorted, plane wave approximations.
doi: 10.1103/PhysRevC.21.1718
1980VA05 Phys.Rev. C21, 1626 (1980) J.P.Vary, R.H.Belehrad, R.J.McCarthy Valence-Core Self-Consistency in the A = 17 System NUCLEAR STRUCTURE 16,17O; calculated self-consistent hole, particle energies, wave functions. Brueckner calculation, effective interaction, perturbation theory.
doi: 10.1103/PhysRevC.21.1626
1978CO08 J.Phys.(London) G4, 183 (1978) S.A.Coon, R.J.McCarthy, C.P.Malta A Three-Nucleon Force and A = 18 Shell-Model Spectra NUCLEAR STRUCTURE 18O, 18F; calculated levels.
doi: 10.1088/0305-4616/4/2/009
1977SA05 Z.Phys. A280, 259 (1977) M.S.Sandel, R.J.McCarthy, B.R.Barrett Core Polarization Revisited NUCLEAR STRUCTURE 18O, 18F; calculated levels.
doi: 10.1007/BF01434351
1975MC03 Phys.Rev. C11, 383 (1975) Effects of Ground-State Correlations on Muon Capture Matrix Elements NUCLEAR REACTIONS 4He, 16O(μ-, X); calculated total muon capture rate.
doi: 10.1103/PhysRevC.11.383
1974DA29 Phys.Rev. C10, 2607 (1974) K.T.R.Davies, R.J.McCarthy, J.W.Negele, P.U.Sauer Renormalized Brueckner-Hartree-Fock and Density Dependent Hartree-Fock Theories of Finite Nuclei NUCLEAR STRUCTURE 40Ca; calculated charge density distribution.
doi: 10.1103/PhysRevC.10.2607
1974GA27 Nucl.Phys. A228, 246 (1974) A Self-Consistent Particle Spectrum for Brueckner Calculations NUCLEAR STRUCTURE 16O; calculated levels, binding energy per nucleon.
doi: 10.1016/0375-9474(74)90430-8
1974MC04 Phys.Rev. C9, 809 (1974) Effect of Short-Range Correlations on Coulomb Matrix Elements NUCLEAR STRUCTURE 6Be, 6He; calculated Coulomb shift.
doi: 10.1103/PhysRevC.9.809
1973DA07 Phys.Rev. C7, 943 (1973) K.T.R.Davies, R.J.McCarthy, P.U.Sauer Higher-Order Corrections to Brueckner-Hartree-Fock Binding Energies and Radii NUCLEAR STRUCTURE 16O, 40Ca, 208Pb calculated binding energies, nuclear radii.
doi: 10.1103/PhysRevC.7.943
1972BA29 Nucl.Phys. A184, 13 (1972) B.R.Barrett, R.G.L.Hewitt, R.J.McCarthy Binding-Energy Calculations for 16O and their Dependence on the Treatment of the Pauli Operator in the G-Matrix NUCLEAR STRUCTURE 16O; calculated binding energy, single-particle energies, occupation probabilities. g-matrix element, Pauli operator.
doi: 10.1016/0375-9474(72)90441-1
1972DA18 Phys.Rev. C6, 1461 (1972) K.T.R.Davies, R.J.McCarthy, P.U.Sauer Renormalized Brueckner-Hartree-Fock Calculations Using Different Prescriptions for the Intermediate-State Spectrum NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated levels, single-particle energies, occupation probabilities, binding energies, rms radii. Renormalized Brueckner-Hartree-Fock theory.
doi: 10.1103/PhysRevC.6.1461
1971BA14 Phys.Rev. C3, 1137 (1971) B.R.Barrett, R.G.L.Hewitt, R.J.McCarthy Simple and Exact Method for Calculating the Nuclear Reaction Matrix NUCLEAR STRUCTURE 18O, 18F; calculated levels. Shell model.
doi: 10.1103/PhysRevC.3.1137
1971DA15 Phys.Rev. C4, 81 (1971) Brueckner-Hartree-Fock Calculations of Spherical Nuclei in a Harmonic-Oscillator Basis. III. Renormalized Calculations Using the Reid Potential NUCLEAR STRUCTURE 16O, 40,48Ca, 208Pb; calculated levels, occupation probabilities, binding energy, charge radius. g-matrix, Brueckner-Hartree-Fock formalism. Element-114, Element-126; calculated single-particle energies.
doi: 10.1103/PhysRevC.4.81
1969MC07 Nucl.Phys. A130, 305 (1969) Reaction Matrix Calculations in Finite Nuclei NUCLEAR STRUCTURE 16O; calculated single-particle states, binding energy.
doi: 10.1016/0375-9474(69)90732-5
1969ME06 Nucl.Phys. A130, 322 (1969) R.Mercier, E.U.Baranger, R.J.McCarthy A Shell-Model Calculation with Reaction Matrix Elements NUCLEAR STRUCTURE 18F, 18O; calculated levels.
doi: 10.1016/0375-9474(69)90733-7
1968MC05 Phys.Rev.Letters 20, 671 (1968) Binding Energy of O16 with a Velocity-Dependent Nucleon Potential
doi: 10.1103/PhysRevLett.20.671
1967MC09 Nucl.Phys. A99, 65 (1967) Calculation of 16O Binding Energy
doi: 10.1016/0375-9474(67)90209-6
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