NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = M.K.Singham Found 12 matches. 1992BA64 Phys.Lett. 296B, 5 (1992) J.Bartel, M.B.Johnson, M.K.Singham, W.Stocker Pion Inelastic Scattering and the Neutron Density in 152Sm NUCLEAR REACTIONS 152Sm(π+, π+), (π-, π-), (π+, π+'), (π-, π-'), E=180 MeV; analyzed σ(θ). 152Sm deduced neutron radius features, n-, p-deformations.
doi: 10.1016/0370-2693(92)90795-6
1992SA02 Phys.Rev. C45, 2027 (1992) G.R.Satchler, M.K.Singham, M.B.Johnson Comment on ' Pion Scattering from 39K and 58Ni ' and Virtual Excitation Effects on Elastic Scattering NUCLEAR REACTIONS 58Ni(π+, π+), (π+, π+'), E=162 MeV; calculated σ(θ); deduced weak virtual excitation effects. Coupled-channels, phenomenological, microscopic interaction models.
doi: 10.1103/PhysRevC.45.2027
1989BA75 Ann.Phys.(New York) 196, 89 (1989) J.Bartel, M.B.Johnson, M.K.Singham Pion Single-Charge-Exchange Scattering and Nuclear Structure in Deformed Nuclei NUCLEAR REACTIONS 165Ho(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), (π-, π0), E=165 MeV; calculated σ(θ). Coupled-channel optical model.
doi: 10.1016/0003-4916(89)90046-8
1989KO04 Phys.Rev. C39, 704 (1989) Pion Charge Exchange and the Optical Theorem NUCLEAR STRUCTURE 60Ni, 90Zr, 208Pb, 56Fe, 93Nb, 209Bi; calculated pion charge exchange features; deduced isotensor optical potential term features. Optical theorem.
doi: 10.1103/PhysRevC.39.704
1986SI07 Phys.Rev. C33, 2194 (1986) Nuclear Wave Function Considerations in Pion Photoproduction NUCLEAR REACTIONS 13C(γ, π+), E=194 MeV; calculated σ(θ); deduced wave function, Δ-isobar term roles.
doi: 10.1103/PhysRevC.33.2194
1986SI13 Phys.Rev. C34, 637 (1986) Radiative Pion Capture on 13C NUCLEAR REACTIONS 13C(π+, γ), E=115.5 MeV; calculated radiative capture σ(θ); deduced small core polarization, precursor effects. 13C(γ, π-), E not given; calculated σ(θ). DWIA.
doi: 10.1103/PhysRevC.34.637
1986SI22 Nucl.Phys. A460, 597 (1986) Electromagnetic and Weak Constraints on the Ground State Wave Functions of 13C and 13N NUCLEAR REACTIONS 13C(γ, π-), E not given; calculated σ(θ). 13C, 13N levels deduced electromagnetic, weak constraints.
doi: 10.1016/0375-9474(86)90527-0
1985SI05 Phys.Rev.Lett. 54, 1642 (1985); Erratum Phys.Rev. Lett. 55, 1156 (1985) Transverse Form Factors for 13C(e, e)13C(g.s.) and 13C(e, e')13C(*)(15.11 MeV) NUCLEAR REACTIONS 13C(e, e), (e, e'), E not given; calculated form factors; deduced configuration mixing effects.
doi: 10.1103/PhysRevLett.54.1642
1981SI09 Ann.Phys.(New York) 135, 71 (1981) Charged Pion Photoproduction from Light Nuclei NUCLEAR REACTIONS 12C(γ, π-), E=17, 50, 116 MeV; 12C(γ, π+), E=17, 29 MeV; 10B(γ, π+), E=15, 50, 112 MeV; 14N(γ, π-), E=30, 50, 80 MeV; 14N(γ, π+), E=30, 50, 80, 112 MeV; 6Li(γ, π+), E=38 MeV; calculated σ(θ). DWIA, optical potentials, pion-nucleus final state interactions.
doi: 10.1016/0003-4916(81)90144-5
1980SI07 Phys.Rev. C21, 1039 (1980) Role of Gamow-Teller Suppression and M1 Radiative Widths on π- Photoproduction from 14N NUCLEAR REACTIONS 14N(γ, π-), E=145-325 MeV; calculated σ(θ), total σ; deduced structure effects, pion distortions, Blomqvist-Laget operator.
doi: 10.1103/PhysRevC.21.1039
1979SI16 Phys.Rev.Lett. 43, 1476 (1979) M.K.Singham, G.N.Epstein, F.Tabakin Photoproduction of 0-200 MeV Pions from 12C and 7Li NUCLEAR REACTIONS 7Li, 12C(γ, π-), E not given; calculated σ. Blomqvist-Laget operator, distorted waves.
doi: 10.1103/PhysRevLett.43.1476
1978EP01 Phys.Rev. C17, 702 (1978) G.N.Epstein, M.K.Singham, F.Tabakin 12C(γ, π-)12N(g.s.) Near Threshold NUCLEAR REACTIONS 12C(γ, π-), E ≤ threshold + 10 MeV; calculated σ(E), total σ(E).
doi: 10.1103/PhysRevC.17.702
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