NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = M.W.Kermode Found 28 matches. 2001VA26 Can.J.Phys. 79, 715 (2001) The Pion Cut and the Negative-Energy Behaviour of Neutron-Proton Effective-Range Functions Near Threshold NUCLEAR STRUCTURE 2H; calculated neutron-proton interaction effective-range parameters, related features.
doi: 10.1139/cjp-79-4-715
1999ST10 J.Phys.(London) G25, 1057 (1999); Corrigendum J.Phys.(London) G25, 1779 (1999) T.L.Stewart, M.W.Kermode, N.Rowley, D.J.Beachey Lifetimes and Preformation Factors for the α-Decay of the Even-Even Actinides NUCLEAR STRUCTURE Z=88-96; A=220-248; calculated α-decay associated amplitudes, pre-formation factors. Lifetime, branching data input.
doi: 10.1088/0954-3899/25/5/309
1996ST14 Phys.Rev.Lett. 77, 36 (1996) T.L.Stewart, M.W.Kermode, D.J.Beachey, N.Rowley, I.S.Grant, A.T.Kruppa α Decay of Deformed Actinide Nuclei RADIOACTIVITY 221Fr, 227Pa, 241Am, 253Es(α); calculated α-decay associated anisotropies. Branching ratios data input.
doi: 10.1103/PhysRevLett.77.36
1996ST28 Nucl.Phys. A611, 332 (1996) T.L.Stewart, M.W.Kermode, D.J.Beachey, N.Rowley, I.S.Grant, A.T.Kruppa α-Particle Decay Through a Deformed Barrier RADIOACTIVITY A=220-248; Z=88-96; calculated α-decay associated amplitudes vs phases. 233,229U, 247,257Es, 237Np, 241Pu, 243,245Cm, 249Bk, 249Cf(α); calculated α-decay associated anisotropies, branching ratios in some cases. Eigenchannel formalism, sub-barrier fusion.
doi: 10.1016/S0375-9474(96)00404-6
1995VA17 J.Phys.(London) G21, 651 (1995) W.van Dijk, M.W.Kermode, D.J.Beachey The Energy Dependence of the Mixing Parameter ϵ for 3S1-3D1 Neutron-Proton Scattering NUCLEAR REACTIONS 1H(n, n), E ≤ 120 MeV; calculated tan (ϵ) vs E; deduced 3S1-3D1 mixing parameter energy dependence.
doi: 10.1088/0954-3899/21/5/009
1994VA01 Phys.Rev. C49, 895 (1994) W.van Dijk, M.W.Kermode, S.A.Moszkowski Shape Dependence of the Deuteron Radius NUCLEAR STRUCTURE 2H; calculated radius shape dependence; deduced D-state, potential nonlocality roles.
doi: 10.1103/PhysRevC.49.895
1992MU08 Phys.Rev. C45, 2603 (1992) M.M.Mustafa, E.-S.M.Hassan, M.W.Kermode, E.M.Zahran Extracting a Value of the Deuteron Radius by Reanalysis of the Experimental Data NUCLEAR STRUCTURE 1,2H, 1n; analyzed electric form factors data. 2H deduced rms radius.
doi: 10.1103/PhysRevC.45.2603
1992RO05 J.Phys.(London) G18, 165 (1992) N.Rowley, G.D.Jones, M.W.Kermode Deformation and α-Decay Anisotropies RADIOACTIVITY 249Cf, 243,241Am, 231Pa, 223Ra(α); analyzed α-decay anisotropy data; deduced α-capture related sign dependence on decay of deformed nucleus polarized in strong magnetic field.
doi: 10.1088/0954-3899/18/1/013
1992VA03 Phys.Rev. C45, 1528 (1992); Erratrum Phys.Rev. C46, 1564 (1992) Bar-Shape and Eigenshape Parameters from the Zero-Energy Wave Functions NUCLEAR REACTIONS 1H(n, n), E=low; calculated bar-shape, eigenshape parameters; deduced effective range parameters. Reid hard-core potential model, fit to effective range.
doi: 10.1103/PhysRevC.45.1528
1991KE01 Phys.Rev. C43, 416 (1991) M.W.Kermode, S.A.Moszkowski, M.M.Mustafa, W.van Dijk Nonlocality and the Radius of the Deuteron NUCLEAR STRUCTURE 2H; calculated S-, D-state wave functions; deduced nonlocality effects.
doi: 10.1103/PhysRevC.43.416
1991KE03 J.Phys.(London) G17, 105 (1991) M.W.Kermode, W.van Dijk, D.W.L.Sprung, M.M.Mustafa, S.A.Moszkowski Structure Effects in the Deuteron Wavefunction NUCLEAR STRUCTURE 2H; calculated S-, D-state wave functions, rms radius; deduced nucleon quark structure role.
doi: 10.1088/0954-3899/17/2/004
1991MU17 Few-Body Systems 11, 83 (1991) The Nonlocal Tensor Operator S(N)12(ρ, ρ') NUCLEAR STRUCTURE 2H; calculated matter radius, D-state probability, quadrupole moment vs tensor nonlocality strength.
doi: 10.1007/BF01318553
1988KA13 Nucl.Phys. A481, 94 (1988) A.Kabir, M.W.Kermode, N.Rowley Fusion Oscillations for 16O with 12C NUCLEAR REACTIONS, ICPND 16O(12C, X), E(cm) ≈ 7-27 MeV; calculated fusion σ(E).
doi: 10.1016/0375-9474(88)90475-7
1988KE06 Phys.Rev. C38, 2461 (1988) Comment on ' Model Wave Functions for the Deuteron ' NUCLEAR STRUCTURE 2H; analyzed deuteron wave function model; deduced tensor potential role.
doi: 10.1103/PhysRevC.38.2461
1986CO17 J.Phys.(London) G12, L291 (1986) S.G.Cooper, M.W.Kermode, L.J.Allen Optical Potential for 12 - 12C Scattering at 1016 MeV Obtained by Inversion NUCLEAR REACTIONS 12C(12C, 12C), E=1016 MeV; calculated potential parameters vs ion-ion separation distance. Inverse scattering method, WKB approximation.
doi: 10.1088/0305-4616/12/12/005
1986KE11 Phys.Lett. 174B, 357 (1986) M.W.Kermode, S.G.Cooper, S.Klarsfeld A Positive Short Range Tensor Model for the Deuteron NUCLEAR STRUCTURE 2H; calculated binding energy, quadrupole moment, rms radius. Positive short range tensor model.
doi: 10.1016/0370-2693(86)91015-4
1983MC01 J.Phys.(London) G9, 275 (1983) A.McKerrell, J.P.McTavish, M.W.Kermode, R.Huby The S-Wave Component of the Deuteron Wavefunction NUCLEAR STRUCTURE 2H; calculated electric form factor. Unitarily transformed deuteron wave function, S-wave node. NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated σ(capture). 2H(γ, p), E ≈ 5-100 MeV; calculated photodisintegration σ(E). Unitarily transformed deuteron wave function, S-wave node.
doi: 10.1088/0305-4616/9/3/007
1982AL04 Phys.Lett. 109B, 259 (1982) The Determination of the Deuteron Asymptotic D- to S-Ratio from Elastic dp Scattering NUCLEAR REACTIONS 2H(p, p), E=not given; analyzed data. 2H deduced asymptotic D- to S-state ratio.
doi: 10.1016/0370-2693(82)90430-0
1982KE03 J.Phys.(London) G8, L71 (1982) M.W.Kermode, L.J.Allen, J.P.McTavish On the Determination of the Asymptotic D- to S-State Ratio of the Deuteron Wavefunction from Sub-Coulomb (d, p) Measurements NUCLEAR STRUCTURE 2H; calculated asymptotic D- to S-state ratio; deduced bounds.
doi: 10.1088/0305-4616/8/6/004
1981AL14 J.Phys.(London) G7, 1367 (1981) L.J.Allen, J.P.McTavish, M.W.Kermode, A.McKerrell The Root-Mean-Square Radius of the Deuteron NUCLEAR STRUCTURE 2H; calculated rms, charge radii. Model-dependent, model-independent analyses.
doi: 10.1088/0305-4616/7/10/014
1981KE13 Z.Phys. A303, 167 (1981) M.W.Kermode, A.McKerrell, J.P.McTavish, L.J.Allen The Asymptotic S-State Amplitude of the Deuteron Wave Function NUCLEAR STRUCTURE 2H; calculated asymptotic S-state amplitude bounds, meson exchange current, relativistic effect, isobar contribution limits to quadrupole moment. Impulse approximation, different realistic interactions.
doi: 10.1007/BF01420275
1980MC02 J.Phys.(London) G6, 319 (1980) Proton-Proton Potential Models Obtained from the Virginia Phase-Shift Analysis NUCLEAR REACTIONS 1H(p, p), E=1-500 MeV; calculated equivalent local potentials; deduced nucleon structure effects.
doi: 10.1088/0305-4616/6/3/008
1977KE08 J.Phys.(London) G3, 565 (1977) Proton-Proton Scattering in the 3P0 and 3P1 States NUCLEAR REACTIONS 1H(p, p); calculated potentials.
doi: 10.1088/0305-4616/3/4/016
1976MC08 J.Phys.(London) G2, L83 (1976) A Comparison of the Livermore Constrained and Unconstrained n-p Phase-Shifts NUCLEAR REACTIONS 1H(n, n); calculated potential parameters.
doi: 10.1088/0305-4616/2/6/002
1976MC09 J.Phys.(London) G2, 375 (1976) Nonlocal Potentials for Proton-Proton Scattering NUCLEAR REACTIONS 1H(p, p); calculated potentials, phase-shifts.
doi: 10.1088/0305-4616/2/6/006
1975KE03 Can.J.Phys. 53, 207 (1975) M.W.Kermode, Y.Nogami, W.Van Dijk Coulomb Effect on the Proton-Proton Low Energy Scattering Parameters NUCLEAR REACTIONS 1H(p, p), E=low; calculated effect of Coulomb force on pp scattering.
doi: 10.1139/p75-031
1969KE09 Nucl.Phys. A134, 336 (1969) 8Be Parameters from α-α Scattering NUCLEAR STRUCTURE 8Be; calculated levels, level-width from α-α phase shifts.
doi: 10.1016/0375-9474(69)91056-2
1967KE10 Phys.Letters 25B, 183 (1967) The Excited 4+ States of 8Be
doi: 10.1016/0370-2693(67)90029-9
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