NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.E.Shamu Found 28 matches. 1999SH38 J.Phys.(London) G25, L125 (1999) R.E.Shamu, S.M.Ferguson, R.L.Schutt Symmetry Dependence of the Phenomenological Optical Model for Neutron-Nucleus Scattering NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(n, X), E=10-500 MeV; calculated total σ; deduced optical model parameters, symmetry dependence features. Comparisons with data.
doi: 10.1088/0954-3899/25/11/103
1993SH29 J.Phys.(London) G19, L169 (1993) Coupled-Channels Optical-Model Analysis of n-208Pb Scattering at Low Energies NUCLEAR REACTIONS 208Pb(n, n), (n, n'), E=8.5-10 MeV; analyzed σ(θ), σ data. Coupled-channels, optical model analyses, first-order vibrational model.
doi: 10.1088/0954-3899/19/11/004
1991SH04 J.Phys.(London) G17, 525 (1991) R.E.Shamu, J.Barnes, S.M.Ferguson, G.Haouat, J.Lachkar The Limitations of the One-Channel Phenomenological Optical Model NUCLEAR REACTIONS 208Pb(n, n), E=7.5-13.5 MeV; analyzed σ(θ); deduced model limitations. Optical model.
doi: 10.1088/0954-3899/17/4/011
1989BA30 J.Phys.(London) G15, L179 (1989) Search for Anomalous Behaviour in the Real n-208Pb Optical Potential at Low Energies NUCLEAR REACTIONS 208Pb(n, X), E=0.6-14 MeV; calculated σ(E); deduced model parameter energy dependence. Optical model.
doi: 10.1088/0954-3899/15/9/001
1988SC04 Phys.Lett. 203B, 22 (1988) R.L.Schutt, R.E.Shamu, P.W.Lisowski, M.S.Moore, G.L.Morgan Nucleon Scattering from 208Pb at Low and Intermediate Energies NUCLEAR REACTIONS 208Pb(n, n), E=2-250 MeV; analyzed σ(E). 208Pb(n, n), E=13.5-40 MeV; analyzed σ(θ); deduced model parameters. Phenomenological optical model.
doi: 10.1016/0370-2693(88)91562-6
1986SA18 Phys.Lett. 175B, 266 (1986) L.J.Satkowiak, S.M.Ferguson, R.E.Shamu, M.Soga Optical Model Potential for Neutrons in the Resonance Region NUCLEAR REACTIONS 208Pb(n, n), E ≈ 1-15 MeV; calculated σ(E); deduced optical model parameters.
doi: 10.1016/0370-2693(86)90853-1
1982LI23 Phys.Rev.Lett. 49, 255 (1982) P.W.Lisowski, R.E.Shamu, G.F.Auchampaugh, N.S.P.King, M.S.Moore, G.L.Morgan, T.S.Singleton Search For Resonance Structure In The np Total Cross Section Below 800 Mev NUCLEAR REACTIONS 1H(n, x), E=39-793 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12761.
doi: 10.1103/PhysRevLett.49.255
1980LA18 Nucl.Phys. A345, 193 (1980) Ch.Lagrange, J.Lachkar, G.Haouat, R.E.Shamu, M.T.McEllistrem Quadrupole Moments and Nucleon Excitation Strengths in Even-A Sm Isotopes NUCLEAR REACTIONS 148,152,154Sm(n, n), (n, n'), E=7 MeV; 148,152,154Sm(p, p), (p, p'), E=16 MeV; analyzed σ(θ); deduced optical model parameters. 148,152,154Sm levels deduced β2.
doi: 10.1016/0375-9474(80)90418-2
1980SH20 Phys.Rev. C22, 1857 (1980) R.E.Shamu, E.M.Bernstein, J.J.Ramirez, Ch.Lagrange Effects of Deformation on Neutron Total Cross Sections of Even-A Nd and Sm Isotopes NUCLEAR REACTIONS 142,144,146,148,150Nd(n, n), E=0.75-13.89 MeV; 148,150,152,154Sm(n, n), E=0.75-14.49 MeV; measured total σ(E); deduced deformation effects, isotopic dependence. 142,144,146,148,150Nd, 148,150,152,154Sm(n, n'), E=4, 7 MeV; analyzed data; 142,144,146,148,150Nd, 148,150,152,154Sm level deduced β2. Coupled-channels calculation.
doi: 10.1103/PhysRevC.22.1857
1979HA31 Phys.Rev. C20, 78 (1979) G.Haouat, J.Lachkar, C.Lagrange, M.T.McEllistrem, Y.Patin, R.E.Shamu, J.Sigaud Optical Potential and Nuclear Deformation for Even Nd Isotopes from Fast Neutron Scattering NUCLEAR REACTIONS 142,144,146,148,150Nd(n, n), (n, n'), E=7.0 MeV; measured σ(En, θ). 142,144,146,148,150Nd deduced optical model parameters, β2.
doi: 10.1103/PhysRevC.20.78
1977MC02 Phys.Rev. C15, 927 (1977) M.T.McEllistrem, R.E.Shamu, J.Lachkar, G.Haouat, C.Lagrange, Y.Patin, J.Sigaud, F.Cocu Deformation Effects in Neutron Scattering from the Sm Isotopes NUCLEAR REACTIONS 148,150,152,154Sm(n, n), (n, n'), E=7 MeV; measured σ(θ); deduced coupled-channels potential parameters. 148,150,152,154Sm deduced β2.
doi: 10.1103/PhysRevC.15.927
1976SH06 Phys.Lett. 61B, 29 (1976) R.E.Shamu, C.H.Lagrange, E.M.Bernstein, J.J.Ramirez, T.Tamura, C.Y.Wong Quadrupole Deformation Parameters of 148,152,154Sm Determined from Neutron Total Cross Sections NUCLEAR REACTIONS 148,152,154Sm(n, X), E=0.75-14.5 MeV; measured relative σ. 148,152,154Sm deduced β.
doi: 10.1016/0370-2693(76)90553-0
1975LA18 Phys.Lett. 58B, 293 (1975) C.Lagrange, R.E.Shamu, T.Burrows, G.P.Glasgow, G.Hardie, F.D.McDaniel Effect of Nuclear Deformation on Neutron Elastic Scattering NUCLEAR REACTIONS 148,154Sm(n, n'), E=6.25 MeV; measured σ(En', θ). 148,154Sm(n, n), E=6.25 MeV; measured σ(θ). 148,154Sm deduced β.
doi: 10.1016/0370-2693(75)90656-5
1974SH06 Nucl.Instrum.Methods 114, 605 (1974) R.E.Shamu, E.M.Bernstein, M.J.Parrott Accelerator Energy Calibration Using the 12C(α, n0)15O Threshold NUCLEAR REACTIONS 7Li, 13C, 19F(p, n), 2H(16O, n); measured Q.
doi: 10.1016/0029-554X(74)90187-6
1973SH15 Phys.Lett. 45B, 241 (1973) R.E.Shamu, E.M.Bernstein, D.Blondin, J.J.Ramirez, G.Rochau Effects of Nuclear Deformation on Neutron Total Cross Sections NUCLEAR REACTIONS 150,152,154Sm(n, X), E=0.8-15 MeV; measured σ(E). Transmission method.
doi: 10.1016/0370-2693(73)90193-7
1972BE15 Phys.Rev.Lett. 28, 923 (1972) E.M.Bernstein, J.J.Ramirez, R.E.Shamu, Pui-Wah Cheng, M.Soga Spectroscopic Determinations from Resonance Spin-Flip NUCLEAR REACTIONS 12C(p, p'), E approx 8 MeV; measured σ(θ), spin-flip probability; deduced resonance/backgroung spin-flip interference.
doi: 10.1103/PhysRevLett.28.923
1972SH08 Nucl.Phys. A189, 220 (1972) R.E.Shamu, E.M.Bernstein, D.Blondin, J.J.Ramirez The Mass of 15O NUCLEAR REACTIONS 15N(p, n); measured threshold energy, Q. 15O deduced mass. Enriched target.
doi: 10.1016/0375-9474(72)90655-0
1971BE07 Phys.Rev. C3, 427 (1971) E.M.Bernstein, R.E.Shamu, L.Y.Kuo, L.D.Oppliger, G.Hardie, M.Soga Large Isospin Mixing in 16O States Near 18 MeV NUCLEAR REACTIONS 12C(α, n), (α, p), E=13-16 MeV; measured σ(E;θ). 16O deduced levels, level-width, isospin-mixed doublet.
doi: 10.1103/PhysRevC.3.427
1970BE58 Phys.Lett. 33B, 465 (1970) E.M.Bernstein, G.R.Boss, G.Hardie, R.E.Shamu The One-Phonon Octupole Vibration of 151Eu NUCLEAR REACTIONS 151Eu(d, d'), E=12 MeV; measured σ(Ed', θ). 151Eu deduced levels, multiplet.
doi: 10.1016/0370-2693(70)90218-2
1964SH30 Phys.Rev. 135, B99 (1964) Neutron-alpha scattering in the 20-MeV range NUCLEAR REACTIONS 4He(n, d), 4He(n, n), 4He(n, x), E=16.4-29 MeV; measured products, 2-HE-4, 3H, 2H; deduced σ, σ(E), σ(θ). Data were imported from EXFOR entry 30405.
doi: 10.1103/PhysRev.135.B99
1963OH02 Nucl.Phys. 45, 523 (1963) The Elastic Scattering of Deuterons by Carbon NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90828-9
1963SH06 Phys.Letters 4, 286 (1963) R.E.Shamu, G.G.Ohlsen, P.G.Young The He5 States at High Excitation Energies NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90603-6
1963SH10 Bull.Am.Phys.Soc. 8, No.6, 477, N3 (1963) R.E.Shamu, J.G.Jenkin, B.A.Robson Neutron-Alpha Scattering in the 20-MeV Range
1962AU03 Phys.Rev. 126, 1532 (1962) S.M.Austin, H.H.Barschall, R.E.Shamu Scattering of Neutrons by α Particles NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.126.1532
1962SH09 Nuclear Phys. 31, 166 (1962) The Disintegration of Neon and Krypton by Neutrons NUCLEAR STRUCTURE 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90738-1
1961AU03 TID-14475 (1961); Nuclear Sci.Abstr. 16, 1038, Abstr. 8103 (1962) S.M.Austin, H.H.Barschall, R.E.Shamu NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
1960AU02 Bull.Am.Phys.Soc. 5, No.6, 410, D11 (1960) Angular Distributions in n-α Elastic Scattering NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
1960SH09 Bull.Am.Phys.Soc. 5, No.6, 410, D10 (1960) R.E.Shamu, W.Benenson, R.L.Walter Disintegration of Ne and Kr by Fast Neutrons NUCLEAR STRUCTURE 17O; measured not abstracted; deduced nuclear properties.
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