NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = S.Mellema Found 9 matches. 1987ME10 Phys.Rev. C36, 577 (1987) S.Mellema, J.S.Petler, R.W.Finlay, F.S.Dietrich, J.A.Carr, F.Petrovich Microscopic Distorted-Wave Approximation Study of Low-Energy Nucleon Scattering from 89Y NUCLEAR REACTIONS 89Y(n, n), (n, n'), E=11 MeV; measured σ(θ). 89Y levels deduced B(λ), transition densities. Tof. Optical model. Microscopic distorted wave calculations.
doi: 10.1103/PhysRevC.36.577
1986ME01 Phys.Rev. C33, 481 (1986) S.Mellema, R.W.Finlay, F.S.Dietrich Neutron Inelastic Scattering from 54,56Fe NUCLEAR REACTIONS 56,54Fe(n, n'), E=11, 26 MeV; measured σ(θ); deduced optical model parameters. 54,56Fe levels deduced β. DWBA, coupled-channels analyses.
doi: 10.1103/PhysRevC.33.481
1986ME02 Phys.Lett. 166B, 282 (1986) S.Mellema, T.R.Wang, W.Haeberli Evidence for Multipolarities other than E2 in the 2H(d, γ)4He Reactions NUCLEAR REACTIONS 2H(polarized d, γ), E=10 MeV; measured σ(θ), vector, tensor analyzing power vs θ.
doi: 10.1016/0370-2693(86)90799-9
1986ME16 Phys.Rev. C34, 2043 (1986) S.Mellema, T.R.Wang, W.Haeberli Tensor-Force Effects in the 2H(d(pol), γ)4He Reaction and the D State of 4He NUCLEAR REACTIONS 2H(polarized d, γ), E=10 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced partial-wave amplitudes, phases. 4He transitions deduced γ-multipolarity, multipole strengths.
doi: 10.1103/PhysRevC.34.2043
1984ME07 Phys.Rev. C29, 2385 (1984) S.Mellema, R.W.Finlay, F.S.Dietrich, F.Petrovich Isovector Effects in Nucleon Inelastic Scattering in a Density-Dependent Folding Model NUCLEAR REACTIONS 56,54Fe(p, p'), (n, n'), E=11-26 MeV; analyzed σ(θ); deduced isovector effects. 54,56Fe levels deduced neutron, proton transition matrix element ratio. Microscopic DWBA, folding model potentials from density-dependent interactions.
doi: 10.1103/PhysRevC.29.2385
1983DI11 Phys.Rev.Lett. 51, 1629 (1983) F.S.Dietrich, R.W.Finlay, S.Mellema, G.Randers-Pehrson, F.Petrovich Isospin Dependence of the Microscopic Optical Model for Nucleon Scattering NUCLEAR REACTIONS 208Pb(n, n), E=7-24 MeV; measured σ(θ). 208Pb(p, p), E=21-61.4 MeV; analyzed σ(θ); deduced optical model isospin dependence. Microscopic folding model study.
doi: 10.1103/PhysRevLett.51.1629
1983MA19 Nucl.Sci.Eng. 83, 13 (1983) A.Marcinkowski, R.W.Finlay, G.Randers-Pehrson, C.E.Brient, R.Kurup, S.Mellema, A.Meigooni, R.Tailor Neutron Emission Cross Sections at 25.7 MeV: 51V, 56Fe, 65Cu, 93Nb, and 209Bi NUCLEAR REACTIONS 51V, 56Fe, 65Cu, 93Nb, 209Bi(n, xn), E=25.7 MeV; measured σ(θ), σ(En, θ). Monoisotopic targets, tof.
doi: 10.13182/NSE83-13
1983ME21 Phys.Rev. C28, 2267 (1983) S.Mellema, R.W.Finlay, F.S.Dietrich, F.Petrovich Microscopic and Conventional Optical Model Analysis of Fast Neutron Scattering from 54,56Fe NUCLEAR REACTIONS 54Fe(n, n), E=20, 22, 24, 26 MeV; 56Fe(n, n), E=20, 26 MeV; measured σ(θ); deduced optical model parameters. Phenomenological, microscopic models.
doi: 10.1103/PhysRevC.28.2267
1982FI08 Nucl.Instrum.Methods 198, 197 (1982) R.W.Finlay, C.E.Brient, D.E.Carter, A.Marcinkowski, S.Mellema, G.Randers-Pehrson, J.Rapaport The Ohio University Beam Swinger Facility NUCLEAR REACTIONS B(d, n), E=8 MeV; 12C(n, n), (n, n'), E=24 MeV; measured σ(En); 208Pb(n, n), (n, n'), E=7.2 MeV; measured σ(θ). Tof, beam swinger magnet.
doi: 10.1016/0167-5087(82)90256-3
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