NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = G.Randers-Pehrson Found 9 matches. 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
1983MA24 Nucl.Phys. A402, 220 (1983) A.Marcinkowski, R.W.Finlay, G.Randers-Pehrson, C.E.Brient, J.E.O'Donnell, K.Stankiewicz Neutron Emission Spectra and Angular Distributions at 25.7 MeV Neutron Bombarding Energies NUCLEAR REACTIONS 51V, 56Fe, 65Cu, 93Nb, 209Bi(n, xn), E=25.7 MeV; measured σ(θ, En). Pre-equilibrium theory analysis. Enriched targets.
doi: 10.1016/0375-9474(83)90495-5
1983TA09 Nucl.Phys. A401, 237 (1983) R.C.Tailor, J.Rapaport, R.W.Finlay, G.Randers-Pehrson Neutron Scattering from 26Mg NUCLEAR REACTIONS 26Mg(n, n), (n, n'), E=24 MeV; measured σ(E, θ); deduced optical model parameters. 26Mg levels deduced deformation parameters, neutron, proton transition matrix elements ratio. Enriched target. DWBA, coupled-channels model analyses.
doi: 10.1016/0375-9474(83)90528-6
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
1982GR26 Nucl.Instrum.Methods 203, 269 (1982) S.M.Grimes, P.Grabmayr, R.W.Finlay, S.L.Graham, G.Randers-Pehrson, J.Rapaport A Technique to Correct for Backgrounds Caused by Break-Up Neutrons from the D(d, n) Reaction NUCLEAR REACTIONS 2H, 3,4He(d, n), E=8 MeV; measured σ(En). 2H(d, n), E=8.03, 6.04 MeV; 3He(d, n), E=7.78, 8.28, 6.4, 6.15 MeV; measured breakup σ(θn=0°).
doi: 10.1016/0167-5087(82)90636-6
1982YA05 Nucl.Phys. A390, 449 (1982) Yan Yiming, C.E.Brient, R.W.Finlay, G.Randers-Pehrson, A.Marcinkowski, R.C.Tailor, J.Rapaport Interaction of 11 MeV Neutrons with 89Y NUCLEAR REACTIONS 89Y(n, n), (n, n'), E=11 MeV; measured σ(E, θ); deduced optical model parameters. 89Y levels deduced deformation parameters. DWBA, collective model.
doi: 10.1016/0375-9474(82)90278-0
1981KU12 Nucl.Phys. A367, 157 (1981) V.Kulkarni, J.Rapaport, R.W.Finlay, G.Randers-Pehrson, R.D.Koshel Differential Cross-Section Measurements of the 2H(n, p)2n and 2H(n, d)n Reactions and the n - n Scattering Length NUCLEAR REACTIONS 2H(n, p), E=11, 25 MeV; measured σ(Ep, θp); deduced n-n scattering length. 2H(n, d), E=9, 11 MeV; measured σ(θ). Magnetic quadrupole triplet spectrometer, kinematically incomplete deuteron breakup. Faddeev three-body formalism.
doi: 10.1016/0375-9474(81)90511-X
1970CO06 Nucl.Phys. A142, 445 (1970) M.D.Cooper, A.S.Figuera, G.Pfeufer, G.Randers-Pehrson Behavior of the Cross Section for the 9Be(p, p)9Be Reaction Near the 2.06 MeV (p, n) Threshold NUCLEAR REACTIONS 9Be(p, p), E=1.99-2.10 MeV; measured σ(E).
doi: 10.1016/0375-9474(70)90540-3
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