NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = R.W.Finlay Found 71 matches. 2004OS02 Phys.Rev. C 70, 054613 (2004) J.H.Osborne, F.P.Brady, J.L.Romero, J.L.Ullmann, D.S.Sorenson, A.Ling, N.S.P.King, R.C.Haight, J.Rapaport, R.W.Finlay, E.Bauge, J.P.Delaroche, A.J.Koning Measurement of neutron elastic scattering cross sections for 12C, 40Ca, and 208Pb at energies from 65 to 225 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(n, n), E=65-225 MeV; measured σ(θ). Comparison with model predictions, previous results.
doi: 10.1103/PhysRevC.70.054613
2003DI03 Phys.Rev. C 67, 044606 (2003) F.S.Dietrich, J.D.Anderson, R.W.Bauer, S.M.Grimes, R.W.Finlay, W.P.Abfalterer, F.B.Bateman, R.C.Haight, G.L.Morgan, E.Bauge, J.-P.Delaroche, P.Romain Importance of isovector effects in reproducing neutron total cross section differences in the W isotopes NUCLEAR REACTIONS 182,184,186W(n, X), E=5-560 MeV; measured total σ. Comparison with model predictions.
doi: 10.1103/PhysRevC.67.044606
2003OP01 Phys.Rev.Lett. 91, 212302 (2003) A.K.Opper, E.Korkmaz, D.A.Hutcheon, R.Abegg, C.A.Davis, R.W.Finlay, P.W.Green, L.G.Greeniaus, D.V.Jordan, J.A.Niskanen, G.V.O'Rielly, T.A.Porcelli, S.D.Reitzner, P.L.Walden, S.Yen Charge Symmetry Breaking in np → dπ0 NUCLEAR REACTIONS 1H(n, π0), E=279.5 MeV; measured σ(θ), forward-backward asymmetry; deduced charge symmetry breaking. Comparison with model predictions.
doi: 10.1103/PhysRevLett.91.212302
2001AB14 Phys.Rev. C63, 044608 (2001) W.P.Abfalterer, F.B.Bateman, F.S.Dietrich, R.W.Finlay, R.C.Haight, G.L.Morgan Measurement of Neutron Total Cross Sections up to 560 MeV NUCLEAR REACTIONS H, Li, 6,7Li, B, 10,11B, C, 13C, F, Mg, S, P, K, Ca, Ti, V, Cr, Mn, Fe, Ni, Co, Y, Mo, In, W, 197Au, Hg, Pb, Th, 238U(n, X), E < 600 MeV; measured transmission neutron spectra; deduced total σ. Comparisons with model predictions, previous results.
doi: 10.1103/PhysRevC.63.044608
2000AB40 Phys.Rev. C62, 064312 (2000) W.P.Abfalterer, R.W.Finlay, S.M.Grimes Level Widths and Level Densities of Nuclei in the 32 ≤ A ≤ 60 Mass Region Inferred from Fluctuation Analysis of Total Neutron Cross Sections NUCLEAR REACTIONS C, F, 31P, 32S, 39K, 51V, 56Fe, 59Co(n, X), E=0.75-11.3 MeV; measured total σ. 32P, 33S, 40K, 52V, 57Fe, 60Co deduced level widths, level density parameters. White neutron source, fluctuation analysis.
doi: 10.1103/PhysRevC.62.064312
2000OP01 Nucl.Phys. A663-664, 505c (2000) A.K.Opper, E.G.Auld, R.M.Churchman, C.A.Davis, R.W.Finlay, P.W.Green, L.G.Greeniaus, D.A.Hutcheon, D.V.Jordan, E.J.Korkmaz, J.A.Niskanen, G.V.O'Rielly, T.Porcelli, S.D.Reitzner, P.L.Walden, S.Yen Charge Symmetry Breaking in the Reaction np → dπ0 NUCLEAR REACTIONS 1H(n, π0), E=279.5 MeV; measured deuteron spectra, forward-backward asymmetry.
doi: 10.1016/S0375-9474(99)00642-9
1998AB21 Phys.Rev.Lett. 81, 57 (1998) W.P.Abfalterer, F.B.Bateman, F.S.Dietrich, Ch.Elster, R.W.Finlay, W.Glockle, J.Golak, R.C.Haight, D.Huber, G.L.Morgan, H.W.Witala Inadequacies of the Nonrelativistic 3N Hamiltonian in Describing the n + d Total Cross Section NUCLEAR REACTIONS 1,2H(n, X), E=7-600 MeV; measured σ; deduced possible relativistic effects. Fadeev calculations.
doi: 10.1103/PhysRevLett.81.57
1994IS08 At.Data Nucl.Data Tables 58, 245 (1994) Calculated Differential Elastic and Inelastic Neutron Scattering by 12C and 16O between 30 and 60 MeV NUCLEAR REACTIONS 12C, 16O(n, n), (n, n'), E ≤ 60 MeV; analyzed data; deduced Legendre coefficient expansions applicable to transport, dosimetry, scintillator response calculations. DWBA.
doi: 10.1006/adnd.1994.1030
1993AB03 Phys.Rev. C47, 1033 (1993) W.Abfalterer, R.W.Finlay, S.M.Grimes, V.Mishra Level Densities of 28Al, 29Si, and 41Ca Inferred from Fluctuation Measurements NUCLEAR REACTIONS 27Al, 28Si, 40Ca(n, n), E=4-20 MeV; measured σ(E). 28Al, 29Si, 41Ca deduced level density.
doi: 10.1103/PhysRevC.47.1033
1993FI01 Phys.Rev. C47, 237 (1993) R.W.Finlay, W.P.Abfalterer, G.Fink, E.Montei, T.Adami, P.W.Lisowski, G.L.Morgan, R.C.Haight Neutron Total Cross Sections at Intermediate Energies NUCLEAR REACTIONS 9Be, C, N, O, 27Al, Si, 40Ca, Cu, 90Zr, 93Nb, Sn, Ta, 208Pb, 209Bi(n, X), E ≤ 600 MeV; measured transmission vs neutron energy; deduced total σ(E), neutron mean free path. Enriched 40Ca, 90Zr, 208Pb targets.
doi: 10.1103/PhysRevC.47.237
1993JI01 Phys.Rev. C47, 1697 (1993) Analysis of Total Neutron-Nucleus Cross Sections using Relativistic Impulse Approximation NUCLEAR REACTIONS 208Pb, 90Zr, 40Ca(n, n), E=100-600 MeV; calculated σ(E). Relativistic impulse approximation.
doi: 10.1103/PhysRevC.47.1697
1993MA33 Nucl.Phys. A561, 387 (1993) A.Marcinkowski, J.Rapaport, R.W.Finlay, C.Brient, M.Herman, M.B.Chadwick Neutron Emission Cross Sections at Low Bombarding Energies and the Novelty in Multistep Compound Reaction Model NUCLEAR REACTIONS 165Ho, 181Ta(n, xn), E=6.7, 20 MeV; measured σ(E(n), θ); deduced reaction mechanism. Modified statistical multistep model analysis.
doi: 10.1016/0375-9474(93)90018-S
1991LI36 Phys.Rev. C44, 2794 (1991) A.Ling, X.Aslanoglou, F.P.Brady, R.W.Finlay, R.C.Haight, C.R.Howell, N.S.P.King, P.W.Lisowski, B.K.Park, J.Rapaport, J.L.Romero, D.S.Sorenson, W.Tornow, J.L.Ullmann Ground-State Gamow-Teller Strength in 64Ni(n, p)64Co Cross Sections at 90-240 MeV NUCLEAR REACTIONS 64Ni(n, p), E=90-240 MeV; measured σ(E, θ); deduced unit σ. DWIA analysis.
doi: 10.1103/PhysRevC.44.2794
1990DA10 Phys.Rev. C42, 1013 (1990) n + 209Bi Mean Field between - 20 and 60 MeV NUCLEAR REACTIONS 209Bi(n, n), E=7.5-24 MeV; measured σ(θ); deduced model parameters. Dispersive optical model analysis.
doi: 10.1103/PhysRevC.42.1013
1989FI02 Phys.Rev. C39, 804 (1989) R.W.Finlay, J.Wierzbicki, R.K.Das, F.S.Dietrich Phenomenological Analysis of Dispersion Corrections for Neutron and Proton Scattering from 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p), E=9-61 MeV; 208Pb(polarized n, n), E=4-40 MeV; analyzed σ(θ), A(θ); deduced optical model parameters, dispersion correction.
doi: 10.1103/PhysRevC.39.804
1989HE27 Phys.Rev.Lett. 63, 2457 (1989) W.Heeringa, H.O.Klages, Chr.Wolfl, R.W.Finlay Spin-Spin Cross Sections of 27Al and 93Nb for Neutrons from 20 to 50 MeV NUCLEAR REACTIONS 93Nb(polarized n, n), E=19-50 MeV; 27Al(polarized n, n), E=22-50 MeV; measured spin-spin σ; deduced spin-spin potential parameters.
doi: 10.1103/PhysRevLett.63.2457
1989HE32 Phys.Rev.Lett. 63, 2456 (1989) W.Heeringa, H.O.Klages, Chr.Wolfl, R.W.Finlay Spin-Spin Cross Sections Of 27Al And 93Nb For Neutrons From 20 To 50 Mev NUCLEAR REACTIONS 27Al(n, x), 93Nb(n, x), E=19-50 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 22175.
doi: 10.1103/PhysRevLett.63.2456
1989MA42 Nucl.Phys. A501, 1 (1989) A.Marcinkowski, R.W.Finlay, J.Rapaport, P.E.Hodgson, M.B.Chadwick Neutron Emission Cross Sections on 184W at 11.5 and 26 MeV and the Neutron-Nucleus Scattering Mechanism NUCLEAR REACTIONS 184W(n, xn), (n, n), E=11.5, 26 MeV; measured σ(En, θ). Statistical multistep theory analysis. Tof.
doi: 10.1016/0375-9474(89)90562-9
1988CH07 Phys.Rev. C37, 910 (1988) Evidence for Dispersion Relation Corrections in Inelastic Nucleon Scattering to the 3- State in 208Pb NUCLEAR REACTIONS 208Pb(n, n'), E=5-11 MeV; analyzed σ(θ). 208Pb level deduced deformation length. Dispersion corrected potentials.
doi: 10.1103/PhysRevC.37.910
1988IS03 Phys.In Med.Biol. 33, 315 (1988) M.S.Islam, R.W.Finlay, J.S.Petler, J.Rapaport, R.Alarcon, J.Wierzbicki Neutron Scattering Cross Sections and Partial Kerma Values for Oxygen, Nitrogen and Calcium at 18 < En < 60 MeV NUCLEAR REACTIONS 14N, 16O, 40Ca(n, n), (n, n'), E=18-60 MeV; measured σ(θ); deduced optical model parameters, partial kerma factors. Previously acquired data included in analysis.
1987AL02 Nucl.Phys. A462, 413 (1987) R.Alarcon, J.Rapaport, R.W.Finlay Nucleon Elastic Scattering from 40Ca between 11 and 48 MeV NUCLEAR REACTIONS Ca(n, n), E=19, 21.7, 25.5 MeV; measured σ(θ); 40Ca(n, n), (p, p), E=11-48 MeV; analyzed σ(θ). Optical model.
doi: 10.1016/0375-9474(87)90397-6
1987IS04 Nucl.Phys. A464, 395 (1987) M.S.Islam, R.W.Finlay, J.S.Petler Elastic and Inelastic Scattering of Nucleons from 16O NUCLEAR REACTIONS 16O(n, n), (n, n'), E=18-26 MeV; measured σ(θ). 16O(p, p), (p, p'), E=23.4-65.8 MeV; analyzed σ(θ); deduced elastic, inelastic contributions. DWBA, coupled-channels analyses.
doi: 10.1016/0375-9474(87)90307-1
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
1986DE10 Phys.Rev. C33, 1826 (1986) J.P.Delaroche, M.S.Islam, R.W.Finlay Giant Resonance Coupling and l-Dependent Potentials for 16O NUCLEAR REACTIONS 16O(n, n), (p, p), E=18-46 MeV; measured σ(E, θ); deduced giant resonance coupling, l-dependent potential effects. Natural target, coupled channel analysis.
doi: 10.1103/PhysRevC.33.1826
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
1985AN07 Nucl.Instrum.Methods 234, 483 (1985) J.R.M.Annand, R.W.Finlay, M.A.Polster Timing Characteristic of Large Cylindrical NE213 Counters NUCLEAR REACTIONS B(d, n), E=6.7, 7.5 MeV; measured σ(En). Tof, cylindrical NE213 scintillation counters.
doi: 10.1016/0168-9002(85)90995-7
1985AN15 Nucl.Phys. A443, 249 (1985) J.R.M.Annand, R.W.Finlay, F.S.Dietrich A Low-Energy Optical-Model Analysis of 208Pb and 209Bi NUCLEAR REACTIONS 208Pb, 209Bi(n, n), (n, n'), E=4-7 MeV; measured σ(E, θ); deduced optical model parameters. Statistical model analysis, DWBA, coupled-channel calculations.
doi: 10.1016/0375-9474(85)90263-5
1985AN20 Nucl.Phys. A442, 234 (1985) Direct Neutron Scattering from 182W and 184W NUCLEAR REACTIONS 182W, 184W(n, n'), E=4.87, 6 MeV; measured σ(θ). 182,184W levels deduced electromagnetic transition matrix elements, β2, β4, β6 parameters. Rotation-vibration model, dynamic deformation theory, coupled-channel analysis.
doi: 10.1016/0375-9474(85)90143-5
1985FI02 Phys.Lett. 155B, 313 (1985) R.W.Finlay, J.R.M.Annand, J.S.Petler, F.S.Dietrich Anomalous Behavior of the n + 208Pb Potential near the Fermi Energy NUCLEAR REACTIONS 208Pb, 209Bi(n, n), (n, n'), E=4-7 MeV; measured σ(θ); deduced potential parameters, Fermi surface anomaly.
doi: 10.1016/0370-2693(85)91577-1
1985FI09 Nucl.Instrum.Methods Phys.Res. B10/11, 396 (1985) R.W.Finlay, A.S.Meigooni, J.S.Petler, J.P.Delaroche Partial Kerma Factors for Neutron Interactions with 12C at 20 < E(n) < 65 MeV NUCLEAR REACTIONS 12C(n, n), (n, n'), E=20-26 MeV; measured σ(θ); deduced model parameters.
doi: 10.1016/0168-583X(85)90277-0
1985ME16 Nucl.Phys. A445, 304 (1985) A.S.Meigooni, R.W.Finlay, J.S.Petler, J.P.Delaroche Nucleon-Induced Excitation of Collective Bands in 12C NUCLEAR REACTIONS 12C(n, n), (n, n'), E=20.8, 22, 24, 26 MeV; measured σ(θ). 12C levels deduced deformation parameters, K, π assignments. Natural target. Coupled-channels analysis.
doi: 10.1016/0375-9474(85)90072-7
1985PE10 Phys.Rev. C32, 673 (1985) J.S.Petler, M.S.Islam, R.W.Finlay, F.S.Dietrich Microscopic Optical Model Analysis of Nucleon Scattering from Light Nuclei NUCLEAR REACTIONS 13C(n, n), E=24 MeV; 14N(n, n), E=20, 25 MeV; 16O, 27Al(n, n), E=18-26 MeV; measured σ(θ) vs E; 12C(n, n), E=20-40 MeV; 12C(p, p), E=35-46 MeV; 14N(p, p), E=35.2 MeV; 16O(p, p), E=24.5, 30.1, 39.7 MeV; analyzed σ(θ). Micropscopic optical model.
doi: 10.1103/PhysRevC.32.673
1984FI12 Phys.Rev. C30, 796 (1984) R.W.Finlay, J.R.M.Annand, T.S.Cheema, J.Rapaport, F.S.Dietrich Energy Dependence of Neutron Scattering from 208Pb in the Energy Range 7-50 MeV NUCLEAR REACTIONS 208Pb(n, n), E=7, 20, 22, 24 MeV; 208Pb(n, n'), E=7, 20, 22 MeV; measured σ(E, θ); deduced optical model parameters. 208Pb level deduced octupole deformation parameter.
doi: 10.1103/PhysRevC.30.796
1984KU09 Nucl.Phys. A420, 237 (1984) J.P.Kurup, R.W.Finlay, J.Rapaport, J.P.Delaroche Strong coupling and isospin effects in neutron scattering from 76, 80Se NUCLEAR REACTIONS 76Se, 80Se(n, n), (n, n'), E=8, 10 MeV; measured σ(θ), σ(En); deduced optical model parameters. 80,76Se levels deduced deformation parameters. Tof. Coupled-channels analyses.
doi: 10.1016/0375-9474(84)90441-X
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
1984WO06 Phys.Rev. C29, 1710 (1984) C.Wong, S.M.Grimes, R.W.Finlay Analysis of (p, p), (p, n), and (n, n) Scattering on the Even Tin Isotopes using the Lane Coupled Equations NUCLEAR REACTIONS 116,118,122,124Sn(p, n), E=24.5 MeV; measured σ(θ), σ(En); deduced isocalar, isovector strengths of potential. 116,120,124Sn(n, n), E=11 MeV; analyzed σ(θ); deduced potential parameters. Lane model, imaginary potential Coulomb correction.
doi: 10.1103/PhysRevC.29.1710
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
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
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
1981MO02 Nucl.Phys. A352, 221 (1981) R.A.Moyer, R.W.Finlay, G.M.Crawley Energy Dependence in Proton Inelastic Scattering NUCLEAR REACTIONS 92Mo(p, p), (p, p'), E=24.89, 29.84, 34.9, 45.3 MeV; measured σ(θ); deduced optical-model parameters. 92Mo levels deduced deformation lengths. Magnetic spectrometer, enriched target.
doi: 10.1016/0375-9474(81)90377-8
1980CO05 Phys.Rev. C21, 2147 (1980) J.R.Comfort, S.M.Austin, P.T.Debevec, G.L.Moake, R.W.Finlay, W.G.Love Inelastic Excitation of 12C and 14N by 122 MeV Protons and Implications for the Effective Nucleon-Nucleon Interaction NUCLEAR REACTIONS 12C, 14N(p, p), (p, p'), E=122 MeV; measured σ(Ep, θ). 12C level deduced β2. DWIA analysis, spin-orbit tensor effective interaction. Exchange terms.
doi: 10.1103/PhysRevC.21.2147
1980FI03 Nucl.Phys. A338, 45 (1980) R.W.Finlay, J.Rapaport, M.H.Hadizadeh, M.Mirzaa, D.E.Bainum Isospin Effects in Nucleon Inelastic Scattering from Single-Closed-Shell Nuclei (II). The Z = 50 Isotopes NUCLEAR REACTIONS 116,118,120,122,124Sn(n, n'), E=11 MeV; 116Sn(n, n'), E=24 MeV; measured σ(θ). 116,118,120,122,124Sn levels deduced deformation parameters. Enriched targets.
doi: 10.1016/0375-9474(80)90120-7
1980FI08 Nucl.Phys. A344, 257 (1980) R.W.Finlay, M.H.Hadizadeh, J.Rapaport, D.E.Bainum Neutron Inelastic Scattering to Octupole States in Single-Closed-Shell Nuclei NUCLEAR REACTIONS 88Sr, 90Zr, 116,118,120,124Sn(n, n), E=11 MeV; measured σ(θ). 88Sr, 90Zr, 116,118,120,124Sn level deduced deformation lengths. Enriched targets. DWBA analysis.
doi: 10.1016/0375-9474(80)90676-4
1980GR15 Nucl.Phys. A350, 167 (1980) P.Grabmayr, J.Rapaport, R.W.Finlay Elastic and Inelastic Scattering of 24 MeV Nucleons from Oxygen Isotopes NUCLEAR REACTIONS 16,18O(n, n), (n, n'), E=24 MeV; measured σ(E, θ); deduced optical model parameters. 16,18O deduced deformation lengths, transition matrix elements. Enriched targets. Coupled-channels, DWBA analyses.
doi: 10.1016/0375-9474(80)90395-4
1980RA10 Nucl.Phys. A341, 56 (1980) J.Rapaport, M.Mirzaa, M.Hadizadeh, D.E.Bainum, R.W.Finlay Neutron Elastic Scattering from 116,118,120,122,124Sn NUCLEAR REACTIONS 116,118,120,122,124Sn(n, n), E=11 MeV; 116,118,124Sn(n, n), E=24 MeV; measured σ(E, θ). 118,120,124Sn(n, n), E=5.0-10.6, 20-26 MeV; measured total σ; deduced optical-model parameters. Enriched samples.
doi: 10.1016/0375-9474(80)90361-9
1979FI04 Phys.Lett. 84B, 169 (1979) R.W.Finlay, J.Rapaport, V.R.Brown, V.A.Madsen, J.R.Comfort Isovector Deformation Parameters and Core Polarization NUCLEAR REACTIONS 116,118,120,122,124Sn(n, n), (n, n'), E=11 MeV; analyzed σ. 116,118,120,122,124Sn levels deduced T=0, T=1, quadrupole deformation parameters. Shell-model interpretation, core polarization of valence neutrons.
doi: 10.1016/0370-2693(79)90275-2
1979RA02 Nucl.Phys. A313, 1 (1979) J.Rapaport, T.S.Cheema, D.E.Bainum, R.W.Finlay, J.D.Carlson Neutron Elastic Scattering from 92,96,98,100Mo between E = 7 and 26 MeV NUCLEAR REACTIONS 92,96,98,100Mo(n, n), E=7, 9, 11, 20, 26 MeV; measured σ(E, θ); deduced optical model parameters.
doi: 10.1016/0375-9474(79)90565-7
1979RA23 Nucl.Phys. A330, 15 (1979) J.Rapaport, V.Kulkarni, R.W.Finlay A Global Optical-Model Analysis of Neutron Elastic Scattering Data NUCLEAR REACTIONS Ca(n, n), E=11, 20, 26 MeV; 90Zr(n, n), E=11 MeV; 92Mo, 208Pb(n, n), E=7, 9, 11, 20, 26 MeV; 116,124Sn(n, n), E=11, 24 MeV; measured σ(E, θ); deduced optical-model parameters.
doi: 10.1016/0375-9474(79)90533-5
1978BA60 Nucl.Phys. A311, 492 (1978) D.E.Bainum, R.W.Finlay, J.Rapaport, M.H.Hadizadeh, J.D.Carlson, J.R.Comfort Isospin Effects in Nucleon Inelastic Scattering from Single-Closed Shell Nuclei (I). The N = 50 Isotones NUCLEAR REACTIONS 88Sr, 90Zr, 92Mo(n, n), (n, n'), E=11 MeV; measured σ(θ); deduced optical model parameters, deformation parameters. Enriched targets.
doi: 10.1016/0375-9474(78)90526-2
1978RA04 Nucl.Phys. A296, 95 (1978) J.Rapaport, T.S.Cheema, D.E.Bainum, R.W.Finlay, J.D.Carlson Neutron Scattering from 208Pb NUCLEAR REACTIONS 208Pb(n, n), E=7, 9, 11, 20, 26 MeV; 208Pb(n, n'), E=11, 26 MeV; measured σ(E, θ); deduced optical model parameters. 208Pb levels deduced deformation parameters β3, β5.
doi: 10.1016/0375-9474(78)90414-1
1978SE02 Nucl.Phys. A298, 269 (1978) E.H.Sexton, R.E.Benenson, A.J.Elwyn, J.E.Monahan, F.T.Kuchnir, F.P.Mooring, J.F.Lemming, R.W.Finlay Polarization of Neutrons from (p, n) Reactions on Medium-Weight Nuclei At Isobaric Analog Resonances NUCLEAR REACTIONS 51V, 55Mn(p, n), E=1.5-2.36 MeV; measured relative σ(E, θ), neutron polarization. Natural targets.
doi: 10.1016/0375-9474(78)90257-9
1977BA38 Phys.Rev.Lett. 39, 443 (1977) D.E.Bainum, R.W.Finlay, J.Rapaport, J.D.Carlson, J.R.Comfort Isospin Dependence of Experimental Nuclear Deformations NUCLEAR REACTIONS 90Zr, 92Mo, 118,120,122,124Sn(n, n'), E=11 MeV; measured tof σ(θ). 90Zr, 92Mo, 118,120,122,124Sn deduced β.
doi: 10.1103/PhysRevLett.39.443
1977BA49 Phys.Rev. C16, 1377 (1977); Erratum Phys.Rev. C17, 856 (1978) D.E.Bainum, R.W.Finlay, J.Rapaport, J.D.Carlson, W.G.Love Excitation of Low-Lying Collective States in 40Ca and 208Pb by Inelastic Neutron Scattering NUCLEAR REACTIONS 208Pb(n, n), (n, n'), E=11, 25.7 MeV; 40Ca(n, n), (n, n'), E=11, 20 MeV; measured σ(θ). 208Pb, 40Ca deduced β. Distorted wave analysis.
doi: 10.1103/PhysRevC.16.1377
1977RA12 Nucl.Phys. A286, 232 (1977) J.Rapaport, J.D.Carlson, D.Bainum, T.S.Cheema, R.W.Finlay Neutron Elastic Scattering on T = 0 Nuclei NUCLEAR REACTIONS Si, S, Ca(n, n), E=11, 20, 26 MeV; measured σ(E, θ); deduced optical-model parameters.
doi: 10.1016/0375-9474(77)90404-3
1976FI04 Nucl.Phys. A261, 413 (1976) R.W.Finlay, C.McKenna, J.R.Comfort, D.Bainum Energy Levels in 98Tc from the 98Mo(p, n)98Tc and 97Mo(3He, d)98Tc Reactions NUCLEAR REACTIONS 98Mo(p, n), (p, nγ), E=2.4-4.2 MeV; 97Mo(3He, d), E=19.0-23.0 MeV; measured En(θ), Ed(θ), Eγ, σ(E), nγ-, γγ-coin; deduced Q for (p, n). 98Tc deduced levels, L, J, π. Enriched targets.
doi: 10.1016/0375-9474(76)90155-X
1974CO27 Phys.Rev. C10, 1236 (1974) J.R.Comfort, R.W.Finlay, C.M.McKenna, P.T.Debevec Masses of Technetium Isotopes NUCLEAR REACTIONS 96,97,98Mo(p, n), E=4-5 MeV; 96,97Mo(3He, d), E=19-23 MeV; measured Q. 96,97,98Tc deduced mass excesses.
doi: 10.1103/PhysRevC.10.1236
1973CO05 Nucl.Phys. A203, 89 (1973) J.M.Cox, H.D.Knox, R.O.Lane, R.W.Finlay Evidence for Assignment of 14.0 MeV State in 11B from 10B(n, n)10B NUCLEAR REACTIONS 10B(n, n), E=2.63 MeV; measured σ(θ), polarization. 11B deduced levels, J, π, L, resonance parameters. Enriched target.
doi: 10.1016/0375-9474(73)90425-9
1973KN06 Nucl.Phys. A217, 611 (1973) H.D.Knox, J.M.Cox, R.W.Finlay, R.O.Lane Differential Cross Section and Polarization for 2.63 MeV Neutrons Scattered from 12C NUCLEAR REACTIONS 12C(n, n), E=2.63 MeV; measured total σ, σ(θ), n-polarization. Deduced phase shifts.
doi: 10.1016/0375-9474(73)90415-6
1968BR05 Phys.Letters 26B, 248 (1968) R.C.Braley, M.A.Nagarajan, M.W.Gilpatrick, R.W.Finlay On the Reaction C12(n, n'γ)C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90548-0
1967BE75 Phys.Rev. 156, 1201 (1967) P.L.Beach, R.W.Finlay, R.L.Cassola, R.D.Koshel Elastic scattering of neutrons from O and Ar at 14.0 MeV NUCLEAR REACTIONS O(n, n), Ar(n, n), E=14 MeV; measured products, O, Ar; deduced σ, σ(E), σ(θ). Data were imported from EXFOR entry 11418.
doi: 10.1103/PhysRev.156.1201
1966FR18 Phys.Rev. 144, 854 (1966) A.J.Frasca, R.W.Finlay, R.D.Koshel, R.L.Cassola Elastic Neutron Scattering from B, C, K and Ca At 14.0 MeV NUCLEAR REACTIONS B, C, K, Ca(n, n), E=14 MeV; measured products, B, C, K, Ca; deduced σ, σ(E), σ(θ). Data were imported from EXFOR entry 10254.
doi: 10.1103/PhysRev.144.854
1964CA12 Phys. Rev. 134, B929 (1964) Circular Polarization Measurements in Eu154 NUCLEAR STRUCTURE 154Eu; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B929
1962FI02 Phys.Rev. 128, 2309 (1962) Angular Distributions for the F19(d, n)Ne20 Reaction NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.128.2309
1962FI09 Bull.Am.Phys.Soc. 7, No.8, 551, T10 (1962) Angular Distributions in the F19(d, n)Ne20 Reaction NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
1962FI12 TID-17720, p.8 (1962) NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
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