NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = G.Fink Found 10 matches. 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
1993PA18 Phys.Rev. C48, 711 (1993) B.K.Park, J.Rapaport, G.Fink, J.L.Ullmann, A.G.Ling, D.S.Sorenson, F.P.Brady, J.L.Romero, C.R.Howell, W.Tornow, W.Unkelbach Energy Dependence of Multipole Strength Distributions in the 32S(n, p)32P Reaction NUCLEAR REACTIONS 32S(n, p), E=60-220 MeV; measured σ(θ, Ep), σ(θ); deduced Gamow-Teller transition strengths. Shell model, RPA comparison.
doi: 10.1103/PhysRevC.48.711
1992WI08 Z.Phys. A341, 453 (1992) G.-D.Wicke, G.Mondry, F.Smend, G.Fink, P.Doll, S.Hauber, M.Haupenthal, H.Schieler, H.O.Klages Radiative Capture of Polarized Neutrons by 12C in the Energy Range E(n) = 20-35 MeV NUCLEAR REACTIONS 12C(polarized n, γ), E=20-35 MeV; measured γ(θ), asymmetry vs E, γ(recoil)-coin; deduced E2, E1 capture interference. Direct semidirect model.
doi: 10.1007/BF01301389
1991FI07 Nucl.Phys. A530, 331 (1991) G.Fink, P.Doll, S.Hauber, M.Haupenthal, H.O.Klages, H.Schieler, F.Smend, G.D.Wicke Neutron-Proton Capture Using Polarized Neutrons from 19 to 50 MeV NUCLEAR REACTIONS 1H(polarized n, γ), E=19-50 MeV; measured σ(θ), analyzing power vs θ. NE213 target.
doi: 10.1016/0375-9474(91)90806-H
1990FI08 Nucl.Phys. A518, 561 (1990) G.Fink, P.Doll, T.D.Ford, R.Garrett, W.Heeringa, K.Hofmann, H.O.Klages, H.Krupp Backward Angle np Differential Cross Sections from 22 to 50 MeV NUCLEAR REACTIONS 1H(n, n), E=22-50 MeV; measured σ(E, θ). Polyethylene target.
doi: 10.1016/0375-9474(90)90146-D
1986DO12 Nucl.Instrum.Methods Phys.Res. A250, 526 (1986) P.Doll, G.Fink, F.P.Brady, R.Garrett, H.O.Klages, H.Krupp ΔE-E Telescope Systems for Detecting Charged Particles Produced with a ' White ' Neutron Beam NUCLEAR REACTIONS 1H(n, p), E=25 MeV; measured σ(θ). White neutron source, ΔE-E charged particle telescope.
doi: 10.1016/0168-9002(86)91104-6
1936FI01 Phys.Rev. 50, 738 (1936) The production and absorption of thermal energy neutrons NUCLEAR REACTIONS 1H(n, γ), Li(n, X), B(n, X), 103Rh(n, γ), Ag(n, γ), Cd(n, γ), 127I(n, γ), Sm(n, γ), Gd(n, γ), Hg(n, γ), E=0.0253 eV; measured products, 2H, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 13845.
doi: 10.1103/PhysRev.50.738
1936RA01 Phys.Rev. 49, 104 (1936) F.Rasetti, E.Segre, G.Fink, J.R.Dunning, G.B.Pegram On the Absorption Law for Slow Neutrons NUCLEAR REACTIONS Cd, Ag(n, X), E<1 eV; measured reaction products, En, In; deduced transmission coefficients, 1/v absorption law.
doi: 10.1103/PhysRev.49.104
1935DU04 Phys.Rev. 48, 265 (1935) J.R.Dunning, G.B.Pegram, G.A.Fink, D.P.Mitchell Interaction of Neutrons with Matter
doi: 10.1103/PhysRev.48.265
1935DU05 Phys.Rev. 48, 704 (1935) J.R.Dunning, G.B.Pegram, G.A.Fink, D.P.Mitchell, E.Segre Velocity of Slow Neutrons by Mechanical Velocity Selector
doi: 10.1103/PhysRev.48.704
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