NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = W.Wylie Found 10 matches. 1985SC08 Nucl.Sci.Eng. 89, 87 (1985) H.R.Schelin, E.Farrelly Pessoa, W.R.Wylie, J.L.Cardoso, Jr., R.A.Douglas The 10,11B(p, n)10,11C Reactions Between E(p) = 13.7 and 14.7 MeV NUCLEAR REACTIONS 10,11B(p, n), E=13.7-14.7 MeV; measured absolute σ(θ) vs E.
doi: 10.13182/NSE85-A17886
1984SC04 Nucl.Phys. A414, 67 (1984) H.R.Schelin, E.Farrelly Pessoa, W.R.Wylie, E.W.Cybulska, K.Nakayama, L.M.Fagundes, R.A.Douglas The 12C(d, n)13N Reaction between E(d) = 7.0 and 13.0 MeV NUCLEAR REACTIONS 12C(d, n), E=7, 9.1, 13 MeV; measured σ(En), σ(E), absolute σ(θ). 12C(d, n), E=10.6-13 MeV; measured σ(E). 13N levels deduced S. Hauser-Feshbach reduction factors. Tof. DWBA analysis.
doi: 10.1016/0375-9474(84)90497-4
1983GU03 Nucl.Phys. A395, 1 (1983) P.P.Guss, K.Murphy, R.C.Byrd, C.E.Floyd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power for the 2H(d, n)3He(g.s.) Reaction from 5.5 to 11.5 MeV NUCLEAR REACTIONS 2H(polarized d, n), E=5.5, 7, 8.5, 10, 11.5 MeV; measured A(θ). Report discrepancies with previous measurements. Polynomial expansions analysis.
doi: 10.1016/0375-9474(83)90085-4
1983WO02 Nucl.Phys. A394, 139 (1983) E.Woye, W.Tornow, G.Mack, C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power A(y)(θ) for 12C(n, n0, 1)12C between 8.9 and 14.9 MeV Neutron Energy NUCLEAR REACTIONS 12C(n, n), (n, n'), E=8.9-14.9 MeV; measured A(E, θ); deduced optical potential parameters. 12C level deduced quadrupole deformation.
doi: 10.1016/0375-9474(83)90167-7
1971WY03 Helv.Phys.Acta 44, 757 (1971) Elastic Scattering of Protons from Chromium NUCLEAR REACTIONS Cr(p, p), E=2.4-4.1 MeV measured σ(E). 53Mn deduced isobaric analog resonance, level-width, Coulomb displacement energy. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0103. 1970BA31 Phys.Rev. C2, 859 (1970) R.M.Bahnsen, W.R.Wylie, H.W.Lefevre Thick-Target O16(d, n)F17 Yield Curves NUCLEAR REACTIONS 16O(d, n), E=2.0-4.2 MeV; measured σ(E;En, θ).
doi: 10.1103/PhysRevC.2.859
1970BR20 Nucl.Phys. A151, 211 (1970) H.Brandle, W.R.Wylie, F.Zamboni, W.Zych The Isobaric Analog Pair 57Fe - 57Co NUCLEAR REACTIONS 56Fe(p, γ), Ep=1.2-1.6 MeV; 56Fe(p, p), Ep=3.7-4.3 MeV; measured σ(E;θ). 57Co resonances deduced, J, π, level-width, p-width, isobaric analog. Natural iron target.
doi: 10.1016/0375-9474(70)90980-2
1970WY02 Nucl.Instrum.Methods 79, 245 (1970) W.R.Wylie, R.M.Bahnsen, H.W.Lefevre Differential excitation curves from thick target neutron spectra NUCLEAR REACTIONS 16O(d, n)17F, E<4.5 MeV; measured reaction products, En, In; deduced σ(θ).
doi: 10.1016/0029-554X(70)90147-3
1967WY02 Bull.Am.Phys.Soc. 12, 894 H10 (1967) W.R.Wylie, R.M.Bahnsen, H.W.Lefevre C12(d, n)N13 g.s. Excitation Curves as a Function of Angle by a Thick-Target Method NUCLEAR REACTIONS 12C(d, n), E=2.2-4 MeV; measured reaction products, TOF, En, In; deduced neutron spectra, thick target yields.
1966WY01 Bull.Am.Phys.Soc. 11, 903 P5 (1966) W.R.Wylie, J.L.Binney, R.M.Bahnsen, H.W.Lefevre Thick Target C12(d, n)N13 Neutron Spectrum NUCLEAR REACTIONS 12C(d, n), E not given; measured reaction products, TOF, En, In; deduced neutron spectra, thick target yields.
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