NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = F.J.Vaughn Found 30 matches. 1970VA26 Phys.Rev. C2, 1657 (1970) F.J.Vaughn, R.A.Chalmers, D.Kohler, L.F.Chase, Jr. Cross Sections for the 7Be(p, γ)8B Reaction NUCLEAR REACTIONS 7Be(p, γ), E=0.953-3.281 MeV; measured σ(E), delayed-α spectrum. 8B deduced resonance, level-width.
doi: 10.1103/PhysRevC.2.1657
1969GR42 Bull.Am.Phys.Soc. 14, No.8, 853, FC13 (1969); Priv.Comm. (Jan. 1972) H.A.Grench, F.J.Vaughn, K.E.Bender 190Os(n, n')190Os Cross-Section Measurements near Threshold NUCLEAR REACTIONS 190Os(n, n'), E ∼ 400 keV; measured reaction products; deduced σ. Comparison with Hauser-Feshbach theory.
1967GR02 Nucl.Phys. A94, 157 (1967) H.A.Grench, K.L.Coop, H.O.Menlove, F.J.Vaughn A Study of the Spin Dependence of the Nuclear Level Density by Means of the 89Y(n, γ)90g,90mY Reactions with Fast Neutrons NUCLEAR REACTIONS 89Y(n, γ)90Y/90mY, E = 0.14-1.22, 14.8 MeV; measured σ(E). Natural target. RADIOACTIVITY 90mY [from 89Y(n, γ)]; measured T1/2.
doi: 10.1016/0375-9474(67)90816-0
1966FO11 Phys.Rev. 152, 980 (1966) D.B.Fossan, R.A.Chalmers, S.R.Salisbury, F.J.Vaughn Study of N16 by N15 + n Total-Cross-Section Measurement NUCLEAR STRUCTURE 16N, 15N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.152.980
1965CH03 Bull.Am.Phys.Soc. 10, No.1, 91, HC1 (1965) L.F.Chase, Jr., H.A.Grench, R.E.McDonald, F.J.Vaughn Decay of N18 NUCLEAR STRUCTURE 18N; measured not abstracted; deduced nuclear properties.
1965HA37 Nucl.Phys. 69, 37 (1965) K.K.Harris, H.A.Grench, R.G.Johnson, F.J.Vaughn, R.Sher The Au197(n, γ)Au198 cross section from 1 keV to 683 keV NUCLEAR REACTIONS 197Au(n, γ), E=13.1-691.2 keV; measured products , Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 12197.
doi: 10.1016/0029-5582(65)90500-6
1965HA39 Nucl.Instrum.Methods 33, 257 (1965) K.K.Harris, H.A.Grench, R.G.Johnson, F.J.Vaughn The V51(p, n)Cr51 reaction as a neutron source of known intensity NUCLEAR REACTIONS 51V(p, n), E=1.5-2.2 MeV; measured products, 51Cr, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry T0030.
doi: 10.1016/0029-554X(65)90050-9
1965SA24 Nucl.Phys. 64, 343 (1965) S.R.Salisbury, D.B.Fossan, F.J.Vaughn The Total Neutron Cross Section Of O18 From 2.45 To 19.0 Mev NUCLEAR REACTIONS 18O(n, x), E=2.4-19 MeV; measured products; deduced σ, σ(E), resonance parameters. Data were imported from EXFOR entry 11382.
doi: 10.1016/0029-5582(65)90362-7
1965VA03 Nucl.Phys. 64, 336(1965) F.J.Vaughn, H.A.Grench, W.L.Imhof, J.H.Rowland, M.Walt The Total Neutron Cross Section of O18 from 0.14 to 2.47 MeV NUCLEAR REACTIONS 18O(n, X), E=0.14-2.47 MeV; measured σ(E). 19O deduced levels, J, π, level-width. Enriched target.
doi: 10.1016/0029-5582(65)90361-5
1965VA06 Phys.Rev.Letters 15, 555 (1965) F.J.Vaughn, R.A.Chalmers, L.F.Chase, Jr., S.R.Salisbury New Isotope of Fluorine: F22 NUCLEAR STRUCTURE 22F; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.15.555
1964CH19 Phys. Rev. Letters 13, 665 (1964) L.F.Chase, Jr., H.A.Grench, R.E.McDonald, F.J.Vaughn New Isotope of Nitrogen: N18 NUCLEAR STRUCTURE 18N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.13.665
1964IM03 Nucl.Phys. 59, 81 (1964) W.L.Imhof, F.J.Vaughn, L.F.Chase, Jr., H.A.Grench, M.Walt A Search for H4 and Li4 RADIOACTIVITY 4H, 4Li; measured no β(16-21 MeV). NUCLEAR REACTIONS 3He(n, γ), En=thermal, 0.03-1.20 keV; 3H(d, p), Ed=2.5 MeV; 3He(p, γ), Ep=0.5-2.6 MeV; 3He(d, n), Ed=0.5-2.3 MeV; measured no β; deduced σ limits. 3He(p, γ) measured no γ; deduced σ limit for -0.6 < Q < +4.0 MeV.
doi: 10.1016/0029-5582(64)90114-2
1964SA07 WASH-1046, p.72 (1964) S.R.Salisbury, D.B.Fossan, F.J.Vaughn Fast-Neutron Total Cross Section of O18 NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.
1964VA02 Bull.Am.Phys.Soc. 9, No.1, 20, BC10 (1964); Oral Report F.J.Vaughn, L.F.Chase, Jr., H.A.Grench, J.W.Hilson O18(n, γ)O19 Cross Section from 0.2 to 1.0 MeV NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11445. 1962CH14 Phys.Rev. 127, 859 (1962) L.F.Chase, Jr., R.G.Johnson, F.J.Vaughn, E.K.Warburton Endothermic Deuteron Stripping Reactions. III. The C14(d, pγ)C15 and Li7(d, pγ)Li8 Reactions NUCLEAR STRUCTURE 7Li, 14C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.127.859
1962GR03 Bull.Am.Phys.Soc. 7, No.4, 268, CB1 (1962) H.A.Grench, W.L.Imhof, F.J.Vaughn Search for H4 and Li4 NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
1962HA30 Bull.Am.Phys.Soc. 7, No.8, 553, U11 (1962) K.K.Harris, J.H.Ferziger, R.Sher, H.A.Grench, R.G.Johnson, F.J.Vaughn Neutron-Capture Cross Sections for Au197 from 10-600 keV NUCLEAR STRUCTURE 198Au; measured not abstracted; deduced nuclear properties.
1962IM01 Phys.Rev. 125, 1334 (1962) W.L.Imhof, R.G.Johnson, F.J.Vaughn, M.Walt Cross Sections for the B11(n, γ)B12 Reaction NUCLEAR STRUCTURE 112Ag, 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.125.1334
1962JO10 Bull.Am.Phys.Soc. 7, No.8, 552, U10 (1962) R.G.Johnson, H.A.Grench, F.J.Vaughn, K.K.Harris V51(p, n)Cr51 Reaction as an Absolute Neutron Source NUCLEAR STRUCTURE 51Cr; measured not abstracted; deduced nuclear properties.
1961CH01 Bull.Am.Phys.Soc. 6, No.1, 25, I8 (1961) L.F.Chase, Jr., R.G.Johnson, F.J.Vaughn, E.K.Warburton Angular Distributions of the 0.75-MeV γ Ray from C14(d, pγ)C15 Reaction and the 0.98-MeV γ Ray from the Li7(d, pγ)Li8 NUCLEAR STRUCTURE 15C, 8Li; measured not abstracted; deduced nuclear properties.
1961GR20 Bull.Am.Phys.Soc. 6, No.5, 430, J8 (1961) H.A.Grench, W.L.Imhof, F.J.Vaughn Fast-Neutron-Capture Cross Section of Ni64 NUCLEAR STRUCTURE 64Ni; measured not abstracted; deduced nuclear properties.
1961JO07 Bull.Am.Phys.Soc. 6, No.3, 236, DA8 (1961) R.G.Johnson, L.F.Chase, Jr., F.J.Vaughn The C13(He3, n)O15 Reaction NUCLEAR STRUCTURE 15O; measured not abstracted; deduced nuclear properties.
1961JO24 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.591 (1961) R.G.Johnson, L.F.Chase, Jr., F.J.Vaughn An Investigation of the C13(He3, n0)O15 and the C14(He3, n0)O16 Reactions NUCLEAR STRUCTURE 13C, 14C; measured not abstracted; deduced nuclear properties.
1961VA33 Bull.Am.Phys.Soc. 6, No.4, 374, X1 (1961) F.J.Vaughn, H.A.Grench, W.L.Imhof, J.H.Rowland, M.Walt Total Neutron Cross Section of O18 NUCLEAR STRUCTURE 19O; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11370. 1960IM01 Bull.Am.Phys.Soc. 5, No.4, 245, HA2 (1960) W.L.Imhof, R.G.Johnson, F.J.Vaughn, M.Walt Neutron Yield from the C13(p, n)N13 Reaction NUCLEAR STRUCTURE 12B; measured not abstracted; deduced nuclear properties.
1960VA04 Phys.Rev. 118, 683 (1960) F.J.Vaughn, W.L.Imhof, R.G.Johnson, M.Walt Total Neutron Cross Sections of Helium, Neon, Argon, Krypton, and Xenon NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.118.683
1960VA11 Bull.Am.Phys.Soc. 5, No.6, 404, B2 (1960) F.J.Vaughn, L.F.Chase, Jr., R.G.Johnson Cross Sections and Angular Distributions of Neutrons from C13(d, n)N14 (Ground State, 2.31-, 3.95-, 4.91-, and 5.10-MeV Levels of N14) NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1959IM04 Phys.Rev. 114, 1037 (1959) W.L.Imhof, R.G.Johnson, F.J.Vaughn, M.Walt Cross Sections for the Li7(n, γ)Li8 Reaction
doi: 10.1103/PhysRev.114.1037
1959JO22 Bull.Am.Phys.Soc. 4, No.6, 373, T9 (1959) R.G.Johnson, W.L.Imhof, F.J.Vaughn Cross Sections for the B11(n, γ)B12 Reaction
1958VA07 Bull.Am.Phys.Soc. 3, No.3, 165, B7 (1958) F.J.Vaughn, W.I.Imhof, R.G.Johnson, M.Walt Total Neutron Cross Sections of Neon, Argon, Krypton, and Xenon
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