NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = H.D.Knox Found 21 matches. 2006LE35 Nucl.Sci.Eng. 154, 261 (2006) G.Leinweber, D.P.Barry, M.J.Trbovich, J.A.Burke, N.J.Drindak, H.D.Knox, R.V.Ballad, R.C.Block, Y.Danon, L.I.Severnyak Neutron Capture and Total Cross-Section Measurements and Resonance Parameters of Gadolinium NUCLEAR REACTIONS 155,157Gd(n, X), (n, γ), E ≈ 0-300 eV; measured transmission and capture σ; deduced resonance parameters. Comparison with previous results.
doi: 10.13182/NSE05-64
2002LE26 Nucl.Sci.Eng. 142, 1 (2002) G.Leinweber, J.A.Burke, H.D.Knox, N.J.Drindak, D.W.Mesh, W.T.Haines, R.V.Ballad, R.C.Block, R.E.Slovacek, C.J.Werner, M.J.Trbovich, D.P.Barry, T.Sato Neutron Capture and Transmission Measurements and Resonance Parameter Analysis of Samarium NUCLEAR REACTIONS Sm(n, X), (n, γ), E ≈ 0-30 eV; measured transmission and capture σ. 144,147,148,149,150,152,154Sm deduced resonance parameters, resonance integral. 144,147,148,149,150,151,152,154Sm(n, γ), E=thermal; deduced capture σ. Comparison with previous results.
doi: 10.13182/NSE02-A2283
2000LE01 Nucl.Sci.Eng. 134, 50 (2000) G.Leinweber, J.Burke, C.R.Lubitz, H.D.Knox, N.J.Drindak, R.C.Block, R.E.Slovacek, C.J.Werner, N.C.Francis, Y.Danon, B.E.Moretti Neutron Capture and Total Cross-Section Measurements and Resonance Parameter Analysis of Zirconium up to 2.5 keV NUCLEAR REACTIONS Zr(n, X), (n, γ), E < 2.5 keV; measured capture and transmission σ. 91,96Zr deduced resonance parameters.
doi: 10.13182/NSE00-A2099
1990SA24 Phys.Rev. C42, 190 (1990) E.T.Sadowski, H.D.Knox, D.A.Resler, R.O.Lane Higher Excitation Levels of 11B via the 10B(n, n) and 10B(n, n')10B(*) (0.72, 1.74, 2.15, 3.59, 4.77 MeV) Reactions NUCLEAR REACTIONS 10B(n, n), (n, n'), E=3-12 MeV; measured σ(θ, E). 11B deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1103/PhysRevC.42.190
1989RE01 Phys.Rev. C39, 766 (1989) D.A.Resler, H.D.Knox, P.E.Koehler, R.O.Lane, G.F.Auchampaugh Structure of 14C via Elastic and Inelastic Neutron Scattering from 13C: Measurement and R-matrix analysis NUCLEAR REACTIONS 13C(n, n), (n, n'), E=4.5-11 MeV; measured σ(θ); deduced 13C(n, α)10Be σ. 14C deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1103/PhysRevC.39.766
1987KN04 Nucl.Phys. A466, 245 (1987) H.D.Knox, D.A.Resler, R.O.Lane Reactions leading to the 7Li and 8Li Systems: Shell model and R-matrix calculations NUCLEAR REACTIONS 6,7Li(n, n), E < 8 MeV; 3H(α, α), E < 21 MeV; calculated σ(θ) vs E. 7,8Li deduced levels, J, π, reduced widths. Shell model. NUCLEAR STRUCTURE 7,8Li; calculated levels, reduced width amplitudes. Shell model.
doi: 10.1016/0375-9474(87)90441-6
1987RE01 Phys.Rev. C35, 855 (1987) D.A.Resler, R.O.Lane, H.D.Knox Selective Sequential 2n Decay of 14C(*) States Populated by 13C + n NUCLEAR REACTIONS 13C(n, n), (n, n'), E=4.55-10.99 MeV; measured σ(θn, En); 13C(n, 2n), E=8.24 MeV; measured σ; deduced 2n sequential decay mechanism. 13,14C deduced levels, decay characteristics. Tof.
doi: 10.1103/PhysRevC.35.855
1986KN08 Radiat.Eff. 95, 1 (1986) Use of Shell Model Calculations in R-Matrix Studies of Neutron-Induced Reactions NUCLEAR REACTIONS 6,7Li(n, n), (n, n'), (n, t), 6Li(n, p), (n, d), E ≤ 8 MeV; calculated σ(E, θ). R-matrix calculations. NUCLEAR STRUCTURE 7,8Li; calculated level structure. Shell model.
doi: 10.1080/00337578608208665
1986KO10 Nucl.Phys. A453, 429 (1986) P.E.Koehler, H.D.Knox, D.A.Resler, R.O.Lane, G.F.Auchampaugh Structure of 19O from Measurement and R-Matrix Analysis of σ(θ) for 18O(n, n)18O and 18O(n, n')18O*(1.98 MeV) NUCLEAR REACTIONS 18O(n, n), (n, n'), E=5-7.5 MeV; measured σ(θ). 19O deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1016/0375-9474(86)90446-X
1983KN06 Nucl.Phys. A403, 205 (1983) Structure of 7Li and Mechanisms of the Low Energy 6Li + n Reactions NUCLEAR REACTIONS 6Li(n, n), (n, t), E=thermal-4 MeV; analyzed data; deduced reaction mechanisms. 7Li deduced levels, J, π, reduced width. R-matrix analysis.
doi: 10.1016/0375-9474(83)90225-7
1983KO03 Nucl.Phys. A394, 221 (1983) P.E.Koehler, H.D.Knox, D.A.Resler, R.O.Lane, D.J.Millener Structure of 12B from Measurement and R-Matrix Analysis of σ(θ) for 11B(n, n)11B and 11B(n, n')11B*(2.12 MeV), and Shell-Model Calculations NUCLEAR STRUCTURE 12B; calculated levels, spectroscopic amplitudes. Shell model. NUCLEAR REACTIONS 11B(n, n), (n, n'), E=4.8-7.6 MeV; measured σ(θ). 12B deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1016/0375-9474(83)90170-7
1982KN02 Nucl.Phys. A378, 503 (1982) Structure of 13C from an R-Matrix Analysis of 12C+n Scattering and Reaction Cross Sections NUCLEAR REACTIONS 12C(n, n), (n, n'), (n, α), E=0.0-9 MeV; analyzed data . 13C deduced levels, J, π, reduced widths. R-matrix analysis, comparison to model predictions.
doi: 10.1016/0375-9474(82)90462-6
1981KN03 Nucl.Phys. A359, 131 (1981) States in 8Li from an R-Matrix Analysis of 7Li(n, n)7Li and 7Li(n, n')7Li*(0.478, 4.63) Measurements NUCLEAR REACTIONS 7Li(n, n), (n, n'), E < 8 MeV; analyzed data. 8Li deduced levels, J, reduced widths, π. R-matrix analysis.
doi: 10.1016/0375-9474(81)90216-5
1981LA05 Phys.Rev. C23, 1883 (1981) R.O.Lane, H.D.Knox, P.Hoffmann-Pinther, R.M.White, G.F.Auchampaugh States in 14C from σ(total) and σ(elastic)(θ) for 13C + n: Measurement, R-matrix analysis, and model calculations NUCLEAR STRUCTURE 14C; calculated levels. Weak coupling model, effective interactions. NUCLEAR REACTIONS 13C(n, n), E=1.25-6.5 MeV; measured σ(θ). 14C deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1103/PhysRevC.23.1883
1980WH01 Nucl.Phys. A340, 13 (1980) R.M.White, R.O.Lane, H.D.Knox, J.M.Cox States in 12B from Measurement and R-Matrix Analysis of σ(θ) for 11B(n, n)11B NUCLEAR REACTIONS 11B(n, n), E=2.6-8 MeV; measured σ(θ). 12B deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1016/0375-9474(80)90320-6
1979KN01 Nucl.Sci.Eng. 69, 223 (1979) Differential Neutron Scattering Cross Sections of Lithium-6 and Lithium-7 for Neutrons of 4 to 7.5 MeV Energy NUCLEAR REACTIONS 6,7Li(n, n), E=4-7.5 MeV; measured σ(θ); deduced disagreement between observed, evaluated σ for 7Li.
doi: 10.13182/NSE79-A20612
1978KN01 Nucl.Sci.Eng. 65, 65 (1978) Differential Elastic Scattering Cross Sections of Boron-10 for Neutrons of 4 to 8 MeV Energy NUCLEAR REACTIONS 10B(n, n), E=4-8 MeV; measured σ(E, θ).
doi: 10.13182/NSE78-A27126
1975GR24 Phys.Rev.Lett. 35, 917 (1975) R.G.Graves, M.Jain, H.D.Knox, E.P.Chamberlin, L.C.Northcliffe Measurement of the 2H(p, n)pp Transverse Polarization Transfer Coefficient at 20.4 MeV NUCLEAR REACTIONS 2H(polarized p, n), E=20.4 MeV; measured transverse polarization transfer coefficient.
doi: 10.1103/PhysRevLett.35.917
1975KN02 Phys.Lett. 56B, 33 (1975) H.D.Knox, R.G.Graves, F.N.Rad, M.L.Evans, L.C.Northcliffe, H.Nakamura, H.Noya Comparison of a D(α, n)αp Measurement with a Modified Impulse Approximation Prediction NUCLEAR REACTIONS 2H(polarized α, n), E=42.3 MeV; measured neutron polarization; calculated σ.
doi: 10.1016/0370-2693(75)90492-X
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
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