NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.C.Davis Found 23 matches. 1993HE25 At.Data Nucl.Data Tables 54, 181 (1993) B.L.Henke, E.M.Gullikson, J.C.Davis X-Ray Interactions: Photoabsorption, Scattering, Transmission, and Reflection at E = 50-30, 000 eV, Z = 1-92 COMPILATION Z=1-92; compiled theoretical σ of the primary interactions of low-energy x-rays within condensed matter, viz. photoabsorption and coherent scattering within 50 eV to 30 KeV range.
doi: 10.1006/adnd.1993.1013
1986BR03 Phys.Rev. C33, 1235 (1986) V.R.Brown, C.Wong, C.H.Poppe, J.D.Anderson, J.C.Davis, S.M.Grimes, V.A.Madsen Cross Sections for the Ti(p, n) Reaction to Analogs of Ground and 2+ Excited States NUCLEAR REACTIONS, ICPND 46,47,48,49,50Ti(p, n), E=11.5-26 MeV; measured σ(En), σ(θ); deduced σ, β(n)/β(p). 46,48,50Ti levels deduced β.
doi: 10.1103/PhysRevC.33.1235
1985GR09 Phys.Rev. C31, 1679 (1985) S.M.Grimes, J.D.Anderson, J.C.Davis, R.H.Howell, C.Wong, A.W.Carpenter, J.A.Carr, F.Petrovich Gamow-Teller Matrix Elements from the 11B(p, n)11C Reaction at E(p) ≈ 26 MeV NUCLEAR REACTIONS, ICPND 11B(p, n), E=16-26 MeV; measured σ(En), σ(θ); deduced residual producation σ. 11C levels deduced Gamow-Teller matrix elements. DWA analysis, Cohen-Kurath wave functions, G-matrix based interactions.
doi: 10.1103/PhysRevC.31.1679
1976MA07 Phys.Rev. C13, 548 (1976) V.A.Madsen, V.R.Brown, S.M.Grimes, C.H.Poppe, J.D.Anderson, J.C.Davis, C.Wong Effect of Inelastic Coupling on 0+ Analog Transitions NUCLEAR REACTIONS 92,98,100Mo(p, n), E=18, 22, 26 MeV; measured σ(θ). 92,98,100Mo(p, n), E=16, 26 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.13.548
1976PO06 Phys.Rev. C14, 438 (1976) C.H.Poppe, J.D.Anderson, J.C.Davis, S.M.Grimes, C.Wong Cross Sections for the 7Li(p, n)7Be Reaction between 4.2 and 26 MeV NUCLEAR REACTIONS 7Li(p, n), E=4.2-26 MeV; measured σ(E, θ) to 7Be ground state, first excited state; θ=3.5°-159°.
doi: 10.1103/PhysRevC.14.438
1975GR01 Phys.Rev. C11, 158 (1975) S.M.Grimes, C.H.Poppe, J.D.Anderson, J.C.Davis, W.H.Dunlop, C.Wong Energy Dependence of the (p, n) Analog Cross Sections of the Molybdenum Isotopes between 16 and 26 MeV NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, n), E=16, 18, 20, 22, 24, 26 MeV; measured σ(E, En, θ).
doi: 10.1103/PhysRevC.11.158
1975WO01 Phys.Rev. C11, 137 (1975) C.Wong, V.R.Brown, J.D.Anderson, J.C.Davis, S.M.Grimes, C.H.Poppe, V.A.Madsen Population of Analogs of Excited States in 63Cu(p, n) at 16, 19, and 22 MeV NUCLEAR REACTIONS 63Cu(p, n), E=16, 19, 22 MeV; 64Zn(p, n), E=22 MeV; measured σ(En, θ). 63Zn deduced analog states.
doi: 10.1103/PhysRevC.11.137
1975WO11 Phys.Rev. C12, 2115 (1975) C.Wong, J.D.Anderson, V.R.Brown, J.C.Davis, S.M.Grimes, V.A.Madsen, C.H.Poppe Excited Analogs in 62Ni and 63Cu(p, n) and the Weak-Coupling Model NUCLEAR REACTIONS 62Ni(p, n), E=16, 19, 22 MeV; measured σ(θ) ground-state, excited-state analog; calculated σ(θ) using weak-coupling model.
doi: 10.1103/PhysRevC.12.2115
1974AN10 Yad.Fiz. 19, 943 (1974); Sov.J.Nucl.Phys. 19, 483 (1975) J.D.Anderson, H.H.Barschall, J.C.Davis Total Cross Section of 207Pb for Neutrons Near 17 MeV NUCLEAR REACTIONS 207Pb(n, X), E=16.8 MeV; measured σ. 208Pb deduced absence of previously reported resonance.
1974HA42 Phys.Rev. C10, 1111 (1974) L.F.Hansen, J.C.Davis, F.S.Dietrich, M.C.Gregory, R.P.Koopman Levels of 64Ga via the 64Zn(p, n) and 64Zn(p, nγ) Reactions NUCLEAR REACTIONS 64Zn(p, n), E=10, 10.5 MeV; measured σ(En, θ). 64Zn(p, nγ), E=8.0-10.5 MeV; measured σ(E, Eγ), γ(t); deduced Q. 64Ga deduced levels, T1/2, J, π.
doi: 10.1103/PhysRevC.10.1111
1974PO11 Phys.Rev.Lett. 33, 856 (1974) C.H.Poppe, S.M.Grimes, J.D.Anderson, J.C.Davis, W.H.Dunlop, C.Wong Anomalous Behavior of the (p, n) Analog Reaction on the Molybdenum Isotopes NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, n), E=16-26 MeV; measured σ(E, θ). 92,94,95,96,97,98,100Tc analog state deduced cross section ratios.
doi: 10.1103/PhysRevLett.33.856
1973DA21 Phys.Rev. C8, 863 (1973) J.C.Davis, J.D.Anderson, S.M.Grimes, C.Wong Proton-Proton Final-State Interaction in the 2H(p, n)2p Reaction NUCLEAR REACTIONS 2H(p, n), E=16-26 MeV; measured σ(E;En). Deduced p-p scattering length.
doi: 10.1103/PhysRevC.8.863
1973GR13 Phys.Rev.Lett. 30, 992 (1973) S.M.Grimes, J.D.Anderson, J.C.Davis, W.H.Dunlop, C.Wong Cross-Section Measurements for the (p, n) Analog Transition in 181Ta, 197Au, and 209Bi NUCLEAR REACTIONS 181Ta, 197Au, 209Bi(p, n), E=25, 27 MeV; 181W, 197Hg, 209Po IAR measured σ(θ); 209Po IAR deduced level-width.
doi: 10.1103/PhysRevLett.30.992
1973GR32 Phys.Rev. C8, 1770 (1973) S.M.Grimes, J.D.Anderson, J.C.Davis, C.Wong Nonequilibrium Contributions to the 51V(p, n)51Cr Reaction for 18 < E < 26 MeV NUCLEAR REACTIONS 51V(p, n), Ep=18, 20, 22, 24, 26 MeV; measured σ(En, θ), θ=24-144°.
doi: 10.1103/PhysRevC.8.1770
1973WE19 Nucl.Sci.Eng. 52, 35 (1973) K.A.Weaver, J.D.Anderson, H.H.Barschall, J.C.Davis Neutron Spectra from Deuteron Bombardment of D, Li, Be, and C NUCLEAR REACTIONS 2H, Li, Be, C(d, xn), E < 20 MeV; measured σ(E;En).
doi: 10.13182/NSE73-A23287
1973WO05 Phys.Rev. C7, 1895 (1973) C.Wong, J.D.Anderson, J.C.Davis, S.M.Grimes Energy Dependence of the 51V(p, n)51Cr Analog Transition between 16 and 26 MeV NUCLEAR REACTIONS 51V(p, n), E=16-26 MeV; measured σ(E;En, θ) for 51Cr analog state.
doi: 10.1103/PhysRevC.7.1895
1972QU02 Nucl.Phys. A183, 173 (1972) P.A.Quin, J.C.Davis, D.Hilscher The 89Y(d, n0)90Zr Reaction and Coulomb Effects in Stripping Reactions NUCLEAR REACTIONS 89Y(d, n0), Ed=11.0 MeV; measured polarization parameter iT11(θ). Natural target.
doi: 10.1016/0375-9474(72)90937-2
1971DA07 Phys.Rev. C3, 1798 (1971) Fast-Neutron Total Cross Section of Deuterium NUCLEAR REACTIONS 2H(n, X), E=1.5-27.5 MeV; measured σ(nT)(E).
doi: 10.1103/PhysRevC.3.1798
1971DA24 Phys.Rev. C4, 1061 (1971) J.C.Davis, K.A.Weaver, D.Hilscher, H.H.Barschall, A.B.Smith Total Cross Section of Protons for 2.5-MeV Neutrons NUCLEAR REACTIONS 1H(n, X), E=2.5 MeV measured σ(nT).
doi: 10.1103/PhysRevC.4.1061
1971HI07 Nucl.Phys. A173, 216 (1971) D.Hilscher, P.A.Quin, J.C.Davis Comparison of the Vector Analysing Powers of the Mirror Reactions 3H(polarized d, n)4He and 3He(Polarized d, p)4He NUCLEAR REACTIONS 3H(polarized d, n)4He, 3He(polarized d, p)4He, E=6, 10 MeV; measured vector analyzing power it11(Ed;θ). Enriched targets.
doi: 10.1016/0375-9474(71)90757-3
1971HI09 Nucl.Phys. A174, 417 (1971) D.Hilscher, J.C.Davis, P.A.Quin Vector Analyzing Power of (d, n) Reactions on 11B, 12C, 14N and 15N NUCLEAR REACTIONS 11B, 14N, 15N(d, n), Ed=10.0, 11.8 MeV; 12C(d, n), Ed=8.5 MeV; measured polarization parameter iT11(Ed, θ); relative cross section σ(Ed, θ) for 12C, 14N(d, n). 12C level, 15O ground state deduced J, π.
doi: 10.1016/0375-9474(71)90674-9
1969DA13 Nucl.Phys. A134, 361 (1969) Neutron Energy Determinations NUCLEAR REACTIONS 12C, 16O(n, X), E=3-8 MeV; measured σ(E). 20Ne(n, α), E=3-6 MeV; measured σ(E). 13C, 17O, 21Ne deduced resonances.
doi: 10.1016/0375-9474(69)91059-8
1968DA31 Phys.Lett. B 27, 636 (1968) Adjustments in the n-p singlet effective range NUCLEAR REACTIONS 1H(n, X), 14N(n, p), 20Ne(n, α), 12C, 16O(n, n), E<5 MeV; analyzed available data; deduced σ, single effective ranges.
doi: 10.1016/0370-2693(68)90301-8
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