NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = C.M.Castaneda Found 23 matches. 2007CA24 Nucl.Instrum.Methods Phys.Res. B260, 508 (2007) C.M.Castaneda, D.G.Gearhart, R.M.Gearhart, B.Sanii, P.A.J.Englert, J.F.Dempsey, J.C.Young, D.M.Drake, R.C.Reedy Gamma ray production cross sections from the bombardment of Mg, Al, Si, Ca and Fe with medium energy neutrons NUCLEAR REACTIONS Mg, Al, Si, Ca, Fe(n, γX), E=6.5, 17.4, 22.2, 32.5, 42.1, 64.5 MeV; measured Eγ, Iγ, production cross sections. Compared results to model calculations.
doi: 10.1016/j.nimb.2007.04.019
1996LA36 Trans.Amer.Nucl.Soc. 74, 134 (1996) M.C.Lagunas-Solar, N.X.Zeng, I.Mirshad, C.M.Castaneda Cyclotron Production of Molybdenum-99 via Proton-Induced Uranium-238 Fission NUCLEAR REACTIONS 238U(p, F)99Mo, E=12.0-67.5 MeV; measured production σ. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0961. 1996WA06 Phys.Rev. C53, 1718 (1996) K.Wang, C.J.Martoff, D.Pocanic, S.S.Hanna, F.P.Brady, J.L.Romero, C.M.Castaneda, J.R.Drummond, B.McEachern, D.S.Sorenson Reaction 13C(n, p)13B at 65 MeV NUCLEAR REACTIONS 13C(n, p), E=65 MeV; measured spectra, σ(θ); deduced v(c)(στ). 13B levels deduced spin-dipole transition role, possible analog resonance.
doi: 10.1103/PhysRevC.53.1718
1995RE25 Nucl.Instrum.Methods Phys.Res. A361, 574 (1995) P.S.Rezentes, J.L.Romero, C.M.Castaneda Correction of Particle and Energy Losses in a Thick Target for Charged Particle Spectra NUCLEAR REACTIONS 12C(n, αX), E=39.7 MeV; analyzed σ(θα, Eα). 28Si(n, αX), E=32.2, 50 MeV; analyzed α-spectra. Particle, energy loss corrections included. RADIOACTIVITY 234U(α); analyzed α-spectra. Particle, energy loss corrections included.
doi: 10.1016/0168-9002(95)00146-8
1991BR10 Phys.Rev. C43, 2284 (1991) F.P.Brady, T.D.Ford, G.A.Needham, J.L.Romero, D.S.Sorenson, C.M.Castaneda, J.L.Drummond, E.L.Hjort, B.McEachern, N.S.P.King, D.J.Millener 12C(n, p)12B Reaction at 56, 60, and 65 MeV NUCLEAR REACTIONS 12C(n, p), E=56, 60, 65 MeV; measured σ(E, θ). 12C(p, p), E=65 MeV; 12C(n, p), E=62, 65 MeV; calculated σ(θ). Microscopic DWBA, shell model analyses. NUCLEAR STRUCTURE 12C, 12B; calculated levels, wave functions, one-body density-matrix elements. Shell model.
doi: 10.1103/PhysRevC.43.2284
1989BR17 Phys.Rev. C40, R475 (1989) F.P.Brady, T.D.Ford, J.L.Romero, C.M.Castaneda, J.R.Drummond, E.L.Hjort, N.S.P.King, B.McEachern, D.S.Sorenson, Z.Aung, A.Klein, W.G.Love, J.K.Wambach Gamow-Teller and Spin-Dipole Strength in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(θp, Ep). 90Y deduced Gamow-Teller, spin dipole transition strength.
doi: 10.1103/PhysRevC.40.R475
1989FO04 Nucl.Instrum.Methods Phys.Res. A274, 253 (1989) T.D.Ford, F.P.Brady, C.M.Castaneda, J.R.Drummond, B.McEachern, J.L.Romero, D.S.Sorenson A Large Dynamic Range Detector for Measurement of Neutron-Induced Charged Particle Spectra Down to Zero Degrees NUCLEAR REACTIONS 12C(n, p), E=60, 65 MeV; measured σ(θ) on Gamow-Teller, GDR resonances. Large dynamic range detector.
doi: 10.1016/0168-9002(89)90388-4
1987FO10 Phys.Lett. 195B, 311 (1987) T.D.Ford, J.L.Romero, F.P.Brady, C.M.Castaneda, J.R.Drummond, B.McEachern, D.S.Sorenson, Zin Aung, N.S.P.King, A.Klein, W.G.Love Excitation of Isovector Monopole and Quadrupole Giant Resonances in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(E(p), θ(p)), σ(θ(p)). 90Y deduced isovector monopole, quadrupole giant resonances. RPA-DWA analyses.
doi: 10.1016/0370-2693(87)90023-2
1986DR08 Radiat.Eff. 94, 285 (1986) J.R.Drummond, F.P.Brady, J.L.Romero, T.D.Ford, C.M.Castaneda, B.McEachern, M.A.Hamilton A Measurement of the N-P 180/90 Degree Cross Section Ratio at 65 and 50 MeV NUCLEAR REACTIONS 1H(n, n), E=50, 65 MeV; measured σ(θ=180°)/σ(θ=90°). Position sensitive wire chamber, CH2 target.
doi: 10.1080/00337578608208393
1986FO10 Radiat.Eff. 96, 77 (1986) T.D.Ford, F.P.Brady, C.M.Castaneda, J.L.Romero, J.R.Drummond, B.McEachern Development of a Facility for (n, px) Measurements Down to Zero Degrees at 65 MeV Incident Energy NUCLEAR REACTIONS 12C(n, p), E=65 MeV; measured σ(Ep). Zero degree facility.
doi: 10.1080/00337578608211718
1986HA19 Radiat.Eff. 94, 235 (1986) M.A.Hamilton, T.D.Ford, F.P.Brady, J.L.Romero, C.M.Castaneda, J.R.Drummond Fe(nat)(n, n'x) Spectra at 65.5 MeV NUCLEAR REACTIONS Fe(n, n'X), E=65.5 MeV; measured continuum spectra, σ(E); deduced GDR, neutron to proton matrix element ratio.
doi: 10.1080/00337578608208382
1986ZA01 Phys.Rev. C33, 66 (1986) C.I.Zanelli, F.P.Brady, J.L.Romero, C.M.Castaneda, D.L.Johnson Neutron Total Cross Section in Ca and Fe at 35.3, 40.3, and 50.4 MeV NUCLEAR REACTIONS Ca, Fe(n, n), E=35.3, 40.3, 50.4 MeV; 12C(n, n), E=50.4 MeV; measured σ.
doi: 10.1103/PhysRevC.33.66
1984BR03 J.Phys.(London) G10, 363 (1984) F.P.Brady, G.A.Needham, J.L.Ullmann, C.M.Castaneda, T.D.Ford, N.S.P.King, J.L.Romero, M.L.Webb, V.R.Brown, C.H.Poppe Excitation of Analogue Isovector Resonances via the (n, p) Reaction at 60 MeV NUCLEAR REACTIONS 6,7Li, 12C, 16O, 28Si, 58,60,62,64Ni, 209Bi(n, p), E=60 MeV; measured σ(θ); deduced effective nucleon-nucleon interaction isovector spin-dependent component, analog isovector resonance excitation mechanism. 28Al deduced Gamow-Teller type transition. 7He deduced L=1 dipole strength contribution. 6He, 12B deduced L=1 strength spin character, Gamow-Teller type transition. 16N deduced L=1 strength spin character.
doi: 10.1088/0305-4616/10/3/011
1984BR32 Nucl.Instrum.Methods 228, 89 (1984) F.P.Brady, T.D.Ford, G.A.Needham, J.L.Romero, C.M.Castaneda, M.L.Webb A Multiwire Chamber System for Measurements of Neutron Spectra NUCLEAR REACTIONS 7Li(p, n), E=62 MeV; measured σ(Ep, θn=0°); 40Ca(n, xn), E=65.5 MeV; measured σ(θ=9°, En). Multi-wire chamber system.
doi: 10.1016/0168-9002(84)90014-7
1984FO23 Nucl.Instrum.Methods 228, 81 (1984) T.D.Ford, G.A.Needham, F.P.Brady, J.L.Romero, C.M.Castaneda A Multiwire Chamber System for Measurments of Charged Particle Spectra NUCLEAR REACTIONS 12C(n, p), E=60 MeV; measured σ(Ep) vs θ. Multi-wire chamber system.
doi: 10.1016/0168-9002(84)90013-5
1984UL01 Nucl.Phys. A427, 493 (1984) J.L.Ullmann, F.P.Brady, C.M.Castaneda, D.H.Fitzgerald, G.A.Needham, J.L.Romero, N.S.P.King Analog Giant Dipole Ni(n, p) at 59.6 MeV NUCLEAR REACTIONS 58,60,62,64Ni(n, p), E=59.6 MeV; measured σ(θ). 58,60,62,64Co deduced GDR analog, sum rule, blocking. Enriched targets.
doi: 10.1016/0375-9474(84)90227-6
1983BR32 Phys.Rev.Lett. 51, 1320 (1983) F.Brady, G.A.Needham, J.L.Romero, C.M.Castaneda, T.D.Ford, J.L.Ullmann, M.L.Webb New Giant Dipole Strength in 6Li and 7Li as Revealed via (n, p) at 60 MeV
doi: 10.1103/PhysRevLett.51.1320
1983CA19 Phys.Rev. C28, 1493 (1983) C.M.Castaneda, J.L.Ullmann, F.P.Brady, J.L.Romero, N.S.P.King, M.Blann Precompound Analyses of 58-64Ni(n, px) Reactions NUCLEAR REACTIONS 58,60,62,64Ni(n, pX), E=60 MeV; measured σ(θp), σ vs nucleon kinetic energy; deduced neutron number dependence, best fit model. Hybrid, geometry dependent hybrid models, neutron skin effect.
doi: 10.1103/PhysRevC.28.1493
1982BR04 Phys.Rev.Lett. 48, 860 (1982) F.P.Brady, C.M.Castaneda, G.A.Needham, J.L.Ullmann, J.L.Romero, T.Ford, M.L.Johnson, N.S.P.King, C.M.Morris, F.Petrovich, R.H.Howell Isovector and Gamow-Teller Strength from Small-Angle (n, p) Reactions at 60 MeV NUCLEAR REACTIONS 6Li, 12C, 28Si(n, p), E=60 MeV; measured σ(Ep), σ(θ); deduced effective isovector spin-flip nucleon-nucleon interaction. 6He, 12B, 28Al level deduced Gamow-Teller transition strength.
doi: 10.1103/PhysRevLett.48.860
1982UL01 Nucl.Phys. A386, 179 (1982) J.L.Ullmann, F.P.Brady, D.H.Fitzgerald, G.A.Needham, J.L.Romero, C.M.Castaneda, N.S.P.King Analog Giant Dipole Excitation in Si(n, p) at 59.6 MeV NUCLEAR REACTIONS 28Si(n, p), E=59.6 MeV; measured σ(θ). 28Al deduced parent analog giant dipole resonance strength. Natural target.
doi: 10.1016/0375-9474(82)90407-9
1980CA03 Phys.Rev. C21, 179 (1980) C.M.Castaneda, H.A.Smith, Jr., P.P.Singh, H.Karwowski Mechanisms of Production of Fast Particles with Z = 1, 2 in 6Li-Induced Reactions Far Above the Coulomb Barrier NUCLEAR REACTIONS 197Au, 56Fe(6Li, X), E=75 MeV; measured σ(fragment, θ), αd-, αp-, dγ-, pγ-coin, αd(θ), αγ(θ), dγ(θ), pγ(θ); deduced reaction mechanism.
doi: 10.1103/PhysRevC.21.179
1978CA15 Phys.Lett. 77B, 371 (1978) C.M.Castaneda, H.A.Smith, Jr., P.P.Singh, J.Jastrzebski, H.Karwowski, A.K.Gaigalas Gamma-Rays from the Transfer of α and d Fragments in 6Li Induced Reactions Far Above the Coulomb Barrier NUCLEAR REACTIONS 197Au(6Li, X), E=75 MeV; measured particle γ-coin; deduced reaction mechanism.
doi: 10.1016/0370-2693(78)90580-4
1977CA22 Phys.Rev. C16, 1437 (1977) C.M.Castaneda, H.A.Smith, Jr., T.E.Ward, T.R.Nees Investigation of 6Li-Induced Reactions from 54 to 99 MeV on Pd Targets NUCLEAR REACTIONS 104,105Pd(6Li, xnypγ), E=54-99 MeV; measured γ-spectra; deduced In, Cd, Ag isotopic yields, α-d breakup. Geometry dependent hybrid model.
doi: 10.1103/PhysRevC.16.1437
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