NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = C.Westerfeldt Found 30 matches. 2011MU10 Phys.Rev. C 83, 064605 (2011) J.M.Mueller, R.J.Charity, R.Shane, L.G.Sobotka, S.J.Waldecker, W.H.Dickhoff, A.S.Crowell, J.H.Esterline, B.Fallin, C.R.Howell, C.Westerfeldt, M.Youngs, B.J.Crowe, III, R.S.Pedroni Asymmetry dependence of nucleon correlations in spherical nuclei extracted from a dispersive-optical-model analysis NUCLEAR REACTIONS 40,48Ca(n, n), E=11.9, 16.9 MeV; measured E(n), I(n), σ, σ(E, θ), time-of-flight spectra. 40Ca(n, n), E=9.9-85.0; 48Ca(n, n), E=7.97-16.9 MeV; 54Ca(n, n), E=5.5-26.0 MeV; 58,60Ni(n, n), E=4.5-24.0 MeV; 92Mo(n, n), E=7.0-30.4 MeV; 116,118Sn(n, n), E=9.95-24.0 MeV; 120Sn(n, n), E=9.94-16.91 MeV; 124Sn(n, n), E=11.0-24.0 MeV; 208Pb(n, n), E=4.0-185.0 MeV; 50Ti(p, p), E=6.0-65.0 MeV; 52Cr(p, p), E=10.77-39.9 MeV; 54Fe, 64Ni(p, p), E=9.69-65.0 MeV; 58Ni(p, p), E=7.0-192.0 MeV; 60Ni(p, p), E=7.0-178.0 MeV; 62Ni(p, p), E=8.02-156.0 MeV; 90Zr(p, p), E=5.57-185.0 MeV; 92Mo(p, p), E=12.5-49.45 MeV; 114Sn(p, p), E=30.4 MeV; 116Sn(p, p), E=16.0-61.4 MeV; 118,122,124Sn(p, p), E=16.0-49.35 MeV; 120Sn(p, p), E=9.8-156.0 MeV; 208Pb(p, p), E=9.0-200.0 MeV; analyzed total cross sections, σ(E, θ), single-particle levels, spectroscopic factors, occupation probabilities, mass dependence on cross section. Dispersal optical model (DOM) analysis.
doi: 10.1103/PhysRevC.83.064605
2002RU11 Phys.Rev. C66, 022801 (2002) R.C.Runkle, A.E.Champagne, C.Fox, C.Iliadis, J.Pollanen, A.Stephan, C.Westerfeldt Search for a resonance in the 14N(p, γ) 15O reaction at E p =127 keV NUCLEAR REACTIONS 14N(p, γ), E=135-300 keV; measured Eγ, Iγ; deduced resonance strength upper limit.
doi: 10.1103/PhysRevC.66.022801
1997VA02 Phys.Rev. C55, 1119 (1997) G.A.Vavrina, E.G.Bilpuch, C.R.Bybee, G.E.Mitchell, E.F.Moore, J.D.Shriner, J.F.Shriner, Jr., P.M.Wallace, C.R.Westerfeldt Spectroscopy of the 29Si(p, γ) Reaction for E(p) = 1.00-1.75 MeV NUCLEAR REACTIONS, ICPND 29Si(p, γ), E=1-1.75 MeV; measured Eγ, Iγ, σ(E). 30P deduced levels, J, π, γ strengths, branching ratios. Enriched targets.
doi: 10.1103/PhysRevC.55.1119
1996WA33 Phys.Rev. C54, 2916 (1996) P.M.Wallace, E.G.Bilpuch, C.R.Bybee, G.E.Mitchell, E.F.Moore, J.D.Shriner, J.F.Shriner, Jr., G.A.Vavrina, C.R.Westerfeldt Spectroscopy of the 29Si(p, γ) Reaction for E(p) = 1.75 - 2.51 MeV NUCLEAR REACTIONS 29Si(p, γ), E=1.75-2.51 MeV; measured σ(p, γ), Eγ, Iγ. 30P deduced levels, J, π, T, γ-branching ratios. Enriched targets.
doi: 10.1103/PhysRevC.54.2916
1995SH54 Nucl.Instrum.Methods Phys.Res. B99, 641 (1995) J.F.Shriner, Jr., E.G.Bilpuch, C.R.Bybee, G.E.Mitchell, E.F.Moore, J.D.Shriner, C.R.Westerfeldt A Compton-Suppressed Spectrometer for Studies of Chaos in Nuclei NUCLEAR REACTIONS 29Si(p, γ), E=2.4866 MeV; measured Eγ, Iγ. Compton-suppressed spectrometer.
doi: 10.1016/0168-583X(94)00760-8
1992CO17 Z.Phys. A343, 185 (1992) C.T.Coburn, J.F.Shriner, Jr., C.R.Westerfeldt Entrance Channel Correlations for 2+ Resonances in p + 27Al NUCLEAR REACTIONS 27Al(p, p), (p, α), E ≈ 2.16-2.19 MeV; measured σ(θ) vs E. 28Si deduced resonances, Γp, Γα, reduced width amplitudes, entrance channel correlations role.
doi: 10.1007/BF01291823
1992FR10 Phys.Rev. C45, 2746 (1992) S.C.Frankle, G.E.Mitchell, J.F.Shriner, Jr., E.G.Bilpuch, C.R.Westerfeldt Proton Resonances in 30P NUCLEAR REACTIONS 29Si(p, γ), (p, p'γ), E=2.025-3.310 MeV; 29Si(p, p), (p, p'), E=0.94-3.32 MeV; measured σ(θ) vs E. 30P deduced levels, J, π, γ transition strengths, Γ(p), Γγ.
doi: 10.1103/PhysRevC.45.2746
1991LI14 Phys.Rev. C44, 345 (1991) J.Li, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell, F.Yang Test of Level Densities with Proton Resonances NUCLEAR REACTIONS 48Ti(p, p), (p, p'), E=3.08-3.86 MeV; measured σ(θ) vs E. 49V deduced levels, J, π, level densities, IAS. Multi-channel R-matrix code.
doi: 10.1103/PhysRevC.44.345
1990BU02 Z.Phys. A335, 31 (1990) J.S.Bull, E.G.Bilpuch, G.E.Mitchell, J.F.Shriner, Jr., C.R.Westerfeldt Entrance Channel Correlations for 2+ Resonances in p + 39K NUCLEAR REACTIONS 39K(p, p), (p, α), E ≈ 3.54-3.555 MeV; measured σ(θ) vs E. 40Ca deduced resonances, J, π, reduced widths.
1989VA15 Phys.Rev. C40, 1959 (1989) J.R.Vanhoy, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Proton Resonances in 34Cl from E(x) = 6.3 to 8.8 MeV NUCLEAR REACTIONS 33S(p, p), (p, p'), E=1.2-3.77 MeV; measured σ(θ). 34Cl deduced levels, J, π, T, reduced width, partial wave strength functions.
doi: 10.1103/PhysRevC.40.1959
1988FA01 Phys.Rev. C37, 28 (1988) D.F.Fang, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Proton Resonances in 32S from E(x) = 9.83 to 12.74 MeV NUCLEAR REACTIONS 31P(p, p), (p, p'), (p, α), E=1.00-4.01 MeV; measured σ(θ) vs E; deduced 28Si(α, p0) reaction rates. 32S deduced levels, J, π, analog states, Γp, proton resonance strengths.
doi: 10.1103/PhysRevC.37.28
1988WE19 Nucl.Instrum.Methods Phys.Res. A270, 467 (1988) C.R.Westerfeldt, R.O.Nelson, E.G.Bilpuch, G.E.Mitchell A Microcomputer-Based System for Measuring Excitation Functions with Good Energy Resolution NUCLEAR REACTIONS 27Al(p, γ), E=2.043-2.046 MeV; measured γ yield. 31P(p, p), E=1-4 MeV; measured σ(θ) vs E. Microcomputer based system.
doi: 10.1016/0168-9002(88)90717-6
1987VA24 Phys.Rev. C36, 920 (1987) J.R.Vanhoy, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Proton Resonances in 24Mg from E(x) = 12.7 to 15.7 MeV NUCLEAR REACTIONS 23Na(p, p), (p, p'), (p, α), E=1.08-4.15 MeV; measured σ(E, θ). 24Mg levels deduced J, π, Γp, Γp', Γα0, Γα1, channel spin mixing, L mixing. Enriched target.
doi: 10.1103/PhysRevC.36.920
1986RA11 Z.Phys. A324, 477 (1986) P.Ramakrishnan, G.E.Mitchell, J.F.Shriner, Jr., E.G.Bilpuch, C.R.Westerfeldt Amplitude and Width Correlations for (3/2)+ Resonances in 57Co NUCLEAR REACTIONS 56Fe(p, p'γ), E=3.1-4 MeV; measured pγ(θ). 57Co levels deduced J, π, reduced widths, amplitude, width correlation coefficients. Statistical theory.
1984AD07 J.Phys.(London) G10, 1747 (1984) G.Adams, E.G.Bilpuch, G.E.Mitchell, R.O.Nelson, C.R.Westerfeldt Proton Resonances in 26Al NUCLEAR REACTIONS 25Mg(p, p), (p, p'), E=0.7-2.18 MeV; measured σ(θ) vs E. 26Al levels deduced J, π, Γp, Γp', IAR, channel spin, L-mixings, Coulomb energies, spectroscopic factors. Enriched target.
doi: 10.1088/0305-4616/10/12/013
1984NE03 Phys.Rev. C29, 1656 (1984) R.O.Nelson, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Proton Resonances in 28Si from E(x) = 12.5 to 13.4 MeV NUCLEAR REACTIONS 27Al(p, p), (p, α), E=0.92-1.85 MeV; measured σ(θ) vs E. 28Si deduced level J, π, Γp, Γα, channel spin mixing, L mixing, IAS, Coulomb energies, spectroscopic factors. R-matrix analysis.
doi: 10.1103/PhysRevC.29.1656
1984NE04 Phys.Rev. C30, 755 (1984) R.O.Nelson, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Proton Resonances in 28Si from E(x) = 13.4 to 14.5 MeV NUCLEAR REACTIONS 27Al(p, p), (p, α), E=0.92-1.85 MeV; measured σ(E, θ). 28Si levels deduced J, π, Γp, Γα, channel spin mixing, l-mixing, IAR, Coulomb energies, spectroscopic factors.
doi: 10.1103/PhysRevC.30.755
1984RA20 Z.Phys. A319, 315 (1984) P.Ramakrishnan, G.E.Mitchell, E.G.Bilpuch, J.F.Shriner, Jr., C.R.Westerfeldt Statistical Properties of (5/2)+ Resonances in 57Co NUCLEAR REACTIONS 56Fe(p, p'γ), E=3.1256-4.0016 MeV; measured σ(θp), γ(θ). 57Co resonances deduced inelastic reduced widths, amplitude products, statistical properties.
doi: 10.1007/BF01412545
1984WE10 Nucl.Instrum.Methods 219, 284 (1984) C.R.Westerfeldt, E.G.Bilpuch, M.E.Bleck, D.A.Outlaw, W.K.Wells, J.F.Wilkerson, T.B.Clegg A System for Producing High-Resolution Polarized and Unpolarized Beams with a Tandem Accelerator NUCLEAR REACTIONS 54Fe(p, p), E=4.341-4.345 MeV; measured σ(θ) vs E. 55Co deduced resonance, J, π, Γp. R-matrix analysis. 32S(p, p), E=3.374-3.376 MeV; measured T=3/2 resonance yield; deduced optimum resolution conditions. Polarized, unpolarized beams, foil, gas strippers.
doi: 10.1016/0167-5087(84)90334-X
1983NE04 Phys.Rev. C27, 930 (1983) R.O.Nelson, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Proton Resonances in 30P NUCLEAR REACTIONS 29Si(p, p), (p, p'), E=1.29-3.31 MeV; measured σ(Ep), σ(θ); deduced channel spin mixing. 30P deduced resonances, J, π, Γp, Γp', L, IAS Coulomb energies, S. Enriched target. R-matrix analysis.
doi: 10.1103/PhysRevC.27.930
1983RA15 Z.Phys. A311, 157 (1983) P.Ramakrishnan, B.H.Chou, G.E.Mitchell, E.G.Bilpuch, R.O.Nelson, J.F.Shriner, Jr., C.R.Westerfeldt Statistical Properties of 3/2+ Resonances in 49V NUCLEAR REACTIONS 48Ti(p, p'γ), E=2.4203-3.0815 MeV; measured Eγ, Iγ, γ(θ), pγ-coin, pγ(θ), σ(E). 49V deduced resonances, J, π, inelastic reduced widths, amplitude, width correlations. Statistical analysis.
doi: 10.1007/BF01415100
1983SH22 Z.Phys. A313, 51 (1983) J.F.Shriner, Jr., K.M.Whatley, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Statistical Properties of 3/2- Resonances in 45Sc and 51Mn NUCLEAR REACTIONS 44Ca(p, p'γ), E=2.8-3.01 MeV; 50Cr(p, p'γ), E=3.03-4.3 MeV; measured Eγ, Iγ, σ(θp), σ(θγ). 45Sc, 51Mn deduced resonances, L, J, π, width, amplitude correlations.
doi: 10.1007/BF02115842
1983WH02 J.Phys.(London) G9, 1527 (1983) K.M.Whatley, E.G.Bilpuch, G.E.Mitchell, J.F.Shriner, Jr., C.R.Westerfeldt Statistical Properties of (5/2)+ Resonances in 51Mn NUCLEAR REACTIONS 50Cr(p, p'γ), E=3.26-4.28 MeV; measured σ(θ). 51Mn deduced resonances, J, π, Γp, Γp', amplitude, width correlations.
doi: 10.1088/0305-4616/9/12/013
1982SH12 Z.Phys. A305, 307 (1982) J.F.Shriner, Jr., E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Amplitude Correlations for Inelastic Proton Scattering from 44Ca NUCLEAR REACTIONS 44Ca(p, p'γ), E=2.315-2.9903 MeV; measured σ(θp'), γ(θ). 45Sc resonances deduced reduced widths, channel amplitudes.
doi: 10.1007/BF01419078
1982WE03 Nucl.Instrum.Methods 192, 273 (1982) C.R.Westerfeldt, S.A.Wender, E.G.Bilpuch, G.E.Mitchell, W.K.Wells Measurement of Nuclear E0 Transitions NUCLEAR REACTIONS 72Ge(p, p'e), E=3-4.34 MeV; measured p'e-coin, I(ce)(t), σ(E). 72Ge level deduced T1/2. 73As deduced IAR. Pulsed beam, large solid angle electron detector.
doi: 10.1016/0029-554X(82)90832-1
1981CH16 Z.Phys. A300, 157 (1981) B.H.Chou, G.E.Mitchell, E.G.Bilpuch, C.R.Westerfeldt Amplitude Correlations for Inelastic Proton Scattering from 48Ti NUCLEAR REACTIONS 48Ti(p, p'), E=2.298-3.088 MeV; analyzed σ(θ, Ep', E), Eγ, Iγ. 49V deduced resonances, J, π, reduced widths, channel amplitude correlations. Porter-Thomas, Krieger-Porter distributions. Silicon surface barrier, NaI(Tl) detectors.
doi: 10.1007/BF01412292
1981HA28 Phys.Rev. C24, 786 (1981) D.Halderson, K.W.Kemper, J.D.Fox, R.O.Nelson, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell Width of the 6-, T = 1, E(x) = 14.36 MeV State in 28Si and Its Relationship to Intermediate Energy Inelastic Scattering NUCLEAR REACTIONS 27Al(p, p'), E=2.7-3.06 MeV; measured σ(Ep, θ). 28Si resonance deduced Γ. R-matrix analysis.
doi: 10.1103/PhysRevC.24.786
1981SA24 J.Phys.(London) G7, 1405 (1981) K.B.Sales, G.E.Mitchell, E.G.Bilpuch, C.R.Westerfeldt Proton Strength Functions of 64Zn and 66Zn NUCLEAR REACTIONS 64Zn(p, p), E=2.5-3.24 MeV; 66Zn(p, p), E=2.6-3.26 MeV; measured σ(E, θ). 65,67Ga deduced IAR, J, π, Γp, level spacing, strength function.
doi: 10.1088/0305-4616/7/10/018
1980CH16 Phys.Rev.Lett. 45, 1235 (1980) B.H.Chou, G.E.Mitchell, E.G.Bilpuch, C.R.Westerfeldt Correlations for Reduced-Width Amplitudes in 49V NUCLEAR REACTIONS 48Ti(p, p'), E=2.2-3.1 MeV; analyzed reduced width data; 49V resonances deduced channel amplitude correlations. Channel spin representation, Kreiger-Porter distribution.
doi: 10.1103/PhysRevLett.45.1235
1978WE06 Nucl.Phys. A303, 111 (1978) C.R.Westerfeldt, G.E.Mitchell, E.G.Bilpuch, D.A.Outlaw High Resolution Study of the 26Mg(p, p) Reaction NUCLEAR REACTIONS 26Mg(p, p), E=1.54-3.06 MeV; measured σ(E, θ). 27Al deduced isobaric analog resonances, J, π, Γp, S, Coulomb energies.
doi: 10.1016/0375-9474(78)90045-3
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