NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = K.Murphy Found 27 matches. 2016GR18 Appl.Radiat.Isot. 118, 366 (2016) J.R.Griswold, D.G.Medvedev, J.W.Engle, R.Copping, J.M.Fitzsimmons, V.Radchenko, J.C.Cooley, M.E.Fassbender, D.L.Denton, K.E.Murphy, A.C.Owens, E.R.Birnbaum, K.D.John, F.M.Nortier, D.W.Stracener, L.H.Heilbronn, L.F.Mausner, S.Mirzadeh Large scale accelerator production of 225Ac: Effective cross sections for 78-192 MeV protons incident on 232Th targets NUCLEAR REACTIONS 232Th(p, X)225Ac/226Ac/227Ac/227Th/228Th/99Mo/140Ba/139Ce/141Ce/143Ce/144Ce, E=78-192 MeV; measured reaction products, Eγ, Iγ; deduced effective production σ, yields. Comparison with available data.
doi: 10.1016/j.apradiso.2016.09.026
2016HO08 Appl.Radiat.Isot. 114, 19 (2016) S.Hogle, R.A.Boll, K.Murphy, D.Denton, A.Owens, T.J.Haverlock, M.Garland, S.Mirzadeh Reactor production of Thorium-229 RADIOACTIVITY 229Ra, 229Ac(β-) [from 226,228Ra, 227Ac(n, X), E thermal]; measured decay products; deduced yields.
doi: 10.1016/j.apradiso.2016.05.002
2014NE02 Eur.Phys.J. A 50, 41 (2014) W.G.Newton, J.Hooker, M.Gearheart, K.Murphy, D.-H.Wen, F.J.Fattoyev, B.-A.Li Constraints on the symmetry energy from observational probes of the neutron star crust
doi: 10.1140/epja/i2014-14041-x
1997TE14 Phys.Lett. 413B, 253 (1997) J.A.Templon, B.A.Raue, K.Murphy, D.J.Millener, D.S.Carman, G.M.Huber, B.C.Markham, D.W.Miller, P.Schwandt, L.C.Bland Study of Continuum Nuclear Structure of 12C Via (p, p'X) at Intermediate Energies NUCLEAR REACTIONS 12C(p, p'), (p, 2p), (p, pα), E=156 MeV; measured Ep, Ip, σ(θ, Ep). 12C deduced small continuum nonresonant contribution.
doi: 10.1016/S0370-2693(97)01149-0
1995RA14 Phys.Rev. C52, R445 (1995) B.A.Raue, L.C.Bland, D.S.Carman, G.M.Huber, B.C.Markham, D.W.Miller, K.Murphy, S.F.Pate, J.A.Templon, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz Study of the Isospin Response of the 4He Continuum using the 4He(p, p'X) Reaction NUCLEAR REACTIONS 4He(p, p't), (p, p'3He), (p, p'd), (p, p'X), E=101.2 MeV; measured (particle)(particle)(θ), σ(E) ratio in some cases. 4He deduced resonances single nucleon decay characteristics.
doi: 10.1103/PhysRevC.52.R445
1991HO26 Nucl.Instrum.Methods Phys.Res. B56/57, 459 (1991) C.R.Howell, W.Tornow, H.G.Pfutzner, M.L.Roberts, K.Murphy, P.D.Felsher, G.J.Weisel, G.Mertens, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Neutron-Deuteron Elastic Scattering and Breakup Reactions Below 20 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=12 MeV; 2H(n, X), E=13 MeV; compiled, reviewed analyzing power vs θ, σ(θ1, θ2) vs arc length data for breakup.
doi: 10.1016/0168-583X(91)96070-2
1990HO14 Nucl.Instrum.Methods Phys.Res. A290, 424 (1990) C.R.Howell, W.Tornow, H.G.Pfutzner, A.Li, M.L.Roberts, K.Murphy, P.D.Felsher, G.J.Weisel, A.Naqvi, R.L.Walter, J.M.Lambert, P.A.Treado, I.Slaus Techniques for Vector Analyzing Power Measurements of the 2H(n(pol), np)n Breakup Reaction at Low Energies NUCLEAR REACTIONS 2H(polarized n, np), E=12 MeV; measured σ(En), vector analyzing power. High accuracy, breakup reaction.
doi: 10.1016/0168-9002(90)90560-S
1988HO12 Phys.Rev. C38, 1552 (1988) C.R.Howell, R.S.Pedroni, G.M.Honore, K.Murphy, R.C.Byrd, G.Tungate, R.L.Walter Scattering of Polarized and Unpolarized Nucleons from 28Si NUCLEAR REACTIONS 28Si(polarized n, n), (polarized n, n'), (n, n), (n, n'), E=8-17 MeV; measured σ(En), analyzing power vs θ, σ(θ); deduced model parameters. 28Si levels deduced multipole moments, B(λ). Analyzed other data.
doi: 10.1103/PhysRevC.38.1552
1988HO14 Phys.Rev.Lett. 61, 1565 (1988) C.R.Howell, W.Tornow, I.Slaus, P.D.Felsher, M.L.Roberts, H.G.Pfutzner, Anli Li, K.Murphy, R.L.Walter, J.M.Lambert, P.A.Treado, H.Witala, W.Glockle, T.Cornelius Rigorous Calculations and Measurements of A(y)(θ) for n + d Elastic-Scattering and Breakup Processes NUCLEAR REACTIONS 2H(polarized n, np), E=12 MeV; measured vector analyzing power vs θ. Three-nucleon calculations.
doi: 10.1103/PhysRevLett.61.1565
1987HO09 Few-Body Systems 2, 19 (1987) C.R.Howell, W.Tornow, K.Murphy, H.G.Pfutzner, M.L.Roberts, Anli Li, P.D.Felsher, R.L.Walter, I.Slaus, P.A.Treado, Y.Koike Comparisons of Vector Analyzing-Power Data and Calculations for Neutron-Deuteron Elastic Scattering from 10 to 14 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=10, 12, 14.1 MeV; measured analyzing powers vs θ. Polarized neutron facilities, other data input. Faddeev calculations.
doi: 10.1007/BF01078989
1986MU07 Nucl.Phys. A455, 525 (1986) K.Murphy, R.C.Byrd, C.E.Floyd, P.P.Guss, R.L.Walter Measurements of σ(θ) and A(y)(θ) for the 9Be(p, n)9B Reaction and Lane Model Analysis for the 9Be + Nucleon System NUCLEAR REACTIONS 9Be(polarized p, n), E=8-17.57 MeV; measured σ(θ), A(θ); 9Be(p, p), 9Be(p, n), 9Be(n, n), E=11-17 MeV; analyzed data; deduced potential parameters. Lane model calculations, complex isovector spin-orbit potential, Coulomb correction terms.
doi: 10.1016/0375-9474(86)90320-9
1986MU08 Radiat.Eff. 92, 219 (1986) K.Murphy, R.C.Byrd, C.R.Howell, R.L.Walter Nucleon Scattering from 11B and 10B NUCLEAR REACTIONS 11B(n, n), E=10-17 MeV; measured σ(θ). 11B(polarized n, n), E=10, 15 MeV; measured analyzing power vs θ. 11B(p, n), (polarized p, n), E=12.77-17.22 MeV; measured σ(θ), analyzing power vs θ. 11B(p, p), E=10-17 MeV; measured σ(θ); deduced potential parameters. Lane model analysis.
doi: 10.1080/00337578608208326
1985GU09 Nucl.Phys. A438, 187 (1985) P.P.Guss, R.C.Byrd, C.E.Floyd, C.R.Howell, K.Murphy, G.Tungate, R.S.Pedroni, R.L.Walter, J.P.Delaroche, T.B.Clegg Cross Sections and Analyzing Powers for Fast-Neutron Scattering to the Ground and First Excited States of 58Ni and 60Ni NUCLEAR REACTIONS 58,60Ni(n, n), (polarized n, n), (n, n'), E=8-14 MeV; measured σ(θ), analyzing power vs θ; deduced p, n deformation parameters. Optical model, coupled-channels analysis.
doi: 10.1016/0375-9474(85)90124-1
1984BY03 Nucl.Phys. A427, 36 (1984) R.C.Byrd, C.E.Floyd, K.Murphy, P.P.Guss, R.L.Walter The Analyzing Power for Neutron Scattering from 9Be at 9 to 17 MeV NUCLEAR REACTIONS 9Be(polarized n, n), E=9-17 MeV; measured analyzing power vs θ, σ(θ); deduced Legendre coefficients. Spherical, coupled-channels optical model, imaginary spin-orbit term.
doi: 10.1016/0375-9474(84)90137-4
1983BY01 Nucl.Phys. A399, 94 (1983) R.C.Byrd, C.E.Floyd, P.P.Guss, K.Murphy, R.L.Walter Cross-Section Measurement and Lane Model Analysis for the 9Be(p, n)9B Reaction NUCLEAR REACTIONS 9Be(p, n), E=8.15-15.68 MeV; measured σ(E, θ). 9Be(p, n), E=2-30 MeV; 9Be(p, p), (p, n), (n, n), E=8-16 MeV; analyzed data. Legendre coefficient, Lane model, coupled-channels calculations.
doi: 10.1016/0375-9474(83)90596-1
1983BY03 Nucl.Phys. A410, 29 (1983) R.C.Byrd, W.Tornow, P.W.Lisowski, K.Murphy, R.l.Walter Comparison of Polarization and Analyzing Power for the 15N(p, n)15O Reaction NUCLEAR REACTIONS 15N(polarized p, n), E=3.7-12 MeV; measured A(E, θ), P(E, θ); deduced σ(E, θ), Legendre coefficients, spin-flip asymmetry. Comparison to previous P(θ) measurements.
doi: 10.1016/0375-9474(83)90399-8
1983DE35 Phys.Rev. C28, 1410 (1983) J.P.Delaroche, C.E.Floyd, P.P.Guss, R.C.Byrd, K.Murphy, G.Tungate, R.L.Walter Complex Spin-Orbit Potential for 208Pb(n, n)208Pb at 10 MeV NUCLEAR REACTIONS 208Pb(n, n), (polarized n, n), E=10 MeV; measured σ(θ), A(θ); deduced complex spin-orbit potential. Spherical optical model calculations.
doi: 10.1103/PhysRevC.28.1410
1983FL07 Phys.Rev. C28, 1498 (1983) C.E.Floyd, P.P.Guss, R.C.Byrd, K.Murphy, R.L.Walter, J.P.Delaroche Spin-Orbit Potential Properties Derived from Measurements of Analyzing Powers for Neutron Scattering from 54Fe and 65Cu NUCLEAR REACTIONS 54Fe, 65Cu(polarized n, n), E=10, 14 MeV; 54Fe(polarized n, n'), E=10 MeV; measured analyzing power vs θ; deduced deformed complex spin-orbit potential parameters. Coupled-channels analysis.
doi: 10.1103/PhysRevC.28.1498
1983GU03 Nucl.Phys. A395, 1 (1983) P.P.Guss, K.Murphy, R.C.Byrd, C.E.Floyd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power for the 2H(d, n)3He(g.s.) Reaction from 5.5 to 11.5 MeV NUCLEAR REACTIONS 2H(polarized d, n), E=5.5, 7, 8.5, 10, 11.5 MeV; measured A(θ). Report discrepancies with previous measurements. Polynomial expansions analysis.
doi: 10.1016/0375-9474(83)90085-4
1983WO02 Nucl.Phys. A394, 139 (1983) E.Woye, W.Tornow, G.Mack, C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power A(y)(θ) for 12C(n, n0, 1)12C between 8.9 and 14.9 MeV Neutron Energy NUCLEAR REACTIONS 12C(n, n), (n, n'), E=8.9-14.9 MeV; measured A(E, θ); deduced optical potential parameters. 12C level deduced quadrupole deformation.
doi: 10.1016/0375-9474(83)90167-7
1982FL01 Phys.Rev. C25, 1682 (1982) C.E.Floyd, P.P.Guss, K.Murphy, C.R.Howell, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg Analyzing Powers for Neutron Elastic Scattering at Forward Angles NUCLEAR REACTIONS 40Ca, 54Fe, 65Cu, 120Sn, 208Pb(polarized n, n), E=14 MeV; measured A(θ).
doi: 10.1103/PhysRevC.25.1682
1982GU02 Phys.Rev. C25, 2854 (1982) P.P.Guss, C.E.Floyd, K.Murphy, C.R.Howell, R.S.Pedroni, G.M.Honore, H.G.Pfutzner, G.Tungate, R.C.Byrd, R.L.Walter, J.P.Delaroche Spin-Orbit Deformations Deduced from Analyzing Powers for Inelastic Neutron Scattering from 54Fe, 56Fe, 58Ni, 120Sn, and 208Pb NUCLEAR REACTIONS 54,56Fe, 58,60Ni, 120Sn, 208Pb(polarized n, n'), E=10 MeV; measured A(θ). 54,56Fe, 58,60Ni, 120Sn, 208Pb level deduced spin-orbit to Coulomb deformation parameter ratio. Coupled-channels analysis.
doi: 10.1103/PhysRevC.25.2854
1982TO11 Nucl.Phys. A385, 373 (1982) W.Tornow, E.Woye, G.Mack, C.E.Floyd, K.Murphy, P.P.Guss, S.A.Wender, R.C.Byrd, R.L.Walter, T.B.Clegg, H.Leeb Analyzing Power and Differential Cross Section at 9.9, 11.9 and 13.9 MeV for Ca(n, n)Ca NUCLEAR REACTIONS 40Ca(polarized n, n), E=9.9, 11.9, 13.9 MeV; measured A(E, θ), σ(E, θ); deduced optical model parameters, Coulomb correction terms. Optical potential analysis, l-dependence, Fourier-Bessel expansion of the real central potential.
doi: 10.1016/0375-9474(82)90093-8
1981BY01 Nucl.Phys. A351, 189 (1981) R.C.Byrd, C.E.Floyd, K.Murphy, P.P.Guss, R.L.Walter, S.R.Cotanch Measurement and Lane-Model Analysis of Cross Sections for the 13C(p, n)13N and 15N(p, n)15O Reactions NUCLEAR REACTIONS 13C(p, n), E=10.1-16.75 MeV; 15N(p, n), E=9.05-15.62 MeV; measured σ(Ep, θ). Lane Model analysis.
doi: 10.1016/0375-9474(81)90440-1
1981FL04 Phys.Rev.Lett. 47, 1042 (1981) C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg Determination of the Spin-Orbit Interaction for Neutron-Nucleus Scattering NUCLEAR REACTIONS 54Fe, 65Cu(polarized n, n), E=14 MeV; measured σ(θ), A(θ); deduced neutron-nucleus spin-orbit interaction. Optical model.
doi: 10.1103/PhysRevLett.47.1042
1981MU01 Nucl.Phys. A355, 1 (1981) K.Murphy, R.C.Byrd, P.P.Guss, C.E.Floyd, R.L.Walter The 15N(p, n)15O Reaction below 9.3 MeV NUCLEAR REACTIONS 15N(p, n), E=5.5-9.3 MeV; measured σ(θ); deduced total σ, compared to previous measurements.
doi: 10.1016/0375-9474(81)90128-7
1968HE14 Phys.Letters 27B, 563 (1968) N.Hershkowitz, C.G.Jacobs, Jr., K.A.Murphy Observation of the Mossbauer Effect in 232Th Following Coulomb Excitation NUCLEAR REACTIONS 232Th(γ, γ), E=49.8 keV; measured Mossbauer effect. 232Th level deduced T1/2.
doi: 10.1016/0370-2693(68)90032-4
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