NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.G.Madland Found 42 matches. 2017MA01 Nucl.Phys. A957, 289 (2017); Corrigendum Nucl.Phys. A961, 216 (2017) Refinements in the Los Alamos model of the prompt fission neutron spectrum NUCLEAR REACTIONS 252Cf(n, F), E=thermal; calculated prompt pre-fission neutron spectrum, multiplicity, σ. RADIOACTIVITY 252Cf(SF); calculated prompt pre-fission neutron spectrum, σ; deduced parameters. Refined Los Alamos model. Calculations compared with available data.
doi: 10.1016/j.nuclphysa.2016.09.005
2010TA15 Nucl.Sci.Eng. 166, 254 (2010) P.Talou, T.Kawano, D.G.Madland, A.C.Kahler, D.K.Parsons, M.C.White, R.C.Little, M.B.Chadwick Uncertainty Quantification of Prompt Fission Neutron Spectrum for n(0.5 MeV) + 239Pu NUCLEAR REACTIONS 239Pu(n, F), E<0.5 MeV; calculated fission spectrum uncertainties, probability distribution functions; deduced correlation matrix. Madland-Nix model.
doi: 10.13182/NSE09-10
2009KA24 Phys.Rev. C 80, 024611 (2009) T.Kawano, P.Talou, J.E.Lynn, M.B.Chadwick, D.G.Madland Calculation of nuclear reaction cross sections on excited nuclei with the coupled-channels method NUCLEAR REACTIONS 169Tm(n, n), (n, n'), (n, γ), (n, X), E<20 MeV; calculated σ. 239Pu(n, X), E=0.01-10 MeV; calculated fission σ. Coupled-channels and statistical Hauser-Feshbach model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024611
2008TA30 Nucl.Data Sheets 109, 2858 (2008) P.Talou, D.G.Madland, T.Kawano Uncertainty Quantification on Prompt Fission Neutrons Spectra NUCLEAR REACTIONS 235U(n, f), E= 14 MeV; calculated prompt fission neutron spectrum.
doi: 10.1016/j.nds.2008.11.023
2007YO07 Nucl.Data Sheets 108, 2589 (2007) P.G.Young, M.B.Chadwick, R.E.MacFarlane, P.Talou, T.Kawano, D.G.Madland, W.B.Wilson, C.W.Wilkerson Evaluation of Neutron Reactions for ENDF/B-VII:232-241U and 239PU NUCLEAR REACTIONS 232,233,234,235,236,237,239,240,241U, 239Pu(n, X), E< 30 MeV; evaluated cross sections for ENDF/B-VII.
doi: 10.1016/j.nds.2007.11.002
2006CH50 Nucl.Data Sheets 107, 2931 (2006) M.B.Chadwick, P.Oblozinsky, M.Herman, N.M.Greene, R.D.McKnight, D.L.Smith, P.G.Young, R.E.MacFarlane, G.M.Hale, S.C.Frankle, A.C.Kahler, T.Kawano, R.C.Little, D.G.Madland, P.Moller, R.D.Mosteller, P.R.Page, P.Talou, H.Trellue, M.C.White, W.B.Wilson, R.Arcilla, C.L.Dunford, S.F.Mughabghab, B.Pritychenko, D.Rochman, A.A.Sonzogni, C.R.Lubitz, T.H.Trumbull, J.P.Weinman, D.A.Brown, D.E.Cullen, D.P.Heinrichs, D.P.McNabb, H.Derrien, M.E.Dunn, N.M.Larson, L.C.Leal, A.D.Carlson, R.C.Block, J.B.Briggs, E.T.Cheng, H.C.Huria, M.L.Zerkle, K.S.Kozier, A.Courcelle, V.Pronyaev, S.C.van der Marck ENDF/B-VII.0: Next Generation Evaluated Nuclear Data Library for Nuclear Science and Technology
doi: 10.1016/j.nds.2006.11.001
2006LE02 Phys.Rev. C 73, 014602 (2006) S.Lemaire, P.Talou, T.Kawano, M.B.Chadwick, D.G.Madland Monte Carlo approach to sequential γ-ray emission from fission fragments NUCLEAR REACTIONS 235U(n, F), E=0.53 MeV; calculated neutron and γ-ray multiplicity, average Eγ vs fission fragment mass and total kinetic energy. Monte Carlo approach, comparison with data. RADIOACTIVITY 252Cf(SF); calculated neutron and γ-ray multiplicity, average Eγ vs fission fragment mass and total kinetic energy. Monte Carlo approach, comparison with data.
doi: 10.1103/PhysRevC.73.014602
2006MA37 Nucl.Phys. A772, 113 (2006) Total prompt energy release in the neutron-induced fission of 235U, 238U, and 239Pu NUCLEAR REACTIONS 235U(n, F), E=0-9 MeV; 238U(n, F), E=0-30 MeV;239Pu(n, F), E=0-5.5 MeV; calculated total fission fragment and fission product kinetic energies. 235,238U, 239Pu(n, F), E=0-15 MeV; calculated prompt fission neutron multiplicity and energy, prompt fission γ-ray energy, fission fragment neutron separation energy and excitation energy, prompt fission energy release and deposition. Monte Carlo approach, comparison with data.
doi: 10.1016/j.nuclphysa.2006.03.013
2005LE29 Phys.Rev. C 72, 024601 (2005) S.Lemaire, P.Talou, T.Kawano, M.B.Chadwick, D.G.Madland Monte Carlo approach to sequential neutron emission from fission fragments NUCLEAR REACTIONS 235U(n, F), E=0.53 MeV; calculated prompt fission neutron spectra, multiplicities vs fragment mass. Monte Carlo approach with sequential neutron emission. RADIOACTIVITY 252Cf(SF); calculated prompt fission neutron spectra, multiplicities vs fragment mass. Monte Carlo approach with sequential neutron emission.
doi: 10.1103/PhysRevC.72.024601
2005LI30 Phys.Rev.Lett. 95, 042501 (2005) Yu.A.Litvinov, T.J.Burvenich, H.Geissel, Yu.N.Novikov, Z.Patyk, C.Scheidenberger, F.Attallah, G.Audi, K.Beckert, F.Bosch, M.Falch, B.Franzke, M.Hausmann, Th.Kerscher, O.Klepper, H.-J.Kluge, C.Kozhuharov, K.E.G.Lobner, D.G.Madland, J.A.Maruhn, G.Munzenberg, F.Nolden, T.Radon, M.Steck, S.Typel, H.Wollnik Isospin Dependence in the Odd-Even Staggering of Nuclear Binding Energies NUCLEAR STRUCTURE Hf, W; compiled, analyzed neutron and proton pair-gap energies, odd-even staggering effect. Several models compared with data.
doi: 10.1103/PhysRevLett.95.042501
2004BU18 Acta Phys.Hung.N.S. 19, 149 (2004) T.Burvenich, T.Cornelius, A.Sulaksono, J.A.Maruhn, W.Greiner, D.G.Madland, P.-G.Reinhard, S.Schramm Application and Extrapolation of Mean-Field Models in the Heavy and Superheavy Regions NUCLEAR STRUCTURE 292120; calculated neutron and proton density distributions. Relativistic point-coupling models.
doi: 10.1556/APH.19.2004.1-2.23
2004BU19 Nucl.Phys. A744, 92 (2004) T.J.Burvenich, D.G.Madland, P.-G.Reinhard Adjustment studies in self-consistent relativistic mean-field models NUCLEAR STRUCTURE Sn, Pb; analyzed binding energies, form factors, radii. Relativistic mean-field approach, role of adjustment procedures discussed.
doi: 10.1016/j.nuclphysa.2004.08.017
2004MA60 Nucl.Phys. A741, 52 (2004) D.G.Madland, T.J.Burvenich, J.A.Maruhn, P.-G.Reinhard On the isovector channels in relativistic point coupling models within the Hartree and Hartree-Fock approximations
doi: 10.1016/j.nuclphysa.2004.06.003
2003BU20 Nucl.Phys. A729, 769 (2003) A nucleonic NJL model for finite nuclei: dynamic mass generation and ground-state observables NUCLEAR STRUCTURE 16O, 40Ca, 88Sr, 90Zr, 208Pb; calculated binding energies, radii. 132Sn; calculated binding energy. 16O, 48Ca, 208Pb; calculated charge density distributions. 16O calculated single-particle level energies. Nambu-Jona-Lasinio model.
doi: 10.1016/j.nuclphysa.2003.10.002
2003KL05 Phys.Rev. C 67, 031601 (2003) J.Klug, J.Blomgren, A.Atac, B.Bergenwall, A.Hildebrand, C.Johansson, P.Mermod, L.Nilsson, S.Pomp, U.Tippawan, K.Elmgren, N.Olsson, O.Jonsson, A.V.Prokofiev, P.-U.Renberg, P.Nadel-Turonski, S.Dangtip, P.Phansuke, M.Osterlund, C.Le Brun, J.F.Lecolley, F.R.Lecolley, M.Louvel, N.Marie-Noury, C.Schweitzer, Ph.Eudes, F.Haddad, C.Lebrun, A.J.Koning, E.Bauge, J.P.Delaroche, M.Girod, X.Ledoux, P.Romain, D.G.Madland, K.Amos, P.K.Deb, S.Karataglidis, R.Crespo, A.M.Moro Elastic neutron scattering at 96 MeV from 12C and 208Pb NUCLEAR REACTIONS 12C, 208Pb(n, n), E=96 MeV; measured σ(θ). Comparison with model predictions.
doi: 10.1103/PhysRevC.67.031601
2002BU07 Phys.Rev. C65, 044308 (2002) T.Burvenich, D.G.Madland, J.A.Maruhn, P.-G.Reinhard Nuclear Ground State Observables and QCD Scaling in a Refined Relativistic Point Coupling Model NUCLEAR STRUCTURE Ca, Ni, Sn, Pb, Cf, Fm, No, Rf, Sg, Hs; calculated binding energies. 240Pu; calculated fission barrier. Sn, Pb; calculated radii, surface thickness. 48Ca, 100Sn; calculated total baryon densities. 48Ca; calculated charge form factor. Relativistic point-coupling model, comparison with other models.
doi: 10.1103/PhysRevC.65.044308
2002BU35 Prog.Theor.Phys.(Kyoto), Suppl. 146, 130 (2002) T.Burvenich, D.G.Madland, A.Sulaksono, J.Maruhn, P.-G.Reinhard A Relativistic Point Coupling Model for Nuclear Structure Calculations NUCLEAR STRUCTURE 16O, 40,48Ca, 56,58Ni, 88Sr, 90Zr, 100,112,120,124,132Sn, 136Xe, 144Sm, 202,204,208Pb; calculated binding energies, radii. Relativistic point coupling model.
2002BU37 J.Nucl.Radiochem.Sci. 3, No 1, 191 (2002) T.Burvenich, D.G.Madland, J.A.Maruhn, P.-G.Reinhard A Relativistic Point Coupling Model for Nuclear Structure Calculations
2002IW02 J.Nucl.Sci.Technol.(Tokyo) 39, 332 (2002) A.Iwamoto, P.Moller, D.G.Madland, A.J.Sierk Mass Division in Nuclear Fission and Isotope Effect NUCLEAR STRUCTURE 256,258Fm; calculated fission saddle point shapes; deduced mass-symmetric and mass-asymmetric modes.
doi: 10.1080/18811248.2002.9715198
2001DE16 Phys.Rev.Lett. 86, 3248 (2001) P.K.Deb, K.Amos, S.Karataglidis, M.B.Chadwick, D.G.Madland Predicting Total Reaction Cross Sections for Nucleon-Nucleus Scattering NUCLEAR REACTIONS 12C, 208Pb(n, X), (p, X), E=0-300 MeV; calculated total reaction σ. Optical potential, comparisons with data.
doi: 10.1103/PhysRevLett.86.3248
2001MO13 Nature(London) 409, 785 (2001) P.Moller, D.G.Madland, A.J.Sierk, A.Iwamoto Nuclear Fission Modes and Fragment Mass Asymmetries in a Five-Dimensional Deformation Space NUCLEAR STRUCTURE 228Ra, 234U, 256,258Fm; calculated potential energy surfaces; deduced fission mode features. 220,222,224,226,228,230,232Th, 228,230,232,234,236,238,240U, 234,236,238,240,242,244,246Pu, 240,242,244,246,248,250,252Cm, 246,248,250,252,254,256,258Cf, 246,248,250,252,254,256,258Fm; calculated average fragment mass division in asymmetric fission. Five-dimensional shape-coordinate grid. Comparisons with data.
doi: 10.1038/35057204
1999MB06 Acta Phys.Hung.N.S. 10, 231 (1999) The Los Alamos Model of Neutron Emission in Fission NUCLEAR REACTIONS 235U(n, F), E at rest; calculated prompt neutron spectrum, average multiplicity. Los Alamos model, comparison with data.
1998GI04 Phys.Rev. C57, 1167 (1998) Pseudospin Symmetry and Relativistic Single-Nucleon Wave Functions NUCLEAR STRUCTURE 208Pb; calculated neutron, proton pseudospin doublets wavefunctions, levels; deduced pseudospin symmetry effects. Realistic relativistic mean fields.
doi: 10.1103/PhysRevC.57.1167
1996FR05 Phys.Rev. C53, 3085 (1996) J.L.Friar, D.G.Madland, B.W.Lynn QCD Scales in Finite Nuclei
doi: 10.1103/PhysRevC.53.3085
1993KO04 Nucl.Phys. A552, 469 (1993) Parameter Correlations and Ambiguities in Dirac Phenomenology NUCLEAR REACTIONS 40Ca(polarized p, p), E=181 MeV; analyzed σ(θ), analyzing power, spin rotation function vs θ; deduced equivalent potential families, parameters. Dirac phenomenology.
doi: 10.1016/0375-9474(93)90279-7
1992NI09 Phys.Rev. C46, 1757 (1992) B.A.Nikolaus, T.Hoch, D.G.Madland Nuclear Ground State Properties in a Relativistic Point Coupling Model NUCLEAR STRUCTURE A=4-206; calculated binding energy, rms charge radii, nucleon density distribution rms radii. Relativistic mean field theory, 16O, 88Sr, 208Pb treated as coupling constants optimizing nuclei.
doi: 10.1103/PhysRevC.46.1757
1991WA07 Nucl.Sci.Eng. 108, 109 (1991) R.L.Walsh, G.Chircu, D.G.Madland Calculation of Fission Neutron Spectra for Spontaneous Fission of 240Pu, 238Pu and 242Pu RADIOACTIVITY 240,238,242Pu(SF); calculated fission neutron spectra. Spin-dependent Madland-Nix model.
doi: 10.13182/NSE91-A23810
1990KO07 Nucl.Phys. A509, 664 (1990) Prediction of Intermediate-Energy Neutron Scattering Observables from a Dirac Optical Potential NUCLEAR REACTIONS 208Pb(n, n), E=95-250 MeV; calculated σ(E), σ(θ). Global optical potential, Dirac phenomenology.
doi: 10.1016/0375-9474(90)90247-J
1989KO09 Phys.Rev. C39, 1461 (1989) Dirac Optical Potentials for Nucleon Scattering by 208Pb at Intermediate Energies NUCLEAR REACTIONS 208Pb(p, p), (polarized p, p), E=80-800 MeV; analyzed σ(θ), analyzing power, spin rotation parameters, total reaction σ; deduced model parameters. Dirac optical potentials.
doi: 10.1103/PhysRevC.39.1461
1989MA44 Phys.Rev. C40, 1999 (1989) V.A.Madsen, L.F.Hansen, V.R.Brown, D.G.Madland Correction for Truncation in Coupled-Channels Optical Potentials NUCLEAR REACTIONS 238U(n, n'), E=1, 4, 8 MeV; 238U(p, p'), E=18, 26 MeV; calculated σ. Coupled-channels formalism, truncation.
doi: 10.1103/PhysRevC.40.1999
1989YO11 Trans.Amer.Nucl.Soc. 60, 271 (1989) P.G.Young, E.D.Arthur, M.Bozoian, T.R.England, G.M.Hale, R.J.LaBauve, R.C.Little, R.E.MacFarlane, D.G.Madland, R.T.Perry, W.B.Wilson 7. Transport data libraries for incident proton and neutron energies to 100 MeV NUCLEAR REACTIONS 1H, 9Be, C, O, 27Al, Si, Fe, W, 238U(p, X), 1H, 9Be, C, O, 27Al, Si, Ca, Fe, W, 238U(n, X), E<100 MeV; analyzed available data; deduced σ for transport libraries.
1988MA04 Nucl.Phys. A476, 1 (1988) New Model of the Average Neutron and Proton Pairing Gaps NUCLEAR STRUCTURE 250Cf, 150Sm, 50Cr; N ≤ 160; calculated neutron, proton pairing gaps. 150Eu; calculated residual interaction vs finite difference order.
doi: 10.1016/0375-9474(88)90370-3
1986LA11 Phys.Rev. C33, 1616 (1986) Ch.Lagrange, D.G.Madland, M.Girod Semimicroscopic Calculations of Elastic, Inelastic, and Total Neutron Scattering by 239Pu in the Energy Range 10 keV ≤ E(n) ≤ 10 MeV NUCLEAR REACTIONS 239Pu(n, n), (n, n'), E=10 keV-10 MeV; calculated σ(θ), σ(E). Hartree-Fock method, semi-microscopic optical model.
doi: 10.1103/PhysRevC.33.1616
1986MA67 Radiat.Eff. 96, 103 (1986) D.G.Madland, R.J.Labauve, J.R.Nix Comparisons of Four Representations of the Prompt Neutron Spectrum for the Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); analyzed prompt neutron spectra following fission; calculated threshold integral σ.
doi: 10.1080/00337578608211722
1986NI06 Radiat.Eff. 92, 263 (1986) J.R.Nix, D.G.Madland, A.J.Sierk Effect of Fission Dynamics on the Spectra and Multiplicities of Prompt Fission Neutrons NUCLEAR REACTIONS 235U(n, F), E=0.53 MeV; calculated prompt fission neutron spectra vs E; deduced multiple-chance fission role. Unified macroscopic-microscopic method. NUCLEAR STRUCTURE 240Pu; calculated beyond fission saddle point dynamical evolution; deduced surface plus window dissipation role. Unified macroscopic-microscopic model.
doi: 10.1080/00337578608208336
1983LA03 Nucl.Sci.Eng. 83, 396 (1983) Ch.Lagrange, O.Bersillon, D.G.Madland Coupled-Channel Optical-Model Calculations for Evaluating Neutron Cross Sections of Odd-Mass Actinides NUCLEAR REACTIONS 239Pu(n, n), (n, n'), E=0.01, 1, 4, 6 MeV; 241Pu(n, n), (n, n'), E=1, 4, 6 MeV; calculated total σ, σ(compound nucleus), σ(inelastic), σ(θ); deduced transmission coefficients. Coupled-channels model.
doi: 10.13182/NSE83-A17575
1982MA14 Nucl.Sci.Eng. 81, 213 (1982) New Calculation of Prompt Fission Neutron Spectra and Average Prompt Neutron Multiplicities NUCLEAR REACTIONS, Fission 235U(n, F), E=0.53-15 MeV; 229Th, 239Pu, 249Cf(n, F), E=thermal; calculated prompt fission σ(En), average neutron multiplicities. Evaporation theory.
doi: 10.13182/NSE82-5
1980KY01 Phys.Lett. 91B, 353 (1980) G.S.Kyle, N.M.Hintz, M.S.Oothoudt, M.Kaletka, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr. Elastic and Inelastic Scattering of 800 MeV Protons by 58Ni NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=800 MeV; measured σ(θ). 58Ni levels deduced deformation lengths. DWBA analysis.
doi: 10.1016/0370-2693(80)90994-6
1979BL04 Phys.Rev. C20, 1490 (1979) G.Blanpied, N.M.Hintz, G.S.Kyle, J.W.Palm, R.Liljestrand, M.Barlett, C.Harvey, G.W.Hoffmann, L.Ray, D.G.Madland Proton Scattering from 24Mg at 0.8 GeV NUCLEAR REACTIONS 24Mg(p, p'), E=0.8 GeV; measured σ(θ). 24Mg levels deduced deformation length. Optical model, DWBA, coupled-channels, symmetric, asymmetric rotator model analyses.
doi: 10.1103/PhysRevC.20.1490
1979RA15 Phys.Lett. 83B, 275 (1979) L.Ray, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Kyle, N.M.Hintz, M.A.Oothoudt, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, R.M.Rolfe, C.A.Whitten, Jr. Coupled-Channels Effects in 0.8 GeV Proton Inelastic Scattering from 58Ni NUCLEAR REACTIONS 58Ni(p, p'), E=0.8 GeV; calculated σ(θ). Coupled channel, DWBA calculations with multistep, multiphonon mixing.
doi: 10.1016/0370-2693(79)91106-7
1977MA38 Nucl.Sci.Eng. 64, 859 (1977) The Influence of Isomeric States on Independent Fission Product Yields NUCLEAR REACTIONS 233,235U(n, F), E=th; calculated isomer/ground state yield ratios.
doi: 10.13182/NSE77-A14501
1974MA04 Phys.Rev. C9, 1002 (1974) D.G.Madland, P.Schwandt, W.T.Sloan, P.Shapiro, P.P.Singh Elastic Scattering of 60-MeV Alpha Particles by the Even Nickel Isotopes NUCLEAR REACTIONS 58,60,62,64Ni(α, α), E=60 MeV; 60Ni(α, α), E=75 MeV; measured σ(θ); θ=12-160°, enriched targets. Optical-model analysis.
doi: 10.1103/PhysRevC.9.1002
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