NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = G.P.Nobre Found 33 matches. 2023NE10 Eur.Phys.J. N 9, 35 (2023) D.Neudecker, A.M.Lewis, E.F.Matthews, J.Vanhoy, R.C.Haight, D.L.Smith, P.Talou, S.Croft, A.D.Carlson, B.Pierson, A.Wallner, A.Al-Adili, L.Bernstein, R.Capote, M.Devlin, M.Drosg, D.L.Duke, S.Finch, M.W.Herman, K.J.Kelly, A.Koning, A.E.Lovell, P.Marini, K.Montoya, G.P.A.Nobre, M.Paris, B.Pritychenko, H.Sjostrand, L.Snyder, V.Sobes, A.Solders, J.Taieb Templates of Expected Measurement Uncertainties: a CSEWG Effort NUCLEAR REACTIONS 235U(n, F), E<20 MeV; analyzed available data; deduced nubar mean values and uncertainties.
doi: 10.1051/epjn/2023014
2023NO03 Phys.Rev. C 107, 034612 (2023) G.P.A.Nobre, D.A.Brown, S.J.Hollick, S.Scoville, P.Rodriguez Novel machine-learning method for spin classification of neutron resonances NUCLEAR REACTIONS 52Cr(n, X), E=0.00001-20 MeV; analyzed evaluated and experimental data on neutron resonances; deduced resonances widths, position J, π. Machine learning approach to automate the quantum number assignments to neutron resonances using only the resonances’ energies and widths and not relying on detailed transmission or capture measurements.
doi: 10.1103/PhysRevC.107.034612
2021NO03 Nucl.Data Sheets 173, 1 (2021) G.P.A.Nobre, M.T.Pigni, D.A.Brown, R.Capote, A.Trkov, K.H.Guber, R.Arcilla, J.Gutierrez, A.Cuadra, G.Arbanas, B.Kos, D.Bernard, P.Leconte Newly Evaluated Neutron Reaction Data on Chromium Isotopes NUCLEAR REACTIONS 50,52,53Cr(n, n), (n, γ), (n, X), E<20 MeV; analyzed available data; deduced recommended σ using EMPIRE code within the Hauser-Feshbach framework.
doi: 10.1016/j.nds.2021.04.002
2020NO03 Phys.Rev. C 101, 034608 (2020) G.P.A.Nobre, D.A.Brown, M.W.Herman, A.Golas Constraining level densities through quantitative correlations with cross-section data NUCLEAR REACTIONS 56Fe(n, p)56Mn, E=3-20 MeV; calculated σ(E), and fractional variation in σ relative to change in level densities of target and product nuclei. 56Fe(n, nX), E=9.1, 13.35, 14.06, 14.1 MeV; calculated double differential σ(E, θ). 56Fe(n, n'γ), E<20 MeV; calculated σ(E) for different excitation energies in 56Fe, and fractional variation in σ relative to change in level densities of target and product nuclei. 56Fe, 56Mn; analyzed spin distributions for levels of positive and negative parities, nuclear level densities, and cumulative number of levels, compared to data in RIPL library; analyzed sensitivity matrices connecting variations in level density (LD) at a given excitation energy to cross-section changes at a given incident energy; deduced level densities at an extended range of excitation energy, beyond the separation energy. Calculations based on Gilbert-Cameron (GC) model with parameters fitted based on ENDF/B-VIII.0, and Hartree-Fock-Bogoliubov (HFB) approach. Comparison with experimental data from EXFOR and other literature.
doi: 10.1103/PhysRevC.101.034608
2018BR05 Nucl.Data Sheets 148, 1 (2018) D.A.Brown, M.B.Chadwick, R.Capote, A.C.Kahler, A.Trkov, M.W.Herman, A.A.Sonzogni, Y.Danon, A.D.Carlson, M.Dunn, D.L.Smith, G.M.Hale, G.Arbanas, R.Arcilla, C.R.Bates, B.Beck, B.Becker, F.Brown, R.J.Casperson, J.Conlin, D.E.Cullen, M.-A.Descalle, R.Firestone, T.Gaines, K.H.Guber, A.I.Hawari, J.Holmes, T.D.Johnson, T.Kawano, B.C.Kiedrowski, A.J.Koning, S.Kopecky, L.Leal, J.P.Lestone, C.Lubitz, J.I.Marquez Damian, C.M.Mattoon, E.A.McCutchan, S.Mughabghab, P.Navratil, D.Neudecker, G.P.A.Nobre, G.Noguere, M.Paris, M.T.Pigni, A.J.Plompen, B.Pritychenko, V.G.Pronyaev, D.Roubtsov, D.Rochman, P.Romano, P.Schillebeeckx, S.Simakov, M.Sin, I.Sirakov, B.Sleaford, V.Sobes, E.S.Soukhovitskii, I.Stetcu, P.Talou, I.Thompson, S.van der Marck, L.Welser-Sherrill, D.Wiarda, M.White, J.L.Wormald, R.Q.Wright, M.Zerkle, G.Zerovnik, Y.Zhu ENDF/B-VIII.0: The 8 th Major Release of the Nuclear Reaction Data Library with CIELO-project Cross Sections, New Standards and Thermal Scattering Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 20,21,22Ne, 22,23Na, 24,25,26Mg, 26,27Al, 28,29,30,31,32Si, 31P, 32,33,34,35,36S, 35,36,37Cl, 36,37,38,39,40,41Ar, 39,40,41K, 40,41,42,43,44,45,46,47,48Ca, 45Sc, 46,47,48,49,50Ti, 49,50,51V, 50,51,52,53,54Cr, 54,55Mn, 54,55,56,57,58Fe, 58,59Co, 58,59,60,61,62,63,64Ni, 63,64,65Cu, 64,65,66,67,68,69,70Zn, 69,70,71Ga, 70,71,72,73,74,75,76Ge, 73,74,75As, 74,75,76,77,78,79,80,81,82Se, 79,80,81Br, 78,79,80,81,82,83,84,85,86Kr, 85,86,87Rb, 84,85,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,93,94,95,96,97,98,99,100Mo, 98,99Tc, 96,97,98,99,100,101,102,103,104,105,106Ru, 103,104,105Rh, 102,103,104,105,106,107,108,109,110Pd, 107,108,109,110,111,112,113,114,115,116,117,118Ag, 106,107,108,109,110,111,112,113,114,115,116Cd, 113,114,115In, 112,113,114,115,116,117,118,119,120,121,122,123,124,125,126Sn, 121,122,123,124,125,126Sb, 120,121,122,123,124,125,126,127,128,129,130,121,132Te, 127,128,129,130,131,132,133,134,135I, 123,124,125,126,127,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,131,132,133,134,135,136,137,138,139,140Ba, 138,139,140La, 136,137,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,149,150Nd, 143,144,145,146,147,148,149,151Pm, 144,145,146,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,159,160Gd, 158,159,160,161Tb, 154,155,156,157,158,159,160,161,162,163,164Dy, 165,166Ho, 162,163,164,165,166,167,168,170,170Er, 168,169,170,171Tm, 168,169,170,171,172,173,174,175,176Yb, 175,176Lu, 174,175,176,177,178,179,180,181,182Hf, 180,181,182Ta, 180,181,182,183,184,185,186W, 185,186,187Re, 184,185,186,187,188,189,190,191,192Os, 191,192,193Ir, 190,191,192,193,194,195,196,197,198Pt, 197Au, 196,197,198,199,200,201,202,203,204Hg, 203,204,205Tl, 204,205,206,207,208,209,210Pb, 209,210Bi, 208,209,210Po, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VIII.0 evaluated neutron library. Comparison with ENDF/B-VII.1 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.1, JENDL-4.0u+ and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2018.02.001
2018BR14 Phys.Rev. C 98, 024616 (2018) D.A.Brown, G.P.A.Nobre, M.W.Herman Impact of alternative transmission coefficient parametrizations on Hauser-Feshbach theory NUCLEAR REACTIONS 90Zr, 197Au(n, n), (n, n'), (n, γ), (n, X), E<9 MeV; analyzed elastic, total inelastic, capture, total σ(E) with and without the superradiance modified Hauser-Feshbach equation, using experimental data for resolved resonances, unresolved resonances, and resonances in the fast regions taken from the EXFOR library; investigated neutron transmission coefficients in different formulations: Moldauer's sum rule for resonance reactions, the SPRT method, and the Moldauer-Simonius method.
doi: 10.1103/PhysRevC.98.024616
2018CH12 Nucl.Data Sheets 148, 189 (2018) M.B.Chadwick, R.Capote, A.Trkov, M.W.Herman, D.A.Brown, G.M.Hale, A.C.Kahler, P.Talou, A.J.Plompen, P.Schillebeeckx, M.T.Pigni, L.Leal, Y.Danon, A.D.Carlson, P.Romain, B.Morillon, E.Bauge, F.-J.Hambsch, S.Kopecky, G.Giorginis, T.Kawano, J.Lestone, D.Neudecker, M.Rising, M.Paris, G.P.A.Nobre, R.Arcilla, O.Cabellos, I.Hill, E.Dupont, A.J.Koning, D.Cano-Ott, E.Mendoza, J.Balibrea, C.Paradela, I.Duran, J.Qian, Z.Ge, T.Liu, L.Hanlin, X.Ruan, W.Haicheng, M.Sin, G.Noguere, D.Bernard, R.Jacqmin, O.Bouland, C.De Saint Jean, V.G.Pronyaev, A.V.Ignatyuk, K.Yokoyama, M.Ishikawa, T.Fukahori, N.Iwamoto, O.Iwamoto, S.Kunieda, C.R.Lubitz, M.Salvatores, G.Palmiotti, I.Kodeli, B.Kiedrowski, D.Roubtsov, I.Thompson, S.Quaglioni, H.I.Kim, Y.O.Lee, U.Fischer, S.Simakov, M.Dunn, K.Guber, J.I.Marquez Damian, F.Cantargi, I.Sirakov, N.Otuka, A.Daskalakis, B.J.McDermott, S.C.van der Marck CIELO Collaboration Summary Results: International Evaluations of Neutron Reactions on Uranium, Plutonium, Iron, Oxygen and Hydrogen NUCLEAR REACTIONS 1H, 16O, 56Fe, 235,238U, 239Pu(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.003
2018GA09 Phys.Rev. C 97, 034629 (2018) L.R.Gasques, A.S.Freitas, L.C.Chamon, J.R.B.Oliveira, N.H.Medina, V.Scarduelli, E.S.Rossi, M.A.G.Alvarez, V.A.B.Zagatto, J.Lubian, G.P.A.Nobre, I.Padron, B.V.Carlson Elastic, inelastic, and 1n transfer cross sections for the 10B+ 120Sn reaction NUCLEAR REACTIONS 120Sn(10B, 10B), (10B, 10B'), (10B, 11B), E=37.5 MeV; measured reaction products, particle spectra, σ(θ) for elastic and inelastic scattering using the Silicon Array and Telescopes of Usp for Reactions and Nuclear applications (SATURN) system at the Pelletron accelerator of University of Sao Paulo; analyzed data for σ(θ) using the coupled reaction channel (CRC) and one-step DWBA formalisms. 120Sn; deduced excitation of first 2+ and 3- levels, B(E2), B(E3), and deformation lengths. 10B; deduced excitation of 1+ level, B(E2), deformation length. 119Sn; deduced levels, σ, spectroscopic factors, CRC and DWBA analysis.
doi: 10.1103/PhysRevC.97.034629
2018HE06 Nucl.Data Sheets 148, 214 (2018) M.Herman, A.Trkov, R.Capote, G.P.A.Nobre, D.A.Brown, R.Arcilla, Y.Danon, A.Plompen, S.F.Mughabghab, Q.Jing, G.Zhigang, L.Tingjin, L.Hanlin, R.Xichao, L.Leal, B.V.Carlson, T.Kawano, M.Sin, S.P.Simakov, K.Guber Evaluation of Neutron Reactions on Iron Isotopes for CIELO and ENDF/B-VIII.0 NUCLEAR REACTIONS 56Fe(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.004
2015BR02 J.Phys.(London) G42, 034020 (2015) D.A.Brown, M.Herman, S.Hoblit, E.A.McCutchan, G.P.A.Nobre, B.Pritychenko, A.A.Sonzogni Uncertainty quantification in the Nuclear Data Program NUCLEAR REACTIONS 96Mo, 100Ru, 104Pd, 110Cd, 116Sn, 122,123,124Te, 128,130Xe, 134,136Ba, 142Nd, 148,150Sm, 154Gd, 160Dy, 176Hf, 198Hg, 204Pb(n, γ), E=30 keV; calculated Maxwellian-averaged σ and their uncertainties. ENDF/B-VII.1 evaluated library covariances, s-process.
doi: 10.1088/0954-3899/42/3/034020
2015CH19 J.Phys.(London) G42, 055102 (2015) L.C.Chamon, L.R.Gasques, G.P.A.Nobre, E.S.Rossi, Jr, R.J.de Boer, C.Seymour, M.Wiescher, G.G.Kiss Evidence of a slight nuclear transparency in the alpha-nucleus systems NUCLEAR REACTIONS 120,130Te(α, α'), E<15 MeV; calculated inelastic σ(θ). EMPIRE nuclear model code, comparison with available data.
doi: 10.1088/0954-3899/42/5/055102
2015NO01 Phys.Rev. C 91, 024618 (2015) G.P.A.Nobre, A.Palumbo, M.Herman, D.Brown, S.Hoblit, F.S.Dietrich Derivation of an optical potential for statically deformed rare-earth nuclei from a global spherical potential NUCLEAR REACTIONS 165Ho, 182,184,186W(n, X), E=0.003-200 MeV; calculated total σ(E). 158,160Gd(n, n), (n, n'), E=2.5, 4.1 MeV; Gd(n, n), E=0.334-0.919 MeV; Gd(n, n'), E=4.51-8.41 MeV; 165Ho(n, n), E=0.350, 0.60, 0.79, 0.93 MeV; 165Ho(n, n'), E=1.20, 4.51, 9.99, 11 MeV; 182,184W(n, n), (n, n')E=1.5-6.0 MeV; calculated σ(θ, E). Coupled-channel calculations with optical potential for statically deformed rare-earth nuclei using rotational excited states of the g.s. band. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.024618
2014NO04 Nucl.Data Sheets 118, 224 (2014) G.P.A.Nobre, M.Herman, S.Hoblit, A.Palumbo, R.Capote, A.Trkov Fitting Prompt Fission Neutron Spectra Using Kalman Filter Integrated with Empire Code NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated prompt fission neutron spectra using Los Alamos and Kornilov models incorporated in EMPIRE code; deduced parameters. Compared with data and one model to the other.
doi: 10.1016/j.nds.2014.04.041
2014NO06 Nucl.Data Sheets 118, 266 (2014) G.P.A.Nobre, A.Palumbo, D.Brown, M.Herman, S.Hoblit, F.S.Dietrich Towards a Coupled-channel Optical Potential for Rare-earth Nuclei NUCLEAR REACTIONS 152Sm, 156Gd, 162,166Dy, 180Hf(n, x), E=0.002-20 MeV;184W(n, x), E=0.05-20 MeV; calculated total σ. 184W(n, γ), E=0.003-40 MeV; calculated σ. 184W(n, n), E=1.5-6.0 MeV;184W(n, n'), E=1.5-3.5 MeV;calculated σ(θ) using optical model, coupled channels with quadrupole- and hexadecupole deformed potential and other corrections. Compared to EXFOR data.
doi: 10.1016/j.nds.2014.04.054
2014PA47 Nucl.Data Sheets 118, 596 (2014) G.Palmiotti, M.Salvatores, G.Aliberti, M.Herman, S.D.Hoblit, R.D.McKnight, P.Oblozinsky, P.Talou, G.M.Hale, H.Hiruta, T.Kawano, C.M.Mattoon, G.P.A.Nobre, A.Palumbo, M.Pigni, M.E.Rising, W.-S.Yang, A.C.Kahler Combined Use of Integral Experiments and Covariance Data
doi: 10.1016/j.nds.2014.04.145
2014ZA12 Nucl.Instrum.Methods Phys.Res. A 749, 19 (2014) V.A.B.Zagatto, J.R.B.Oliveira, P.R.P.Allegro, L.C.Chamon, E.W.Cybulska, N.H.Medina, R.V.Ribas, W.A.Seale, C.P.Silva, L.R.Gasques, G.S.Zahn, F.A.Genezini, J.M.B.Shorto, J.Lubian, R.Linares, D.L.Toufen, M.A.G.Silveira, E.S.Rossi Jr, G.P.Nobre γ-Particle coincidence technique for the study of nuclear reactions NUCLEAR REACTIONS 110Pd(18O, 18O'), E=53.6 MeV; measured products, 110Pd; deduced σ(θ). Data were imported from EXFOR entry D0739.
doi: 10.1016/j.nima.2014.02.014
2013BO19 Comput.Phys.Commun. 184, 085101 (2013) S.Bogner, A.Bulgac, J.Carlson, J.Engel, G.Fann, R.J.Furnstahl, S.Gandolfi, G.Hagen, M.Horoi, C.Johnson, M.Kortelainen, E.Lusk, P.Maris, H.Nam, P.Navratil, W.Nazarewicz, E.Ng, G.P.A.Nobre, E.Ormand, T.Papenbrock, J.Pei, S.C.Pieper, S.Quaglioni, K.J.Roche, J.Sarich, N.Schunck, M.Sosonkina, J.Terasaki, I.Thompson, J.P.Vary, S.M.Wild Computational nuclear quantum many-body problem: The UNEDF project NUCLEAR REACTIONS 3He(d, p), 7Be(p, γ), E<1MeV; 172Yb, 188Os, 238U(γ, X), E<24 MeV; calculated σ. Comparison with experimental data. NUCLEAR STRUCTURE 100Zr; calculated quadrupole deformation parameter, radii, neutron separation energy.
doi: 10.1016/j.cpc.2013.05.020
2011CH57 Nucl.Data Sheets 112, 2887 (2011) M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2011.11.002
2011NO17 Phys.Rev. C 84, 064609 (2011) G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel Toward a microscopic reaction description based on energy-density-functional structure models NUCLEAR REACTIONS 90Zr(n, X), E=10, 20, 30 MeV; 58Ni(n, X), E=20, 30 MeV; 58Ni(p, X), E=10-70 MeV; 48Ca(p, X), E=10-50 MeV; 40,48Ca, 58Ni, 144Sm(n, X), (p, X), E=30 MeV; 90Zr(p, X), E=20-70 MeV; calculated reaction cross section. 90Zr(p, p), E=40, 65 MeV; calculated σ(θ). Random-phase, Hartree-Fock-Bogoliubov (HFB) framework and Skyrme density functional with coupling to all RPA and QRPA inelastic channels including deuteron formation. Assessed effects of couplings between inelastic resonances from higher-order channels. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064609
2011NO18 J.Phys.:Conf.Ser. 312, 082033 (2011) G.P.A.Nobre, I.J.Thompson, J.E.Escher, F.S.Dietrich Reaction cross-section predictions for nucleon induced reactions NUCLEAR REACTIONS 58Ni(n, X), E=20, 30 MeV;90Zr(n, X), E=10, 20, 40 MeV;144Sm(n, X), E=30 MeV;40,48Ca, 58Ni(p, X), E=10, 20, 30, 40 MeV;90Zr(p, X), E=10, 20, 30, 40, 50, 60, 70 MeV;144Sm(p, X), E=30 MeV; calculated reaction σ using optical model with QRPA target excitations and coupling to inelastic and transfer channels. Proton reactions compared to data.
doi: 10.1088/1742-6596/312/4/082033
2010NO06 Phys.Rev.Lett. 105, 202502 (2010) G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel Coupled-Channel Calculation of Nonelastic Cross Sections Using a Density-Functional Structure Model NUCLEAR REACTIONS 40,48Ca, 58Ni, 90Zr, 144Sm(p, X), (n, X), E<40 MeV; calculated total reaction σ. Complete microscopic calculation, comparison with experimental data.
doi: 10.1103/PhysRevLett.105.202502
2009CH01 J.Phys.(London) G36, 025102 (2009) L.C.Chamon, G.P.A.Nobre, B.V.Carlson Effect on the heavy-ion fusion and elastic scattering cross sections of common approximations assumed in coupled-channel calculations
doi: 10.1088/0954-3899/36/2/025102
2009PE14 Nucl.Phys. A826, 211 (2009) D.Pereira, C.P.Silva, J.Lubian, E.S.Rossi, L.C.Chamon, G.P.A.Nobre, T.Correa Understanding fusion suppression and enhancement in the 18O + 58, 60, 64Ni systems NUCLEAR REACTIONS 58,60,64Ni(18O, 18O), (18O, 18O'), (18O, 16O), E=34.5-65 MeV; analyzed σ(θ), σ, fusion σ, B(E2) using coupled-channels analysis; deduced spectroscopic factors. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.06.015
2007NO06 Nucl.Phys. A786, 90 (2007) G.P.A.Nobre, L.C.Chamon, B.V.Carlson, I.J.Thompson, L.R.Gasques Tunneling through a parabolic barrier coupled to an oscillatory degree of freedom: Application to heavy-ion fusion at sub-barrier energies NUCLEAR REACTIONS 58,64Ni(58Ni, X), (64Ni, X), E(cm)=85-115 MeV; calculated fusion excitation functions.
doi: 10.1016/j.nuclphysa.2007.02.005
2007NO08 Phys.Rev. C 75, 044606 (2007) G.P.A.Nobre, L.C.Chamon, L.R.Gasques, B.V.Carlson, I.J.Thompson Consistent analysis of fusion data without adjustable parameters for a wide variety of heavy-ion systems NUCLEAR REACTIONS 12C, 92Zr, 208Pb(12C, X), 16O, 144,148,152,154Sm, 182,186W, 208Pb, 238U(16O, X), 208Pb(18O, X), 68Zn, 92Zr, 100Mo, 144Sm, 208Pb(28Si, X), 92,94,98,100Mo, 104Ru, 108,110Pd, 182W, 208Pb(32S, X), 90,98Zr, 92,100Mo, 104Ru, 108,110Pd(36S, X), 112,122Sn, 144,148,154Sm(40Ar, X), 40,48Ca, 48Ti, 90,98Zr, 192Os, 194Pt(40Ca, X), 90,98Zr(48Ca, X), 58,64Ni, 74Ge, 112,124Sn(58Ni, X), 64Ni, 74Ge, 100Mo(64Ni, X), 70,76Ge, 92Mo, 104Ru(86Kr, X), 90,96Zr(90Zr, X), E ≈ barrier; calculated fusion σ. Sao Paolo potential, comparison with data.
doi: 10.1103/PhysRevC.75.044606
2007NO12 Phys.Rev. C 76, 024605 (2007) G.P.A.Nobre, C.P.Silva, L.C.Chamon, B.V.Carlson Consistent analysis of fusion data without adjustable parameters for systems involving odd nuclei NUCLEAR STRUCTURE Li, Be, B, N, O, F, Al, s, Cl, Sc, Ti, V, Co, Ni, Cu, Ge, Y, Zr, Nb, Ru, Rh, Pd, Sn, Sm, Tb, Ho, Pb, Bi, Th; calculated deformation parameters. NUCLEAR REACTIONS 14N, 159Tb, 232Th(11B, X), E not given; 159Tb(10B, X), E not given; 59Co, 209Bi(16O, X), E not given; 144Sm(17O, X), E not given; 65Cu(18O, X), E not given; 70,73,74,76Ge(27Al, X), E not given; 59Co(14N, X), E not given; 209Bi(15N, X), E not given; 208Pb, 232Th(19F, X), E not given; 93Nb, 101Ru, 103Rh, 105Pd(32S, X), (36S, X), E not given; 27Al, 58,60,62,64Ni, 59Co, 92Zr, 112Sn(35Cl, X), E not given; 58,60,62,64Ni(37Cl, X), E not given; calculated fusion cross sections.
doi: 10.1103/PhysRevC.76.024605
2007NO14 Phys.Rev. C 76, 044608 (2007) Comparison between the zero point motion and generalized frozen approximation models in accounting for heavy-ion fusion data NUCLEAR REACTIONS 208Pb, 238U(16O, X), 182W, 208Pb(32S, X), 96Zr, 192Os, 194Pt(40Ca, X), 148,154Sm(40Ar, X), 74Ge(58Ni, X), 64Ni, 100Mo(64Ni, X), E=not given; calculated cross sections, comparisons with experimental values.
doi: 10.1103/PhysRevC.76.044608
2006PE26 Phys.Rev. C 74, 034608 (2006) D.Pereira, E.S.Rossi, Jr., G.P.A.Nobre, L.C.Chamon, C.P.Silva, L.R.Gasques, M.A.G.Alvarez, R.V.Ribas, J.R.B.Oliveira, N.H.Medina, M.N.Rao, E.W.Cybulska, W.A.Seale, N.Carlin, P.R.S.Gomes, J.Lubian, R.M.Anjos 18O+110Pd: Measurements and realistic coupled-channel analysis in a transitional region NUCLEAR REACTIONS 110Pd(18O, 18O'), (18O, 16O), (18O, 14C), E=40-58 MeV; measured Eγ, Iγ, (particle)γ-coin; deduced excitation functions. Coupled-channels analysis.
doi: 10.1103/PhysRevC.74.034608
2005AL03 Nucl.Phys. A748, 59 (2005) J.J.S.Alves, P.R.S.Gomes, J.Lubian, L.C.Chamon, D.Pereira, R.M.Anjos, E.S.Rossi, Jr., C.P.Silva, M.A.G.Alvarez, G.P.A.Nobre, L.R.Gasques Consistent analysis of peripheral reaction channels and fusion for the 16, 18O + 58Ni systems NUCLEAR REACTIONS 58Ni(16O, 16O), (16O, 16O'), (16O, 12C), E=46 MeV; 58Ni(18O, 18O), (18O, 18O'), (18O, 17O), (18O, 16O), E=46 MeV; measured elastic, inelastic, and transfer σ(E, θ). Coupled-channels analysis, comparison with previous results.
doi: 10.1016/j.nuclphysa.2004.10.020
2005AL45 Braz.J.Phys. 35, 909 (2005) J.J.S.Alves, P.R.S.Gomes, J.Lubian, L.C.Chamon, R.M.Anjos, D.Pereira, E.S.Rossi, Jr., C.P.Silva, M.A.G.Alvarez, G.P.A.Nobre, L.R.Gasques Elastic, Inelastic Scatterings and Transfer Reactions for 16, 18O on 58Ni Described by the Sao Paulo Potential NUCLEAR REACTIONS 58Ni(16O, 16O), (16O, 16O'), (16O, X), (18O, 18O), (18O, 18O'), (18O, X), E=46 MeV; measured elastic, inelastic, and transfer σ(θ). Comparison with model predictions.
doi: 10.1590/S0103-97332005000500052
2005CH74 Braz.J.Phys. 35, 906 (2005) L.C.Chamon, G.P.A.Nobre, D.Pereira, C.P.Silva, E.S.Rossi, Jr., L.R.Gasques, B.V.Carlson Coulomb and Nuclear Potentials Between Deformed Nuclei Applied to the Fusion Process NUCLEAR REACTIONS 64Ni(64Ni, X), E(cm)=85-110 MeV; calculated fusion σ. Coulomb and nuclear interactions, barrier penetration model. Comparison with data.
doi: 10.1590/S0103-97332005000500051
2004CH36 Phys.Rev. C 70, 014604 (2004) L.C.Chamon, G.P.A.Nobre, D.Pereira, E.S.Rossi, Jr., C.P.Silva, L.R.Gasques, B.V.Carlson Coulomb and nuclear potentials between deformed nuclei NUCLEAR STRUCTURE Z=0-100; compiled, analyzed quadrupole and octupole deformation lengths. NUCLEAR REACTIONS 58Ni(58Ni, X), E not given; calculated Coulomb and nuclear potentials, deformation and orientation dependence.
doi: 10.1103/PhysRevC.70.014604
2003GA18 Phys.Rev. C 67, 067603 (2003) L.R.Gasques, L.C.Chamon, D.Pereira, M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, G.P.A.Nobre, B.V.Carlson Systematical study of the optical potential for systems like A+58Ni from sub-barrier data analyses NUCLEAR REACTIONS 58Ni(28Si, 28Si), E=74, 75.5, 77 MeV; measured σ(θ); deduced optical model parameters. 28Si deduced density distribution. NUCLEAR STRUCTURE 4,6He, 12C, 16,18O, 28Si; analyzed scattering data; deduced radii, density distributions.
doi: 10.1103/PhysRevC.67.067603
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