NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Herman Found 120 matches. Showing 1 to 100. [Next]2023LE13 Eur.Phys.J. N 9, 34 (2023) A.M.Lewis, A.D.Carlson, D.L.Smith, D.P.Barry, R.C.Block, S.Croft, Y.Danon, M.Drosg, M.W.Herman, D.Neudecker, N.Otuka, H .Sjostrand, V.Sobes Templates of expected measurement uncertainties for total neutron cross-section observables
doi: 10.1051/epjn/2023018
2023LE14 Eur.Phys.J. N 9, 33 (2023) A.M.Lewis, D.Neudecker, A.D.Carlson, D.L.Smith, I.Thompson, A.Wallner, D.P.Barry, L.A.Bernstein, R.C.Block, S.Croft, Y.Danon, M.Drosg, R.C.Haight, M.W.Herman, H.Y.Lee, N.Otuka, H.Sjostrand, V.Sobes Templates of expected measurement uncertainties for neutron-induced capture and charged-particle production cross section observables
doi: 10.1051/epjn/2023015
2023MU06 Phys.Rev. C 107, 034606 (2023) M.R.Mumpower, D.Neudecker, H.Sasaki, T.Kawano, A.E.Lovell, M.W.Herman, I.Stetcu, M.Dupuis Collective enhancement in the exciton model NUCLEAR REACTIONS 239Pu(n, 2n), E=6-24 MeV; calculated σ(E). 239Pu(n, xn), E=14 MeV; 181Ta, 165(n, xn), E=20 MeV; calculated neutron emission spectra. Calculation with statistical model framework CoH3 with increased one-particle-one-hole state density used in the exciton model. Comparison to experimental data and ENDF/B-VIII.0. NUCLEAR STRUCTURE 239Pu; calculated 1p-1h state densities.
doi: 10.1103/PhysRevC.107.034606
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
2023VA11 Eur.Phys.J. N 9, 31 (2023) J.R.Vanhoy, R.C.Haight, S.F.Hicks, M.Devlin, D.Neudecker, M.Herman, A.Koning, K.J.Kelly, I.Thompson Templates of expected measurement uncertainties for (n, xn) cross sections NUCLEAR REACTIONS 56Fe, 23Na(n, n'), 9Be(n, X), E=3.5, 6 MeV; analyzed available data; deduced a template for evaluating experimental uncertainties for neutron elastic and inelastic scattering σ and γ-ray production σ from (n, xn) measurements at laboratories with monoenergetic or white neutron sources.
doi: 10.1051/epjn/2023019
2022KU12 Phys.Rev. C 105, 044608 (2022) S.A.Kuvin, H.Y.Lee, B.DiGiovine, C.Eiroa-Lledo, A.Georgiadou, M.Herman, T.Kawano, V.Mocko, S.Mosby, C.Vermeulen, D.Votaw, M.White, L.Zavorka, G.Perdikakis, P.Tsintari, H.I.Kim Direct measurement of 59Ni(n, p) 59Co and 59Ni(n, α)56Fe at fast-neutron energies from 500 keV to 10 MeV NUCLEAR REACTIONS 59Ni(n, p), (n, α), E=0.5-10 MeV; measured Ep, Ip, Eα, Iα, neutron time of flight, np-coin, nα-coin; deduced Q, inclusive and exclusive σ(E). Comparison to statistical Hauser-Feschbach calculations (TALYS, CoH3), evaluated data (ENDF/B-VIII.0, JEFF-3.3, JENDL-4.0) and other experimental results. Low Energy (n, z) (LENZ) setup consisting of annular double-sided silicon strip detectors at the WNR facility at the Los Alamos Neutron Science Center (LANSCE).
doi: 10.1103/PhysRevC.105.044608
2021HE28 Ann.Nucl.Energy 163, 108494 (2021) M.Herman, D.A.Brown, R.Capote, M.B.Chadwick, W.Haeck, J.D.Hutchinson, T.Kawano, D.Neudecker, G.Palmiotti, M.Salvatores, P.Talou, A.Trkov, M.C.White Infrastructure for the new paradigm of nuclear reaction evaluation NUCLEAR REACTIONS 105Pd(n, γ), 235U, 239Pu(n, F), E<20 MeV; analyzed available data; deduced pilot assimilation project needs.
doi: 10.1016/j.anucene.2021.108494
2021NE06 Phys.Rev. C 104, 034611 (2021) D.Neudecker, O.Cabellos, A.R.Clark, M.J.Grosskopf, W.Haeck, M.W.Herman, J.Hutchinson, T.Kawano, A.E.Lovell, I.Stetcu, P.Talou, S.Vander Wiel Informing nuclear physics via machine learning methods with differential and integral experiments NUCLEAR REACTIONS 238U(n, n'), E=14 MeV; analyzed pulsed-sphere neutron-leakage experimental spectrum obtained at LLNL facility, and compared with evaluated data in ENDF/B-VIII.0. 241Pu(n, F), E=0.1-1.0, 14 MeV; analyzed differential and integral experimental data for fission σ(E) by combining experimental σ data, nuclear-physics theory and neutron-transport simulations of the experiments using machine learning (ML) random forest algorithm and expert judgment. Relevance to improvement of description of nuclear-physics observables in particular application areas.
doi: 10.1103/PhysRevC.104.034611
2021SI16 Phys.Rev. C 103, 054605 (2021) M.Sin, R.Capote, M.W.Herman, A.Trkov, B.V.Carlson Modeling photon-induced reactions on 233-238U actinide targets NUCLEAR REACTIONS 233,234,235,236,237,238U(γ, X), (γ, γ), (γ, F), (γ, n), (γ, 2n), (γ, 3n), E=3-30 MeV; calculated photoreaction total, photoabsorption, fission, elastic and (γ, xn) σ(E) using the EMPIRE-3.2 code and compared with the available experimental data in the EXFOR library, and with the evaluated data from JENDL/PD-2016 and IAEA-Photonuclear Data Library 1999 (IAEA-PD); deduced set of giant dipole resonances (GDR) parameters consistent with all the available experimental data. Discussed differences and the similarities between the models and parameters used in calculations of photon- and neutron-induced reactions on the same nuclei, with focus on fission process.
doi: 10.1103/PhysRevC.103.054605
2020KI03 Nucl.Instrum.Methods Phys.Res. A963, 163699(2020) H.I.Kim, H.Y.Lee, T.Kawano, A.Georgiadou, S.A.Kuvin, L.Zavorka, M.W.Herman New evaluation on angular distributions and energy spectra for neutron-induced charged-particle measurements
doi: 10.1016/j.nima.2020.163699
2020NE07 Nucl.Data Sheets 167, 36 (2020) D.Neudecker, M.Grosskopf, M.Herman, W.Haeck, P.Grechanuk, S.Vander Wiel, M.E.Rising, A.C.Kahler, N.Sly, P.Talou Enhancing nuclear data validation analysis by using machine learning
doi: 10.1016/j.nds.2020.07.002
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
2018CA08 Nucl.Data Sheets 148, 254 (2018) R.Capote, A.Trkov, M.Sin, M.T.Pigni, V.G.Pronyaev, J.Balibrea, D.Bernard, D.Cano-Ott, Y.Danon, A.Daskalakis, T.Goricanec, M.W.Herman, B.Kiedrowski, S.Kopecky, E.Mendoza, D.Neudecker, L.Leal, G.Noguere, P.Schillebeeckx, I.Sirakov, E.S.Soukhovitskii, I.Stetcu, P.Talou IAEA CIELO Evaluation of Neutron-induced Reactions on 235U and 238U Targets NUCLEAR REACTIONS 235,238U(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.005
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
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
2017SI01 Nucl.Data Sheets 139, 138 (2017) M.Sin, R.Capote, M.W.Herman, A.Trkov Modelling Neutron-induced Reactions on 232-237U from 10 keV up to 30 MeV NUCLEAR REACTIONS 232,233,234,235,236,237U(n, X), E=0.01-30 MeV; calculated σ using EMPIRE nuclear model code and RIPL library. Comparison with available data.
doi: 10.1016/j.nds.2017.01.003
2016SI08 Phys.Rev. C 93, 034605 (2016) M.Sin, R.Capote, M.W.Herman, A.Trkov Extended optical model for fission NUCLEAR REACTIONS 238U, 239Pu(n, F), E=0.001-7 MeV; calculated fission σ(E) considering partial and full damping for class-II vibrational states. 234,235U(n, F), E=0.001-7 MeV; calculated fission σ(E) considering full damping for class-II vibrational states, and different degrees of damping for class-III vibrational states associated with partial absorption for discrete and continuum fission channel spectrum, partial absorption for discrete and full absorption for continuum fission channel spectrum, and total absorption for discrete and continuum fission channel spectrum. Comparison with Neutron Standards least-squares fit of available experimental data from EXFOR database. Extension of the optical model for fission. Relevance to CIELO and CHANDA international collaborative projects for evaluated reaction libraries.
doi: 10.1103/PhysRevC.93.034605
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
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
2014AR07 Nucl.Data Sheets 118, 422 (2014) Continuous Integration and Deployment Software to Automate Nuclear Data Verification and Validation
doi: 10.1016/j.nds.2014.04.096
2014BR09 Nucl.Data Sheets 118, 144 (2014) D.A.Brown, R.Arcilla, R.Capote, S.F.Mughabghab, M.W.Herman, A.Trkov, H.I.Kim Zirconium Evaluations for ENDF/B-VII.2 for the Fast Region COMPILATION 90,91,92,93,94,95,96Zr(n, x), E=0=20 MeV; calculated, evaluated σ, σ(θ) including resonance region using EMPIRE-3.1 code. Compared with available data and evaluated databases.
doi: 10.1016/j.nds.2014.04.021
2014CA15 Nucl.Data Sheets 118, 26 (2014) R.Capote, A.Trkov, M.Sin, M.Herman, A.Daskalakis, Y.Danon Physics of Neutron Interactions with 238U: New Developments and Challenges NUCLEAR REACTIONS 238U(n, x), E=0.01-20 MeV; calculated σ to different discrete states and to continuum. 238U(n, n), E=0-3.5 MeV; calculated average scattering angle. 238U(n, n), E=650 keV; calculated σ(θ). EMPIRE code; calculations compared to data and some reactions also to evaluated libraries.
doi: 10.1016/j.nds.2014.04.003
2014CA18 Nucl.Data Sheets 118, 276 (2014) B.V.Carlson, L.Brito, D.F.Mega, R.Capote, M.Herman, M.E.Rego Exclusive Multiple Emission Cross Sections in the Hybrid Monte Carlo Pre-equilibrium Model and in EMPIRE-3.1 NUCLEAR REACTIONS 59Co(p, 2n), (p, 3n), E=50, 100, 200 MeV; calculated exclusive neutron σ(En) using hybrid Monte Carlo simulation model; discussed implementation to EMPIRE-3.1.
doi: 10.1016/j.nds.2014.04.057
2014CH24 Nucl.Data Sheets 118, 1 (2014) M.B.Chadwick, E.Dupont, E.Bauge, A.Blokhin, O.Bouland, D.A.Brown, R.Capote, A.Carlson, Y.Danon, C.De Saint Jean, M.Dunn, U.Fischer, R.A.Forrest, S.C.Frankle, T.Fukahori, Z.Ge, S.M.Grimes, G.M.Hale, M.Herman, A.Ignatyuk, M.Ishikawa, N.Iwamoto, O.Iwamoto, M.Jandel, R.Jacqmin, T.Kawano, S.Kunieda, A.Kahler, B.Kiedrowski, I.Kodeli, A.J.Koning, L.Leal, Y.O.Lee, J.P.Lestone, C.Lubitz, M.MacInnes, D.McNabb, R.McKnight, M.Moxon, S.Mughabghab, G.Noguere, G.Palmiotti, A.Plompen, B.Pritychenko, V.Pronyaev, D.Rochman, P.Romain, D.Roubtsov, P.Schillebeeckx, M.Salvatores, S.Simakov, E.Sh.Soukhovitskii, J.C.Sublet, P.Talou, I.Thompson, A.Trkov, R.Vogt, S.van der Marck The CIELO Collaboration: Neutron Reactions on 1H, 16O, 56Fe, 235, 238U, and 239Pu COMPILATION 1H, 16O, 56Fe, 235,238U, 239Pu(n, x), E≈0-20 MeV; analyzed available data on σ, neutron multiplicity, criticality using ENDF/B-VII.1, JENDL-4.0, JEFF-3.1, ROSFOND 2010, CENDL-3.1, EAF-2010 evaluated nuclear libraries, Atlas of Neutron Resonances, Neutron Cross Section Standards evaluations; deduced recommendations for CIELO library, parameters, Maxwellian-averaged, thermal, californium σ, Westcott factors, resonance integrals. Compared with available data.
doi: 10.1016/j.nds.2014.04.002
2014DU08 Nucl.Data Sheets 120, 264 (2014) E.Dupont, M.B.Chadwick, Y.Danon, C.De Saint Jean, M.Dunn, U.Fischer, R.A.Forrest, T.Fukahori, Z.Ge, H.Harada, M.Herman, M.Igashira, A.Ignatyuk, M.Ishikawa, O.Iwamoto, R.Jacqmin, A.C.Kahler, T.Kawano, A.J.Koning, L.Leal, Y.O.Lee, R.McKnight, D.McNabb, R.W.Mills, G.Palmiotti, A.Plompen, M.Salvatores, P.Schillebeeckx Working Party on International Nuclear Data Evaluation Cooperation (WPEC)
doi: 10.1016/j.nds.2014.07.063
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
2014OT01 Nucl.Data Sheets 120, 272 (2014) N.Otuka, E.Dupont, V.Semkova, B.Pritychenko, A.I.Blokhin, M.Aikawa, S.Babykina, M.Bossant, G.Chen, S.Dunaeva, R.A.Forrest, T.Fukahori, N.Furutachi, S.Ganesan, Z.Ge, O.O.Gritzay, M.Herman, S.Hlavac, K.Kato, B.Lalremruata, Y.O.Lee, A.Makinaga, K.Matsumoto, M.Mikhaylyukova, G.Pikulina, V.G.Pronyaev, A.Saxena, O.Schwerer, S.P.Simakov, N.Soppera, R.Suzuki, S.Takacs, X.Tao, S.Taova, F.Tarkanyi, V.V.Varlamov, J.Wang, S.C.Yang, V.Zerkin, Y.Zhuang Towards a More Complete and Accurate Experimental Nuclear Reaction Data Library (EXFOR): International Collaboration Between Nuclear Reaction Data Centres (NRDC)
doi: 10.1016/j.nds.2014.07.065
2014PA33 Nucl.Data Sheets 120, 180 (2014) EMPIRE: A Reaction Model Code for Nuclear Astrophysics NUCLEAR REACTIONS 232Th(n, F), 132Ba, 92Mo, 120Te(α, n), E<20 MeV; 64,70Zn(n, γ), E<100 keV; 102Pd(p, γ), E<6 MeV. calculated σ, S-factors using EMPIRE nuclear model code.
doi: 10.1016/j.nds.2014.07.040
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
2014SA35 Nucl.Data Sheets 118, 38 (2014) M.Salvatores, G.Palmiotti, G.Aliberti, P.Archier, C.De Saint Jean, E.Dupont, M.Herman, M.Ishikawa, T.Ivanova, E.Ivanov, S.-J.Kim, I.Kodeli, G.Manturov, R.McKnight, S.Pelloni, C.Perfetti, A.J.M.Plompen, B.T.Rearden, D.Rochman, K.Sugino, A.Trkov, W.Wang, H.Wu, W.-S.Yang Methods and Issues for the Combined Use of Integral Experiments and Covariance Data: Results of a NEA International Collaborative Study NUCLEAR REACTIONS 238U(n, n'), E=100 eV-10 MeV;239,241Pu(n, F), E=100 eV-10 MeV; calculated relative σ uncertaintites. 239Pu(n, γ), E=100 ev-10 MeV; calculated parameters uncertainty.
doi: 10.1016/j.nds.2014.04.005
2012PR16 Nucl.Phys.News 22, 23 (2012) National Nuclear Data Center: A Worldwide User Facility 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: 10.1080/10619127.2012.683724
2011CH46 J.Korean Phys.Soc. 59, 847s (2011) Y.-S.Cho, P.Oblozinsky, S.F.Mughabghab, C.M.Mattoon, M.Herman Practical Method for Estimating Neutron Cross Section Covariances in the Resonance Region NUCLEAR REACTIONS 55Mn(n, n), (n, γ), E=1-300000 eV; evaluated σ, uncertainties, covariances.
doi: 10.3938/jkps.59.847
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
2011HE16 J.Korean Phys.Soc. 59, 1028s (2011) M.Herman, J.Katakura, A.J.Koning, C.Nordborg International Cooperation in Nuclear Data Evaluation
doi: 10.3938/jkps.59.1028
2011HE17 J.Korean Phys.Soc. 59, 1034s (2011) Development of ENDF/B-VII.1 and its covariance component COMPILATION 1,3H, 9Be, 19F, 22Na, 27Al, 35,37Cl, 39,41K, 45Sc, 46,47,49,50Ti, 52,53Cr, 55Mn, 58,60Ni, 74,75As, 78Kr, 87Rb, 89Y, 90,96Zr, 97Mo, 113Cd, 123,124Xe, 180,182,183,184,186W, 185,187Re, 233,235,236,237,238,239U, 239,240Pu, 240,241,242,242mAm; calculated, evaluated σ, covariance matrices suggested to ENDF/B-VII.1.
doi: 10.3938/jkps.59.1034
2011HO19 Nucl.Data Sheets 112, 3075 (2011) S.Hoblit, Y.-S.Cho, M.Herman, C.M.Mattoon, S.F.Mughabghab, P.Oblozinsky, M.T.Pigni, A.A.Sonzogni Neutron Cross Section Covariances for Structural Materials and Fission Products
doi: 10.1016/j.nds.2011.11.006
2011KA31 Nucl.Data Sheets 112, 2997 (2011) A.C.Kahler, R.E.MacFarlane, R.D.Mosteller, B.C.Kiedrowski, S.C.Frankle, M.B.Chadwick, R.D.McKnight, R.M.Lell, G.Palmiotti, H.Hiruta, M.Herman, R.Arcilla, S.F.Mughabghab, J.C.Sublet, A.Trkov, T.H.Trumbull, M.Dunn ENDF/B-VII.1 Neutron Cross Section Data Testing with Critical Assembly Benchmarks and Reactor Experiments
doi: 10.1016/j.nds.2011.11.003
2011PA31 J.Korean Phys.Soc. 59, 1123s (2011) G.Palmiotti, H.Hiruta, M.Salvatores, M.Herman, P.Oblozinsky, M.T.Pigni Use of Covariance Matrices in a Consistent (Multiscale) Data Assimilation for Improvement of Basic Nuclear Parameters in Nuclear Reactor Applications: from Meters to Femtometers
doi: 10.3938/jkps.59.1123
2011PA33 J.Korean Phys.Soc. 59, 1264s (2011) G.Palmiotti, M.Assawaroongruengchot, M.Salvatores, M.Herman, P.Oblozinsky, C.Mattoon, M.Pigni Nuclear Data Target Accuracies for Generation-IV Systems Based on the Use of New Covariance Data
doi: 10.3938/jkps.59.1264
2011PI01 Phys.Rev. C 83, 024601 (2011) M.T.Pigni, M.Herman, P.Oblozinsky, F.S.Dietrich Sensitivity analysis of neutron total and absorption cross sections within the optical model NUCLEAR REACTIONS 56Fe(n, X), E=0.001-200 MeV; calculated total neutron cross section and compared to experimental data ENDF/B-VII.0 evaluation, sensitivity of the total and absorption cross sections to perturbations of the potential strengths, radii, and diffuseness parameters. A=20-200; calculated fractional uncertainties for neutron total and absorption across sections on 75 target nuclei obtained for three different global spherical optical potentials (Koning-Delaroche, Walter-Guss, Becchetti-Greenlees) for E(n)=0.001-200 MeV. Comparisons with Ramsauer model for neutron energies above 4 MeV. Optical model parametrization and applicability.
doi: 10.1103/PhysRevC.83.024601
2011SI23 J.Korean Phys.Soc. 59, 1015s (2011) M.Sin, P.Oblozinsky, M.Herman, R.Capote Fission Cross section Calculations of Actinides with EMPIRE Code NUCLEAR REACTIONS 233,234,236U, 237Np, 238,239,240,241,242Pu, 241,243Am, 242,243,244,245,246Cm(n, f), E=1 keV-20 MeV;233U, 237Np, 239Pu, 240Pu(n, X), E=1 keV-20 MeV;239Pu(n, 2n), E=5-20 MeV;241Am(n, 2n), E=7-20 MeV;236U, 241Am(n, γ), E=1 keV-20 MeV;238,239,240,241Pu(γ, f), E≈5-20 MeV; calculated σ using EMPIRE code. Comparison with EXFOR data.
doi: 10.3938/jkps.59.1015
2009CA27 Nucl.Data Sheets 110, 3107 (2009) R.Capote, M.Herman, P.Oblozinsky, P.G.Young, S.Goriely, T.Belgya, A.V.Ignatyuk, A.J.Koning, S.Hilaire, V.A.Plujko, M.Avrigeanu, O.Bersillon, M.B.Chadwick, T.Fukahori, Z.Ge, Y.Han, S.Kailas, J.Kopecky, V.M.Maslov, G.Reffo, M.Sin, E.Sh.Soukhovitskii, P.Talou RIPL - Reference Input Parameter Library for Calculation of Nuclear Reactions and Nuclear Data Evaluations
doi: 10.1016/j.nds.2009.10.004
2009PI04 Nucl.Sci.Eng. 162, 25 (2009) M.T.Pigni, M.Herman, P.Oblozinsky Extensive Set of Cross-Section Covariance Estimates in the Fast Neutron Region
doi: 10.13182/NSE162-25
2008AR12 Nucl.Data Sheets 109, 2910 (2008) R.Arcilla, A.C.Kahler, P.Oblozinsky, M.Herman Processing Neutron Cross Section Covariances using NJOY-99 and PUFF-IV
doi: 10.1016/j.nds.2008.11.033
2008AV03 Nucl.Phys. A806, 15 (2008) M.Avrigeanu, S.V.Chuvaev, A.A.Filatenkov, R.A.Forrest, M.Herman, A.J.Koning, A.J.M.Plompen, F.L.Roman, V.Avrigeanu Fast-neutron induced pre-equilibrium reactions on 55Mn and 63, 65Cu at energies up to 40 MeV NUCLEAR REACTIONS 55Mn, 63,65Cu(n, X), (n, γ), E=0.001?50 MeV; 52,53,54Cr, 55Mn, 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,68Zn(p, X), (p, n), (p, γ), E=1?20 MeV; analyzed total, activation and capture σ and particle emission spectra using an optical model with emphasis on pre-equilibrium emission. Comparison with all available data.
doi: 10.1016/j.nuclphysa.2008.03.010
2008HE14 Nucl.Data Sheets 109, 2752 (2008) M.Herman, M.T.Pigni, P.Oblozinsky, S.F.Mughabghab, C.M.Mattoon, R.Capote, Y.-S.Cho, A.Trkov Development of Covariance Capabilities in EMPIRE Code NUCLEAR REACTIONS 89Y(n, 2n), E < 35 MeV; 93Nb(n, X), E < 15 MeV; analyzed cross sections.
doi: 10.1016/j.nds.2008.11.005
2008KI12 Nucl.Sci.Eng. 160, 168 (2008) H.Kim, M.Herman, S.F.Mughabghab, P.Oblozinsky, D.Rochman, Y.-O.Lee Evaluation of Neutron Cross Sections for a Complete Set of Nd Isotopes NUCLEAR REACTIONS 142,143,144,145,146,147,148,150Nd(n, X), E < 20 MeV; analyzed cross sections.
doi: 10.13182/NSE160-168
2008KI15 Nucl.Instrum.Methods Phys.Res. B266, 3513 (2008) H.Kim, M.Herman, S.F.Mughabghab, P.Oblozinsky, Y.-O.Lee Evaluation of neutron cross sections for a complete set of Dy isotopes NUCLEAR REACTIONS 156,158,160,161,162,163,164Dy(n, X), E= 10- eV - 20 MeV; analyzed neutron σ; comparison with experimental data and ENDF/B-VI.8, JEFF-3.1 data libraries; EMPIRE-2.19.
doi: 10.1016/j.nimb.2008.05.020
2008LI51 Nucl.Data Sheets 109, 2828 (2008) R.C.Little, T.Kawano, G.D.Hale, M.T.Pigni, M.Herman, P.Oblozinsky, M.L.Williams, M.E.Dunn, G.Arbanas, D.Wiarda, R.D.McKnight, J.N.McKamy, J.R.Felty Low-fidelity Covariance Project
doi: 10.1016/j.nds.2008.11.018
2008PI05 Nucl.Data Sheets 109, 2900 (2008) M.T.Pigni, M.Herman, P.Oblozinsky Estimated 55Mn and 90Zr Cross Section Covariances in the Fast Neutron Energy Region NUCLEAR REACTIONS 55Mn(n, n'), (n, 2n), (n, γ), E < 25 MeV; 90Zr(n, n'), (n, 2n), (n, X), E < 25 MeV; analyzed cross sections.
doi: 10.1016/j.nds.2008.11.031
2008RO01 Nucl.Sci.Eng. 158, 68 (2008) D.Rochman, M.Herman, S.F.Mughabghab, P.Oblozinsky New Evaluation of the 99Tc Neutron-Induced Cross Sections for the ENDF/B-VII.0 Library NUCLEAR REACTIONS 99Tc(n, γ), E=0-11 MeV; 99Tc(n, n'), (n, 2n), E=0-20 MeV; 99Tc(n, p), E=4-20 MeV; 99Tc(n, α), E=5-20 MeV; 99Tc(n, X), E=2-20 MeV; analyzed total and elastic cross sections, capture cross sections, resonance integrals, inelastic cross sections.
doi: 10.13182/NSE08-A2739
2008WI14 Phys.Rev. C 78, 064611 (2008) H.Wienke, R.Capote, M.Herman, M.Sin Deformation-dependent Tamura-Udagawa-Lenske multistep direct model NUCLEAR REACTIONS 232Th(n, xn), E=11.9 MeV; 181Ta(n, xn), E=14.1 MeV; 184W(n, xn), E=11.5 MeV; calculated and analyzed σ(θ). Tamura, Udagawa, and Lenske model.
doi: 10.1103/PhysRevC.78.064611
2007HE31 Nucl.Data Sheets 108, 2655 (2007) M.Herman, R.Capote, B.V.Carlson, P.Oblozinsky, M.Sin, A.Trkov, H.Wienke, V.Zerkin EMPIRE: Nuclear Reaction Model Code System for Data Evaluation
doi: 10.1016/j.nds.2007.11.003
2006AV01 Nucl.Phys. A765, 1 (2006) V.Avrigeanu, S.V.Chuvaev, R.Eichin, A.A.Filatenkov, R.A.Forrest, H.Freiesleben, M.Herman, A.J.Koning, K.Seidel Pre-equilibrium reactions on the stable tungsten isotopes at low energy NUCLEAR REACTIONS 180,186W(n, 2n), 182,183,184,186W(n, p), (n, α), 186W(n, n'α), E=13.4-14.9 MeV; measured Eγ, Iγ, activation σ. 181Ta(p, n), E=0-50 MeV; 180,182,183,184,186W, 181Ta(n, γ), E=0-3 MeV; analyzed σ. Comparison with model predictions.
doi: 10.1016/j.nuclphysa.2005.10.003
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
2006PR20 Ann.Nucl.Energy 33, 390 (2006) B.Pritychenko, A.A.Sonzogni, D.F.Winchell, V.V.Zerkin, R.Arcilla, T.W.Burrows, C.L.Dunford, M.W.Herman, V.McLane, P.Oblozinsky, Y.Sanborn, J.K.Tuli Nuclear reaction and structure data services of the National Nuclear Data Center
doi: 10.1016/j.anucene.2005.10.004
2006RO39 Nucl.Sci.Eng. 154, 280 (2006) D.Rochman, M.Herman, P.Oblozinsky, M.Sin Modeling and Neutron-Induced Fission Cross Sections for Americium NUCLEAR REACTIONS 239,240,241,242,242m,243,244,244mAm(n, F), E=0.1-20 MeV; calculated fission σ. Comparison with data.
doi: 10.13182/NSE06-A2633
2006SI23 Phys.Rev. C 74, 014608 (2006) M.Sin, R.Capote, A.Ventura, M.Herman, P.Oblozinsky Fission of light actinides: 232Th(n, f) and 231Pa(n, f) reactions NUCLEAR REACTIONS 232Th, 231Pa(n, F), E < 6 MeV; calculated fission σ; deduced role of vibrational states in resonant structure. Comparisons with data.
doi: 10.1103/PhysRevC.74.014608
2003RE39 Astrophys.J. 582, 1251 (2003) R.Reifarth, C.Arlandini, M.Heil, F.Kappeler, P.V.Sedyshev, A.Mengoni, M.Herman, T.Rauscher, R.Gallino, C.Travaglio Stellar Neutron Capture on Promethium: Implications for the s-Process Neutron Density NUCLEAR REACTIONS 147Pm(n, γ), E=25 keV; measured reaction products, Eγ, Iγ; deduced Maxwellian-averaged σ and its uncertainties. NUCLEAR REACTIONS 147,148,149Pm(n, γ), E=5-100 keV; calculated Maxwellian-averaged σ. COMPILATION 146,147,148Nd, 147,148,149Pm, 147,148,149,150Sm(n, γ), E=10, 25, 30 keV; compiled Maxwellian-averaged σ and its uncertainties.
doi: 10.1086/344718
2001CH67 Bull.Rus.Acad.Sci.Phys. 65, 138 (2001) T.V.Chuvilskaya, Yu.G.Seleznev, A.A.Shirokova, M.Herman Calculated Isomeric Ratios and Excitation Functions for the Reactions 107Ag(α, 2n)109m, gIn, 128, 130Te(6, 4He, n)133mgXe, and 128, 130Te(8, 6He, 3n)133mgXe NUCLEAR REACTIONS 107Ag(α, 2n), 128Te(6He, n), (8He, 3n), 130Te(α, n), (6He, 3n), E=15-31 MeV; calculated isomeric cross section ratios. Comparisons with data.
2000GI18 Bull.Rus.Acad.Sci.Phys. 64, 689 (2000) G.Giardina, P.D'Agostino, A.I.Muminov, A.K.Nasirov, G.Oliva, R.Palamara, R.Ruggeri, A.Taccone, G.Fazio, M.Herman Formation of Evaporation Residues in Synthesis of Superheavy Elements NUCLEAR REACTIONS 232Th, 238U, 244Pu(48Ca, F), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E=215-255 MeV; calculated fusion, quasi-fission, evaporation residue σ, compound nucleus fission barrier vs bombarding energy. Dinuclear system concept, comparison with data.
1999CH46 Bull.Rus.Acad.Sci.Phys. 63, 825 (1999) T.V.Chuvilskaya, Yu.G.Seleznev, A.A.Shirokova, M.Herman Yields of Isomers from the Reactions 107, 109Ag(6, 4He, n, 2n), 41K(αn), and 193Ir(αn) NUCLEAR REACTIONS 107Ag(6He, n), (6He, 2n), 109Ag(α, n), (α, 2n), E=22-29 MeV; 41K, 193Ir(α, n), E=15-27 MeV; calculated σ, isomeric cross section ratio. 193Ir(α, n), E=20-27 MeV; measured isomeric cross section ratio. Statistical model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0835. 1999GI16 Pramana 53, 409 (1999) G.Giardina, P.D'Agostino, G.Fazio, M.Herman, A.I.Muninov, A.Nasirov, G.Oliva, R.Palamara, R.Ruggeri Fusion-Fission Dynamics in the Superheavy Nucleus Production NUCLEAR REACTIONS 208Pb(64Ni, X), E=300-320 MeV; 238U, 244Pu(48Ca, X), E=220-280 MeV; calculated fusion, quasifission σ. 238U, 244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E=220-260 MeV; 208Pb(64Ni, n), E ≈ 310 MeV; calculated excitation functions. Comparisons with data.
doi: 10.1007/s12043-999-0007-x
1998DA27 Bull.Rus.Acad.Sci.Phys. 62, 1736 (1998) P.d'Agostino, G.Fazio, G.Giardina, M.Herman, A.Lamberto, G.F.Rappazzo, R.Sturiale, F.Malaguti, D.O.Eremenko, N.V.Eremin, S.Yu.Platonov, O.A.Yuminov Effect of Nuclear Deformation on Giant Dipole Resonances NUCLEAR STRUCTURE A=51-239; analyzed GDR parameters vs deformation. NUCLEAR REACTIONS 154Sm(12C, X), 27Al, 109Ag(18O, X), E not given; analyzed Eγ, Iγ; deduced GDR deformation effects.
1998SA08 J.Phys.(London) G24, 611 (1998) R.N.Sagaidak, V.I.Chepigin, A.P.Kabachenko, J.Rohac, Yu.Ts.Oganessian, A.G.Popeko, A.V.Yeremin, A.D'Arrigo, G.Fazio, G.Giardina, M.Herman, R.Ruggeri, R.Sturiale Fission-Evaporation Competition in Excited Uranium and Fermium Nuclei NUCLEAR REACTIONS, ICPND 208Pb(20Ne, xn), (22Ne, xn), E=100-160 MeV; 232Th(20Ne, xn), (22Ne, xn)245Fm/246Fm/247Fm/248Fm, E=130-150 MeV; analyzed evaporation residues production σ; deduced compound nuclei neutron evaporation mechanism features. Advanced statistical model calculations.
doi: 10.1088/0954-3899/24/3/012
1994DA04 J.Phys.(London) G20, 365 (1994) A.D'Arrigo, G.Giardina, M.Herman, A.V.Ignatyuk, A.Taccone Semi-Empirical Determination of the Shell Correction Temperature and Spin Dependence by Means of Nuclear Fisson NUCLEAR REACTIONS 210Po(p, F), E=20-61 MeV; 201Tl, 212Po, 173Lu, Ta, At(α, F), E ≈ 15-80 MeV; 206Pb(α, F), 198Pt(12C, F), 192Os(18O, F), E not given; calculated fission σ(E). At, Po, Tl(α, F), E not given; calculated fission probability vs excitation, deduced shell effects temperature, angular momentum dependence.
doi: 10.1088/0954-3899/20/2/015
1994DA28 Phys.Lett. 334B, 1 (1994) A.D'Arrigo, G.Giardina, M.Herman, M.Sacchi, A.Taccone Sensitivity of the Evaporation Residue Production to Dynamical Effects in Highly Fissile Compound Nuclei NUCLEAR REACTIONS 197Au(20Ne, X), E ≤ 152 MeV; analyzed evaporation residue σ; deduced shape evolution, nuclear dissipation dependences, nuclear viscosity. Statistical model.
doi: 10.1016/0370-2693(94)90582-7
1993MA33 Nucl.Phys. A561, 387 (1993) A.Marcinkowski, J.Rapaport, R.W.Finlay, C.Brient, M.Herman, M.B.Chadwick Neutron Emission Cross Sections at Low Bombarding Energies and the Novelty in Multistep Compound Reaction Model NUCLEAR REACTIONS 165Ho, 181Ta(n, xn), E=6.7, 20 MeV; measured σ(E(n), θ); deduced reaction mechanism. Modified statistical multistep model analysis.
doi: 10.1016/0375-9474(93)90018-S
1992DA16 Phys.Rev. C46, 1437 (1992) A.D'Arrigo, G.Giardina, M.Herman, A.Taccone Angular Momentum Effects in Heavy-Ion-Induced Fission NUCLEAR REACTIONS, ICPND 142Nd(16O, F), 134Ba(24Mg, F), 126Te(32S, F), 94Zr(64Ni, F), E not given; calculated fission σ(E). Statistical model, collective effects in nonadiabatic approach.
doi: 10.1103/PhysRevC.46.1437
1992DA21 J.Phys.(London) G18, 2009 (1992) A.D'Arrigo, G.Giardina, M.Herman, F.Malaguti, A.Taccone, G.Vannini Influence of Angular Momentum on Fission Probability Energy Distribution NUCLEAR REACTIONS 133Cs(16O, F), E=166 MeV; 159Tb(16O, F), E=93-166 MeV; 169Tm(12C, F), 165Ho(16O, F), E not given; calculated fission probability vs excitation; deduced angular momendum role. 28Si(16O, F), E=100 MeV; 28Si(28Si, F), E=150 MeV; calculated compound system fission T1/2.
doi: 10.1088/0954-3899/18/12/016
1992HE02 Nucl.Phys. A536, 124 (1992) M.Herman, G.Reffo, H.A.Weidenmuller Multistep-Compound Contribution to Precompound Reaction Cross Section NUCLEAR REACTIONS 93Nb(n, n'), E=14.6 MeV; 93Nb(n, xn), E=13.47 MeV; calculated nucleon spectra, angle integrated σ. Multi-step compound reactions.
doi: 10.1016/0375-9474(92)90249-J
1992HE19 Phys.Rev. C46, 2493 (1992) Gamma Emission in Precompound Reactions. II. Numerical Application NUCLEAR REACTIONS 93Nb, 59Co, 181Ta(n, γ), E=14.1 MeV; analyzed total γ-spectra. Precompound reactions, parameter free interpretation.
doi: 10.1103/PhysRevC.46.2493
1991BR02 Phys.Rev. C43, 201 (1991) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann Isospin Breaking Effects in the Reaction 4He(d, 3He)3H at Low Energies NUCLEAR REACTIONS 4He(d, 3He), E=23-25 MeV; measured σ(θ); deduced σ asymmetry, S-matrix elements. Resonating group model predictions comparison.
doi: 10.1103/PhysRevC.43.201
1990BR09 Phys.Rev. C41, 2435 (1990) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann Isospin Breaking in the Analyzing Power of 3H(3He, 2H)4He and the Inverse Reaction NUCLEAR REACTIONS 3H(polarized 3He, d), E=18 MeV; calculated analyzing power; deduced isospin symmetry violation matrix element. Resonating group model.
doi: 10.1103/PhysRevC.41.2435
1990BU05 Phys.Rev. C41, 1530 (1990) R.Butsch, M.Thoennessen, D.R.Chakrabarty, M.G.Herman, P.Paul Nuclear Deformation in Excited Pb Isotopes from Giant Dipole γ-Ray-Fission Angular Correlations NUCLEAR REACTIONS 181Ta(19F, X), (19F, F), E=105, 141 MeV; measured Eγ, Iγ, fission (fragment)γ-coin. 200Pb deduced GDR energy, width, deformation parameter. Statistical model analysis.
doi: 10.1103/PhysRevC.41.1530
1990SZ05 Phys.Rev. C41, 2164 (1990) E.M.Szanto, R.Liguori Neto, M.C.S.Figueira, A.Szanto de Toledo, M.G.Herman, N.G.Nicolis, P.M.Stwertka, T.M.Cormier Search for Valence Proton Effects in Sub-Barrier Fusion Reactions NUCLEAR REACTIONS, ICPND 50Ti, 51V, 52,54Cr, 54Fe(35Cl, X), E(cm) ≈ 50-80 MeV; measured fusion, residual production σ(E); deduced valence proton effects role.
doi: 10.1103/PhysRevC.41.2164
1990WA07 Nuovo Cim. 103A, 761 (1990) Analysis of Emission Models in FKK Multistep Compound Model NUCLEAR REACTIONS 93Nb(n, n'), E=14.6 MeV; calculated spectra for different exit modes. Multi-step compound model.
1989AR04 Phys.Rev. C40, 55 (1989) N.Arena, Seb.Cavallaro, G.Fazio, G.Giardina, A.Italiano, M.Herman, M.Bruno, F.Cannata, M.D'Agostino, M.Lombardi Three-Body Effects in the 7Li(d, ααn) Reaction NUCLEAR REACTIONS 7Li(d, 2α), E=6.8 MeV; measured σ(θ1, θ2) vs arc length; deduced three body effects. 5He deduced (3/2)+ level width. Enriched target.
doi: 10.1103/PhysRevC.40.55
1989AR08 Phys.Rev. C40, 1126 (1989) N.Arena, Seb.Cavallaro, A.D'Arrigo, G.Fazio, G.Giardina, A.Italiano, M.Herman, M.Lombardi Width of the Level at E(x) ≈ 18 MeV in 5Li NUCLEAR REACTIONS 6Li(3He, pα), E=11, 13, 14 MeV; measured σ(θα, θp) vs arc length; analyzed αα-bidimensional spectra. 5Li deduced (1/2)+ level, width. Enriched target.
doi: 10.1103/PhysRevC.40.1126
1989AR20 Nuovo Cim. 102A, 1327 (1989) N.Arena, Seb.Cavallaro, P.D'Agostino, G.Fazio, G.Giardina, A.Italiano, F.Mezzanares, M.Herman, M.Lombardi 5Li(g.s.) Energy Spectrum Deduced by the 6Li(3He, αp)α Reaction NUCLEAR REACTIONS 6Li(3He, pα), E=2.5 MeV; measured σ(θα1, θα2) vs arc length. 5Li deduced level energy, Γ. R-matrix calculation.
doi: 10.1007/BF02800341
1989BR23 Nucl.Phys. A501, 462 (1989) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann, B.Vuaridel, W.Gruebler, V.Konig, P.A.Schmelzbach, K.Elsener Barshay-Temmer Test for the 4He(d(pol), 3He)3H Reaction NUCLEAR REACTIONS 4He(d, 3He), E(cm)=14-33 MeV; measured σ(θ, E), iT11(θ, E); deduced asymmetries with respect to θ(cm)=90°, isospin violation magnitude. Resonating group calculations.
doi: 10.1016/0375-9474(89)90141-3
1989HE06 Phys.Rev. C39, 1269 (1989) Early Stage Equilibration Dynamics in a Two-Component Nuclear System NUCLEAR STRUCTURE 90Zr; calculated two, four exciton states for neutrons, protons.
doi: 10.1103/PhysRevC.39.1269
1989HE25 Phys.Rev. C40, 2870 (1989) M.Herman, G.Reffo, M.Rosetti, G.Giardina, A.Italiano Eigenvalue Spacings of the Shell-Model Hamiltonian NUCLEAR STRUCTURE N ≤ 170; Z ≤ 110; analyzed shell model Hamiltonian eigenvalue spacing; deduced particle-hole state density estimating methods.
doi: 10.1103/PhysRevC.40.2870
1989VO10 Phys.Rev. C40, R2441 (1989) R.J.Vojtech, R.Butsch, V.M.Datar, M.G.Herman, R.L.McGrath, P.Paul, M.Thoennessen High Energy Photon Production in Low Energy 12C + 112,124Sn Collisions NUCLEAR REACTIONS 112,124Sn(12C, X), E=7.5, 10.5 MeV/nucleon; measured γ yield, σ(θγ, Eγ); deduced source velocity, γ yield isotopic dependence. Statistical model calculations.
doi: 10.1103/PhysRevC.40.R2441
1988BR18 Phys.Rev. C38, 521 (1988) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.F.Hofmann, B.Vuaridel, V.Konig, W.Gruebler, P.A.Schmelzbach, K.Elsener, M.Bittcher, D.Singy Role of Tensor Forces in the 4He(d(pol), 3He)3H Reaction NUCLEAR REACTIONS 4He(polarized d, 3He), E(cm)=23 MeV; calculated σ(θ), analyzing power vs θ; deduced S-matrix elements, observables tensor force dependences.
doi: 10.1103/PhysRevC.38.521
1988CH11 Phys.Rev. C37, 1437 (1988) D.R.Chakrabarty, M.Thoennessen, S.Sen, P.Paul, R.Butsch, M.G.Herman Giant Dipole Resonances in Excited Er Isotopes NUCLEAR REACTIONS 141Pr(19F, X), E=94.1, 96.5, 111.1, 129 MeV; measured γ spectra. 160Er deduced GDR energies, widths, deformation parameters, shape evolution. Statistical model analysis.
doi: 10.1103/PhysRevC.37.1437
1988HE04 Phys.Rev. C37, 797 (1988) Effect of Nuclear Deformation on Few-Quasiparticle State Densities NUCLEAR STRUCTURE 27Al, 100Mo, 170Er; calculated few-quasiparticle state density; deduced pairing effects role.
doi: 10.1103/PhysRevC.37.797
1988HE09 Phys.Lett. 203B, 29 (1988) M.G.Herman, T.M.Cormier, M.Satteson Statistical Origin of the Highest-Energy Fusion-Induced Gamma Rays NUCLEAR REACTIONS 54Fe(35Cl, X), E=95-150 MeV; measured γ-multiplicities, γ-spectra; deduced GDR statistical decay of mass=85, 86, 87 nuclei.
doi: 10.1016/0370-2693(88)91564-X
1988TH01 Phys.Rev. C37, 1762 (1988) M.Thoennessen, D.R.Chakrabarty, R.Butsch, M.G.Herman, P.Paul, S.Sen Onset of Deformation in Pb Isotopes at High Excitation Energies NUCLEAR REACTIONS 181Ta(19F, X), E=93, 105 MeV; measured Eγ, Iγ. 200Pb deduced GDR, width, deformation parameter, shape transition. Statistical model.
doi: 10.1103/PhysRevC.37.1762
1987HE15 Phys.Rev. C36, 1546 (1987) Realistic Few-Quasiparticle Level Densities in Spherical Nuclei NUCLEAR STRUCTURE 48Ti, 52Cr, 56Fe, 58Ni, 88Sr, 116Sn, 136Ba, 208Pb, 46Sc, 54Mn, 86Rb, 116In, 134Cs, 206Tl; calculated pairing interaction induced energy shifts.
doi: 10.1103/PhysRevC.36.1546
1987TH07 Phys.Rev.Lett. 59, 2860 (1987) M.Thoennessen, D.R.Chakrabarty, M.G.Herman, R.Butsch, P.Paul Giant Dipole Resonance in Highly Excited Thorium: Evidence for strong fission hindrance NUCLEAR REACTIONS 208Pb(16O, X), E=100, 120, 140 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ), yield ratios. 224Th deduced giant dipole resonance, level density parameters, fission hindrance factors.
doi: 10.1103/PhysRevLett.59.2860
1986MA09 Z.Phys. A323, 91 (1986) A.Marcinkowski, K.Stankiewicz, U.Garuska, M.Herman Cross Sections of Fast Neutron Induced Reactions on Molybdenum Isotopes NUCLEAR REACTIONS 92,95,96,97,98Mo(n, p), E=13-16.6 MeV; 92,100Mo(n, α), (n, 2n), 92,94Mo(n, 2n), E=13.4-16.6 MeV; 100Mo(n, 2n), E=13-16.6 MeV; measured residual, isomer production σ(E); deduced evaporation, preequilibrium emission role. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30809. 1986MA26 Radiat.Eff. 93, 265 (1986) A.Marcinkowski, M.Herman, K.Stankiewicz, U.Garuska Cross Sections of Fast Neutron Induced Reactions on Molybdenum Isotopes NUCLEAR REACTIONS 95,92,96,97Mo(n, p), 100Mo(n, α), E=threshold-16 MeV; 92Mo(n, α), E=6-20 MeV; 92Mo(n, 2n), E=12-19 MeV; 100Mo(n, 2n), E=8-19 MeV; measured σ(E). Activation technique, evaporation, preequilibrium emission model analyses.
doi: 10.1080/00337578608207468
1986NI07 Phys.Lett. 178B, 339 (1986) N.G.Nicolis, T.M.Cormier, P.M.Stwertka, M.G.Herman Angular-Momentum Limitations in the High-Spin Gamma-Decay of Medium-Mass Evaporation Residues NUCLEAR REACTIONS, ICPND 54Fe(28Si, X)80Sr/79Sr/78Sr/79Rb/76Kr/78Kr/74Kr, E=75-145 MeV; measured γ-ray multiplicity, evaporation residue σ(E). NaI γ-ray multiplicity filter. Statistical model calculations.
doi: 10.1016/0370-2693(86)91390-0
1985AN21 Nucl.Phys. A443, 404 (1985) P.Andersson, R.Zorro, I.Bergqvist, M.Herman, A.Marcinkowski Cross Sections for 197Au(n, γ)198Au and 115In(n, γ)116mIn in the Neutron Energy Region 2.0-7.7 MeV NUCLEAR REACTIONS 197Au, 115In(n, γ), E=2-7.7 MeV; measured σ(E). Compound nucleus analysis.
doi: 10.1016/0375-9474(85)90408-7
1985HE05 Acta Phys.Pol. B16, 87 (1985) M.Herman, A.Marcinkowski, G.Reffo Fast Neutron Capture on Ir Isotopes NUCLEAR REACTIONS 191,193Ir(n, γ), E=0.5-1 MeV; measured capture σ(E); deduced reaction mechanism, level density parameter systematics.
1985ST01 Phys.Lett. 150B, 91 (1985) P.M.Stwertka, T.M.Cormier, M.Herman, N.G.Nicolis Inhibition of Nucleon Decay from High Spin Nuclei near the N = 82 Shell Closure NUCLEAR REACTIONS 124,118,112Sn(28Si, X), E ≈ 100-180 MeV; measured fusion σ(E); deduced average neutron multiplicity. Statistical model comparison.
doi: 10.1016/0370-2693(85)90145-5
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