NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = E.S.Soukhovitskii Found 48 matches. 2021ZH36 J.Phys.(London) G48, 075101 (2021) X.Zhao, W.Sun, E.Sh.Soukhovitskii, D.S.Martyanov, J.M.Quesada, R.Capote Nucleon scattering analysis with a lane-consistent dispersive optical potential for Hf, W and Ta isotopes NUCLEAR REACTIONS 182,184,186W, 178,180Hf, 181Ta(n, X), (n, n), (n, n'), E<200 MeV; calculated σ, σ(θ); deduced optical model parameters. Comparison with experimental data.
doi: 10.1088/1361-6471/abe280
2019ZH56 J.Phys.(London) G46, 055103 (2019) X.Zhao, W.Sun, E.S.Soukhovitskii, D.S.Martyanov, J.M.Quesada, R.Capote Analysis of neutron bound states of 208Pb by a dispersive optical model potential NUCLEAR REACTIONS 208Pb(n, X), (n, n), E<100 MeV; analyzed available data. 208Pb; calculated energy levels, J, π using Bear-Hodgon(BH) and Woods-Saxon potentials, rms radii of valence neutron particle and hole states, σ, σ(θ) using the real dispersive optical model potential for nucleon scattering; deduced optical model parameters.
doi: 10.1088/1361-6471/ab0010
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
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
2017MA52 Chin.Phys.C 41, 094105 (2017) D.S.Martyanov, E.Sh.Soukhovitskii, R.Capote, J.M.Quesada, S.Chiba Predicting the optical observables for nucleon scattering on even-even actinides NUCLEAR REACTIONS 228,230,232Th, 232,234,236,238U, 238,240,242,244Pu, 246,248Cm, 250Cf(n, X), E<200 MeV; analyzed available data; deduced extended Lane consistent dispersive coupled-channel optical model for nucleon scattering.
doi: 10.1088/1674-1137/41/9/094105
2016SO16 Phys.Rev. C 94, 064605 (2016); Erratum Phys.Rev. C 102, 059901 (2020) E.Sh.Soukhovitskii, R.Capote, J.M.Quesada, S.Chiba, D.S.Martyanov Nucleon scattering on actinides using a dispersive optical model with extended couplings NUCLEAR REACTIONS 233,235,238U, 232Th(n, X), E=0.001-200 MeV; calculated total σ(E) using dispersive potential with multiple-band couplings, compound-nucleus formation cross section using the rigid-rotor RIPL 2408 potential and the potential derived in the present work. Dispersive isospin-dependent coupled-channels optical model analysis, and extended Tamura's coupling formalism for low-lying bands of vibrational nature in even-even and single-particle nature in odd-A actinides. Comparison with experimental data and with RIPL 2408 potential. 232Th, 233,235,238U, 239Pu; calculated average resonance parameters using derived optical model potential, and compared with experimental data and with RIPL 2408 potential and evaluated data, ground-state deformation parameters β2, β4 and β6, and interband effective coupling parameters.
doi: 10.1103/PhysRevC.94.064605
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
2014QU02 Nucl.Data Sheets 118, 270 (2014) J.M.Quesada, R.Capote, E.Sh.Soukhovitskii, S.Chiba Rotational-vibrational Description of Nucleon Scattering on Actinide Nuclei Using a Dispersive Coupled-channel Optical Model NUCLEAR REACTIONS 232Th, 238U(p, x), E=threshold-100 MeV; calculated total σ using DCCOMP (dispersive optical model with different types of rotational bands). Compared with data and calculations with RIPL potentials.
doi: 10.1016/j.nds.2014.04.055
2014SU13 Nucl.Data Sheets 118, 191 (2014) W.Sun, R.Li, E.S.Soukhovitskii, J.M.Quesada, R.Capote A Fully Lane-consistent Dispersive Optical Model Potential for Even Fe Isotopes Based on a Soft-rotator Model NUCLEAR REACTIONS 54,56Fe(n, n), E=0-20 MeV; calculated σ using DCCOM (Lane-consistent dispersive CC optical model); deduced optical model parameters. Cross sections compared to data. 54Fe(n, n'), E=9.9-16.9 MeV;54Fe(p, p'), E=10.0=40.0 MeV;56Fe(n, n'), E=9.993 MeV;56Fe(p, p'), E=17.2-65.0 MeV; calculated analyzing power to discrete states. Compared to data. NUCLEAR STRUCTURE 54,58Fe; calculated collective levels, J, π using soft rotator model. Compared with data.
doi: 10.1016/j.nds.2014.04.034
2014TR06 Nucl.Data Sheets 118, 161 (2014) A.Trkov, R.Capote, L.C.Leal, D.W.Muir, E.Sh.Soukhovitskii Fluctuations Above the Resonance Range in Evaluated Data of 55Mn NUCLEAR REACTIONS 55Mn(n, x), E=0.1-2 MeV; calculated, total σ using EMPIRE; deduced fluctuation coarse graining, total coarse-grained σ, elastic coarse-grained σ(θ). Compared with data.
doi: 10.1016/j.nds.2014.04.026
2011LE31 J.Korean Phys.Soc. 59, 1019s (2011) J.-Y.Lee, E.Sh.Soukhovitskii, Y.Kim, R.Capote, S.Chiba, J.M.Quesada Self-Consistent Analyses of Nuclear Level Structures, and Nucleon Interaction Data of Even-even Sn Isotopes NUCLEAR REACTIONS 120Sn(n, n), E=0.1-200 MeV;120Sn(n, p), E=10-200 Mev; calculated σ; 120Sn(n, n), (n, n'), E=0.94, 11.0, 13.9, 16.1 MeV;120Sn(p, p), E=9.7, 16.0, 20.4, 24.6, 30.3, 40.0, 61.5, 100.4, 134.7, 156.0 MeV;120Sn(p, p'), E=20.4, 24.6, 61.5 MeV; calculated σ(θ); 116Sn(p, n), E=22.8 MeV;118Sn(p, n), E=22.8, 25 MeV;120Sn(p, n), E=22.8, 25, 35, 45 MeV; calculated σ(θ). Deduced optical potential parameters. Soft-rotator model, coupled-channels optical model with dispersive Lane-consistent potential. Comparison with data. NUCLEAR STRUCTURE 120Sn; calculated levels, J, π, rotational band using soft-rotator model. Comparison with data.
doi: 10.3938/jkps.59.1019
2011TR09 Nucl.Data Sheets 112, 3098 (2011) A.Trkov, R.Capote, E.Sh.Soukhovitskii, L.C.Leal, M.Sin, I.Kodeli, D.W.Muir Covariances of Evaluated Nuclear Cross Section Data for 232Th, 180, 182, 183, 184, 186W and 55Mn
doi: 10.1016/j.nds.2011.11.007
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
2009KU13 J.Nucl.Sci.Technol.(Tokyo) 46, 914 (2009) S.Kunieda, S.Chiba, K.Shibata, A.Ichihara, O.Iwamoto, N.Iwamoto, T.Fukahori, E.Sh.Sukhovitskii Extensive Study of the Soft-Rotator Model Hamiltonian Parameters for Medium and Heavy Even-Even Nuclei NUCLEAR STRUCTURE 56,58Fe, 60,62,64Ni, 64,66,68,70Zn, 70,72,74,76Ge, 74,76,78,80,82Se, 86Sr, 96,98,100Mo, 102Ru, 104,106,108,110Pd, 106,108,110,112,114,116Cd, 116,118,120,122,124Sn, 122,124,126,128,130Te, 144,150Nd, 148,150,152,154Sm, 160Gd, 164Dy, 166,168Er, 174,176Yb, 178,180Hf, 182,184W, 192Os, 194Pt, 232Th, 238U; calculated excitation energy levels, J, π, quadrupole deformation parameters, B(E2), B(E3); deduced shell structure effects, agreement with mass-model results. Comparison with experimental results, SRM-CC analysis. NUCLEAR REACTIONS 56,58Fe, 60,62,64Ni, 64,66,68,70Zn, 70,72,74,76Ge, 74,76,78,80,82Se, 86Sr, 96,98,100Mo, 102Ru, 104,106,108,110Pd, 106,108,110,112,114,116Cd, 116,118,120,122,124Sn, 122,124,126,128,130Te, 144,150Nd, 148,150,152,154Sm, 160Gd, 164Dy, 166,168Er, 174,176Yb, 178,180Hf, 182,184W, 192Os, 194Pt, 232Th, 238U(p, p'), E = 22.3, 65 MeV; calculated inelastic proton σ(θ). Coupled-channel optical model analysis.
doi: 10.3327/jnst.46.914
2009LE20 Phys.Rev. C 79, 064612 (2009) J.-Y.Lee, I.Hahn, Y.Kim, S.-W.Hong, S.Chiba, E.Sh.Soukhovitskii Optical potentials for nuclear level structures and nucleon interactions data of tin isotopes based on the soft-rotator model NUCLEAR STRUCTURE 116,118,120,122Sn; calculated levels, J, π and deformation parameters based on the soft rotor model. Comparison with experimental data. NUCLEAR REACTIONS 116,118,120,122Sn(n, n), (n, n'), E=9.95-24 MeV; 116,118,120,122Sn(p, p), (p, p'), E=9.7-156.0 MeV; analyzed σ, σ(θ), optical potential parameters using coupled-channels optical-model calculations. 120Sn(n, X), E=0.1-200 MeV; 120Sn(p, X), E=10-200 MeV; calculated total σ. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064612
2008CA32 J.Nucl.Sci.Technol.(Tokyo) 45, 333 (2008) R.Capote, S.Chiba, E.Sh.Soukhovitskii, J.M.Quesada, E.Bauge A Global Dispersive Coupled-Channel Optical Model Potential for Actinides
doi: 10.1080/18811248.2008.9711442
2008HA28 J.Phys.(London) G35, 095103 (2008) L.Hao, W.Sun, E.Sh.Soukhovitskii A global dispersive coupled-channel potential for the A = 24-122 mass range up to 200 MeV NUCLEAR REACTIONS 24Mg, 28Si, 32S, 40Ca, 48Ti, 52Cr, 56Fe, 58Ni, 90Zr, 98Mo, 120Sn(n, X), E=1 keV-200 MeV; 28Si, 40Ca, 56Fe, 90Zr, 120Sn(p, X), E=1 keV-200 MeV; analyzed σ, σ(θ), analyzing power Ay(θ); deduced global optical model parameters; dispersive coupled channel optical model approach.
doi: 10.1088/0954-3899/35/9/095103
2007KU14 J.Nucl.Sci.Technol.(Tokyo) 44, 838 (2007) S.Kunieda, S.Chiba, K.Shibata, A.Ichihara, E.Sh.Sukhovitskii Coupled-channels Optical Model Analyses of Nucleon-induced Reactions for Medium and Heavy Nuclei in the Energy Region from 1keV to 200 MeV NUCLEAR REACTIONS Fe, Ni, Cu, Y, Zr, Nb, Mo, Sn, W, Au, Pb, Bi, Th, U(n, X), (p, X), E=1 keV - 200 MeV; analyzed cross sections using coupled channel method.
doi: 10.1080/18811248.2007.9711321
2007OK01 Phys.Rev. C 75, 034616 (2007) N.T.Okumusoglu, F.Korkmaz Gorur, J.Birchall, E.Sh.Soukhovitskii, R.Capote, J.M.Quesada, S.Chiba Angular distributions of protons scattered by 40Ar nuclei with excitation of the 2+(1.46 MeV) and 3-(3.68 MeV) collective levels for incident energies of 25.1, 32.5, and 40.7 MeV NUCLEAR REACTIONS 40Ar(p, p), (p, p'), E=25.1, 32.5, 40.7 MeV; measured σ(E, θ), Ay(θ). 40Ar deduced deformation parameters. Isospin dependent soft-rotator coupled-channels optical model analysis.
doi: 10.1103/PhysRevC.75.034616
2007QU04 Phys.Rev. C 76, 057602 (2007) J.M.Quesada, R.Capote, E.Sh.Soukhovitskii, S.Chiba Approximate Lane consistency of the dispersive coupled-channels potential for actinides NUCLEAR REACTIONS 238U, 232Th(p, n), E=26 MeV; calculated angular distributions, compared with experimental data.
doi: 10.1103/PhysRevC.76.057602
2005CA56 Phys.Rev. C 72, 064610 (2005) R.Capote, E.Sh.Soukhovitskii, J.M.Quesada, S.Chiba Is a global coupled-channel dispersive optical model potential for actinides feasible? NUCLEAR REACTIONS 232Th, 238U(n, X), (p, X), E=0.001-200 MeV; analyzed data; deduced parameters. Dispersive coupled-channels optical model.
doi: 10.1103/PhysRevC.72.064610
2005SU16 Phys.Rev. C 72, 024604 (2005) E.Sh.Sukhovitskii, R.Capote, J.M.Quesada, S.Chiba Dispersive coupled-channel analysis of nucleon scattering from 232Th up to 200 MeV NUCLEAR REACTIONS 232Th(n, X), (p, X), E=0.001-200 MeV; analyzed σ, σ(θ); deduced optical model parameters. Dispersive isospin-dependent relativistic coupled-channels optical model analysis.
doi: 10.1103/PhysRevC.72.024604
2004SU12 J.Phys.(London) G30, 905 (2004) E.Sh.Sukhovitskii, S.Chiba, J.-Y.Lee, O.Iwamoto, T.Fukahori Global coupled-channel optical potential for nucleon-actinide interaction from 1 keV to 200 MeV NUCLEAR REACTIONS 232Th, 233,235,238U, 239,240,242Pu(n, X), E=0.1-200 MeV; calculated total σ, resonance parameters. 232Th, 238U(n, n), (n, n'), E=3.4-15 MeV; 232Th, 238U(p, p), (p, p'), E=20-65 MeV; calculated σ(θ). 232Th, 233,235,238U, 239,240,242Pu deduced deformation parameters. Global coupled-channel optical potential, comparison with data.
doi: 10.1088/0954-3899/30/7/007
2003SU02 J.Nucl.Sci.Technol.(Tokyo) 40, 69 (2003) E.Sh.Sukhovitsky, S.Chiba, J.-Y.Lee, B.-T.Kim, S.-W.Hong Analysis of Nucleon Scattering Data of 52Cr with a Coupling Scheme Built with the Soft-rotator Model NUCLEAR REACTIONS 52Cr(n, n), (n, n'), (p, p), (p, p'), E=7-200 MeV; analyzed total σ, σ(E, θ); deduced global optical model parameters. Coupled-channels model. NUCLEAR STRUCTURE 52Cr; analyzed levels, J, π; deduced parameters. Soft rotor model.
2003SU31 J.Nucl.Sci.Technol.(Tokyo) 40, 635 (2003) W.Sun, Y.Watanabe, E.Sh.Sukhovitskii, O.Iwamoto, S.Chiba Coupled-Channels Analysis of Nucleon Interaction Data of 28, 30Si up to 200 MeV Based on the Soft Rotator Model NUCLEAR REACTIONS 28Si(n, n), (n, n'), (p, p), (p, p'), E=14-180 MeV; 30Si(p, p'), E=52 MeV; calculated σ(θ). 28Si(p, X), E=5-200 MeV; calculated reaction σ. Soft rotator model, coupled-channels approach, comparison with data. NUCLEAR STRUCTURE 28,30Si; calculated levels, J, π. Soft rotator model.
doi: 10.1080/18811248.2003.9715401
2002SO19 J.Nucl.Sci.Technol.(Tokyo) 39 sup.2, 144 (2002) Analyses of Nucleon Interaction with 238U up to 150 MeV Incident Energies Using Coupled-Channels Approach with a Saturated Coupling Scheme Based on Soft-Rotator Nuclear Model Hamiltonian NUCLEAR REACTIONS 238U(n, X), (n, n), (n, n'), (p, p), (p, p'), E<150 MeV; analyzed 238U collective nuclear level structure and nucleon interaction usingcoupled-channels optical model with a saturated coupling built on the wave functions of the soft-rotator nuclear Hamiltonian. Comparison with experimental data.
doi: 10.1080/00223131.2002.10875061
2002SO20 J.Nucl.Sci.Technol.(Tokyo) 39 sup.2, 697 (2002) Soft-Rotator Model and Coupled-Channels Approach for Consistent Description of the Nuclear Collective Levels and Their Excitation by Nucleons NUCLEAR STRUCTURE 76Se; calculated B(Eλ) using Coupled-channels optical model approach built on the wave functions of the soft-rotator nuclear Hamiltonian.
doi: 10.1080/00223131.2002.10875195
2002SU21 J.Nucl.Sci.Technol.(Tokyo) 39, 816 (2002) E.S.Sukhovitsky, S.Chiba, J.-Y.Lee, Y.-O.Lee, J.Chang, T.Maruyama, O.Iwamoto Nuclear Level Structure, B(E2) Gamma-Transitions and Nucleon Interaction Data for 56Fe by a Unified Soft-Rotator Model and Couple-Channels Framework NUCLEAR STRUCTURE 56Fe; calculated levels, J, π, B(E2). Soft-rotator model, comparison with data. NUCLEAR REACTIONS 56Fe(n, X), E < 160 MeV; calculated total neutron σ. 56Fe(n, n), E=8-75 MeV; 56Fe(n, n'), E=8-26 MeV; 56Fe(p, p), E=7-156 MeV; 56Fe(p, p'), E=7-62 MeV; calculated σ(θ). Coupled-channels approach, comparison with data.
2001LE24 J.Korean Phys.Soc. 38, 88 (2001) J.-Y.Lee, E.S.Sukhovitsky, Y.-O.Lee, J.Chang, S.Chiba, O.Iwamoto Analyses of the Nuclear Level Structure and Nucleon Interaction Data for 56Fe Based on the Soft-Rotator Model NUCLEAR STRUCTURE 56Fe; calculated levels, J, π, configurations. Soft-rotator model. NUCLEAR REACTIONS 56Fe(n, X), E=0-160 MeV; calculated total σ. 56Fe(n, n), (n, n'), (p, p), (p, p'), E=8-75 MeV; calculated σ(θ). Soft-rotator model, coupled-channels approach. Comparisons with data.
2000CH31 J.Nucl.Sci.Technol.(Tokyo) 37, 498 (2000) S.Chiba, O.Iwamoto, E.S.Sukhovitsky, Y.Watanabe, T.Fukahori Coupled-Channels Optical Potential for Interaction of Nucleons with 12C Up to 150 MeV in the Soft-Rotator Model NUCLEAR REACTIONS 12C(n, n), (n, n'), (p, p), (p, p'), E=20-150 MeV; calculated σ(θ), σ(E, θ), B(E2); deduced parameters. Soft-rotator nuclear model, coupled-channels method. Comparisons with data.
doi: 10.1080/18811248.2000.9714923
2000SU09 J.Nucl.Sci.Technol.(Tokyo) 37, 120 (2000) E.S.Sukhovitsky, O.Iwamoto, S.Chiba, T.Fukahori Nucleon Optical Potential of Uranium-238 up to 150 MeV NUCLEAR REACTIONS 238U(n, X), E < 150 MeV; calculated total σ. 238U(n, n), (n, n'), E=3.4-14 MeV; 238U(p, p), (p, p'), E=20-65 MeV; calculated σ(θ). Optical model, comparisons with data.
2000SU19 Phys.Rev. C62, 044605 (2000) E.Sh.Sukhovitsky, Y.-O.Lee, J.Chang, S.Chiba, O.Iwamoto Nucleon Interaction with 58Ni up to 150 MeV Studied in the Coupled-Channels Approach Based on the Soft-Rotator Nuclear Structure Model NUCLEAR STRUCTURE 58Ni; calculated levels, J, π. Soft-rotator model. Comparison with data. NUCLEAR REACTIONS 58Ni(n, n), E < 150 MeV; calculated σ. 58Ni(n, n), (n, n'), (p, p), (p, p'), E=5-65 MeV; calculated σ(E, θ). Coupled channels method. Comparisons with data.
doi: 10.1103/PhysRevC.62.044605
1999SU01 Nucl.Phys. A646, 19 (1999) E.Sh.Sukhovitsky, S.Chiba, O.Iwamoto Coupled-Channels Optical Model Calculations with Account of Nuclear Volume Conservation NUCLEAR REACTIONS 12C(n, n'), E=20-40 MeV; calculated σ(θ); deduced optical model parameters, volume conservation role. Coupled-channels, soft-rotator model.
doi: 10.1016/S0375-9474(98)00630-7
1998SU23 Nucl.Phys. A640, 147 (1998) E.Sh.Sukhovitsky, S.Chiba, O.Iwamoto, Y.V.Porodzinsky Nucleon Interaction with 12C Studied by the Soft-Rotator Model and a Limit on the Charge-Symmetry Breaking in the Nuclear Mean Field NUCLEAR REACTIONS 12C(n, n), (n, n'), (p, p), (p, p'), E=20-50 MeV; calculated σ(θ); deduced optical model parameters, limit on charge-symmetry breaking. Soft-rotator model, coupled channels model.
doi: 10.1016/S0375-9474(98)00440-0
1997CH39 Nucl.Phys. A624, 305 (1997) S.Chiba, O.Iwamoto, Y.Yamanouti, M.Sugimoto, M.Mizumoto, K.Hasegawa, E.S.Sukhovitsky, Y.V.Porodzinsky, Y.Watanabe Consistent Description of Collective Level Structure and Neutron Interation Data for 12C in the Framework of the Soft-Rotator Model NUCLEAR REACTIONS 12C(n, n), (n, n'), E=28.2 MeV; measured σ(θ); deduced optical model parameters. 12C levels deduced quadrupole deformation parameter, B(E2). Soft-rotor model, coupled-channels analysis.
doi: 10.1016/S0375-9474(97)00474-0
1996PO03 Yad.Fiz. 59, No 2, 247 (1996); Phys.Atomic Nuclei 59, 228 (1996) Yu.V.Porodzinsky, E.Sh.Sukhovitsky Analysis of Neutron Scattering by Even-Even Nuclei with Allowance for Dynamical Octupole Deformations NUCLEAR STRUCTURE 76Se, 238U; calculated levels. Quadrupole-deformed nonaxial rotor. NUCLEAR REACTIONS 238U, 76Se(n, n), E ≤ 20 MeV; analyzed σ(E). 76Se(n, n), (n, n'), E=5-10 MeV; analyzed σ(θ); deduced model parameters, deformations. 76Se, 238U levels deduced B(λ). Quadrupole-deformed nonaxial rotor based wave functions, strong coupling scheme.
1994PO23 Yad.Fiz. 57, No 11, 1923 (1994); Phys.Atomic Nuclei 57, 1851 (1994) Yu.V.Porodzinsky, E.Sh.Sukhovitsky On the Magnitude of the Cross Section for Neutron Absorption by Actinides in the Energy Range 8-14 MeV NUCLEAR REACTIONS 238U(n, X), E ≈ 7-15 MeV; calculated σ(E). 238U(n, n'), E=7.54-14 MeV; calculated σ(θ); deduced σ(absorption) underestimation evidence.
1993PO16 Yad.Fiz. 56, No 10, 64 (1993); Phys.Atomic Nuclei 56, 1336 (1993) Yu.V.Porodzinsky, E.Sh.Sukhovitsky Nuclear Dynamics and Analysis of Scattering of Neutrons by the Nucleus 238U NUCLEAR STRUCTURE 238U; calculated levels. Phenomenological collective model. NUCLEAR REACTIONS 238U(n, n'), (n, n), E=3.4-8.56 MeV; calculated σ(θ), σ(E); deduced model parameters. 238U levels deduced B(λ), quadrupole moments, quadrupole, hexadecapole deformations.
1992PO08 Yad.Fiz. 55, 2368 (1992); Sov.J.Nucl.Phys. 55, 1315 (1992) Yu.V.Porodzinsky, E.Sh.Sukhovitsky Incorporating Hard Hexadecapole Modes in a Phenomenological Collective Nuclear Model with Five Dynamical Variables NUCLEAR STRUCTURE 238U, 76Se; calculated levels, B(λ). Collective model, five dynamical variables.
1991PO02 Yad.Fiz. 53, 64 (1991); Sov.J.Nucl.Phys. 53, 41 (1991) Yu.V.Porodzinsky, E.Sh.Sukhovitsky Rotational-Vibrational States of Nonaxial Deformable Even-Even Nuclei NUCLEAR STRUCTURE 238U; calculated levels. Hamiltonian with five dynamical variables, nonaxiality, deformable nuclei, rotational-vibrational excitations.
1991PO20 Yad.Fiz. 54, 942 (1991); Sov.J.Nucl.Phys. 54, 570 (1991) Yu.V.Porodzinsky, E.Sh.Sukhovitsky Dynamics of Nucleon Scattering by Even-Even Deformed Nonaxial Nuclei NUCLEAR STRUCTURE 232Th; calculated levels, B(λ). Phenomenological collective model, nucleon scattering data analysis.
1990GO13 Yad.Fiz. 51, 660 (1990); Sov.J.Nucl.Phys. 51, 418 (1990) A.A.Golubova, I.E.Kashuba, Yu.V.Porodzinsky, E.Sh.Sukhovitsky 76,78,80,82Se(n, n), (n, n'): Isospin effects in the neutron optical potential NUCLEAR REACTIONS 76,78,80,82Se(n, n), (n, n'), E=1.5-5 MeV; analyzed σ(θ). 76,78,80,82Se levels deduced B(λ), quadrupole moments. Coupled-channels formalism.
1989KA48 Ukr.Fiz.Zh. 34, 1150 (1989) I.E.Kashuba, Yu.V.Porodzinsky, E.Sh.Sukhovitsky The Neutron Scattering with Excitation of the Low-Lying States in 52Cr NUCLEAR REACTIONS 52Cr(n, n), (n, n'), E=1.5-8.6 MeV; calculated σ(E, θ). 52Cr(n, X), E < 20 MeV; calculated σ; deduced model parameters. Coupled-channels method, non-axial soft rotor model.
1988KA40 Yad.Fiz. 48, 1688 (1988) I.E.Kashuba, Yu.V.Porodzinsky, E.Sh.Sukhovitsky Application of Davydov-Chaban Model to Describe Fast Neutron Scattering from Even-Even Nuclei NUCLEAR REACTIONS 56Fe(n, n'), (n, n), E=1.5-20 MeV; calculated σ(θ). Davydov-Chaban model, coupled-channel formalism.
1987KA48 Yad.Fiz. 46, 1406 (1987) I.E.Kashuba, V.A.Konshin, Yu.V.Porodzinsky, E.Sh.Sukhovitsky Analysis of Fast Neutron Scattering by 238U Nuclei in the Soft Nonaxial Rotator Model NUCLEAR REACTIONS 238U(n, n'), E ≈ 1-2.5 MeV; analyzed σ(E). 238U deduced levels, J, π, band characteristics.
1986KO28 Radiat.Eff. 95, 85 (1986) V.A.Konshin, A.B.Klepatskij, V.M.Maslov, E.S.Sukhovitskij Possibilities of Updating Pu Fast Neutron Cross Sections with a Theoretical Analysis NUCLEAR REACTIONS 238,239,240,241,242,243,244Pu(n, F), (n, 2n), (n, 3n), E=threshold-20 MeV; calculated fission, reaction σ(E). Various theoretical models.
doi: 10.1080/00337578608208671
1985IG01 Yad.Fiz. 42, 569 (1985) A.V.Ignatyuk, A.B.Klepatsky, V.M.Maslov, E.Sh.Sukhovitsky Analysis of Cross Sections of U and Pu Isotope Fission Induced by Neutrons in the Range of the First ' Plateau ' NUCLEAR REACTIONS 239,240,241,242,244,245Pu, 234,235,236,237,238,239,240U(n, F), E=1-5.5 MeV; analyzed fission σ(E). 240,241,242,243,245,246Pu, 235,236,237,238,239,240,241U deduced fission barriers, transitional states statistical characteristics.
1975SU06 Vestsi Akad.Navuk BSSR Ser.Fiz.Energ.Navuk No.2, 23 (1975) E.S.Sukhovitskii, A.R.Benderskii, V.A.Konshin Analysis of the Angular Distributions of Neutrons Elastically Scattered by 235U NUCLEAR REACTIONS 235U(n, n), E=0.5-14 MeV; analyzed data.
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