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NSR database version of April 11, 2024.

Search: Author = E.S.Soukhovitskii

Found 48 matches.

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1579.

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
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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
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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
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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
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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
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2002SO19      J.Nucl.Sci.Technol.(Tokyo) 39 sup.2, 144 (2002)

E.S.Soukhovitskii, S.Chiba

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
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2002SO20      J.Nucl.Sci.Technol.(Tokyo) 39 sup.2, 697 (2002)

E.S.Soukhovitskii, S.Chiba

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22160.

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
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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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Note: The following list of authors and aliases matches the search parameter E.S.Soukhovitskii: , E.S.SOUKHOVITSKII, E.S.SUKHOVITSKII, E.S.SUKHOVITSKIJ, E.S.SUKHOVITSKY