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NSR database version of April 27, 2024.

Search: Author = E.S.Sukhovitskii

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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
Citations: PlumX Metrics

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, ^{74,76,78,80,82}Se, ⁸⁶Sr, ^96,98,100Mo, ¹⁰²Ru, ^{104,106,108,110}Pd, ^{106,108,110,112,114,116}Cd, ^{116,118,120,122,124}Sn, ^{122,124,126,128,130}Te, ^144,150Nd, ^{148,150,152,154}Sm, 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, ^{74,76,78,80,82}Se, ⁸⁶Sr, ^96,98,100Mo, ¹⁰²Ru, ^{104,106,108,110}Pd, ^{106,108,110,112,114,116}Cd, ^{116,118,120,122,124}Sn, ^{122,124,126,128,130}Te, ^144,150Nd, ^{148,150,152,154}Sm, 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 ^{116,118,120,122}Sn; calculated levels, J, π and deformation parameters based on the soft rotor model. Comparison with experimental data.

NUCLEAR REACTIONS ^{116,118,120,122}Sn(n, n), (n, n'), E=9.95-24 MeV; ^{116,118,120,122}Sn(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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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 A_y(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, 30}Si 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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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 ^{238,239,240,241,242,243,244}Pu(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 ^{239,240,241,242,244,245}Pu, ^{234,235,236,237,238,239,240}U(n, F), E=1-5.5 MeV; analyzed fission σ(E). ^{240,241,242,243,245,246}Pu, ^{235,236,237,238,239,240,241}U 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.

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