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NSR database version of April 27, 2024.

Search: Author = S.V.Zhdanov

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2011GO27      J.Korean Phys.Soc. 59, 919s (2011)

D.M.Gorodisskiy, K.V.Kovalchuk, S.I.Mulgin, A.Ya.Rusanov, S.V.Zhdanov

PYF: Predictions of Fragment Mass Yields for Transmutation of Minor Actinides

NUCLEAR REACTIONS ²³⁵U(p, f), E=12.5 MeV;²³²Th, ²³⁸U(n, f), E≈5 MeV;²³⁸U(n, f), E=16.5 MeV;²³⁷Np(n, f), E=5.4, 5.5, 16.5, 18 MeV;²³⁹Pu(n, f), E=5.3, 7.9, 14.0, 14.5 MeV;²⁴²Pu(n, f), E=15.1 MeV; calculated fragment yields using PYF code; deduced model parameters. Presented also simple formulae. Comparison to data. Also calculations for unknown target (n, f), E=13, 27.5, 50, 99.5, 160 MeV.

doi: 10.3938/jkps.59.919
Citations: PlumX Metrics

2009MU08      Nucl.Phys. A824, 1 (2009)

S.I.Mulgin, S.V.Zhdanov, N.A.Kondratiev, K.V.Kovalchuk, A.Ya.Rusanov

The modal structure of fragment mass and energy yields from the 10.3-30.0 MeV proton induced fission of ²³²Th and ²³⁵U

NUCLEAR REACTIONS ²³²Th, ²³⁵U(p, F), E=10.3-30.0 MeV; measured fission fragment kinetic energy and mass distributions using a surface-barrier silicon detector. Multi-modal fission characteristics discussed.

doi: 10.1016/j.nuclphysa.2009.03.013
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0697.

2008GO01      Ann.Nucl.Energy 35, 238 (2008)

D.M.Gorodisskiy, K.V.Kovalchuk, S.I.Mulgin, A.Ya.Rusanov, S.V.Zhdanov

Systematics of fragment mass yields from fission of actinide nuclei induced by the 5-200 MeV protons and neutrons

NUCLEAR REACTIONS ²³²Th, ^235,236U, ²⁴⁰Pu(p, X), E=10.3, 12.5, 22.0 MeV; ²³²Th, ²³⁷Np, ²³⁸U, ²³⁹Pu(n, X), E=5.0-5.6 MeV; ²³⁸Np, ²³⁹U(n, X), E=16.5 MeV; ²³⁸U(n, X), E=13-160 MeV; calculated fission fragment yields. Compared results to data.

doi: 10.1016/j.anucene.2007.06.002
Citations: PlumX Metrics

2006IT05      Phys.Lett. B 640, 32 (2006)

I.M.Itkis, A.A.Bogachev, A.Yu.Chizhov, D.M.Gorodisskiy, M.G.Itkis, G.N.Kniajeva, N.A.Kondratiev, E.M.Kozulin, L.Krupa, S.I.Mulgin, I.V.Pokrovsky, E.V.Prokhorova, A.Ya.Rusanov, V.M.Voskressenski, S.V.Zhdanov

What can one learn about lithium breakup from the fission reaction of ²³²Th(⁶Li, f) at energies around the Coulomb barrier?

NUCLEAR REACTIONS ²³²Th(⁶Li, F), E=28.5-62.5 MeV; measured fission fragments energy and mass distributions, folding angle distributions; deduced incomplete and complete fusion contributions.

doi: 10.1016/j.physletb.2006.07.026
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1442.

2006IT09      Phys.Lett. B 640, 23 (2006)

I.M.Itkis, A.A.Bogachev, A.Yu.Chizhov, D.M.Gorodisskiy, M.G.Itkis, G.N.Knyazheva, N.A.Kondratiev, E.M.Kozulin, L.Krupa, S.I.Mulgin, I.V.Pokrovsky, E .V.Prokhorova, A.Ya.Rusanov, V.M.Voskressenski, S.V.Zhdanov

What can one learn about lithium breakup from the fission reaction of ²³²Th(⁶Li, f) at energies around the Coulomb barrier

NUCLEAR REACTIONS ²³²Th(⁶Li, f), E=28.5-62.5 MeV; measured products; deduced yields. Data were imported from EXFOR entry O1442.

doi: 10.1016/j.physletb.2006.07.026
Citations: PlumX Metrics

2003GO13      Yad.Fiz. 66, 1226 (2003); Phys.Atomic Nuclei 66, 1190 (2003)

D.M.Gorodisskiy, S.I.Mulgin, A.Ya.Rusanov, S.V.Zhdanov

Isotopic Invariance of Fission Fragment Charge Distributions for Actinide Nuclei at Excitation Energies above 10 MeV

NUCLEAR REACTIONS ²³³Pa, ^{234,236,237,239}Np, ^{239,240,241,243}Am, ²⁴⁵Bk(p, F), E=10.3, 22.0 MeV; measured fission fragment charge and mass distributions; deduced weak dependence on compound nucleus neutron number.

doi: 10.1134/1.1586436
Citations: PlumX Metrics

2002GO32      Phys.Lett. 548B, 45 (2002)

D.M.Gorodisskiy, S.I.Mulgin, V.N.Okolovich, A.Y.Rusanov, S.V.Zhdanov

Isotopic and isotonic effects in fission-fragment mass yields of actinide nuclei

NUCLEAR REACTIONS ²³²Th, ^{233,235,236,238}U, ^{238,239,240,242}Pu, ²⁴⁴Cm(p, F), E=10.3 MeV; measured fission fragment mass distributions; deduced isotopic and isotonic effects.

doi: 10.1016/S0370-2693(02)02838-1
Citations: PlumX Metrics

2000MA65      Eur.Phys.J. A 8, 295 (2000)

O.N.Malyshev, A.V.Belozerov, M.L.Chelnokov, V.I.Chepigin, V.A.Gorshkov, A.P.Kabachenko, A.P.Popeko, J.Rohac, R.N.Sagaidak, A.V.Yeremin, S.I.Mulgin, S.V.Zhdanov

The New Isotope ²¹⁷U

NUCLEAR REACTIONS ¹⁸²W(⁴⁰Ar, 5n), E=193 MeV; measured σ.

RADIOACTIVITY ²¹⁷U(α) [from ¹⁸²W(⁴⁰Ar, 5n)]; measured Eα, T_1/2. Comparison with neighboring nuclei.

doi: 10.1007/s100500070082
Citations: PlumX Metrics

2000PO12      Phys.Rev. C62, 014615 (2000)

I.V.Pokrovsky, M.G.Itkis, I.M.Itkis, N.A.Kondratiev, E.M.Kozulin, E.V.Prokhorova, V.S.Salamatin, V.V.Pashkevich, S.I.Mulgin, A.Ya.Rusanov, S.V.Zhdanov, G.G.Chubarian, B.J.Hurst, R.P.Schmitt, C.Agodi, G.Bellia, L.Calabretta, K.Lukashin, C.Maiolino, A.Kelic, G.Rudolf, L.Stuttge, F.Hanappe

Fission Modes in the Reaction ²⁰⁸Pb(¹⁸O, f)

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁸O, F), E=78 MeV; measured fission fragments kinetic energy, mass distributions; deduced high-energy fission mode. Multicomponent analysis method.

doi: 10.1103/PhysRevC.62.014615
Citations: PlumX Metrics

1999MU15      Phys.Lett. 462B, 29 (1999)

S.I.Mulgin, V.N.Okolovich, S.V.Zhdanov

Observation of New Channel in the Proton-Induced Low-Energy Fission of Nuclei from ²³³Pa to ²⁴⁵Bk

NUCLEAR REACTIONS ²³²Th, ^235,236U, ²⁴⁰Pu, ²⁴⁴Cm(p, F), E=10.3 MeV; measured fission fragments mass and energy distributions; deduced model parameters for different fission modes.

doi: 10.1016/S0370-2693(99)00859-X
Citations: PlumX Metrics

1998MU33      Nucl.Phys. A640, 375 (1998)

S.I.Mulgin, K.-H.Schmidt, A.Grewe, S.V.Zhdanov

Shell Effects in the Symmetric-Modal Fission of Pre-Actinide Nuclei

NUCLEAR STRUCTURE ^187,189Ir, ¹⁹⁸Hg, ¹⁹⁵Au, ²⁰¹Tl, ^208,210,212Po, ²⁰⁷Bi, ²¹³At; analyzed fission mass yields vs excitation energy; deduced shell effects, deformed shell closures.

doi: 10.1016/S0375-9474(98)00332-7
Citations: PlumX Metrics

1997MU33      Nucl.Instrum.Methods Phys.Res. A388, 254 (1997)

S.I.Mulgin, V.N.Okolovich, S.V.Zhdanov

Two-Parametric Method for Silicon Detector Calibration in Heavy Ion and Fission Fragment Spectrometry

doi: 10.1016/S0168-9002(96)01211-9
Citations: PlumX Metrics

1994SC17      Phys.Lett. 325B, 313 (1994)

K.-H.Schmidt, A.Heinz, H.-G.Clerc, B.Blank, T.Brohm, S.Czajkowski, C.Donzaud, H.Geissel, E.Hanelt, H.Irnich, M.C.Itkis, M.de Jong, A.Junghans, A.Magel, G.Munzenberg, F.Nickel, M.Pfutzner, A.Piechaczek, C.Rohl, C.Scheidenberger, W.Schwab, S.Steinhauser, K.Summerer, W.Trinder, B.Voss, S.V.Zhdanov

Low-Energy Fission Studies of Neutron-Deficient Projectile Fragments of ²³⁸U

NUCLEAR REACTIONS C, ¹H, ²⁰⁸Pb(²³⁸U, F), E=relativistic; measured projectile fragmentation followed by residue fission fragment charge distribution. Neutron-deficient actinium, Th, U, protoactinium isotopes.

doi: 10.1016/0370-2693(94)90017-5
Citations: PlumX Metrics

1993ZH05      Yad.Fiz. 56, No 2, 55 (1993); Phys.Atomic Nuclei 56, 175 (1993)

S.V.Zhdanov, M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin, M.I.Subbotin

Fragment Energy Distributions and Fission Dynamics of Heated Nuclei

NUCLEAR REACTIONS ²⁰⁷Pb, ¹⁹⁷Au, ^186,190Os, ¹⁸³W(³He, F), E=51.2 MeV; ¹⁹³Ir, ^188,186Os, ¹⁸⁵Re, ¹⁹⁷Au(³He, F), E=60 MeV; measured fission fragment mass, energy distributions; deduced energy distribution moments. ²¹⁰Po, ^193,191,189Pt, ²⁰⁰Tl, ¹⁸⁶Os, ¹⁹⁴Au deduced fission dynamics.

1992ZH32      Yad.Fiz. 55, 3169 (1992); Sov.J.Nucl.Phys. 55, 1766 (1992)

S.V.Zhdanov, M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin, M.I.Subbotin

Higher Moments of Energy Distributions of Fragments of Symmetric Fission

NUCLEAR REACTIONS ²³²Th(p, F), E=7.4-30 MeV; ²³²Th(³He, F), E=60 MeV; ²⁰⁹Bi, ¹⁹⁷Au(α, F), E=35.9-50 MeV; ²⁰⁶Pb(α, F), E=50 MeV; ²⁰⁷Pb(³He, t), E=60 MeV; measured fission fragment mass, energy distribution. ²¹³At, ²¹⁰Po, ²⁰¹Tl, ²³⁵U, ²³³Pa deduced fission characteristics.

1991BE17      Yad.Fiz. 53, 656 (1991); Sov.J.Nucl.Phys. 53, 411 (1991)

S.D.Beizin, S.V.Zhdanov, M.G.Itkis, V.N.Okolovich, G.N.Smirenkin, M.I.Subbotin

Study of the Trimodal Structure of the Mass and Energy Distributions of Fission Fragments of Transactinide Nuclei

NUCLEAR REACTIONS, ICPND ²³³Pa, ^{234,235,237,239}Np, ^{239,240,241,243}Am, ²⁴⁵Bk(p, F), E=10 MeV; measured fission fragment yields, mass, energy distributions; deduced fission mode dependence on nucleon composition.

1989BE33      Yad.Fiz. 50, 320 (1989)

S.D.Beizin, S.V.Zhdanov, M.G.Itkis, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin, M.I.Subbotin

Actinide Fission Induced by 60-MeV ³He Ions

NUCLEAR REACTIONS, ICPND ²³²Th, ^233,235,236U, ^{238,239,240,242}Pu, ²⁴⁴Cm(³He, F), E=60 MeV; measured fission fragment yields, kinetic energy vs mass. ^{241,242,243,245}Cm, ²⁴⁷Cf, ²³⁵U, ^{236,238,239,241}Pu deduced fission mechanism.

1989BE41      Yad.Fiz. 50, 626 (1989)

S.D.Beizin, S.V.Zhdanov, M.G.Itkis, V.N.Okolovich, G.N.Smirenkin, M.I.Subbotin

Measurements and Three-Component Analysis of Mass-Energy Distributions of Fragments from Proton-Induced Fission of Nuclei ²³²Th and ^233,235U

NUCLEAR REACTIONS, ICPND ²³²Th, ^233,235U(p, F), E=7.4 MeV; measured fission fragment yield vs mass, energy. Three-component analysis.

1989ZH16      Yad.Fiz. 50, 913 (1989)

S.V.Zhdanov, S.D.Beizin, M.G.Itkis, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin, M.I.Subbotin

Study of the Shape of Energy Distributions of Fission Fragments

NUCLEAR REACTIONS, ICPND ²⁰⁹Bi(p, F), E=30 MeV; measured fission fragment yields vs mass, charge. ²¹⁰Po deduced fission features.