NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.I.Mulgin Found 32 matches. 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
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
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
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
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
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, 234,236,237,239Np, 239,240,241,243Am, 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
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, 233,235,236,238U, 238,239,240,242Pu, 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
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, T1/2. Comparison with neighboring nuclei.
doi: 10.1007/s100500070082
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
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
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
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
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.
1991IT01 Yad.Fiz. 53, 1225 (1991); Sov.J.Nucl.Phys. 53, 757 (1991); Erratum Sov.J.Nucl.Phys. 55, 1607 (1992) M.G.Itkis, N.A.Kondratev, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Low-Energy Fission of Nuclei Lighter Than Hg NUCLEAR REACTIONS 194Pt, 186,188Os(p, F), E ≤ 30 MeV; 191Ir, 185Re(α, F), E=40-50 MeV; 191Ir, 185Re(3He, F), E=60 MeV; measured fission fragment yield, total kinetic energy vs mass. 187,189Ir, 195Au deduced fission saddle point shell corrections features.
1991IT02 Yad.Fiz. 53, 1238 (1991); Sov.J.Nucl.Phys. 53, 764 (1991) M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Energy Balance for Nuclear Fission in the Pb Region NUCLEAR STRUCTURE A=170-258; analyzed fission data; deduced asymmetric fission features. Energy balance formalism.
1991RA17 Yad.Fiz. 53, 1200 (1991); Sov.J.Nucl.Phys. 53, 741 (1991) E.M.Rastopchin, S.I.Mulgin, Yu.B.Ostapenko, V.V.Pashkevich, M.I.Svirin, G.N.Smirenkin Statistical and Dynamical Aspects of Preactinide Fissility NUCLEAR STRUCTURE 186,187,188,191Os, 193,196,197Pt, 198,199,200,202Hg, 206,205,207,208Pb, 173Lu, 212Po; A=160-220; analyzed fission data; deduced fissility features. NUCLEAR REACTIONS Ag(3He, F), E not given; 197Au(α, F), E=32.6-47.5 MeV; analyzed fission data; deduced fissility features.
1990IT03 Yad.Fiz. 52, 944 (1990); Sov.J.Nucl.Phys. 52, 601 (1990); Erratum Sov.J.Nucl.Phys. 55, 1607 (1992) M.G.Itkis, N.A.Kondratev, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Mass Asymmetry of Symmetric Fission of Nuclei with A ≈ 200 NUCLEAR REACTIONS, ICPND 197Au(p, F), E=22.4-30 MeV; 197Au(α, F), E=32.6-50 MeV; 194Pt(α, F), E=50 MeV; measured fission fragment mass yield, total kinetic energy distributions. 198Hg, 201Tl deduced fission characteristics. Fast semiconductor (E1-E2) spectrometer. Cold fission.
1988GR28 Yad.Fiz. 48, 312 (1988); Sov.J.Nucl.Phys. 48, 197 (1988) E.N.Gruzintsev, M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, O.I.Serdyuk, G.N.Smirenkin, M.I.Subbotin Characteristic Features of First and Second Moments of Fission-Fragment Energy Distribution as Functions of Nucleon Composition NUCLEAR STRUCTURE 201,200Tl, 206,207,209,208Bi, 210,211,212,208,207Po, 213,212At; A=165-213, Z=68-85; analyzed fission data; deduced fission fragment energy first, second moments characteristics.
1988IT01 Yad.Fiz. 47, 7 (1988) M.G.Itkis, N.A.Kondratyev, Yu.V.Kotlov, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Low-Energy Fission of Gold Nuclei by Protons and α Particles NUCLEAR REACTIONS, ICPND 197Au(α, F), E=35.9 MeV; 197Au(p, F), E=26 MeV; measured fission fragment mass, energy distributions, yields. 198Hg, 201Tl deduced fission properties.
1988ZA07 Ukr.Fiz.Zh. 33, 809 (1988) N.I.Zaika, Yu.V.Kibkalo, V.P.Tokarev, V.A.Shityuk, E.N.Gruzintsev, M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, V.N.Tolstikov Energy Dependence of Characteristics of Actinide Nuclei Fission by 3He Ions with Energies of 40-60 MeV NUCLEAR REACTIONS, ICPND 235,236U(3He, F), E=40-60 MeV; measured fission σ(E), σ(θ); deduced anisotropy vs E, θ.
1987GR19 Yad.Fiz. 45, 1547 (1987) E.N.Gruzintsev, M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Fission of Mercury Nuclei in Reactions Induced by Protons, 3He Ions and α Particles NUCLEAR REACTIONS 197,198Hg(p, F), (3He, F), (α, F), E ≈ 30-60 MeV; measured fission fragment mass distributions.
1987GR35 Yad.Fiz. 46, 1604 (1987) E.N.Gruzintsev, M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Energy Dependence of Dispersions in the Fragment Mass Distributions for Fission of Pre-Actinide Nuclei NUCLEAR REACTIONS 209Bi(p, F), 206Pb(α, F), 207Pb(3He, F), E not given; calculated fission fragment yield mass distribution.
1987IT03 Europhys.Lett. 4, 275 (1987) M.G.Itkis, J.V.Kotlov, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin, V.N.Tolstikov Barriers and ' Anomaly ' of Symmetric to Asymmetric Yield Ratio in Fission of 213At NUCLEAR REACTIONS, ICPND 209Bi(α, F), E=17-31 MeV; measured total, asymmetric fission σ(E), fragment yield vs mass, energy distributions. 213At deduced symmetric, asymmetric fission barrier heights.
doi: 10.1209/0295-5075/4/3/004
1987IT06 Yad.Fiz. 46, 1380 (1987) M.G.Itkis, Yu.V.Kotlov, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Fission of 213At near the Threshold NUCLEAR REACTIONS, ICPND 209Bi(α, F), E=30.9, 31.7 MeV; measured fission fragment mass, energy distributions; deduced fragment yield ratio. 213At deduced fission barrier features.
1986BE20 Yad.Fiz. 43, 1373 (1986) S.D.Beizin, M.G.Itkis, I.A.Kamenev, S.I.Mulgin, V.N.Okolovich, G.N.Smirenkin Angular Anisotropy and Critical Angular Momentum in Nuclear Fission Induced by Light Charged Particles NUCLEAR REACTIONS, ICPND 209Bi, 206Pb, 205Tl, 197Au, 185Re, 182W(p, F), (α, F), E ≈ 35-75 MeV; measured fission fragment σ(θ); deduced reaction, fission σ(E). 211,210Po, 212,213At, 206Pb, 201Tl, 199,198Hg, 189Ir, 186Os, 181W, 170Yb deduced l(critical).
1986GR05 Z.Phys. A323, 307 (1986) Ye.N.Gruzintsev, M.G.Itkis, J.V.Kotlov, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Stability of Heated Nuclei against Mass-Asymmetric Deformations in the Fission Process NUCLEAR REACTIONS 162Dy, 169Tm, 176Hf, 181Ta, 180W(3He, F), E=60-65 MeV; measured fission fragment mass distribution. 165Er, 183Os, 184Re, 179W, 172Lu deduced stiffness parameter, fission barriers.
1986GR12 Yad.Fiz. 43, 1101 (1986) E.N.Gruzintsev, M.G.Itkis, S.I.Mulgin, V.N.Okolovich, A.Ya.Rusanov, G.N.Smirenkin Mass Distributions of Fission Fragments from Heated Nuclei and the Droplet Model NUCLEAR REACTIONS, ICPND 162Dy, 169Tm, 176Hf, 181Ta, 180W(3He, F), E=60-65 MeV; measured fission fragment yields, mass distributions. 165Er, 172Lu, 179W, 184Os, 179Re deduced saddle point parameter stability, barriers.
1986IT01 Yad.Fiz. 43, 1125 (1986) M.G.Itkis, S.I.Mulgin, A.Ya.Rusanov, V.N.Okolovich, G.N.Smirenkin On Formation of Mass Distributions of Fragments from Fission of Nuclei Lighter than Thorium NUCLEAR REACTIONS, ICPND 206Pb, 209Bi(α, F), 207Pb, 209Bi(3He, F), 209Bi(p, F), E not given; analyzed fission fragment mass variance vs temperature data. 212Po, 213At deduced fragment yield vs mass. 226Ra(p, F), E=13 MeV; 226Ra(α, F), E=17 MeV; calculated fragment yield vs mass.
1984IG01 Yad.Fiz. 40, 625 (1984) A.V.Ignatyuk, M.G.Itkis, I.A.Kamenev, S.I.Mulgin, V.N.Okolovich, G.N.Smirenkin Investigation of Fissility of Pre-Actinide Nuclei Induced by Protons and α Particles NUCLEAR REACTIONS 209Bi, 205Tl, 197Au, 185Re(p, F), E=40-70 MeV; 209Bi, 206Pb, 197Au, 185Re, 182W, 177Hf(α, F), E=40-80 MeV; measured fission σ(E). 181W, 186Os, 189,201Tl, 210Po, 213At deduced fission thresholds. Statistical approach, pairing correlations, collective, shell effects in level density. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0623. 1984IG02 Yad.Fiz. 40, 1404 (1984) A.V.Ignatyuk, M.G.Itkis, I.A.Kamenev, S.I.Mulgin, V.N.Okolovich, Yu.B.Ostapenko, G.N.Smirenkin Analysis of Fissility and Fission Barriers of Pre-Actinide Nuclei NUCLEAR REACTIONS 209Bi, 204,206,207,208Pb(e, F), E=30-50 MeV; analyzed fission yield vs E. Superfluid model. NUCLEAR STRUCTURE A=170-213; analyzed fission data; deduced nuclear masses, deformation energy isospin parameter modification.
1979ZH02 Yad.Fiz. 30, 981 (1979); Sov.J.Nucl.Phys. 30, 510 (1979) O.A.Zhukova, S.I.Mulgin, A.V.Yushkov Analysis of Elastic Scattering of 3He Ions within the Framework of the S-Matrix Formalism NUCLEAR REACTIONS 58Ni(3He, 3He), E=22-51.3 MeV; 90Zr(3He, 3He), E=12, 25, 43.7 MeV; 91Zr(3He, 3He), E=25 MeV; 92Zr(3He, 3He), E=25, 51.3 MeV; 118Sn(3He, 3He), E=20-31.2 MeV; 150Sm(3He, 3He), E=20 MeV; 209Bi(3He, 3He), E=31.2 MeV; analyzed σ(θ). S-matrix formalism.
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