NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Y.S.Lutostansky Found 36 matches. 2023FA08 Physics of Part.and Nuclei 54, 547 (2023) A.N.Fazliakhmetov, Yu.S.Lutostansky, G.A.Koroteev, A.P.Osipenko, V.N.Tikhonov Influence of the Fermi Function on the Neutrino Capture Cross Section NUCLEAR REACTIONS 127I(ν, X), E<20 MeV; calculated σ, the Fermi function using different variants; deduced Fermi function impact on the neutrino-capture σ.
doi: 10.1134/S1063779623030139
2023FA14 Phys.Atomic Nuclei 86, 736 (2023) A.N.Fazliakhmetov, Yu.S.Lutostansky, B.K.Lubsandorzhiev, G.A.Koroteev, A.Yu.Lutostansky, V.N.Tikhonov Structure of the Charge-Exchange Strength Function of Tellurium Isotopes 128 and 130 NUCLEAR REACTIONS 128,130Te(3He, t), E<20 MeV; analyzed available data; deduced the charge-exchange strength functions in the microscopic theory of finite Fermi systems, the Gamow–Teller and pygmy resonances, implications for the calculation and analysis of the process of neutrino capture by atomic nuclei.
doi: 10.1134/S1063778823050162
2023LU08 Physics of Part.and Nuclei 54, 436 (2023), Erratum Physics of Part.and Nuclei 54, 801 (2023) Yu.S.Lutostansky, G.A.Koroteev, A.Yu.Lutostansky, A.P.Osipenko, V.N.Tikhonov, A.N.Fazliakhmetov Resonance Structure of the Neutrino-Capture Cross Section and Double Beta Decay of 100Mo Nuclei NUCLEAR REACTIONS 100Mo(ν, X), E<20 MeV; calculated σ for capture of solar neutrinos, strength functions within the self-consistent theory of finite Fermi systems; deduced contribution of background solar neutrinos to the double beta decay of 100Mo.
doi: 10.1134/S1063779623030206
2023LU11 Phys.Atomic Nuclei 86, 205 (2023) Tin Anomaly in Coulomb Energies and Analog Resonances of Neutron-Rich Tin Isotopes NUCLEAR STRUCTURE 110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Sn, 110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Sb; calculated energies of analog resonances of tin isotopes, Coulomb energy differences and analog-resonance energies; deduced anomaly in the distribution of Coulomb energies of tin isotopes.
doi: 10.1134/S1063778823030134
2022LU07 Phys.Atomic Nuclei 85, 231 (2022) Yu.S.Lutostansky, G.A.Koroteev, A.Y.Lutostansky, A.P.Osipenko, V.N.Tikhonov, A.N.Fazliakhmetov Resonance Structure of the Charge-Exchange Strength Function for the Molybdenum Isotopes 98, 100Mo NUCLEAR REACTIONS 98Mo(p, n), 100Mo(3He, t), E<22 MeV; calculated charge-exchange strength function S(E), resonance structures on the basis of the self-consistent theory of finite Fermi systems. Comparison with available data.
doi: 10.1134/S1063778822030127
2022LU12 Phys.Atomic Nuclei 85, 551 (2022) Yu.S.Lutostansky, N.A.Belogortseva, G.A.Koroteev, A.Yu.Lutostansky, A.P.Osipenko, V.N.Tikhonov, A.N.Fazliakhmetov Interaction of Solar Neutrinos with 98Mo and 100Mo Nuclei NUCLEAR REACTIONS 98,100Mo(ν, e-), E<20 MeV; calculated σ, S-factors, solar-neutrino capture rates. Comparison with available data.
doi: 10.1134/s1063778822060096
2020KO27 Bull.Rus.Acad.Sci.Phys. 84, 898 (2020) G.A.Koroteev, N.V.Klochkova, A.P.Osipenko, Yu.S.Lutostansky, V.N.Tikhonov, A.N.Fazliakhmetov Nuclear Resonances and the Interaction between Neutrinos and a Ga-Ge System NUCLEAR REACTIONS 71Ga(ν, E), E<18.79 MeV; calculated σ, rate of neutrino capture; deduced impact of the resonance structure of force function.
doi: 10.3103/S1062873820080195
2020LU05 Phys.Atomic Nuclei 83, 33 (2020) Charge-Exchange Isobaric Resonances and Local-Interaction Parameters NUCLEAR STRUCTURE A=100-140; calculated giant Gamow-Teller isobaric resonances (GTR), analog resonances (AR), pygmy resonances (PR) within the microscopic theory of finite Fermi systems and its model approximation; deduced isobaric resonances energies agree well with data, parameters of isospin-isospin and spin-isospin interaction parameters, parameter values agree in majority with thhe data within the errors.
doi: 10.1134/S106377882001007X
2020LU06 Phys.Atomic Nuclei 83, 39 (2020) Restoration of Wigner's Supersymmetry in Heavy and Superheavy Nuclei NUCLEAR STRUCTURE A=5-244; compiled Gamow-Teller Resonance (GTR) and analog resonance (AR) parameters vs mass number for more than 400 nuclei; deduced Coulomb energy difference ΔEC between neighboring nuclear isobars, isotopicdependence of Coulomb energy difference; deduced going to 0 for heavier nuclei; deduced confirmation of Wigner's SU(4) symmetry.
doi: 10.1134/S1063778820010081
2020LU07 JETP Lett. 111, 603 (2020) Yu.S.Lutostansky, G.A.Koroteev, N.V.Klochkova, A.P.Osipenko, V.N.Tikhonov, A.N.Fazliakhmetov New Capabilities of an Iodine Detector for Solar Neutrinos NUCLEAR REACTIONS 127I(p, n), E<20 MeV; analyzed available data; calculated charge-exchange strength function S(E), neutrino capture rates.
doi: 10.1134/S0021364020110053
2020LU08 Phys.Atomic Nuclei 83, 391 (2020) Yu.S.Lutostansky, G.A.Koroteev, N.V.Klochkova, A.P.Osipenko, V.N.Tikhonov, A.N.Fazliakhmetov Effect of High-Lying Resonances on Cross Sections for Solar-Neutrino Capture by 127I Nuclei
doi: 10.1134/S1063778820020180
2020PA37 Phys.Atomic Nuclei 83, 613 (2020) Nucleosynthesis-Rate Dependence of Abundances of Nuclei Produced in the r-Process ATOMIC MASSES A=90-240; calculated isotopic abundances in the r-process nucleosynthesis.
doi: 10.1134/S1063778820040171
2019LU10 Bull.Rus.Acad.Sci.Phys. 83, 488 (2019) Yu.S.Lutostansky, A.P.Osipenko, V.N.Tikhonov Cross Sections of Solar Neutrino Capture by Nuclei and Charge-Exchange Resonances
doi: 10.3103/S1062873819040178
2019LU15 Phys.Atomic Nuclei 82, 528 (2019) Resonance Structure of the Charge-Exchange Strength Function
doi: 10.1134/S1063778819040112
2019VY01 Bull.Rus.Acad.Sci.Phys. 83, 483 (2019) A.K.Vyborov, L.V.Inzhechik, G.A.Koroteev, Yu.S.Lutostansky, V.N.Tikhonov, A.N.Fazliakhmetov Cross Section of Solar Neutrino Capture by 76Ge Nuclei
doi: 10.3103/S1062873819040294
2019VY02 Phys.Atomic Nuclei 82, 477 (2019) A.K.Vyborov, L.V.Inzhechik, G.A.Koroteev, Yu.S.Lutostansky, V.N.Tikhonov, A.N.Fazliakhmetov Cross Sections for Solar-Neutrino Capture by the 76Ge Nucleus and High-Lying Gamow-Teller Resonances
doi: 10.1134/S1063778819050132
2018LU06 JETP Lett. 107, 79 (2018) Production of Transuranium Nuclides in Pulsed Neutron Fluxes from Thermonuclear Explosions NUCLEAR REACTIONS 238U(n, X), E<5 MeV; calculated yields of transuranium nuclides within the kinetic model of the astrophysical r-process taking into account the time dependence of external parameters and processes accompanying the beta decay of neutron-rich nuclei.
doi: 10.1134/S0021364018020108
2018LU18 Phys.Atomic Nuclei 81, 540 (2018); Yad.Fiz. 81, 515 (2018) Yu.S.Lutostansky, V.N.Tikhonov Resonance Structure of the Charge-Exchange Strength Function and Neutrino-Capture Cross Sections for the Isotopes 71Ga, 98Mo, and 127I
doi: 10.1134/S1063778818040117
2017LU07 Phys.Atomic Nuclei 80, 623 (2017); Yad.Fiz. 80, 311 (2017) Yu.S.Lutostansky, V.N.Tikhonov Special features of the structure of the beta-stability line for nuclei NUCLEAR STRUCTURE Z<110; calculated β-stability line, mass number dependence on Z. Comparison with experimental data.
doi: 10.1134/S106377881703019X
2017PA34 Phys.Atomic Nuclei 80, 657 (2017); Yad.Fiz. 80, 345 (2017) I.V.Panov, Yu.S.Lutostansky, M.Eichler, F.-K.Thielemann Determination of the Galaxy age by the method of uranium-thorium-plutonium isotopic ratios RADIOACTIVITY 244Pu, 238U(α); analyzed available data for 244Pu/238U ratio; deduced Galaxy age, T1/2.
doi: 10.1134/S1063778817040202
2017TO03 Eur.Phys.J. A 53, 33 (2017) S.V.Tolokonnikov, I.N.Borzov, M.Kortelainen, Yu.S.Lutostansky, E.E.Saperstein Alpha-decay energies of superheavy nuclei for the Fayans functional NUCLEAR STRUCTURE 287,288Mc, 291Lv, 293,294Ts, 294Og; calculated Qα values for α-decay chains starting from given nuclei using self-consistent mean-field approach with Fayans FaNDF0 functional and two Skyrme functionals and also using MMM (Macro-Micro Method), T1/2 using semi-phenomenological formulas. Compared with available data and systematics.
doi: 10.1140/epja/i2017-12220-y
2017TO13 Phys.Atomic Nuclei 80, 631 (2017); Yad.Fiz. 80, 319 (2017) S.V.Tolokonnikov, I.N.Borzov, Yu.S.Lutostansky, I.V.Panov, E.E.Saperstein Fission barriers and other characteristics of nuclei from the uranium region NUCLEAR STRUCTURE Z=92, 93, 82, 94; calculated one-, two-neutron separation energies, β-decay energies, charge radii, deformation energy, fission barrier height, neutron single-particle energies. FaNDF0 Fayans energy density functional.
doi: 10.1134/S1063778817040275
2016PA06 Nucl.Phys. A947, 1 (2016) I.V.Panov, Yu.S.Lutostansky, F.-K.Thielemann Beta-decay half-lives for the r-process nuclei RADIOACTIVITY 90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112Sr, 237,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275U(β-); calculated T1/2 using FFST (Finite Fermi Systems Theory) with masses from FRDM or ETFSI. Compared with other calculations and with data. Z=37-50(β-); calculated T1/2. Compared with data.
doi: 10.1016/j.nuclphysa.2015.12.001
2016TO07 Phys.Atomic Nuclei 79, 21 (2016) S.V.Tolokonnikov, I.N.Borzov, Yu.S.Lutostansky, E.E.Saperstein Deformation properties of lead isotopes NUCLEAR STRUCTURE 151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,261,262,263,264,265,266,267,268,269,270,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296Pb; calculated charge radii, magnetic moments, mass excess, 2n separation energy, quadrupole moment, deformation, deformation energy on the basis of energy density functional in the FaNDI Fayans form. Compared with available data.
doi: 10.1134/S1063778816010208
2015LU08 Bull.Rus.Acad.Sci.Phys. 79, 425 (2015); Izv.Akad.Nauk RAS, Ser.Fiz 79, 466 (2015) Yu.S.Lutostansky, V.N.Tikhonov Phenomenological description of the Coulomb energies of medium-heavy and superheavy nuclei NUCLEAR STRUCTURE A=5-244; analyzed available data; calculated Coulomb displacement energies between neighboring isobaric nuclei using a two-parameter formula; deduced impact of deformation for heavy nuclei, advantages over microscopic calculations.
doi: 10.3103/S1062873815040231
2015PA29 Bull.Rus.Acad.Sci.Phys. 79, 437 (2015); Izv.Akad.Nauk RAS, Ser.Fiz 79, 478 (2015) I.V.Panov, Yu.S.Lutostansky, F.-K.Thielemann Half-life of short-lived neutron-excess nuclei that participate in the r -process NUCLEAR STRUCTURE A<220; calculated β-decay rates, T1/2 for r-process nuclei. A quasi-classic model of a strength function based on finite Fermi systems.
doi: 10.3103/S1062873815040243
2015TO07 J.Phys.(London) G42, 075102 (2015) S.V.Tolokonnikov, I.N.Borzov, M.Kortelainen, Y.S.Lutostansky, E.E.Saperstein First applications of the Fayans functional to deformed nuclei NUCLEAR STRUCTURE 220,222,224,226,228,230,232,234,236,238,240,242,244U, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb ; calculated two-neutron separation and deformation energies, quadrupole deformation parameter. Comparison with available data.
doi: 10.1088/0954-3899/42/7/075102
2013PA05 Phys.Atomic Nuclei 76, 88 (2013); Yad.Fiz. 76, 90 (2013) I.V.Panov, I.Yu.Korneev, Yu.S.Lutostansky, F.-K.Thielemann Probabilities of delayed processes for nuclei involved in the r-process NUCLEAR STRUCTURE A=249-260; calculated delayed fission and neutron emission probabilities, B(GT), fission barriers. Generalized Thomas-Fermi model, comparison with available data.
doi: 10.1134/S1063778813010081
2013TO12 Phys.Atomic Nuclei 76, 708 (2013); Yad.Fiz. 76, 758 (2013) S.V.Tolokonnikov, Yu.S.Lutostansky, E.E.Saperstein Self-consistent calculations of alpha-decay energies NUCLEAR STRUCTURE 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236Th, 208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244U, 222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248Pu, 294Og, 293,294Ts, 291Lv; calculated α-decay energies, mass excess. Self-consistent theory of finite Fermi systems, comparison with available data.
doi: 10.1134/S1063778813060136
2012LU09 Bull.Rus.Acad.Sci.Phys. 76, 462 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 520 (2012) Evaluating the yield of transuranium nuclides with masses of up to A = 270 via pulsed nucleosynthesis NUCLEAR REACTIONS 238U, 239Pu, 248Cm, 251Cf(n, X), E not given; calculated yields of transuranium nuclides in high-density neutron flux.
doi: 10.3103/S1062873812040235
2012LU10 Bull.Rus.Acad.Sci.Phys. 76, 476 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 534 (2012) Yu.S.Lutostansky, V.N.Tikhonov Resonance structure of the beta-strength function RADIOACTIVITY 71Ge, 127Xe(EC); calculated β-decay strength functions, resonance structures. Comparison with available data.
doi: 10.3103/S1062873812040247
2011LU13 Bull.Rus.Acad.Sci.Phys. 75, 468 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 504 (2011) The concept of a powerful antineutrino source
doi: 10.3103/S1062873811040320
2011LU15 Bull.Rus.Acad.Sci.Phys. 75, 533 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 569 (2011) Yu.S.Lutostansky, V.I.Lyashuk, I.V.Panov Production of transuranium elements in a binary model under conditions of pulse nucleosynthesis
doi: 10.3103/S1062873811040332
2010GA19 Phys.Atomic Nuclei 73, 1360 (2010); Yad.Fiz. 73, 1403 (2010); Erratum Phys.Atomic Nuclei 73, 2151 (2010) Yu.V.Gaponov, Yu.S.Lutostansky Giant Gamow-Teller resonance in neutron-rich nuclei NUCLEAR REACTIONS 13C, 90Zr(6Li, 6He), E not given; analyzed experimental data; deduced giant Gamow-Teller resonance, Wigner symmetry. RADIOACTIVITY 127Xe(EC), 31,32,33,34Na(β-); analyzed experimental data; calculated T1/2; deduced β-decay strength function.
doi: 10.1134/S1063778810080090
2004LU10 Nucl.Phys. A734, E69 (2004) Properties of nuclei near the neutron-drip line in O - Si region NUCLEAR STRUCTURE Z=8-14; calculated neutron drip-line features. 37Na; calculated single-particle level energies. 29,30,31,32,34,36Ne, 31,32,33,34,35,37,39Na; calculated T1/2, deformation dependence. Comparisons with data.
doi: 10.1016/j.nuclphysa.2004.03.022
2002LU19 Part. and Nucl., Lett. 115, 86 (2002) Yu.S.Lutostansky, S.M.Lukyanov, Yu.E.Penionzhkevich, M.V.Zverev Neutron Drip Line in the Region of 0-Mg Isotopes NUCLEAR REACTIONS Ta(48Ca, X), E=59, 64 MeV; measured fragments isotopic yields; deduced no evidence for 40Mg. 34Ne, 37Na deduced particle stability. 33Ne, 36Na, 39Mg deduced particle instability. NUCLEAR STRUCTURE 24,26O, 29,31F, 32,34Ne, 37,39Na, 42,44Mg; calculated neutron separation energies.
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