NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = V.Y.Denisov Found 105 matches. Showing 1 to 100. [Next]2024DE03 Phys.Rev. C 109, 014607 (2024) Model for compound nucleus formation in various heavy-ion systems
doi: 10.1103/PhysRevC.109.014607
2023DE08 Int.J.Mod.Phys. E32, 2350005 (2023) Simple expressions for calculation of proximity interaction of arbitrarily oriented deformed nuclei NUCLEAR REACTIONS 168,170Er(48Ca, X), E(cm)=140-160 MeV; analyzed available data; deduced σ, simple expressions for the calculation of proximity interaction of arbitrarily oriented deformed nuclei in the linear approximation with respect to the deformation parameters of the colliding nuclei.
doi: 10.1142/S0218301323500052
2023DE14 Phys.Rev. C 107, 054618 (2023) Expression for the heavy-ion fusion cross section NUCLEAR REACTIONS 12C(30Si, X), E=8-24 MeV;12C(24Mg, X), E=7-19 MeV; calculated fusion σ(E). Approximation of the total heavy ion potential around the barrier by the Morse and parabolic potentials. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.054618
2023DE16 At.Data Nucl.Data Tables 152, 101582 (2023) Pre-neutron emission average total kinetic energy of fission fragments NUCLEAR STRUCTURE Z=48-120; analyzed available data; deduced a new expression for a calculation of the pre-neutron emission average total kinetic energy of fission fragments (TKE).
doi: 10.1016/j.adt.2023.101582
2022DA01 Phys.Rev. C 105, 014620 (2022) O.I.Davydovska, V.Yu.Denisov, I.Yu.Sedykh Evaluation of the fission barrier values using the experimental values of the ratio Γf(E)/Γn(E) NUCLEAR STRUCTURE 180,181,182,184W, 185Re, 186,187,188,190Os, 189,191Ir, 192,193,194,196Pt, 195,197Au, 196,198,199,200Hg, 201Tl, 207,209Bi, 208,210,211,212Po, 213At; analyzed experimental data for ratios of fission widths Γf and neutron evaporation width Γn as function of thermal excitation energies of the compound nuclei using statistical approach for fission barrier heights. Comparison with the results of the macroscopic-microscopic finite-range liquid-drop model.
doi: 10.1103/PhysRevC.105.014620
2022DA03 Nucl.Phys. A1018, 122372 (2022) O.I.Davydovska, V.Yu.Denisov, V.A.Nesterov Subbarrier fusion and elastic scattering cross-sections based on modified Thomas-Fermi method potentials NUCLEAR REACTIONS 92Zr, 116Sn(16O, X), E<65 MeV; calculated fusion σ, neutron and proton densities within the modified Thomas-Fermi approach with density-dependent Skyrme forces using the nucleon densities obtained in the same approach.
doi: 10.1016/j.nuclphysa.2021.122372
2022DE01 Phys.Lett. B 824, 136814 (2022) Dependence of average total kinetic energy of fission fragments on excitation energy of fissioning nucleus NUCLEAR REACTIONS 233,235,238U, 239Pu(n, F), E<100 MeV; analyzed available data. 234,236,239U, 240Pu; deduced average total kinetic energy of fission fragments using statistical model.
doi: 10.1016/j.physletb.2021.136814
2022DE02 Phys.Rev. C 105, 014616 (2022) Dependence of average total kinetic energy of fission fragments on the excitation energy of the compound nucleus NUCLEAR REACTIONS 233,235,238U, 239Pu(n, F), E=thermal; analyzed experimental data for average total kinetic energy (TKE) release of fission fragments on the excitation energy of 10-100 MeV for 234,236U, <500 MeV for 239U, and <300 MeV for 240Pu compound nuclei using a simple statistical model. Discussed origin of the energy dependence of the average total kinetic energy in neutron-induced fission.
doi: 10.1103/PhysRevC.105.014616
2022DE13 Eur.Phys.J. A 58, 91 (2022) Multidimensional harmonic oscillator model of subbarrier fusion NUCLEAR REACTIONS 64Ni(64Ni, X), 58Fe(48Ti, X), 58Ni(54Fe, X), E(cm)=65-110 MeV; calculated fusion σ; deduced the new coupled-reaction channel model for the subbarrier fusion of heavy ions.
doi: 10.1140/epja/s10050-022-00746-2
2022DE21 Eur.Phys.J. A 58, 188 (2022) Calculation of the fission fragment characteristics in the three-body model of binary fission NUCLEAR REACTIONS 227,229,230Th, 232,233Th, 231,232Pa, 232,233,234,235,236,237,238U, 237,238Np, 238,239,240,241,242Pu, 241,243Am, 242,243,244,245,246Cm, 248Cm, 249,251Cf, 254Es, 255Fm(n, F), E=0.0000253, 50 keV; calculated potential energy surfaces, fission fragment yields, average total kinetic energy of the primary fragments in the frameworks of the shell-correction approach or the Hartree-Fock-Bogoliubov model with Skyrme force. Comparison with JENDL library.
doi: 10.1140/epja/s10050-022-00841-4
2022DE31 Phys.Lett. B 835, 137569 (2022) Estimation of the double alpha-decay half-life RADIOACTIVITY 108Xe, 224Pu, 222U, 226Pu, 224U, 222Th, 110Xe, 220Ra, 194,196,198Rn, 160W, 224Th, 222Ra, 200,202,204Rn, 112Xe, 154Er, 224Ra, 222Rn, 158Yb, 114Xe, 152,154Dy, 156Er, 150,152Gd, 148Sm, 118Xe, 146Nd(α), (8Be); calculated T1/2, transmission probabilities through the potential barrier for the single and double α decays; deduced model. Comparison with available data.
doi: 10.1016/j.physletb.2022.137569
2021DE10 Eur.Phys.J. A 57, 129 (2021) Calculation of fission fragment characteristics for the reactions nth + 235U and n14MeV+235U NUCLEAR REACTIONS 235U(n, F), E thermal; 235U(n, F), E=14 MeV; calculated potential energy surfaces, radial dependence of α-nucleus potential, mass distributions of fission fragments using 3+4 and 4 body, the deformation energy and the ground-state deformation of fragments in the Strutinsky shell correction approach with the Cherpurnov parametrization of the Woods-Saxon potential. Comparison with experimental data.
doi: 10.1140/epja/s10050-021-00433-8
2021DE15 Chin.Phys.C 45, 044106 (2021) Production of super-heavy nuclei in cold fusion reactions NUCLEAR REACTIONS 208Pb(50Ti, X), (52Cr, X), (54Cr, X), (58Fe, X), (64Ni, X), (70Zn, X), (78Ge, X), E not given; calculated potential energy landscape as a function of the Z and deformation parameter.
doi: 10.1088/1674-1137/abdfc0
2021NE07 Ukr.J.Phys. 66, 857 (2021) V.A.Nesterov, O.I.Davydovska, V.Yu.Denisov Subbarrier-Fusion and Elastic-Scattering Cross-Sections Calculated on the Basis of the Nucleus-Nucleus Potential in the Framework of the Modified Thomas-Fermi Method NUCLEAR REACTIONS 208Pb(16O, X), (12C, X), (16O, 16O), (12C, 12C), E<100 MeV; calculated fusion and elastic σ using the modified Thomas-Fermi approach with density-dependent Skyrme forces.
doi: 10.15407/ujpe66.10.857
2020DA13 Nucl.Phys. A1002, 121994 (2020) O.I.Davydovska, V.A.Nesterov, V.Yu.Denisov The nucleus-nucleus potential within the extended Thomas-Fermi method and the cross-sections of subbarrier fusion and elastic scattering for the systems 16O+58, 60, 62, 64Ni NUCLEAR REACTIONS 58,60,62,64Ni(16O, X), (16O, 16O), E<50 MeV; calculated σ; deduced the parameter values of the imaginary part of the nuclear potential calculated for the Woods-Saxon potentials fitted the extended Thomas-Fermi with Skyrme force potentials. Comparison with available data.
doi: 10.1016/j.nuclphysa.2020.121994
2019DA10 Nucl.Phys. A989, 214 (2019) O.I.Davydovska, V.Yu.Denisov, V.A.Nesterov Comparison of the nucleus-nucleus potential evaluated in the double-folding and energy density approximations and the cross-sections of elastic scattering and fusion of heavy ions NUCLEAR STRUCTURE 16O, 40Ca, 56Fe, 92Zr, 208Pb; calculated mass and charge density distributions, radii using Hartree-Fock model with Skyrme forces SkM* and BCS approximation for nucleon pairing. NUCLEAR REACTIONS 40Ca(40Ca, x), E=53-72 MeV;56Fe, 92Zr, 208Pb(16O, x), E=30-110 MeV; calculated total nucleus-nucleus interaction potentials for all 4 reactions, nuclear parts of the nucleus-nucleus potentials using standard double-folding method and Extended Thomas-Fermi (ETF) with Skyrme potentials with and without DDM3Y1 and ETF-kin; calculated fusion σ using CCFULL code; deduced potential parameters from the fit to the data; calculated fusion σ around the barrier energy, elastic scattering σ(θ) of 208Pb(16O, x) at E=95 MeV, the same quantities for 40Ca(40Ca, x), E=71.8 MeV, 56Fe, 92Zr, (16O, x) at 44 MeV (Fe target) and 56 MeV (Zr target); compared with data; deduced quadrupole, octupole deformation and other potential parameters.
doi: 10.1016/j.nuclphysa.2019.06.004
2019DE01 Chin.Phys.C 43, 014101 (2019) V.Yu.Denisov, O.A.Belyanovska, V.P.Khomenkov, I.Yu.Sedykh, K.M.Sukhyy A simple description of the temperature dependence of the width of the fission-fragment mass yield in 197Au and 209Bi at intermediate energies NUCLEAR REACTIONS 197Au, 209Bi(γ, F), E=460-896 MeV; calculated the temperature dependence of the fission-fragment widths. Comparison with experimental data.
doi: 10.1088/1674-1137/43/1/014101
2019DE26 Eur.Phys.J. A 55, 153 (2019) Empirical relations for the fusion cross sections of heavy ions NUCLEAR REACTIONS 12C(12C, x) to 124Sn(58Ni, x); compiled experimental σ for 85 even-even heavy-ion systems; calculated barrier height B, radius R, curvature hω using Wong formula; deduced formula parameters using fit to the data; calculated, estimated fusion σ, astrophysical S-factor, calculated surface deformation parameter of multipole vibrations of projectile and target nuclei, Q-values of K-neutron pickup or stripping processes, fusion σ for 85 reactions and E=2-164 MeV; 12,14,18C(12C, x), (14C, x)(18C, x), E=2-5.8 MeV; calculated astrophysical S-factor.
doi: 10.1140/epja/i2019-12855-6
2018DE28 Phys.Rev. C 98, 024601 (2018) Calculation of the fission width of an excited nucleus with the fission barrier dependent on excitation energy NUCLEAR STRUCTURE 238Pu, 286Cn; calculated excitation energy dependent fission barrier with pairing, shell correction, and liquid-drop contributions, ratio of fission widths and Bohr-Wheeler fission widths of excited compound nuclei using Strutinsky shell correction prescription and the liquid-drop model.
doi: 10.1103/PhysRevC.98.024601
2018DE41 Eur.Phys.J. A 54, 231 (2018) Calculation of the ratio Γn(E)/Γf(E) in various approaches for the fission width NUCLEAR STRUCTURE 188Os, 210,212Po; calculated excited nuclei width for the neutron emission Γn(E) and that for fission Γf(E) vs E* using the Bohr-Wheeler approach (and also some other methods). Compared with available data.
doi: 10.1140/epja/i2018-12660-9
2017DA15 Ukr.J.Phys. 62, 473 (2017) O.I.Davidovskaya, V.Y.Denisov, B.A.Nesterov Effective Nucleus-Nucleus Potential with Regard for the Contribution of the Kinetic Energy of Nucleons, and the Cross-Sections of Elastic Scattering and Subbarrier Fusion NUCLEAR REACTIONS 208Pb(16O, X), (16O, 16O), E not given; calculated σ of elastic scattering and subbarrier fusion. The microscopic double folding approach.
doi: 10.15407/ujpe62.06.0473
2017DE01 Nucl.Phys. A958, 101 (2017) V.Yu.Denisov, T.O.Margitych, I.Yu.Sedykh Mass yields and kinetic energy of fragments from fission of highly-excited nuclei with A≤220 NUCLEAR STRUCTURE A≤220; calculated quadrupole, octupole, hexadecapole fragment deformation, Q vs mass number. NUCLEAR REACTIONS 142Nd(40Ca, F), E not given;144Sm(36Ar, F), E not given;182W(13C, F), E not given;184W(34S, F), E not given;186W(24Mg, F), E not given;194Pt(16O, F), E not given;197Au(α, F), E not given;208Pb(19F, F), E not given; calculated fission yields vs fragment mass using trajectory concept.
doi: 10.1016/j.nuclphysa.2016.11.007
2017DE04 Phys.Rev. C 95, 014605 (2017) V.Yu.Denisov, N.A.Pilipenko, I.Yu.Sedykh Interaction of three fission fragments and yields of various ternary fragments RADIOACTIVITY 252Cf(SF); calculated differences of the potentials for deformation parameters at the lowest barrier point for fission into 98Zr+22O+132Sn and 72Ni+48Ca+132Sn, dependence of total excitation energy of fragments for the triple spontaneous fission on the masses of the first and third, and first and second fragments, also at an excitation energy of 10 MeV. 250Cf(SF); calculated yield of probability per binary fission event of ternary particles, and compared with experimental data. Simple macroscopic model, with three collinear touching deformed fission fragments formed during the three-fragment fission after scission of necks.
doi: 10.1103/PhysRevC.95.014605
2017DE14 Nucl.Phys. A963, 15 (2017) Fission-fragment mass yields of highly excited nuclei with 119 ≤ A ≤ 218 produced in various reactions NUCLEAR REACTIONS 197Au, 209Bi(γ, f), E=1000 MeV[from bremsstrahlung, stated γ energy is the end-point energy];139La, 165Ho, 197Au(α, f), E not given; calculated fission mass yields. 99Ru(20Ne, f), E=124 MeV;112Sn(12C, f), E=137 MeV;124Sn(20Ne, f), E=140 MeV;154Sm(35Cl, f), E=163.7 MeV;176Yb(28Si, f), E=189 MeV;181Ta(19F, f), E not given;184W(16O, f), E not given;184W28Si, f), E=166, 189 MeV;186W(20Ne, f), E=142, 174 MeV;198Pt, 197Au, 206Pb(12C, f), E not given;197Au(16O, f), E not given; calculated mass yield (in the case of 16O+184W also the charge distribution employing number of states of two-fragment systems at the saddle point. Compared with published data.
doi: 10.1016/j.nuclphysa.2017.04.002
2015BE19 Phys.Scr. 90, 085301 (2015) P.Belli, R.Bernabei, F.Cappella, R.Cerulli, F.A.Danevich, V.Yu.Denisov, A.d'Angelo, A.Incicchitti, V.V.Kobychev, D.V.Poda, O.G.Polischuk, V.I.Tretyak Search for long-lived superheavy eka-tungsten with radiopure ZnWO4 crystal scintillator RADIOACTIVITY Sg(α); measured decay products; Eα, Iα; deduced a limit on possible concentration of superheavy eka-W (seaborgium Sg, Z = 106) in the crystal. Comparison with available data.
doi: 10.1088/0031-8949/90/8/085301
2015DE03 Phys.Rev. C 91, 024603 (2015) Nucleus-nucleus potential with shell-correction contribution
doi: 10.1103/PhysRevC.91.024603
2015DE20 Phys.Rev. C 92, 014602 (2015) V.Yu.Denisov, O.I.Davidovskaya, I.Yu.Sedykh Improved parametrization of the unified model for α decay and α capture RADIOACTIVITY A=105-115(α); A=150-260(α); analyzed known ground-state-to-ground-state α-transition half-lives for 401 nuclides and determined parameters in the framework of unified model for α decay and α capture (UMADAC). Compared theoretical half-lives extracted from empirical parametrization with experimental values. NUCLEAR REACTIONS 40,44Ca, 59Co, 208Pb, 209Bi(α, X); analyzed α-capture cross sections in the framework of unified model for α decay and α capture (UMADAC).
doi: 10.1103/PhysRevC.92.014602
2015DE41 Ukr.J.Phys. 60, 585 (2015) Minimum Barrier Height for Symmetric and Asymmetric Nuclear Systems NUCLEAR REACTIONS 48Ca(48Ca, X), 68Zn(68Zn, X), 96Zr(96Zr, X), 62Zn(64Zn, X), 78Se(58Fe, X), 96Mo(40Ar, X), 116Sn(20Ne, X), E not given. calculated barrier heights and nuclear deformation parameters.
doi: 10.15407/ujpe60.07.0585
2015NA11 Phys.Atomic Nuclei 78, 215 (2015) M.S.Nadirbekov, G.A.Yuldasheva, V.Yu.Denisov Alternating-parity collective states of yrast and nonyrast bands in lanthanide and actinide nuclei NUCLEAR STRUCTURE 164Er, 220Ra, 224Th, 154Sm, 160Gd, 224Ra, 240Pu; calculated energy levels, J, π. A nonadiabatic collective model with a Gaussian potential energy, comparison with experimental data.
doi: 10.1134/S1063778815010159
2014DE09 Phys.Rev. C 89, 044604 (2014) Nucleus-nucleus potential with shell-correction contribution and deep sub-barrier fusion of heavy nuclei NUCLEAR REACTIONS 16O(208Pb, X), E(cm)=60-110 MeV; 48Ca(48Ca, X), E(cm)=46-61 MeV; 58Ni(54Fe, X), E(cm)=85-110 MeV; calculated fusion σ(E), full and macroscopic potential. Macroscopic and shell-correction parts of the nucleus-nucleus potential using CCFULL code and Woods-Saxon potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.044604
2014DE23 Bull.Rus.Acad.Sci.Phys. 78, 654 (2014); Izv.Akad.Nauk RAS, Ser.Fiz 78, 872 (2014) Isotopic and neutron-excess effects in nucleus-nucleus interaction and fusion cross sections NUCLEAR REACTIONS 118Sn(78Ni, X), 124Sn(64Ni, X), 132Sn(64Ni, X), E<180 MeV; calculated fusion σ. Comparison with experimental data.
doi: 10.3103/S1062873814070089
2013DE33 Phys.Rev. C 88, 044608 (2013) Multidimensional model of cluster radioactivity RADIOACTIVITY 228Th(20O), 232U(24Ne), 236Pu(28Mg), 242Cm(34Si); calculated half-lives for cluster decays, potential energy surface plots. Multidimensional cluster-preformation model. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.044608
2012PI19 Iader.Fiz.Enerh. 13, 346 (2012); Nuc.phys.atom.energ. 13, 346 (2012) Capture cross sections for heavy-ion reactions producing compound system with Z = 120 NUCLEAR REACTIONS 249Cf(50Ti, X), E=220-20 MeV;244Pu(48Ca, X), E=190-210 MeV;248Cm(54Cr, X), E=230-270 MeV;244Pu(58Fe, X), E=250-290 MeV; 238U(64Ni, X), E=270-290 MeV; calculated capture and fusion σ. Comparison to available data.
doi: 10.15407/jnpae
2011DE26 Eur.Phys.J. A 47, 80 (2011) Polarized electric dipole moment of well-deformed reflection asymmetric nuclei NUCLEAR STRUCTURE 218,219,220,221,222,223,224,225,226,227,228Th; calculated polarized electric dipole moment, deformation. Dipole moment compared with data.
doi: 10.1140/epja/i2011-11080-9
2010DA12 Ukr.J.Phys. 55, 861 (2010) O.I.Davidovskaya, V.Yu.Denisov Elastic 16O+16O Scattering and Nucleus-Nucleus Potential with a Repulsive Core NUCLEAR REACTIONS 16O(16O, 16O), E=124, 145, 250, 350, 480 MeV; calculated σ(θ); deduced optical model parameters, nucleus-nucleus potential with repulsive core.
2010DE06 Phys.Rev. C 81, 025805 (2010) Fusion of deformed nuclei: 12C+12C NUCLEAR REACTIONS 12C(12C, X), E=2-10 MeV; analyzed σ, astrophysical S-factors using barrier-penetration model calculations for deformed nuclei. Compariosn with experimental data.
doi: 10.1103/PhysRevC.81.025805
2010DE10 Phys.Atomic Nuclei 73, 404 (2010) V.Yu.Denisov, O.I.Davidovskaya Elastic scattering of heavy nuclei and nucleus-nucleus potential with repulsive core NUCLEAR REACTIONS 12C(16O, 16O), E=132-260 MeV; calculated σ(θ); deduced limitations on repulsive core potential. Optical model.
doi: 10.1134/S1063778810030026
2010DE12 Phys.Rev. C 81, 034613 (2010); Erratum Phys.Rev. C 82, 059903 (2010) α decay of even-even superheavy elements RADIOACTIVITY 256,258,260Rf, 264,266,268,270,272,274Sg, 268,270,272,274,276,278,280Hs, 272,274,276,278,280,282,284,286Ds, 276,278,280,282,284,286,288,290Cn, 280,282,284,286,288,290,292,294Fl, 286,288,290,292,294,296,298Lv, 288,290,292,294,296,298,300,302Og, 292,294,296,298,300,302,304,306120, 296,298,300,302,304,306,308,310122, 300,302,304,306,308,310,312,314124, 304,306,308,310,312,314,316,318126(α); calculated half-lives using the Q values of α transitions obtained within different approximations for atomic masses. Comparisons with experimental data.
doi: 10.1103/PhysRevC.81.034613
2010DE16 Bull.Rus.Acad.Sci.Phys. 74, 554 (2010); Izv.Akad.Nauk RAS, Ser.Fiz 74, 587 (2010) α-Decay half-lives, α-capture cross sections, and α-nucleus interaction NUCLEAR STRUCTURE 40,44Ca, 59Co, 208Pb, 209Bi; calculated probabilities of α-transitions; deduced α-nuclear potential.
doi: 10.3103/S1062873810040283
2010DE20 Bull.Rus.Acad.Sci.Phys. 74, 782 (2010); Izv.Akad.Nauk RAS, Ser.Fiz 74, 818 (2010) The interaction and fusion of arbitrarily oriented deformed nuclei NUCLEAR REACTIONS 24Mg(24Mg, X), 28Si(28Si, X), 154Sm(28Si, X), E=20-130 MeV; 238U, 244Pu(48Ca, X), 248Cm(58Fe, X), E=180-275 MeV; 158Gd(150Nd, X), E=370-420 MeV;calculated capture and fusion σ.
doi: 10.3103/S1062873810060110
2010DE22 Phys.Atomic Nuclei 73, 1142 (2010); Yad.Fiz. 73, 1181 (2010) Effect of the Pauli exclusion principle on the potential of nucleus-nucleus interaction NUCLEAR REACTIONS 16O(16O, X), E not given; calculated nucleon-density distributions, nucleus-nucleus potential.
doi: 10.1134/S1063778810070070
2010DE23 Phys.Atomic Nuclei 73, 1152 (2010); Yad.Fiz. 73, 1191 (2010) Interaction and fusion of deformed nuclei NUCLEAR REACTIONS 24Mg(24Mg, X), 28Si(28Si, X), 154Sm(28Si, X), E=20-130 MeV; 238U, 244Pu(48Ca, X), 248Cm(58Fe, X), E=180-275 MeV; 158Gd(150Nd, X), E=370-420 MeV;calculated capture and fusion σ.
doi: 10.1134/S1063778810070082
2009DE16 Phys.Rev. C 79, 054614 (2009); Erratum Phys.Rev. C 82, 059901 (2010) α-decay half-lives: Empirical relations RADIOACTIVITY Z>82, A>208(α); analyzed α-decay half-lives for ground state to ground state decay. Deduced empirical relations.
doi: 10.1103/PhysRevC.79.054614
2009DE28 Ukr.J.Phys. 54, 669 (2009) V.Yu.Denisov, O.I.Davidovskaya Repulsive Core Potential and Elastic Heavy-Ion Collisions NUCLEAR REACTIONS 16O(12C, 12C), E(cm)=132-200 MeV; calculated σ(θ). Optical model with repulsive core.
2009DE32 Phys.Rev. C 80, 034603 (2009); Erratum Phys.Rev. C 82, 059902 (2010) α decays to ground and excited states of heavy deformed nuclei RADIOACTIVITY 222,224,226Ra, 226,228,230,232Th, 228,230,232,234,235,236,238U, 234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 244,246,248,250,252Cf, 248,250,252Fm, 252No(α); calculated half-lives and branching ratios for g.s. to g.s. decays and g.s. to excited states using Unified model for α decay and α capture (UMADAC). Comparison with experimental data.
doi: 10.1103/PhysRevC.80.034603
2009DE35 Ukr.J.Phys. 54, 1073 (2009) Empirical Relations for α-Decay Half-lives
2009DE55 At.Data Nucl.Data Tables 95, 815 (2009); Erratum At.Data Nucl.Data Tables 97, 187 (2011) α-Decay half-lives, α-capture, and α-nucleus potential NUCLEAR STRUCTURE Z=51-118, A=103-293; calculated α-decay T1/2, deformation parameters. UMADAC framework, comparison with experimental data. NUCLEAR REACTIONS 40,44Ca, 59Co, 208Pb, 209Bi(α, X), E=5-25 MeV; calculated α-capture σ. UMADAC framework, CCFULL calculations, comparison with experimental data.
doi: 10.1016/j.adt.2009.06.003
2009DE56 Iader.Fiz.Enerh. 10, 55 (2009); Nuc.phys.atom.energ. 10, 55 (2009) Fusion of deformed nuclei NUCLEAR REACTIONS 24Mg(24Mg, X), E=20-40 MeV;28Si(28Si, X), E=26-60 MeV;154Sm(28Si, X), E=90-130;calculated nucleus-nucleus potentials, fusion σ. 152Sm(150Nd, X), E=367-410 MeV; calculated di-nuclear capture σ. Comparison to experimental data.
doi: 10.15407/jnpae
2008DE25 Ukr.J.Phys. 53, 845 (2008) Interaction between Two Axially Symmetric Nuclei
2008DE39 Iader.Fiz.Enerh. 9 no.3, 33 (2008); Nuc.phys.atom.energ. 9, no.3, 33 (2008) Alpha-nucleus interaction potential NUCLEAR REACTIONS 40Ca(α, X), E=5-25 MeV; 44Ca(α, X), E=9-25 MeV;59Co(α, X), E=8-25 MeV;208Pb(α, X), E=16-25 MeV;209Bi(α, X), E=16-21 MeV; calculated α capture σ. Comparison with experimental data. RADIOACTIVITY A=102-260(α);calculated T1/2. Cluster model with WKB approximation. Comparison with experimental data.
doi: 10.15407/jnpae
2007DE08 Phys.Atomic Nuclei 70, 244 (2007); Yad.Fiz. 70, 267 (2007) Shell corrections, magic numbers, and mean field NUCLEAR STRUCTURE Z=76-140; calculated shell correction energies, dependence on mean-field parameters. 265,266Hs; calculated binding energies. NUCLEAR REACTIONS 208Pb(58Fe, n), E=216 MeV; calculated compound and residual nucleus binding energies, excitation energies. Several models compared.
doi: 10.1134/S1063778807020056
2007DE32 Phys.Rev. C 76, 014602 (2007) Interaction of two deformed, arbitrarily oriented nuclei NUCLEAR REACTIONS 86Kr(86Kr, X), 248Cm(19F, X), 232Th, 238U, 244Pu, 241,243Am, 248Cm, 249Bk, 249,250Cf(22Ne, X), (26Mg, X)E not given; calculated nucleus-nucleus potentials.
doi: 10.1103/PhysRevC.76.014602
2007DE62 Iader.Fiz.Enerh. 8 no.4, 49 (2007); Nuc.phys.atom.energ. 8, no.4, 49 (2007) Interaction potential between two axially symmetric nuclei NUCLEAR REACTIONS 248Cm(22Ne, X), (26Mg, X), 144Nd(70Zn, X), 150Nd(64Zn, X), E not given; calculated nucleus-nucleus potentials.
doi: 10.15407/jnpae
2006BE42 Eur.Phys.J. A 27, Supplement 1, 35 (2006) R.Bernabei, P.Belli, F.Montecchia, F.Nozzoli, F.Cappella, A.Incicchitti, D.Prosperi, R.Cerulli, C.J.Dai, V.Yu.Denisov, V.I.Tretyak Search for rare processes with DAMA/LXe experiment at Gran Sasso RADIOACTIVITY 136Xe; measured T1/2 lower limits for nucleon, di-nucleon, and tri-nucleon channels.
doi: 10.1140/epja/i2006-08-004-y
2006DE24 Ukr.J.Phys. 51, 440 (2006) Distribution of density and potential of nuclear interaction NUCLEAR REACTIONS 16O(16O, X), 58Ni(58Ni, X), 118Sn(118Sn, X), 208Pb(208Pb, X), 100,114,118,124,132Sn, 208Pb(40Ca, X), E not given; calculated interaction potentials, diffuseness parameter. Skyrme force, extended Thomas-Fermi approximation, Hartree-Fock-BCS theory.
2006DE37 Phys.Atomic Nuclei 69, 1472 (2006); Yad.Fiz. 69, 1507 (2006) Potential of Interaction between Nuclei and Nucleon-Density Distribution in Nuclei NUCLEAR STRUCTURE 48Ca, 208Pb; calculated neutron density distributions. NUCLEAR REACTIONS 48Ca, 208Pb(208Pb, X), 118Sn(118Sn, X), 66Zn(66Zn, X), 16O, 208Pb(16O, X), 100,114,118,124,132Sn(64Ni, X), E not given; calculated interaction potentials. 208Pb(16O, X), E(cm)=65-110 MeV; calculated fusion σ.
doi: 10.1134/S1063778806090067
2006DE41 Phys.Rev. C 74, 055804 (2006) Nuclear reactions in hot stellar matter and nuclear surface deformations NUCLEAR REACTIONS 52Fe, 72,76Kr, 80Sr(p, X), E ≈ 0-12 MeV; 52Fe, 80Sr, 22Ne, 24Mg(α, X), E ≈ 0-12 MeV; 22Ne, 32Mg(16O, X), E ≈ 0-15 MeV; calculated S-factor and σ enhancements for capture reactions in stellar environments.
doi: 10.1103/PhysRevC.74.055804
2005DE35 Yad.Fiz. 68, 1179 (2005); Phys.Atomic Nuclei 68, 1133 (2005) Magic Numbers of Ultraheavy Nuclei NUCLEAR STRUCTURE Z=80-400; calculated shell correction energies. RADIOACTIVITY 298Fl, 472164(α); calculated Qα, T1/2.
doi: 10.1134/1.1992567
2005DE57 Eur.Phys.J. A 25, Supplement 1, 619 (2005) Entrance-channel potentials for hot fusion reactions NUCLEAR REACTIONS 247,249Bk, 254Es(48Ca, X), E not given; calculated semi-microscopic entrance channel potentials.
doi: 10.1140/epjad/i2005-06-106-1
2005DE62 Phys.Rev. C 72, 064613 (2005) α-nucleus potential for α-decay and sub-barrier fusion NUCLEAR REACTIONS 40Ca, 59Co, 208Pb(α, X), E ≈ 5-25 MeV; analyzed fusion σ; deduced α-nucleus potential features. RADIOACTIVITY A=261-294; analyzed α-decay T1/2; deduced α-nucleus potential features.
doi: 10.1103/PhysRevC.72.064613
2005DE65 Iader.Fiz.Enerh. 6 no.2, 46 (2005) Ultraheavy nuclei: shell corrections, magic numbers, fission barriers and alpha-decay periods RADIOACTIVITY 298Fl, 472164(α); calculated Q-values, T1/2. Proton and neutron shell corrections calculated with Green formula. Also for Z=210, 274 and A=616, 798.
doi: 10.15407/jnpae
2004DE47 Acta Phys.Hung.N.S. 19, 121 (2004) Entrance-Channel Potentials in Synthesis of the Heaviest Nuclei, Muon Catalysis of Superheavy Element Formation NUCLEAR REACTIONS 236,238,240,242,244Pu(48Ca, X), E not given; calculated entrance-channel potentials. 208Pb(86Kr, X), E not given; calculated entrance-channel potential, effect of bound muon. Semi-microscopic approach.
doi: 10.1556/APH.19.2004.1-2.17
2004TR07 Pisma Zh.Eksp.Teor.Fiz. 79, 136 (2004); JETP Lett. 79, 106 (2004) V.I.Tretyak, V.Yu.Denisov, Yu.G.Zdesenko New Limits on Dinucleon Decay into Invisible Channels RADIOACTIVITY 2n, 2H; measured T1/2 lower limits for decay to invisible channels.
doi: 10.1134/1.1719123
2003BA42 Phys.Lett. B 563, 23 (2003) H.O.Back, M.Balata, A.de Bari, T.Beau, A.de Bellefon, G.Bellini, J.Benziger, S.Bonetti, C.Buck, B.Caccianiga, L.Cadonati, F.Calaprice, G.Cecchet, M.Chen, A.Di Credico, O.Dadoun, D.D'Angelo, V.Yu.Denisov, A.Derbin, M.Deutsch, F.Elisei, A.Etenko, F.von Feilitzsch, R.Fernholz, R.Ford, D.Franco, B.Freudiger, C.Galbiati, F.Gatti, S.Gazzana, M.G.Giammarchi, D.Giugni, M.Goeger-Neff, A.Goretti, C.Grieb, C.Hagner, G.Heusser, A.Ianni, A.M.Ianni, H.de Kerret, J.Kiko, T.Kirsten, V.Kobychev, G.Korga, G.Korschinek, Y.Kozlov, D.Kryn, M.Laubenstein, E.Litvinovich, C.Lendvai, P.Lombardi, I.Machulin, S.Malvezzi, J.Maneira, I.Manno, D.Manuzio, G.Manuzio, F.Masetti, A.Martemianov, U.Mazzucato, K.McCarty, E.Meroni, L.Miramonti, M.E.Monzani, P.Musico, L.Niedermeier, L.Oberauer, M.Obolensky, F.Ortica, M.Pallavicini, L.Papp, L.Perasso, A.Pocar, O.A.Ponkratenko, R.S.Raghavan, G.Ranucci, A.Razeto, A.Sabelnikov, C.Salvo, R.Scardaoni, D.Schimizzi, S.Schoenert, H.Simgen, T.Shutt, M.Skorokhvatov, O.Smirnov, A.Sonnenschein, A.Sotnikov, S.Sukhotin, V.Tarasenkov, R.Tartaglia, G.Testera, V.I.Tretyak, D.Vignaud, R.B.Vogelaar, V.Vyrodov, M.Wojcik, O.Zaimidoroga, Yu.G.Zdesenko, G.Zuzel New limits on nucleon decays into invisible channels with the BOREXINO counting test facility RADIOACTIVITY 12C(n); 13C(p); measured T1/2 lower limits for bound nucleon decay to invisible channels.
doi: 10.1016/S0370-2693(03)00636-1
2002DE06 Phys.Lett. 526B, 315 (2002) Interaction Potential between Heavy Ions NUCLEAR REACTIONS 16O, 90Zr, 208Pb(16O, X), (90Zr, X), (208Pb, X), E not given; calculated nuclear potentials. Semimicroscopic model.
doi: 10.1016/S0370-2693(01)01513-1
2002DE27 Yad.Fiz. 65, 847 (2002); Phys.Atomic Nuclei 65, 814 (2002) Binding Energies of Nuclei and Their Density Distributions in a Nonlocal Extended Thomas-Fermi Approximation NUCLEAR STRUCTURE 32,40,48,56Ca, 48,50,58,60,62,64,78Ni, 90Zr, 100,114,124,132Sn, 140Ce, 208Pb, 296Fl, 300Og, 302120, 308126; calculated binding energies, radii, chemical potentials, particle density distributions. Nonlocal extended Thomas-Fermi approximation, Skyrme forces.
doi: 10.1134/1.1481472
2002DE58 Eur.Phys.J. A 15, 375 (2002) Entrance channel potentials in the synthesis of the heaviest nuclei NUCLEAR REACTIONS 64Ni, 198Pt, 208Pb, 238U, 252Cf(58Fe, X), 198Pt, 208Pb, 238U, 244Pu, 248Cm, 252Cf(48Ca, X), 198Pt, 208Pb, 238U, 252Cf(50Ti, X), (54Cr, X), (64Ni, X), (70Zn, X), (78Ge, X), 198Pt, 208Pb(86Kr, X), 130,136Xe(124Sn, X), (136Xe, X), 150Nd(136Xe, X), (144Ce, X), 238U(42Ca, X), 238U, 252Cf(58Ni, X), (68Ni, X), (74Se, X), 198Pt, 238U, 252Cf(82Se, X), 244Pu, 248Cm, 252Cf(40Ca, X), 198Pt(40Ar, X), (96Zr, X), (100Mo, X), E not given; calculated semi-microscopic potentials, dependence on deformation, orientation. Implications for superheavy element production discussed.
doi: 10.1140/epja/i2002-10039-3
2002DE70 J.Nucl.Radiochem.Sci. 3, No 1, 23 (2002) Formation of Superheavy Elements and Ternary Fission Fragment Mass Distribution NUCLEAR REACTIONS 207,208,210Pb(62Ni, n), (64Ni, n), E(cm) ≈ 228-242 MeV; 186W, 198Pt(76Ge, n), E(cm) ≈ 234-260 MeV; 180Hf, 192Os(82Se, n), E(cm) ≈ 246-270 MeV; 208Pb(54Cr, n), E(cm) ≈ 196-208 MeV; calculated excitation functions. NUCLEAR STRUCTURE 236U, 258Fm; calculated ternary fission fragment mass distributions.
2001DE23 Prog.Part.Nucl.Phys. 46, 303 (2001) Production of Superheavy Elements in Symmetric Reactions NUCLEAR REACTIONS 130,136Xe(136Xe, n), 207,208,210Pb(58Fe, n), 136Xe(124Sn, n), 208Pb(50Ti, n), E(cm) ≈ 180-320 MeV; calculated excitation functions. Comparisons with data.
doi: 10.1016/S0146-6410(01)00135-1
2001DE63 Iader.Fiz.Enerh. 2 no.1, 42 (2001) Properties of the ground states of spherical atomic nuclei in the frameworks of the extended Thomas-Fermi method NUCLEAR STRUCTURE 32,40,48,56Ca, 48,50,58,60,62,64,78Ni, 90Zr, 100,114,124,132,142,152Sn, 140Ce, 208Pb, 296Fl, 300Og, 302120, 308126, 310126, 436164, 482164; calculated binding energies, radii, chemical potentials, particle density distributions. Nonlocal extended Thomas-Fermi approximation, Skyrme forces.
doi: 10.15407/jnpae
2000BE56 Phys.Lett. 493B, 12 (2000) R.Bernabei, M.Amato, P.Belli, R.Cerulli, C.J.Dai, V.Yu.Denisov, H.L.He, A.Incicchitti, H.H.Kuang, J.M.Ma, F.Montecchia, O.A.Ponkratenko, D.Prosperi, V.I.Tretyak, Yu.G.Zdesenko Search for the Nucleon and Di-Nucleon Decay into Invisible Channels RADIOACTIVITY 129Xe(p), (n); measured T1/2 limits for nucleon and dinucleon decays that do not conserve baryonic number. Gran Sasso underground detector.
doi: 10.1016/S0370-2693(00)01112-6
2000DE09 Phys.Rev. C61, 034606 (2000) Formation of Superheavy Elements in Cold Fusion Reactions NUCLEAR REACTIONS 207,208,210Pb(58Fe, n), (62Ni, n), (64Ni, n), (66Zn, n), (68Zn, n), (70Zn, n), (74Ge, n), (76Ge, n), (78Ge, n), E(cm) ≈ 210-300 MeV; 208Pb(50Ti, n), (54Cr, n), (80Se, n), (82Se, n), (59Co, n), (65Cu, n), (71Ga, n), (75As, n), E(cm) ≈ 180-300 MeV; 209Bi(50Ti, n), (54Cr, n), (59Co, n), (64Ni, n), (70Zn, n), (78Ge, n), E(cm) ≈ 180-230 MeV; calculated excitation functions; deduced reaction mechanism features. Comparisons with data.
doi: 10.1103/PhysRevC.61.034606
2000DE12 Eur.Phys.J. A 7, 87 (2000) Subbarrier Heavy Ion Fusion Enhanced by Nuclear Transfer NUCLEAR REACTIONS 58,62,64Ni(28Si, X), (30Si, X), E(cm)=46-66 MeV; 90,96Zr(40Ca, X), 64Ni(58Ni, X), E(cm)=85-115 MeV; 94,100Mo(28Si, X), E(cm)=66-96 MeV; 58Ni(16O, X), (18O, X), (20O, X), (22O, X), (24O, X), E(cm)=20-40 MeV; 124,126,128,130,132Sn(28Si, X), E(cm)=75-95 MeV; calculated fusion σ, mean induced angular momentum; deduced enhancement due to few-nucleon transfer. Coupled-channels approach, comparisons with data.
doi: 10.1007/s100500050015
2000DE14 Phys.Rev. C61, 044318 (2000) Single- and Double-Phonon Giant Monopole Resonances in a Nonlinear Approach
doi: 10.1103/PhysRevC.61.044318
2000DE27 Acta Phys.Pol. B31, 479 (2000) Production of Superheavy Elements in Cold Fusion Reactions NUCLEAR REACTIONS 207,208,210Pb(58Fe, n), (62Ni, n), (64Ni, n), (74Ge, n), (76Ge, n), (78Ge, n), E(cm)=210-284 MeV; calculated excitation functions.
1999DE38 Yad.Fiz. 62, No 8, 1431 (1999); Phys.Atomic Nuclei 62, 1349 (1999) Subbarrier Fusion of Heavy Ions and Subbarrier Few-Nucleon Transfers: Fusion and nuclei far from the beta-stability line NUCLEAR REACTIONS 100Mo(32S, X), 96Mo(36S, X), E(cm)=70-92 MeV; 58,62,64Ni(28Si, X), (30Si, X), E(cm)=47-64 MeV; 58Ni(16O, X), (18O, X), (20O, X), (22O, X), E(cm)=20-37 MeV; calculated fusion σ; deduced role of transfer channels, low-lying surface vibration.
1999DE44 Yad.Fiz. 62, No 11, 1946 (1999); Phys.Atomic Nuclei 62, 1806 (1999) Mean Angular Momenta of Nuclear-Fission Fragments RADIOACTIVITY 252Cf(SF); calculated fission fragments mean angular momenta. Statistical model calculations, comparison with data. NUCLEAR REACTIONS 232Th(α, F), E=25.8-41.4 MeV; 238U(α, F), E=18.3-30.2 MeV; calculated fission fragments mean angular momenta. Statistical model calculations, comparison with data.
1998DE03 Phys.Rev. C57, 666 (1998) N-Phonon Giant Resonances in the Nonlinear Hydrodynamic Approach and the Nucleon-Nucleon Interaction
doi: 10.1103/PhysRevC.57.666
1998DE11 Yad.Fiz. 61, No 2, 197 (1998); Phys.Atomic Nuclei 61, 149 (1998) One- and Two-Phonon Giant Resonances in the Nonlinear Hydrodynamic Approximation and Equation of State of Nuclear Matter
1998RO11 Nucl.Phys. A632, 275 (1998) G.Royer, R.K.Gupta, V.Yu.Denisov Cluster Radioactivity and Very Asymmetric Fission Through Compact and Creviced Shapes RADIOACTIVITY 222,223,224,226Ra(14C), 228Th(20O), 230Th, 231Pa, 232,233,234U(24Ne), 234,235U, 236,238Pu(28Mg), 238Pu(32Si); calculated cluster decay potential barriers, deformation energy, Q-values, T1/2. Liquid drop model. NUCLEAR STRUCTURE 222,223,224,226Ra, 228,230Th, 231Pa, 232,233,234,235U, 236,238Pu; calculated cluster decay potential barriers, deformation energy, Q-values, T1/2. Liquid drop model.
doi: 10.1016/S0375-9474(97)00801-4
1998VI05 Yad.Fiz. 61, No 9, 1562 (1998); Phys.Atomic Nuclei 61, 1452 (1998) I.N.Vishnevsky, V.Yu.Denisov, V.A.Zheltonozhsky, S.V.Reshitko, L.V.Sadovnikov, N.V.Strilchuk Mean Angular Momenta of Fragments from 232Th Fission NUCLEAR REACTIONS 232Th(n, F)91Rb/97Nb/120In/131Sb/133Sb/132Te/134Te/133I/135I/135Xe, E=14 MeV; measured Eγ, Iγ; deduced fission fragments mean angular momenta, energy distribution parameters. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32213. 1998VI10 Bull.Rus.Acad.Sci.Phys. 62, 1818 (1998) I.N.Vishnevsky, V.Yu.Denisov, V.A.Zheltonozhsky, S.V.Reshitko, L.V.Sadovnikov, N.V.Strilchuk Average Angular Momenta of the 232Th Fission Fragments NUCLEAR REACTIONS 232Th(n, F), (d, F)90Rb/95Nb/117In/130Sb/132Sb/131Te/133Te/132I/134I/133Xe/148Pm, E=14 MeV; measured fission fragments isomeric ratios, average angular momenta. Comparison with model predictions.
1997KU30 Z.Phys. A359, 257 (1997) S.Yu.Kun, V.Yu.Denisov, A.V.Vagov A Quantum Chaotic Clock and Damping of the Coherent Nuclear Rotation in the 28Si + 64Ni Dissipative Collision NUCLEAR REACTIONS 64Ni(28Si, X), E=120-126.75 MeV; analyzed Z=12, 13 fragments σ(E), σ(θ); deduced time power spectra, damping, chaotic effects.
doi: 10.1007/s002180050400
1996DE13 Yad.Fiz. 59, No 1, 78 (1996); Phys.Atomic Nuclei 59, 72 (1996) Multidimensional Semimicroscopic Model of the Subbarrier Fusion of Heavy Ions NUCLEAR REACTIONS, ICPND 64Ni(64Ni, X), E ≈ 90-100 MeV; 74Ge(74Ge, X), E ≈ 110-150 MeV; calculated fusion σ(E).
1996DE29 Yad.Fiz. 59, No 6, 981 (1996); Phys.Atomic Nuclei 59, 938 (1996) V.Yu.Denisov, O.I.Davidovskaya Polarization Electric Dipole Moment in Nonaxial Nuclei NUCLEAR STRUCTURE 218Ra, 148Nd; calculated polarization electric dipole moments, B(E1); 64Zn, 70Ge, 78,80Kr, 92Mo, 106Pd, 144Sm, 206Pb; calculated B(E1). Nonaxial nuclei, nucleon surfaces radii related by linear equation.
1995DE13 Nucl.Phys. A589, 17 (1995) Collective States of Even-Even and Odd Nuclei with β2, β3, ..., β(N) Deformations NUCLEAR STRUCTURE 144,146Ba, 146Ce, 146,148,150Nd, 151Pm, 150Sm, 220,222Rn, 217,219,221Fr, 218,219,220,221,222,223,224,225,226,227,228Ra, 219,223,225,227Ac, 220,221,222,223,224,225,226,228,229Th; calculated levels, B(λ) ratios. Extended generalization of the Davydov-Chaban model.
doi: 10.1016/0375-9474(95)00075-C
1995DE34 Yad.Fiz. 58, No 3, 448 (1995); Phys.Atomic Nuclei 58, 397 (1995) Multidimensional Model of Subbarier Heavy-Ion Fusion NUCLEAR REACTIONS, ICPND 92,96Zr(64Ni, X), E(cm) ≈ 115-165 MeV; 100Mo(64Ni, X), E(cm) ≈ 125-150 MeV; calculated fusion σ(E). Multi-dimensional model.
1994DE06 J.Phys.(London) G20, L43 (1994) Sub-Barrier Fusion of 64Ni + 100Mo NUCLEAR REACTIONS, ICPND 100Mo(64Ni, X), E(cm) ≈ 125-150 MeV; calculated fusion σ(E). Multi-dimensional fusion model, data analysis.
doi: 10.1088/0954-3899/20/2/004
1994MA20 Phys.Rev. C49, 2816 (1994) Collective Modes and Response Functions of Relativistic Asymmetric Nuclear Matter
doi: 10.1103/PhysRevC.49.2816
1993DE08 Yad.Fiz. 56, No 1, 99 (1993); Phys.Atomic Nuclei 56, 57 (1993) V.Yu.Denisov, V.A.Zheltonozhsky, S.V.Reshitko Isomeric Ratios in the Near-Threshold Region in Reactions with Light Charged Particles NUCLEAR REACTIONS, ICPND 184W(p, n), E ≈ 5-21 MeV; 193Ir, 181Ta(α, n), E ≈ 12-24 MeV; 197Au(d, p), E ≈ 4-12 MeV; 198Pt(d, 2n), E=7-14 MeV; measured isomer to ground state σ ratio for residuals.
1993DE18 Yad.Fiz. 56, No 4, 96 (1993); Phys.Atomic Nuclei 56, 477 (1993); CORRIGENDA Phys.Atomic Nuclei 57, 1275 (1994) Collective Excitations in Odd Nuclei with Quadrupole and Octupole Deformations NUCLEAR STRUCTURE 221,223,225Th, 219Ac; calculated levels. 217,210Ra; calculated levels, B(λ) ratio. Simple analytic approach.
1993DZ01 Yad.Fiz. 56, No 3, 30 (1993); Phys.Atomic Nuclei 56, 303 (1993); CORRIGENDA Phys.Atomic Nuclei 57, 1275 (1994) Collective States of Even-Even Nuclei with Quadrupole and Octupole Deformations NUCLEAR STRUCTURE 220,218Ra, 220,222Th; calculated levels, B(λ). Simple analytical model.
1992DE46 Yad.Fiz. 55, 2647 (1992); Sov.J.Nucl.Phys. 55, 1478 (1992) Consistent Calculation of the Polarization Electric Dipole Moment by the Shell-Correction Method NUCLEAR STRUCTURE 220,221,222,223,224,225,226,227,228Th, 218,219,220,221,222,223,224,225,226Ra, 142,143,144,145,146,147Ba; calculated polarization electric dipole moment; deduced dependence on center-of-gravity position. Shell correction method.
1991DE36 Yad.Fiz. 54, 1556 (1991); Sov.J.Nucl.Phys. 54, 952 (1991) Below-Barrier Fusion of Heavy Ions. Symmetric Case NUCLEAR REACTIONS 58Ni(58Ni, X), E(cm)=96 MeV; calculated potential vs internuclear distance, barrier region potential surface contour plots. 58Ni(58Ni, X), E(cm) ≈ 92-112 MeV; calculated fusion σ(E). Shape parametrization of colliding nuclei.
1990DE18 Yad.Fiz. 51, 345 (1990); Sov.J.Nucl.Phys. 51, 221 (1990) Form Factors and Radiative Widths of Giant Multipole Resonances NUCLEAR REACTIONS 58Ni, 89Y(e, e'), E < 32 MeV; analyzed form factor data. 58Ni, 89Y deduced isovector GDR radiative widths.
1990DE30 Yad.Fiz. 51, 1263 (1990); Sov.J.Nucl.Phys. 51, 803 (1990) Interaction Potential of Heavy Ions at Large Distances NUCLEAR REACTIONS 208Pb(16O, 16O), 40Ca(40Ca, 40Ca), 120Sn(120Sn, 120Sn), E not given; calculated corrections to potentials. Point ions, liquid drop model.
1989DE11 Yad.Fiz. 49, 644 (1989) Octupole Deformation and Electric Dipole Transitions in Nuclei NUCLEAR STRUCTURE 217,218,222,224,226,228,230Ra, 220,221,224,226,228Th, 222,224Rn, 224,226,228,230,232U, 144,146Ba, 146Ce; analyzed E1 transition data; deduced static neutron skin role. Nuclei with octupole deformation.
1989DE16 Yad.Fiz. 49, 59 (1989); Sov.J.Nucl.Phys. 49, 38 (1989) Giant Resonances: Zero sound in cold nuclei and first sound in hot nuclei NUCLEAR STRUCTURE 110Sn; calculated GDR width vs temperature. Zero-sound, hydrodynamic resonance excitation.
1988DE12 Yad.Fiz. 47, 52 (1988) Vibrational-Rotational Isovector Giant Resonances in Deformed Nuclei in Gas-Droplet Model NUCLEAR STRUCTURE A=150-250; calculated isovector giant resonance B(E2).
1987DE34 Rev.Roum.Phys. 32, 511 (1987) Isoscalar and Isovector Giant Resonances in the Gas-Droplet Model NUCLEAR STRUCTURE A=40-240; analyzed isoscalar giant quadrupole resonance E, Γ, EWSR. A=20-220; analyzed isoscalar giant octupole resonance E, Γ, EWSR. Gas-Droplet model.
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