NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = L.A.Malov Found 69 matches. 2023MA47 Phys.Rev. C 108, 044302 (2023) L.A.Malov, A.N.Bezbakh, G.G.Adamian, N.V.Antonenko, R.V.Jolos Excitation spectra and electromagnetic transitions between low-lying nonrotational states of odd-proton nuclei with Z = 97 - 109
doi: 10.1103/PhysRevC.108.044302
2022MA46 Phys.Rev. C 106, 034302 (2022) L.A.Malov, A.N.Bezbach, G.G.Adamian, N.V.Antonenko, R.V.Jolos Electromagnetic transitions between low-lying nonrotational states of odd-neutron nuclei in α-decay chains starting from 265, 267, 269Hs RADIOACTIVITY 265,267,269Hs(α); analyzed levels, J, π, reduced γ-transition probabilities of the excited states in α-decay chains of 265,267,269Hs to daughter nuclei up to Fm nuclei using quasiparticle-phonon model. NUCLEAR STRUCTURE 265,267,269Hs, 261,263,265Sg, 257,259,261Rf, 253,255,257No, 249,251,253Fm; calculated levels, J, π, B(E1), B(M1), B(E2), B(E3) using quasiparticle-phonon model.
doi: 10.1103/PhysRevC.106.034302
2022SH07 Phys.Rev. C 105, 024309 (2022) N.Yu.Shirikova, A.V.Sushkov, L.A.Malov, E.A.Kolganova, R.V.Jolos Prediction of the excitation energies of the 2+1 states for superheavy nuclei based on the microscopically derived Grodzins relation NUCLEAR STRUCTURE 256Fm, 260No, 264Rf, 268Sg, 272Hs, 276Ds, 280Cn, 284Fl, 288Lv, 292Og, 296120; calculated J, π, energies of first 2+ states, quadrupole deformation parameters. Grodzins relation derived using the Bohr collective Hamiltonian and the microscopical model of nuclear structure.
doi: 10.1103/PhysRevC.105.024309
2022SH49 Physics of Part.and Nuclei 53, 1138 (2022) N.Y.Shirikova, A.V.Sushkov, L.A.Malov, E.A.Kolganova, R.V.Jolos Microscopically Derived Grodzins Relation and Prediction of the Excitation Energies of the 2+1 States for Some Superheavy Nuclei NUCLEAR STRUCTURE 258Fm, 262No, 266Rf, 270Sg, 274Hs, 278Ds, 282Cn, 286Fl, 290Lv, 294Og, 298120; calculated lowest 2+ syte energies using the microscopic variants of the Grodzins relation.
doi: 10.1134/S1063779622060089
2021AD07 Eur.Phys.J. A 57, 89 (2021) G.G.Adamian, N.V.Antonenko, H.Lenske, L.A.Malov, S.-G.Zhou Self-consistent methods for structure and production of heavy and superheavy nuclei RADIOACTIVITY 295119, 295,297120(α); calculated Q-values, T1/2. Compared with available experimental data.
doi: 10.1140/epja/s10050-021-00375-1
2021MA47 Phys.Rev. C 104, L011304 (2021) L.A.Malov, G.G.Adamian, N.V.Antonenko, H.Lenske Shaping the archipelago of stability by the competition of proton and neutron shell closures NUCLEAR STRUCTURE Z=112-126, N=170-190; calculated ground-state shell correction energies. 298,300,302,304120; calculated ground-state shell correction energies in the nuclei of α-decay chains. 288Fl, 304120; predicted as doubly-magic nuclei after 208Pb. Self-consistent energy-density functional (EDF) theory plus-HFB theory in the framework of microscopic-macroscopic method. Comparison to other theoretical approaches.
doi: 10.1103/PhysRevC.104.L011304
2021MA82 Phys.Rev. C 104, 064303 (2021) L.A.Malov, G.G.Adamian, N.V.Antonenko, H.Lenske Landscape of the island of stability with self-consistent mean-field potentials NUCLEAR STRUCTURE 272Ds; calculated ratio of density-dependent mass and mass of nucleus for proton and neutrons of the spherical nucleus 272Ds. 288Fl, 292Lv, 300120; calculated energy dependencies of the ground-state level-density parameters using mean-field potentials. 243Cm, 251Cf; calculated energies of low-lying one-quasineutron states using phenomenological Woods-Saxon (WS) potentials. 247Bk, 251Es; calculated energies of low-lying one-quasiproton states using phenomenological Woods-Saxon (WS) potentials. 295119, 291Ts, 287Mc, 283Nh, 279Rg; 297120, 293Og, 289Lv, 285Fl, 281Cn; 295120, 291Og, 287Lv, 283Fl, 279Cn; 299120, 295Og, 291Lv, 287Fl, 283Cn; calculated energies, J, π of low-lying one-quasiproton states for α decay chains of 295119 and 295,297,299120. 295119, 291Ts, 287Mc, 283Nh, 279Rg; 296120, 292Og, 288Lv, 284Fl, 280Cn; 297120, 293Og, 289Lv, 285Fl, 281Cn; 295120, 291Og, 287Lv, 283Fl, 279Cn; 299120, 295Og, 291Lv, 287Fl, 283Cn; 301120, 297Og, 293Lv, 289Fl, 285Cn; 304120, 300Og, 296Lv, 292Fl, 288Cn; calculated ground-state shell correction energies for α decay chains of 295119 and 295,296,297,299,301,304120. 286,290Fl, 296,300120; calculated potential energy surfaces in (β2, β4) planes. Microscopic-macroscopic method to calculate the ground-state shell corrections in superheavy nuclei, incorporating effective nucleon mass from the noncovariant energy-density functionals, with Schrodinger-equivalent central and spin-orbit mean-field potentials. Relevance to island of stability of superheavy nuclei and shape coexistence in superheavy nuclei and effect on spectrum of α decay. Comparison with available experimental data.
doi: 10.1103/PhysRevC.104.064303
2020AD06 Phys.Rev. C 101, 034301 (2020) G.G.Adamian, N.V.Antonenko, H.Lenske, L.A.Malov Predictions of identification and production of new superheavy nuclei with Z=119 and 120 ATOMIC MASSES 275,276,277,278,279,280,281,282Ds, 279,280,281,282,283,284,285,286Cn, 281,282,283,284,285,286,287,288,289,290,291,292Fl, 287,288,289,290,291,292,293,294,295,296Lv, 291,292,293,294,295,296,297,298,299,300,301,302Og, 293,294,295,296,297,298,299,300,301,302120, 279,280,281,282,283Rg, 283,284,285,286,287Nh, 287,288,289,290,291Mc, 291,292,293,294,295Ts, 295,296,297,298,299,300,301119; calculated atomic masses, Q(α). Microscopic-macroscopic method with Woods-Saxon potential extracted from the HFB self-consistent consideration. Comparison with other theoretical calculations. NUCLEAR STRUCTURE 279Rg, 283Nh, 287Mc, 291Ts, 295119, 275,277Ds, 279,281Cn, 283,285Fl, 287,289Lv, 291,293Og, 295,297120; calculated low-lying levels, J, π, ground-state shell corrections, Q(α) for the nuclei of α-decay chains of 295119, 295120, and 297120. Microscopic-macroscopic method with Woods-Saxon potential extracted from the HFB self-consistent consideration. Comparison with experimental values, and with other theoretical calculations. NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 249Cf(48Ca, X), (50Ti, X), 238U, 244Pu, 248Cm, (54Cr, X), 238U, 244Pu(58Fe, X), 238U(64Ni, X), 248,249,250,251Cf(48Ti, X), (50Ti, X), 244,245,246,247,248Cm(54Cr, X), 235,236,237,238U, 247,248,249Bk(50Ti, X), E not given; calculated Q-values, evaporation residue production cross sections of superheavy elements. DNS fusion model.
doi: 10.1103/PhysRevC.101.034301
2020JO08 Phys.Atomic Nuclei 83, 550 (2020) R.V.Jolos, E.A.Kolganova, L.A.Malov, E.V.Mardyban, D.A.Sazonov, T.M.Shneidman Phase Transitions and Shape Coexistence in Atomic Nuclei NUCLEAR STRUCTURE 96Zr, 150,152Sm, 152,156Gd, 222Ra, 240Pu, 286Fl; calculated energy levels, J, π, angular momenta, bands, potential energy surfaces.
doi: 10.1134/S1063778820040092
2020RA07 Phys.Rev. C 101, 054315 (2020) A.Rahmatinejad, T.M.Shneidman, N.V.Antonenko, A.N.Bezbakh, G.G.Adamian, L.A.Malov Collective enhancements in the level densities of Dy and Mo isotopes NUCLEAR STRUCTURE 94,96,98Mo, 160,162,164Dy; calculated β2 and β4 deformation parameters, shell corrections, pairing energies, neutron-, and proton-pairing gaps in the ground states, intrinsic level densities, energy dependent level densities, critical temperatures and corresponding critical energies, spin cut-off parameters, number of collective levels, and collective enhancement factors using the superfluid model with single-particle energies from the quasiparticle-phonon model (QPM) and Woods-Saxon potential. Comparison with experimental densities.
doi: 10.1103/PhysRevC.101.054315
2018AD05 Phys.Rev. C 97, 034308 (2018) G.G.Adamian, L.A.Malov, N.V.Antonenko, R.V.Jolos Nonrotational states in isotonic chains of heavy nuclei NUCLEAR STRUCTURE 251Es; calculated energies of single-neutron and proton levels. 251No, 253Fm, 286Fl; calculated potential energy contour in (β2, β4) plane. 243,245,247,249,251Cm, 245,247,249,251,253,255Cf, 249,251,253,255,257,259Fm, 251,253,255,257,259No, 255,257,259,261Rf, 259,261,263,265Sg, 263,265,267,269Hs; calculated equilibrium deformation parameters β2 and β4, ground states, levels, J, π. Microscopic-macroscopic approach using the single-particle Woods-Saxon potential of the quasiparticle-phonon model. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.034308
2018AD21 Eur.Phys.J. A 54, 170 (2018) G.G.Adamian, L.A.Malov, N.V.Antonenko, H.Lenske, K.Wang, S.-G.Zhou Incorporating self-consistent single-particle potentials into the microscopic-macroscopic method
doi: 10.1140/epja/i2018-12603-6
2017AD13 Acta Phys.Pol. B48, 441 (2017) G.G.Adamian, N.V.Antonenko, A.N.Bezbakh, R.V.Jolos, L.A.Malov, K.Wang, S.-G.Zhou, H.Lenske Influence of Properties of Superheavy Nuclei on Their α Decays RADIOACTIVITY 288Mc, 291,293Ts(α); calculated α-decay chains, Qα, mass excess, levels, J, π, T1/2 using microscopic-macroscopic approach based on TCSM (Two-Center Shell Model). NUCLEAR STRUCTURE 291Ts, 287Mc, 283Nh, 279Rg, 275Mt, 271Bh, 267Db, 253Lr, 259Md, 293Ts, 289Mc, 285Nh, 281Rg, 277Mt, 273Bh, 269Db, 265Lr, 261Md, 288Mc, 284Nh, 280Rg, 276Mt, 272Bh, 268Db; calculated low-lying one-quasiparticle levels, J, π, Qα, mass excess.284Nh, 288Mc(α); calculated α-decay scheme (288Mc to 284Nh, 284Nh to 280Rg) using TCSM (Two-Center Shell Model).
doi: 10.5506/APhysPolB.48.441
2017AD29 Phys.Rev. C 96, 044310 (2017) G.G.Adamian, N.V.Antonenko, L.A.Malov, H.Lenske Examination of production and properties of 268-271Hs NUCLEAR REACTIONS 249Cf(22Ne, 3n)268Hs, ECN=35.2 MeV; 249Cf(22Ne, 4n)267Hs, ECN=46 MeV; 248Cm(26Mg, 3n)271Hs, ECN=33.4 MeV; 248Cm(26Mg, 4n)270Hs, ECN=44.8 MeV; 248Cm(26Mg, 5n)269Hs, ECN=50.8 MeV; 244Pu(30Si, 3n)271Hs, ECN=33.4 MeV; 244Pu(30Si, 4n)270Hs, ECN=46 MeV; 244Pu(30Si, 5n)269Hs, ECN=51.4 MeV; 238U(36S, 3n)271Hs, ECN=34.6 MeV; 238U(36S, 4n), 270Hs, ECN=43.6 MeV; 238U(36S, 3n)269Hs, ECN=49.6 MeV; 226Ra(48Ca, 3n)271Hs, ECN=32.8 MeV; 226Ra(48Ca, 4n)270Hs, ECN=38.8 MeV; calculated production σ using dinuclear system model (DNS), and compared with available experimental data. NUCLEAR STRUCTURE 245Pu, 249,252,253Fm, 256,257,259No, 260,261,262,263Rf, 264,265,266,267Sg, 268,269,270,271Hs, 272,273Ds, 277Cn; calculated levels, K- and shape isomers, J, π using microscopic-macroscopic model, and compared with experimental values. 248Fm; calculated quadrupole and hexadecapole deformation parameters as function of elongation parameter in the two-center shell model. 269,270,271Hs, 265,266,267Sg, 261,263Rf; calculated potential energy surfaces in the plane of elongation and deformation parameters. RADIOACTIVITY 277Cn, 273Ds, 269,271Hs, 265,267Sg, 261,263Rf, 257No(α); calculated Q(α), T1/2. Comparison with available experimental values.
doi: 10.1103/PhysRevC.96.044310
2017KA27 Chin.Phys.C 41, 074105 (2017) V.G.Kartavenko, N.V.Antonenko, A.N.Bezbakh, L.A.Malov, N.Yu.Shirikova, A.V.Sushkov, R.V.Jolos Quasiparticle structure of superheavy nuclei in α-decay chains of 285Fl and 291, 293Lv RADIOACTIVITY 285Fl, 281Cn, 277Ds, 273Hs, 269Sg, 265Rf, 291,293Lv, 289Fl, 285Cn, 281Ds, 277Hs, 287Fl, 283Cn, 279Ds, 275Hs, 271Sg(α); calculated the energies of low-lying one-quasiparticle states, J, π. Comparison with available data.
doi: 10.1088/1674-1137/41/7/074105
2015SH07 Eur.Phys.J. A 51, 21 (2015) N.Yu.Shirikova, A.V.Sushkov, L.A.Malov, R.V.Jolos Structure of the low-lying states of the odd-neutron nuclei with Z ≈ 100 NUCLEAR STRUCTURE 245,247,249,251Cm, 247,249,251,253,255Cf, 249,251,253,255,257Fm, 253,255,257,259No, 257,259,261Rf; calculated quadrupole and hexadecupole deformation, single-particle levels, levels, J, π, quasiparticle-phonon structure. Compared with available data.
doi: 10.1140/epja/i2015-15021-4
2014AD23 Phys.Rev. C 90, 034322 (2014) G.G.Adamian, N.V.Antonenko, L.A.Malov, G.Scamps, D.Lacroix Effects of angular dependence of surface diffuseness in deformed nuclei on Coulomb barrier NUCLEAR STRUCTURE 152Sm, 220,238U; calculated neutron, proton density distributions. 220,222,224,226,228,230,232,234Ra, 220,222,224,226,228,230,232,234,236,238Th, 240,242,244,246,248,250,252Cm; calculated isotopic dependency of average surface diffuseness. 226,228,230,232,234,236,238,240U; calculated isotopic dependencies of nucleon density distribution diffuseness. self-consistent calculations. Comparison with phenomenological mean-field potential calculations. NUCLEAR REACTIONS 238U(36S, 36S), (16O, 16O), E not given; calculated dependencies of the Coulomb-barrier heights on the orientation angle. Self-consistent and mean-field potential calculations.
doi: 10.1103/PhysRevC.90.034322
2014AN15 Bull.Rus.Acad.Sci.Phys. 78, 1137 (2014); Izv.Akad.Nauk RAS, Ser.Fiz 78, 1402 (2014) Excited states of deformed nuclei in the quasiparticle-phonon nuclear model NUCLEAR STRUCTURE 251,252,253,254,255Es, 253,252,251,250,249,248,247Cf, 250,251Bk; calculated deformation parameters, energy levels of the ground and lowest nonrotational states.
doi: 10.3103/S1062873814110045
2011AD15 Phys.Rev. C 84, 024324 (2011) G.G.Adamian, N.V.Antonenko, S.N.Kuklin, B.N.Lu, L.A.Malov, S.G.Zhou Behavior of one-quasiparticle levels in odd isotonic chains of heavy nuclei NUCLEAR STRUCTURE 255Fm, 257No, 259Rf, 261Sg, 263Hs; calculated ground state deformation parameters β2 and β4. 239U, 241,243,247Pu, 243,245,247,249Cm, 243,245,247,249,251Cf, 241,243,245,247,249,251,253,255Fm, 245,247,249,251,253,255,257No, 255,257,259Rf, 259,261Sg, 263Hs; calculated one-quasiparticle states in N=147, 149, 151, 153, 155 nuclei. 253No; calculated collective rotational bands. Discussed isomers in odd-A Fm and No nuclei. Two-center shell model (TCSM), quasiparticle-phonon model (QPM), Skyrme-Hartree-Fock-Bogolyubov (SHFB) approach with SLy4 and SkP parameterization. Comparison with experimental data. RADIOACTIVITY 257,257mRf, 257,257mNo(α); calculated Q(α), decay schemes. 253Fm, 253No; deduced levels.
doi: 10.1103/PhysRevC.84.024324
2011BA44 Phys.Atomic Nuclei 74, 1651 (2011) E.B.Balbutsev, L.A.Malov, P.Schuck Spatial dependence of pairing in deformed nuclei NUCLEAR STRUCTURE 134Ba, 174Yb; calculated pairing gaps, coherence lengths. Time-dependent HFB equations.
doi: 10.1134/S1063778811110020
2011JO09 J.Phys.(London) G38, 115103 (2011) R.V.Jolos, L.A.Malov, N.Yu.Shirikova, A.V.Sushkov Structure of some low lying two-quasiparticle and collective states in nuclei with Z ∼ 100 considered in the quasiparticle phonon model NUCLEAR STRUCTURE 246,248Cm, 250,252,254Fm, 248,250,252Cf, 252,254No, 254,256,258,260Rf; calculated energies, J, π for collective states; deduced hexadecouple residual forces. Comparison with experimental data.
doi: 10.1088/0954-3899/38/11/115103
2010AD17 Physics of Part.and Nuclei 41, 1101 (2010) G.G.Adamian, N.V.Antonenko, L.A.Malov, B.N.Lu, S.G.Zhou, W.Scheid Isomeric states in heavy nuclei NUCLEAR STRUCTURE 243Pu, 245Cm, 247Cf, 249Fm, 251No, 270Ds, 266Hs, 262Sg, 258Rf, 254No; calculated one-, two-quasiparticle states and energies, J, π. HB and shell models.
doi: 10.1134/S1063779610070269
2010BA15 Bull.Rus.Acad.Sci.Phys. 74, 857 (2010) Spatial dependence of pair correlations (Nuclear scissors) NUCLEAR STRUCTURE 134Ba; calculated pairing gaps, coherence lengths. Woods-Saxon mean field potential.
doi: 10.3103/S1062873810060262
2008BA15 Bull.Rus.Acad.Sci.Phys. 72, 289 (2008); Izv.Akad.Nauk RAS, Ser.Fiz. 72, 315 (2008) E.B.Balbutsev, L.A.Malov, P.Schuk, M.Urban, X.Vinas Effect of pairing correlations on the nuclear scissors mode NUCLEAR STRUCTURE 134Ba, 144,146,148,150Nd, 148,150,152,154Sm, 156,158,160Gd, 160,162,164Dy, 164,166,168,170Er, 172,174,176Yb, 178,180Hf, 182,184,186W, 190,192Os, 196Pt; calculated scissors mode energies and B(M1) using the generalized method of Wigner function moments.
doi: 10.3103/S1062873808030052
2008BO26 Nucl.Phys. A811, 28 (2008) V.Bondarenko, I.Tomandl, H.-F.Wirth, J.Honzatko, A.M.Sukhovoj, L.A.Malov, L.I.Simonova, R.Hertenberger, T.von Egidy, J.Berzins Nuclear structure of 187W studied with (n, γ) and (d, p) reactions NUCLEAR REACTIONS 186W(n, γ), E=thermal; measured prompt and delayed Eγ, Iγ, γγ-coin; deduced σ. 186W(d, p), E=18, 22 MeV; 186W(polarized d, p), E=18 MeV; measured particle spectra, σ(θ), asymmetry. 187W deduced levels, J, π, branching ratios, neutron binding energy, spectroscopic strengths, band structure. DWBA analysis, quasiparticle-phonon model calculation. Enriched target, Ge detectors, Q3D magnetic spectrograph.
doi: 10.1016/j.nuclphysa.2008.07.017
2003KU44 Bull.Rus.Acad.Sci.Phys. 67, 7 (2003) S.A.Kudrya, V.M.Gorozhankin, K.Ya.Gromov, Sh.R.Malikov, L.A.Malov, V.A.Sergienko, V.I.Fominykh, V.V.Tsupko-Sitnikov, V.G.Chumin, E.A.Yakushev 225Ac → 221Fr alpha decay RADIOACTIVITY 225Ac(α) [from 229Th decay]; measured Eα, Iα, Eγ, Iγ, E(ce), I(ce), αγ-coin; deduced hindrance factors. 221Fr deduced levels, J, π, configurations. Quasiparticle-phonon model analysis.
1998MA93 Bull.Rus.Acad.Sci.Phys. 62, 712 (1998) New Possibilities of Investigating Properties of Deformed Nuclei at the Excitation Energy Up to 20-30 MeV NUCLEAR STRUCTURE 153Sm; calculated single particle states wave function components. Quasiparticle-phonon model, generalized force function.
1997BL11 Nucl.Phys. A624, 433 (1997) N.Blasi, S.Micheletti, M.Pignanelli, R.De Leo, A.Gollwitzer, S.Deylitz, B.D.Valnion, G.Graw, L.A.Malov Study of 153Sm Via the 154Sm(p, d) Reaction NUCLEAR REACTIONS 154Sm(p, d), E=23 MeV; measured σ(Ep, θ). 154Sm deduced levels, J, π. Pick-up reactions, strength distributions.
doi: 10.1016/S0375-9474(97)00383-7
1997BO51 Fiz.Elem.Chastits At.Yadra 22, 1433 (1997); Sov.J.Part.Nucl. 22, 698 (1991) S.T.Boneva, E.V.Vasileva, V.D.Kulik, L.-H.Khiem, L.A.Malov, Y.P.Popov, A.M.Sukhovoi, P.D.Khang, V.A.Khitrov, Y.V.Kholnov, M.R.Beitinsh, V.A.Bondarenko, I.L.Kuvaga, P.T.Prokofev, L.I.Simonova, G.L.Rezvaya Two-photon cascades of radiative neutron capture. II.Fundamental parameters and features of the gamma decay of compound states of complex nuclei
1996MA73 Bull.Rus.Acad.Sci.Phys. 60, 722 (1996) On Electromagnetic Transitions between Highly Excited States in Odd Deformed Nuclei NUCLEAR STRUCTURE 185W; calculated levels, B(λ). Quasiparticle-phonon model.
1992BE17 Z.Phys. A341, 155 (1992) M.R.Beitins, S.T.Boneva, V.A.Khitrov, L.A.Malov, Yu.P.Popov, P.T.Prokofjev, G.L.Rezvaya, L.I.Simonova, A.M.Sukhovoj, E.V.Vasilieva Study of the 187W States Excited in the (n, γ) Reaction NUCLEAR REACTIONS 186W(n, γ), E=thermal; measured Eγ, Iγ, γγ-sum coincidence spectra. 187W deduced levels, J, π, neutron binding energy.
doi: 10.1007/BF01298475
1990DU12 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 1833 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.9, 166 (1990) A.P.Dubensky, V.V.Dubensky, E.A.Boikova, L.A.Malov Photoexcitation Mechanism of Isomeric State 181Ta by γ Quanta of Energy up to 5.5 MeV NUCLEAR REACTIONS 181Ta(γ, γ'), E=3-5.5 MeV bremsstrahlung; measured Eγ, Iγ; deduced reaction mechanism, isomer yield energy dependence. Quasiparticle-phonon model.
1989BO16 Yad.Fiz. 49, 944 (1989) S.T.Boneva, E.V.Vasilieva, L.A.Malov, Yu.P.Popov, A.M.Sukhovoy, V.A.Khitrov Intensive Two-Quantum Cascades and Fragmentation of Quasiparticle States in Some Deformed Nuclei NUCLEAR STRUCTURE 165Dy, 175Yb, 179Hf; calculated Iγ following neutron capture vs excitation; deduced enhancement features. Deformed Woods-Saxon potential.
1985MA05 Z.Phys. A320, 521 (1985) L.A.Malov, F.M.Meliev, V.G.Soloviev Description of Radiative Strength Functions in Deformed Nuclei NUCLEAR STRUCTURE 158Gd, 160,162,164Dy, 166,168Er, 172,174Yb, 176Hf, 232Th, 236,238U; calculated E1, M1 transition strength functions. Quasiparticle-phonon model, RPA comparison.
doi: 10.1007/BF01415730
1985MA61 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2150 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 61 (1985) Calculation of the Neutron s-Wave Strength Function in the Odd Yb, Hf, W and Os Isotopes NUCLEAR STRUCTURE 175,177Yb, 179,181Hf, 181,183,185W, 187Os; calculated s-wave strength function.
1985MA62 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2187 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 97 (1985) Calculation of the Neutron s-Wave Strength Function of the Even Hf and W Isotopes NUCLEAR STRUCTURE 178,180Hf, 182,184W; calculated s-wave neutron strength function. Quasiparticle-phonon model.
1979KI16 Izv.Akad.Nauk SSSR, Ser.Fiz. 43, 2060 (1979); Bull.Acad.Sci.USSR, Phys.Ser. 43, No.10, 36 (1979) V.Kitipova, G.Kyrchev, L.A.Malov Anharmonic and Isovector Effects in the Structure of Low-Lying States with K(π) = 0+, 2+, 0-, 1- of Even-Even Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 166Er, 228Th, 238U, 240Pu; calculated levels, B(Eλ). Qudrupole plus pairing Hamiltonian, anharmonicity, isovector force effects.
1979KO25 Acta Phys.Pol. B10, 649 (1979) The Statistical Direct Reaction Model for the (p, α) Reaction NUCLEAR REACTIONS 162Dy, 166,168Er, 176,178,180Hf(p, α), E=20 MeV; calculated σ. Statistical direct reaction model.
1979KY02 Izv.Akad.Nauk SSSR, Ser.Fiz. 43, 107 (1979); Bull.Acad.Sci.USSR, Phys.Ser. 43, No.1, 88 (1979) Fragmentation of Giant Multipole Resonances among Two-Phonon States in 154Sm NUCLEAR STRUCTURE 154Sm; calculated strength functions, reduced transition probabilities, fragmentation of GDR, T=0, GQR. Quasiparticle phonon model, anharmonic effects.
1978KI15 Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 1842 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.9, 42 (1978) N.A.Kiselev, L.A.Malov, V.O.Nesterenko, V.G.Solovev Calculations of Giant Eλ-Resonances of High Multipolarity in Deformed Nuclei NUCLEAR STRUCTURE 166Er, 238U; calculated force function for excitation of multipoles, λ=4, 5, 6, 7. RPA, semimicroscopic approach.
1978KY01 Nukleonika 23, 133 (1978) G.Kyrchev, L.A.Malov, V.O.Nesterenko, V.G.Soloviev The Description of the Giant Quadrupole Resonance in Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 238U; calculated energies, fragmentation of T=0, 1, GQR resonances. Semimicroscopic method.
1977AK03 J.Phys.(London) G3, 625 (1977) Semi-Microscopic Calculation of the Giant Dipole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 152Sm, 160Gd, 166Er, 174Yb, 178Hf, 186W, 232Th, 234,238U; calculated GDR characteristics. Semi-microscopic model with dipole-dipole forces, pairing.
doi: 10.1088/0305-4616/3/5/009
1977KY01 Yad.Fiz. 25, 951 (1977); Sov.J.Nucl.Phys. 25, 506 (1977) G.Kyrchev, L.A.Malov, V.O.Nesterenko, V.G.Solovev Semi-Microscopic Description of Giant Quadrupole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 150Nd, 152,154Sm, 154,156,158,160Gd, 156,158,160,162,164Dy, 162,164,166,168,170Er, 170,172,174,176Yb, 172,174,176Hf, 228,230,232Th, 232,234,236,238U, 238,240,242Pu, 242,244,246Cm; calculated E2 strength functions.
1977MA21 J.Phys.(London) G3, L-219 (1977) L.A.Malov, V.O.Nesterenko, V.G.Soloviev Low-Energy Octupole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 238U; calculated B(E3).
doi: 10.1088/0305-4616/3/2/012
1977MA43 Yad.Fiz. 26, 729 (1977); Sov.J.Nucl.Phys. 26, 384 (1977) General Regularities of Fragmentation of Single-Particle States in Deformed Nuclei NUCLEAR STRUCTURE 179Hf, 153Sm, 165Dy, 175Yb, 185W, 155Eu, 165Ho, 175Lu, 185Re; calculated fragmentation regularities of single-particle states.
1976IV04 Fiz.Elem.Chastits At.Yadra 7, 450 (1976); Sov.J.Particles Nucl. 7, 175 (1976) S.P.Ivanova, A.L.Komov, L.A.Malov, V.G.Soloviev Two-Quasiparticle and Single-Phonon States of Even-Even Deformed Nuclei in the Region of the Actinides NUCLEAR STRUCTURE 228,230,232Th, 232,234,236,238U, 238,240Pu; calculated energy, structure of 0+ states, β. 244,246,248Cm, 248,250,252Cf, 254,256Fm; calculated β, structure parameters. 254No, 260Rf; calculated structure parameters.
1976MA18 Yad.Fiz. 23, 53 (1976); Sov.J.Nucl.Phys. 23, 27 (1976) Fragmentation of One-Particle States in Deformed Nuclei NUCLEAR STRUCTURE 239U, 169Er; calculated fragmentation of one-particle states.
1976MA42 Phys.Lett. 64B, 247 (1976) L.A.Malov, V.O.Nesterenko, V.G.Soloviev Semimicroscopic Description of Giant Octupole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 150Nd, 154Sm, 154Gd, 162Dy, 166Er, 172Yb, 176Hf, 230,232Th, 234,238U, 244,246Cm; calculated giant octupole resonances, Γ, strength.
doi: 10.1016/0370-2693(76)90191-X
1976MA44 Nucl.Phys. A270, 87 (1976) Fragmentation of Single-Particle States and Neutron Strength Functions In Deformed Nuclei NUCLEAR STRUCTURE 155Sm, 159,161Gd, 161,163,165Dy, 169,171Er, 175Yb, 183,185W, 231,233Th, 233,235,237,239U, 239,241,243Pu, 243,245Cm, 255Fm; calculated neutron strength functions at binding energy.
doi: 10.1016/0375-9474(76)90129-9
1975IV06 Izv.Akad.Nauk SSSR, Ser.Fiz. 39, 1612 (1975); Bull.Acad.Sci.USSR, Phys.Ser. 39, No.8, 38 (1975) S.P.Ivanova, A.L.Komov, L.A.Malov, V.G.Solovev Nonrotational States of Odd Nuclei in the Region 225 ≤ A ≤ 233 NUCLEAR STRUCTURE 225Ra, 229,231,233Th, 233U, 225,227Ac, 231,233Pa; calculated levels, structure parameters.
1975MA09 Phys.Lett. 55B, 17 (1975) L.A.Malov, V.G.Soloviev, V.V.Voronov Level Density for Doubly Odd Deformed Nuclei NUCLEAR STRUCTURE 154Eu, 160Tb, 166Ho, 170Tm, 176Lu, 182Ta, 186Re, 238Np; calculated level density.
doi: 10.1016/0370-2693(75)90175-6
1975MA48 Izv.Akad.Nauk SSSR, Ser.Fiz. 39, 1605 (1975); Bull.Acad.Sci.USSR, Phys.Ser. 39, No.8, 31 (1975) L.A.Malov, V.O.Nesterenko, V.G.Solovev Contribution of Quasiparticle Plus Two Photon Components to the Wave Functions for Low-Lying Nonrotational States of Deformed Nuclei NUCLEAR STRUCTURE 239U, 161Gd; calculated levels, structure parameters.
1975VO06 Yad.Fiz. 21, 40 (1975); Sov.J.Nucl.Phys. 21, 20 (1975) V.V.Voronov, L.A.Malov, V.G.Solovev Calculation of the Level Density in Deformed Nuclei with Allowance for Rotation NUCLEAR STRUCTURE 156,158Gd, 162,164Dy, 168Er, 174Yb, 177Lu, 180,178Hf, 181Ta, 236U, 244Cm; calculated level densities.
1974MA17 Nucl.Phys. A224, 396 (1974) L.A.Malov, V.G.Soloviev, V.V.Voronov Semi-Microscopic Description of the Density of Excited States in Deformed Nuclei NUCLEAR STRUCTURE 153Sm, 156,157,158,159Gd, 162,163,164,165Dy, 167,168,169Er, 172,173,174,175,177Yb, 177Lu, 178,179,180Hf, 181Ta, 184,185W, 236,237,238,239U, 243,244,245Cm; calculated density of states.
doi: 10.1016/0375-9474(74)90695-2
1974VD01 Yad.Fiz. 19, 516 (1974); Sov.J.Nucl.Phys. 19, 260 (1974) A.I.Vdovin, V.V.Voronov, L.A.Malov, V.G.Solovev, C.Stoyanov Mass Number Dependence of the Density of 1/2+ States in the Vicinity of the Neutron Binding Energy NUCLEAR STRUCTURE 139Ba, 141,143Ce, 143,145,147,149Nd, 145,149,153Sm, 157,159Gd, 163,165Dy, 167,169Er, 173,175,177Yb, 179Hf, 185W, 199,201,203Hg, 205Pb calculated level density.
1973IV01 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 911 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.5, 5 (1974) S.P.Ivanova, A.L.Komov, L.A.Malov, V.G.Solovev Nonrotational States of Nuclei with Mass Numbers between 250 and 261 NUCLEAR STRUCTURE 248,250,252Cf, 250,252,254,256Fm, 252,254,256No, 256,258,260Rf; calculated levels, B(E2), B(E3). 251,253Cf, 253,257Fm, 255,257No, 261Rf, 251Es, 257Md, 257Lr; calculated levels.
1972IV02 JINR-E4-6663 (1972) S.P.Ivanova, A.L.Komov, L.A.Malov, V.G.Soloviev Nonrotational States of Some Transcurium Elements
1972SO02 Nucl.Phys. A196, 433 (1972) A Model for Describing the Structure of Highly Excited States in Deformed Nuclei (I) NUCLEAR STRUCTURE 239U; calculated levels, level density at high excitation.
1971GA20 Nucl.Phys. A171, 134 (1971) F.A.Gareev, S.P.Ivanova, L.A.Malov, V.G.Soloviev Single-Particle Energies and Wave Functions for the Saxon-Woods Potential and the Levels of Odd-A Nuclei in the Actinide Region NUCLEAR STRUCTURE 235,237U, 241Pu, 245,247,249Cm, 237Np, 241Am, 249Bk; A=234-250; calculated levels, single-particle energies, wave functions. Saxon-Woods potential, phonon-quasiparticle interaction.
doi: 10.1016/0375-9474(71)90368-X
1971KO08 JINR-P4-5693 (1971) A.L.Komov, L.A.Malov, V.G.Soloviev Non-Rotational States of Odd-Mass Nuclei in the Actinide Region NUCLEAR STRUCTURE 239U, 237,243Pu, 243Cm, 235,239Np, 243Am, 247Bk; calculated non-rotational states, wave functions. Superfluid model.
1971KO31 Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 1550 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 1413 (1972) A.L.Komov, L.A.Malov, V.G.Solovev One-Phonon States in Even-Even Nuclei and Nonrotational States in Some Odd Nuclei in the Actinide Region NUCLEAR STRUCTURE 234,236,238,240U, 236,238,240,242,244Pu, 240,242,244,246,248Cm, 246,248,250Cf, 248,250Fm; calculated 1-phonon states, B(E3). 239U, 235,239Np, 237,243Pu, 243,245Am, 243Cm, 247Bk; calculated non-rotational states.
1971MA41 Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 747 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 686 (1972) L.A.Malov, V.G.Solovev, S.I.Fedotov Nonrational States of Deformed Nuclei with N Odd and 153 < A < 175 NUCLEAR STRUCTURE 153,155Sm, 157,159,161Gd, 159,161Dy, 169,171Er, 167Yb, 173,175Hf; calculated levels, nonrotational states.
1969KO06 Yadern.Fiz. 9, 750 (1969); Soviet J.Nucl.Phys. 9, 436 (1969) A.A.Korneichuk, L.A.Malov, V.G.Solovev, S.I.Fedotov, G.Schulz Quadrupole Single-Phonon States of Even-Even Nuclei in the Region 150 < A < 174 NUCLEAR STRUCTURE A=150-174; calculated quadrupole one-phonon states.
1969MA42 Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 1244 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 1155 (1970) L.A.Malov, V.G.Solovev, U.M.Fainer Nonrotational States of Odd-Z Deformed Nuclei with A between 177 and 187 NUCLEAR STRUCTURE 177Lu, 181Ta, 181,183,185,187Re; calculated levels, nuclear configurations.
1969MA44 Dokl.Akad.Nauk SSSR 186, 299 (1969); Soviet Phys.Doklady 14, 461 (1969) L.A.Malov, V.G.Solovev, U.M.Fainer Quadrupole and Octupole One-Phonon States of Nuclei in the Range 174 < A > 188 NUCLEAR STRUCTURE 174,176,178Yb, 176,178,180Hf, 178,180,182,184,186W, 182,184,186,188Os; calculated β- , γ-vibrational states, octupole K, π = 0, - states, B(E2), B(E3).
1968AR13 Yadern.Fiz. 8, 883 (1968); Soviet J.Nucl.Phys. 8, 514 (1969) D.A.Arsenev, L.A.Malov, V.V.Pashkevich, A.Sobiczewski, V.G.Solovev Equilibrium Deformations of Nuclei in the Region 50 < Z < 82 and 50<N<82 NUCLEAR STRUCTURE 120,122,124,126Xe, 124,126,128,130Ba, 128,130,132Ce, 132Nd; calculated ground-state deformation energies, parameters.
1967MA26 Yadern.Fiz. 5, 566 (1967); Soviet J.Nucl.Phys. 5, 403 (1967) Structure of the Ground and Excited States of Deformed Odd Nuclei in the Actinide Region
1966MA34 Phys.Letters 22, 441 (1966) L.A.Malov, V.G.Soloviev, P.Vogel On the Energies of the Octupole States of Even-Even Nuclei in the Energy Region 228 < A < 254
doi: 10.1016/0031-9163(66)91219-4
1966MA48 Yadern.Fiz. 4, 528 (1966); Soviet J.Nucl.Phys. 4, 376 (1967) L.A.Malov, S.M.Polikanov, V.G.Solovev Structure of Spontaneously Fissionable Isomers
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