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Search: Author = L.A.Malov

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2014AN15      Bull.Rus.Acad.Sci.Phys. 78, 1137 (2014); Izv.Akad.Nauk RAS, Ser.Fiz 78, 1402 (2014)

N.V.Antonenko, L.A.Malov

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
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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
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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
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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
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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
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2010BA15      Bull.Rus.Acad.Sci.Phys. 74, 857 (2010)

E.B.Balbutsev, L.A.Malov

Spatial dependence of pair correlations (Nuclear scissors)

NUCLEAR STRUCTURE 134Ba; calculated pairing gaps, coherence lengths. Woods-Saxon mean field potential.

doi: 10.3103/S1062873810060262
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31650. Data from this article have been entered in the XUNDL database. For more information, click here.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1871.

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
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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
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1985MA61      Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2150 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 61 (1985)

L.A.Malov, D.G.Yakovlev

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)

L.A.Malov, D.G.Yakovlev

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)

M.Kozlowski, L.A.Malov

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)

G.Kyrchev, L.A.Malov

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)

S.V.Akulinichev, L.A.Malov

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1977MA43      Yad.Fiz. 26, 729 (1977); Sov.J.Nucl.Phys. 26, 384 (1977)

L.A.Malov, V.G.Solovev

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)

L.A.Malov, V.G.Solovev

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
Citations: PlumX Metrics

1976MA44      Nucl.Phys. A270, 87 (1976)

L.A.Malov, V.G.Soloviev

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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)

V.G.Soloviev, L.A.Malov

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
Citations: PlumX Metrics

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)

L.A.Malov, V.G.Solovev

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
Citations: PlumX Metrics

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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