NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.V.Jolos Found 205 matches. Showing 1 to 100. [Next]2023JO07 Phys.Atomic Nuclei 86, 165 (2023) Nucleon-Nucleon Interaction As a Basis for Studying the Structure of Heavy Nuclei
doi: 10.1134/S1063778823020072
2023JO09 Int.J.Mod.Phys. E32, 2350042 (2023) R.V.Jolos, E.A.Kolganova, G.Nikoghosyan Collective alpha-mode in the structure of heavy and superheavy nuclei NUCLEAR STRUCTURE 220,222,224,226Rn, 224,226Ra, 228,230Th, 232,234U, 236,238Pu, 240,242Cm, 244,246Cf, 248,250Fm, 252,254No, 256,258Rf, 260,262Sg, 264,266Hs, 268,270Ds; calculated binding energies, α-clusters, α-decay probabilities. Comparison with available data.
doi: 10.1142/S0218301323500428
2023JO11 Int.J.Mod.Phys. E32, 2340002 (2023) R.V.Jolos, E.A.Kolganova, E.V.Mardyban, T.M.Shneidman Reflection-asymmetric mode in the structure of heavy nuclei NUCLEAR STRUCTURE 238,240Pu, 220,222,224,226,228Ra, 152,156Gd, 224,226,228,230,232,234Th, 238U, 144Ba; calculated values of parity splitting as a function of angular momentum, parity splitting in the alternating parity bands; deduced parameters.
doi: 10.1142/S0218301323400025
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
2022MA10 Phys.Rev. C 105, 024321 (2022) E.V.Mardyban, E.A.Kolganova, T.M.Shneidman, R.V.Jolos Evolution of the phenomenologically determined collective potential along the chain of Zr isotopes NUCLEAR STRUCTURE 92,94,96,98,100,102Zn; calculated low-ling collective levels, J, π, B(E2), collective potentials, potential-energy surfaces. Calculations using quadrupole-collective Bohr Hamiltonian. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.024321
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
2022MA66 Phys.Part. and Nucl.Lett. 19, 463 (2022) E.V.Mardyban, T.M.Shneidman, E.A.Kolganova, R.V.Jolos Influence of Triaxiality on the Description of Low-Energy Excitation Spectrum of 96Zr NUCLEAR STRUCTURE 96Zr; calculated potential energies, B(E2); deduced influence of nonaxiality on the description of experimental data, impact of the probabilities of quadrupole transitions by the relative weights of the components with different value of projection K of angular momentum on the symmetry axis.
doi: 10.1134/S1547477122050272
2022MA70 Phys.Part. and Nucl.Lett. 19, 646 (2022) E.V.Mardyban, T.M.Shneidman, E.A.Kolganova, R.V.Jolos Manifestation of Reflection-Asymmetric Deformation in the Structure of Superheavy Nuclei NUCLEAR STRUCTURE 250,252,254,256,258,260,262No, 254,256,258,260,262,264,266Rf, 258,260,262,264,266,268,270Sg, 264,266,268,270,272,274Hs, 268,270,272,274,276,278,280,282Ds; calculated negative parity energy levels, initial parity splitting, transition dipole, quadrupole and octupole moments using the cluster model of a dinuclear system; deduced assessments of the critical angular momenta at which the transition from oscillatory motion to stable reflection-asymmetric deformation.
doi: 10.1134/S1547477122060152
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
2022SH27 Eur.Phys.J. A 58, 98 (2022) N.Yu.Shirikova, A.V.Sushkov, R.V.Jolos Coriolis mixing of the K = 1 and K = 0 mixed symmetry states in the well deformed even-even nuclei NUCLEAR STRUCTURE 156,158,160Gd, 160,162,164Dy; calculated Coriolis mixing matrix elements, eigenvectors of the Hamiltonian matrix. Comparison with Alaga rule.
doi: 10.1140/epja/s10050-022-00748-0
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
2021JO02 Phys.-Usp. 64, 325 (2021) Phase transitions in atomic nuclei NUCLEAR STRUCTURE 96Zr; calculated energy levels, J, π, B(E2), B(M1). Comparison with experimental data.
doi: 10.3367/UFNe.2020.06.038787
2021JO04 Phys.Lett. B 820, 136581 (2021) Derivation of the Grodzins relation in collective nuclear model NUCLEAR STRUCTURE 156,158,160,162,164,166,168,170,172,174,176,178Yb; analyzed available data; deduced the proportionality coefficient for the Grodzins relation using the Bohr collective quadrupole Hamiltonian and a microscopic approach.
doi: 10.1016/j.physletb.2021.136581
2021JO06 Int.J.Mod.Phys. E30, 2150083 (2021) R.V.Jolos, E.A.Kolganova, D.A.Sazonov Collective model with isovector pair and alpha-particle-type correlations NUCLEAR STRUCTURE 56Ni, 52Fe, 60Zn, 48Cr, 64Ge; analyzed available data; deduced relative energies of the ground states of even-even nuclei, relative σ for α-transfer, collective Hamiltonian including isovector pairing and α-particle-type correlation degrees of freedom.
doi: 10.1142/S021830132150083X
2020BE22 Phys.Rev.Lett. 125, 092501 (2020) T.Beck, V.Werner, N.Pietralla, M.Bhike, N.Cooper, U.Friman-Gayer, J.Isaak, R.V.Jolos, J.Kleemann, Krishichayan, O.Papst, W.Tornow, C.Bernards, B.P.Crider, R.S.Ilieva, B.Loher, C.Mihai, F.Naqvi, S.Pascu, E.E.Peters, F.M.Prados-Estevez, T.J.Ross, D.Savran, J.R.Vanhoy, A.Zilges ΔK = 0 m1 Excitation Strength of the Well-Deformed Nucleus 164Dy from K Mixing NUCLEAR REACTIONS 164Dy(γ, γ'), E=3-3.2 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, B(M1), reduced relative decay-intensity ratios, excitation strengths.
doi: 10.1103/PhysRevLett.125.092501
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
2020MA32 Phys.Atomic Nuclei 83, 53 (2020) E.V.Mardyban, T.M.Shneidman, E.A.Kolganova, R.V.Jolos Description of Stabilization of Octupole Deformation in Alternating-Parity Bands of Heavy Nuclei
doi: 10.1134/S1063778820010093
2020MA44 Phys.Rev. C 102, 034308 (2020) E.V.Mardyban, E.A.Kolganova, T.M.Shneidman, R.V.Jolos, N.Pietralla Description of the low-lying collective states of 96Zr based on the collective Bohr Hamiltonian including the triaxiality degree of freedom NUCLEAR STRUCTURE 96Zr; calculated levels, J, π, B(E2), B(M1), quadrupole moment, ρ2 for E0 transitions, potential energy surfaces in (β, γ) planes using geometrical collective model for low-lying positive-parity states. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.034308
2019HE04 Phys.Rev. C 99, 034323 (2019) A.Heusler, R.V.Jolos, P.von Brentano Description of one-particle one-hole configurations coupled to the 3- yrast state in the doubly magic nucleus 208Pb NUCLEAR STRUCTURE 208Pb; analyzed experimental data for levels, J, π, multiplets and IARs to describe coupling of the 3- yrast state in 208Pb to one-particle one-hole configurations using particle-phonon coupling model taken to second order.
doi: 10.1103/PhysRevC.99.034323
2019JO05 Phys.Atomic Nuclei 82, 117 (2019) R.V.Jolos, E.A.Kolganova, D.A.Sazonov Decoupling Parameter for Rotational Bands Based on Mixed-Symmetry States
doi: 10.1134/S1063778819020078
2019NI13 Eur.Phys.J. A 55, 189 (2019) G.Nikoghosyan, E.A.Kolganova, D.A.Sazonov, R.V.Jolos Collective treatment of the isovector pair correlations: Boson representation
doi: 10.1140/epja/i2019-12897-8
2019SA20 Phys.Rev. C 99, 031304 (2019) D.A.Sazonov, E.A.Kolganova, T.M.Shneidman, R.V.Jolos, N.Pietralla, W.Witt Description of shape coexistence in 96Zr based on the quadrupole-collective Bohr Hamiltonian NUCLEAR STRUCTURE 96Zr; calculated low-lying levels, J, π, B(E2), B(M1), ρ2 for E0 transitions, quadrupole moment for 2+, wave functions of the first and second 0+ and 2+ states, and shape coexistent potential using quadrupole-collective Bohr Hamiltonian with the potential having two minima corresponding to spherical and deformed shapes. Comparison with experimental values.
doi: 10.1103/PhysRevC.99.031304
2019SH18 Phys.Rev. C 99, 044319 (2019) N.Yu.Shirikova, A.V.Sushkov, R.V.Jolos, N.Pietralla, T.Beck Excitation energy dependence of the moments of inertia of well deformed nuclei NUCLEAR STRUCTURE 156,158Gd, 160,162,164Dy, 166Er, 178Hf; calculated energies and moments of inertia of 2+ γ-vibrational states, and Kπ=1+ excited states using quasiparticle phonon model with a mean field part, monopole pairing, and multipole-multipole residual interaction; discussed contribution from blocking effect and the Coriolis coupling between quasiparticles and the rotating core. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.044319
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
2018JO03 Physics of Part.and Nuclei 49, 125 (2018) R.V.Jolos, V.G.Kartavenko, E.A.Kolganova Nucleon Isovector Pairing in Nuclei: Microscopic Approach, Boson Representation, and Collective Model NUCLEAR STRUCTURE 56Ni; calculated spectroscopic factors, level energies, J, π. Comparison with available data.
doi: 10.1134/S1063779618020028
2018MA67 Chin.Phys.C 42, 124104 (2018) E.V.Mardyban, T.M.Shneidman, E.A.Kolganova, R.V.Jolos, S.-G.Zhou Analytical description of shape transition in nuclear alternating parity bands NUCLEAR STRUCTURE 222,224,226,228Ra, 224,226,228,230,232,234,236Th, 230,232,234,236,238,240U, 238,240,242,244Pu; calculated parity splitting as a function of angular momentum, transitional dipole moments, E1 matrix element. Comparison with available data.
doi: 10.1088/1674-1137/42/12/124104
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
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
2016CH44 Phys.Rev. C 94, 044301 (2016) Q.B.Chen, S.Q.Zhang, P.W.Zhao, R.V.Jolos, J.Meng Two-dimensional collective Hamiltonian for chiral and wobbling modes
doi: 10.1103/PhysRevC.94.044301
2016HE04 Phys.Rev. C 93, 054321 (2016) A.Heusler, R.V.Jolos, T.Faestermann, R.Hertenberger, H.-F.Wirth, P.von Brentano Complete identification of states in 208Pb below Ex = 6.2 MeV NUCLEAR REACTIONS 208Pb(p, p'), E=14.8-18.1 MeV; 208Pb(d, d'), E=22.0, 24.0 MeV; 207Pb(d, p), E=22.0, 24.0 MeV; measured E(p), I(p), E(d), I(d), differential σ(E), σ(θ) using Q3D magnetic spectrograph at MLL-LMU-Munich and TUM-Garching. Enriched 207Pb target contained small amounts of 206,208Pb. 208Pb; deduced levels, levels populated through seven known isobaric analog resonances in 209Bi, J, π, configurations, multi-particle-hole states, natural-parity states, wave function amplitudes, centroid energies for groups of states; discussed completeness of states at E<6.2 MeV. Comparison with states in 208Pb populated via previously studied reactions, and with evaluated data in Nuclear Data Sheets for A=208 nuclides. 209Bi; deduced new isobaric analog resonance at E=17.60 MeV. Comparison with shell-model calculations for 1p-1h and 2p-2h configurations. Systematics of levels in 207Tl, 209Bi, 207Pb and 209Pb.
doi: 10.1103/PhysRevC.93.054321
2016NE06 Phys.Rev. C 93, 034301 (2016) V.O.Nesterenko, V.G.Kartavenko, W.Kleinig, J.Kvasil, A.Repko, R.V.Jolos, P.-G.Reinhard Skyrme random-phase-approximation description of lowest Kπ = 2+γ states in axially deformed nuclei NUCLEAR STRUCTURE 150,152Nd, 152,154,156Sm, 154,156,158,160Gd, 158,160,162,164,166Dy, 162,164,166,168,170Er, 168,170,172,174,176Yb, 168,170,172,174,176,178,180Hf, 178,180,182,184,186W, 232,234,236,238U; calculated energies and B(E2) of the lowest quadrupole γ-vibrational Kπ=2+ states in axially deformed rare-earth and uranium even-even nuclei. 152Nd, 164Dy, 172Yb, 238U; calculated isoscalar strength function for the ISGQR. Separable random-phase-approximation (SRPA) method based on the Skyrme functional with the Skyrme forces SV-bas and SkM*, and corrected by using pairing blocking effect. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034301
2016WI08 Phys.Rev. C 94, 044302 (2016) J.Wiederhold, R.Kern, C.Lizarazo, N.Pietralla, V.Werner, R.V.Jolos, D.Bucurescu, N.Florea, D.Ghita, T.Glodariu, R.Lica, N.Marginean, R.Marginean, C.Mihai, R.Mihai, I.O.Mitu, A.Negret, C.Nita, A.Olacel, S.Pascu, L.Stroe, S.Toma, A.Turturica Fast-timing lifetime measurement of 152Gd NUCLEAR REACTIONS 149Sm(α, n), E=17.5 MeV; measured Eγ, γγ-coin, level half-lives by γγ(t) fast timing technique (FEST) at NIPNE-Bucharest Tandem accelerator facility. 152Gd; deduced levels, B(E2), E0 transition strength for excited 0+ state to the ground state, indication of a quantum phase transition (QPT). Comparison with previous experimental results. Systematics of B(E2) products and E0 strength for 146,148,150,152,154,156,158Gd, 148,150,152,154Sm. RADIOACTIVITY 152Eu(β-), (EC); measured Eγ, level half-lives by γγ(t) fast-timing technique. 152Gd, 152Sm; deduced levels, B(E2).
doi: 10.1103/PhysRevC.94.044302
2015BE20 Phys.Rev. C 92, 014329 (2015) A.N.Bezbakh, V.G.Kartavenko, G.G.Adamian, N.V.Antonenko, R.V.Jolos, V.O.Nesterenko Quasiparticle structure of superheavy nuclei along the α-decay chain of 288115 NUCLEAR STRUCTURE 268Db, 272Bh, 276Mt, 280Rg, 284Nh, 288Mc; calculated one-quasiproton and one-quasineutron spectra, low-lying two-quasiparticle (neutron-proton) spectra using microscopic Skyrme Hartree-Fock (SHF) approach, and modified two-center shell model (TCSM), with pairing treated at BCS level. RADIOACTIVITY 272Bh, 276Mt, 280Rg, 284Nh, 288Mc(α); calculated Q(α) for ground state and isomer decays. 268Db, 272Bh, 276Mt, 280Rg, 284Nh; calculated decay schemes following α decays, predicted transitions, multipolarities, isomers, two-quasiparticle configurations using microscopic Skyrme Hartree-Fock (SHF) approach, and modified two-center shell model (TCSM), with pairing treated at BCS level. Predicted strong E1, M1 and M2 transitions in 276Mt. Comparison with experimental Q(α) values and available α spectra.
doi: 10.1103/PhysRevC.92.014329
2015JO09 Phys.Rev. C 92, 011302 (2015) R.V.Jolos, A.Heusler, P.von Brentano Proton pairing vibrational states around the doubly magic nucleus 208Pb NUCLEAR STRUCTURE 202Os, 204Pt, 202Os, 206Hg, 208Pb, 210Po, 212Rn, 214Ra, 202,204,206,208,210,212,214Pb; calculated excitation energies of 0+ proton pairing vibrational states around doubly magic 208Pb nucleus, and binding energies using the model of pair addition and pair removal phonons; deduced ratio of pairing force for neutrons and protons from shell model.
doi: 10.1103/PhysRevC.92.011302
2015JO13 Phys.Rev. C 92, 044318 (2015) Stabilization of octupole deformation with angular-momentum increase in the alternating-parity bands NUCLEAR STRUCTURE 144,146Ba, 150,152Sm, 152,156Gd, 218,220,222,224,226Ra, 224,226,228,230,232Th, 238U, 240Pu; analyzed energy levels of the ground state alternating parity bands based on the ratio of the interpolated and the experimental energies of the negative-parity states; deduced stabilization of the octupole deformation with angular-momentum increase.
doi: 10.1103/PhysRevC.92.044318
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
2015SH28 Phys.Rev. C 92, 034302 (2015) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, R.V.Jolos, S.-G.Zhou Cluster approach to the structure of 240Pu NUCLEAR STRUCTURE 240Pu; calculated levels, J, π, rotational bands, parity splitting, average mass asymmetry, B(E2), B(E1), transition dipole moment D0, D0/q0 ratio, B(E1)/B(E2) ratio. Positive parity 0+2 rotational band, alternating-parity rotational bands. Cluster approach, with shape deformation parameters and cluster degrees of freedom. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.034302
2014JO06 Int.J.Mod.Phys. E23, 1450051 (2014) R.V.Jolos, N.Yu.Shirikova, A.V.Sushkov Relation between the mass coefficients for rotational and γ-vibrational motion in axially symmetric deformed nuclei NUCLEAR STRUCTURE 154Sm, 156,158Gd, 158,160,162,164Dy, 162,164,166,168Er, 168,170Yb, 174,176,178Hf; calculated values of the ratio of the mass coefficients.
doi: 10.1142/S0218301314500517
2014JO07 Phys.Atomic Nuclei 77, 983 (2014) Signature and parity splitting in the rotational bands and the chiral bands. Double-minimum potential model NUCLEAR STRUCTURE 232Th, 238U, 240Pu; calculated energy levels of lowest negative parity band. Comparison with experimental data.
doi: 10.1134/S1063778814070096
2013CH07 Phys.Rev. C 87, 024314 (2013) Q.B.Chen, S.Q.Zhang, P.W.Zhao, R.V.Jolos, J.Meng Collective Hamiltonian for chiral modes
doi: 10.1103/PhysRevC.87.024314
2013HE19 Phys.Atomic Nuclei 76, 807 (2013) A.Heusler, R.V.Jolos, P.von Brentano Excitation energies of particle-hole states in 208Pb and the surface delta interaction NUCLEAR STRUCTURE 208Pb; calculated energy levels, J, π. Schematic shell model without residual interaction.
doi: 10.1134/S1063778813070065
2013JO04 Phys.Atomic Nuclei 76, 557 (2013) R.V.Jolos, N.Yu.Shirikova, A.V.Sushkov Relation Between the Mass Coefficients for Rotational and γ-Vibrational Modes in Well-Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 156,158Gd, 158,160,162,164Dy, 162Er; calculated mass coefficients for γ-vibrational and rotational motion. QRPA framework, comparison with available data.
doi: 10.1134/S1063778813050050
2013JO05 Phys.Rev. C 88, 034306 (2013) R.V.Jolos, P.von Brentano, R.F.Casten Anharmonicity of the excited octupole band in actinides using supersymmetric quantum mechanics NUCLEAR STRUCTURE 232Th, 238U, 240Pu; calculated levels, J, π of ground-state, octupole and alternating parity bands. E1 and E2 transition matrix elements. Supersymmetric quantum mechanical techniques. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.034306
2013SH45 Phys.Rev. C 88, 064319 (2013) N.Yu.Shirikova, A.V.Sushkov, R.V.Jolos Low-lying excited states of the odd-proton nuclei with Z ≈ 100 NUCLEAR STRUCTURE 239,243,245,247,249,251Bk, 243,245,247,249,251,253,255Es, 247,249,251,253,255,257Md, 253,255Lr, 253,261,263Db; calculated low-lying levels, J, π, wave functions using Quasiparticle-phonon model. Role of excitation of phonons and the quasiparticle-phonon interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.064319
2012JO01 Rom.J.Phys. 57, 288 (2012) Particle-core Coupling Model Approach to Structure of the Low-Lying States of 11B and the Effect of the Pauli Blocking NUCLEAR STRUCTURE 11B, 11C; calculated dipole magnetic and electric quadrupole moments, B(M1), B(E2), B(GT).
2012JO02 Phys.Rev. C 86, 024319 (2012) R.V.Jolos, P.von Brentano, J.Jolie Second order phase transitions from octupole-nondeformed to octupole-deformed shape in the alternating parity bands of nuclei around 240Pu based on data NUCLEAR STRUCTURE 232Th, 238U, 240Pu; calculated potential energy of the octupole collective motion as function of β3 parameter and angular momentum; analyzed levels, J, π, ground-state alternating parity bands. Supersymmetric quantum mechanics, two-center octupole wave functions ansatz, and Landau theory of phase transitions. Evidence for second order phase transition from reflection-symmetric to reflection-asymmetric shapes.
doi: 10.1103/PhysRevC.86.024319
2012JO05 Phys.Rev. C 86, 044320 (2012) R.V.Jolos, N.Yi.Shirikova, A.V.Sushkov Neutron number dependence of the energies of the γ-vibrational states in nuclei with Z ∼ 100 and the manifestation of pseudospin symmetry NUCLEAR STRUCTURE 246,248Cm, 248,250,252,254,256Cf, 250,252,254,256,258Fm, 252,254,256,258,260No, 254,256,258,260,262Rf; calculated level energies and configurations of 2+ γ-vibrational states using quasiparticle-phonon model. Splitting of pseudospin doublets. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044320
2011DA15 Phys.Rev. C 84, 024302 (2011) J.Darai, J.Cseh, N.V.Antonenko, G.Royer, A.Algora, P.O.Hess, R.V.Jolos, W.Scheid Clusterization in the shape isomers of the 56Ni nucleus NUCLEAR STRUCTURE 56Ni; calculated energetics and deformation parameters of shape isomers, triaxial, superdeformed and hyperdeformed structures with binary cluster configurations. Quasimolecular shape sequence. Generalized Liquid Drop Model. Quasidynamical U(3) symmetry based on a Nilsson calculation.
doi: 10.1103/PhysRevC.84.024302
2011JO04 Phys.Rev. C 84, 014315 (2011) R.V.Jolos, N.Pietralla, N.Yu.Shirikova, V.V.Voronov Schematic microscopic approach to the description of M1 transitions between mixed-symmetry and fully symmetric collective states in γ -soft nuclei based on RPA-IBM boson mapping NUCLEAR STRUCTURE 124,126,128,130,132,134Xe; calculated 2+ mixed-symmetry states, configurations, B(M1), B(M1) ratios. Extended Random-phase approximation plus interacting boson model. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.014315
2011JO07 Phys.Rev. C 84, 024312 (2011) Parity splitting and E1/E2 branching in the alternating parity band of 240Pu from two-center octupole wave functions using supersymmetric quantum mechanics NUCLEAR STRUCTURE 240Pu; calculated level energies of the ground state alternating parity bands, J, π, B(E1)/B(E2). Two-center octupole wave functions using supersymmetric quantum mechanics. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024312
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
2011SH06 Acta Phys.Pol. B42, 481 (2011) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, R.V.Jolos, W.Scheid Multiple Reflection Asymmetric Type Band Structures in 220Th and Dinuclear Model NUCLEAR STRUCTURE 220Th; analyzed lowest negative parity bands; calculated energies, J, π, parity splitting, B(E1)/B(E2). Dinuclear system model, comparison with experimental data.
doi: 10.5506/APhysPolB.42.481
2011SH09 Eur.Phys.J. A 47, 34 (2011) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, R.V.Jolos, W.Scheid Multiple reflection-asymmetric-type band structures in 220Th and dinuclear model NUCLEAR STRUCTURE 220Th; calculated levels, J, π, B(E1), B(E2), rotational band, bands using dinuclear model with collective motion in mass asymmetry. Comparison with data.
doi: 10.1140/epja/i2011-11034-3
2010DA20 J.Phys.:Conf.Ser. 205, 012022 (2010) J.Darai, J.Cseh, A.Lepine-Szily, A.Algora, P.O.Hess, N.V.Antonenko, R.V.Jolos, W.Scheid Exotic shapes and clusterization of atomic nuclei NUCLEAR STRUCTURE 36Ar; calculated quadrupole deformation, rotational band, yrast, superdeformed band, hyperdeformed band, shape isomers using dynamical U(3) symmetry based on Nilsson model. NUCLEAR REACTIONS 24Mg(12C, X), 20Ne(16O, X), E not given; calculated hyperdeformed bands in 36Ar.
doi: 10.1088/1742-6596/205/1/012022
2010KR12 J.Phys.:Conf.Ser. 205, 012037 (2010) A.Krugmann, J.Bonnet, N.Pietralla, R.V.Jolos E0 transition strengths from X(5) to the rigid rotor NUCLEAR STRUCTURE Sm, Gd; calculated B(E0), B(E2), scaling factor within CBS (confined β-soft rotor model).
doi: 10.1088/1742-6596/205/1/0120367
2010RA05 Phys.Lett. B 683, 11 (2010) G.Rainovski, N.Pietralla, T.Ahn, L.Coquard, C.J.Lister, R.V.F.Janssens, M.P.Carpenter, S.Zhu, L.Bettermann, J.Jolie, W.Rother, R.V.Jolos, V.Werner How close to the O(6) symmetry is the nucleus 124Xe? NUCLEAR REACTIONS 12C(124Xe, 124Xe'), E=394 MeV; measured Eγ, Iγ, γγ-coin using DSA technique and the Gammasphere array. 124Xe; deduced levels, J, π, B(E2). Comparison with interacting boson model.
doi: 10.1016/j.physletb.2009.12.007
2009BO10 Phys.Rev. C 79, 034307 (2009) J.Bonnet, A.Krugmann, J.Beller, N.Pietralla, R.V.Jolos E0 transition strengths from X(5) to the rigid rotor NUCLEAR STRUCTURE 152Sm, 156Gd; calculated E0 transition strengths and stiffness parameters between ground-state and β bands within the framework of confined β soft rotor model. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.034307
2009JO02 Phys.Rev. C 79, 044310 (2009) Mass tensor in the Bohr Hamiltonian from the nondiagonal energy weighted sum rules NUCLEAR STRUCTURE 106,108,110Pd, 110,112,114Cd, 134Ba, 150Nd, 150,152,154Sm, 154,156,158,160Gd, 164Dy, 172Yb, 178Hf, 188,190,192Os, 194,196Pt; calculated matrix elements of the deformation dependent components of mass tensor in the Bohr Hamiltonian from the nondiagonal energy weighted sum rules. Comparisons with experimental data for E2 transition rates.
doi: 10.1103/PhysRevC.79.044310
2009JO05 Phys.Rev. C 80, 034308 (2009) X(5)* model and the N=90 nuclei NUCLEAR STRUCTURE 150Nd, 152Sm, 154Gd; calculated B(E2) values of intraband and the interband E2 transitions in ground, β, and γ bands using the X(5) Hamiltonian. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.034308
2009SH41 Eur.Phys.J. A 41, 393 (2009) N.Yu.Shirikova, R.V.Jolos, N.Pietralla, A.V.Sushkov, V.V.Voronov E0 transitional density for nuclei between spherical and deformed shapes NUCLEAR STRUCTURE 150Nd; calculated E0 transition density, matrix elements using the Generator Coordinate Method.
doi: 10.1140/epja/i2009-10831-5
2008JO05 Phys.Rev. C 77, 064317 (2008) Bohr Hamiltonian for collective low-lying vibrational states of well deformed nuclei
doi: 10.1103/PhysRevC.77.064317
2008JO08 Phys.Rev. C 78, 064309 (2008) Bohr Hamiltonian, mass coefficients, and the structure of well deformed axially symmetric nuclei NUCLEAR STRUCTURE 154Sm, 156Gd, 172Yb, 182W; calculated Grodzins products, B(E2), level energies. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.064309
2008PE18 Eur.Phys.J. A 36, 127 (2008) P.Petkov, P.von Brentano, J.Jolie, R.V.Jolos Particle-triaxial rotor calculations for the low-lying states with negative parity in 193Os NUCLEAR STRUCTURE 193Os; calculated excited energy levels, J, π using a particle-triaxial rotor model.
doi: 10.1140/epja/i2007-10586-y
2007AD23 Int.J.Mod.Phys. E16, 1021 (2007) G.G.Adamian, N.V.Antonenko, R.V.Jolos, S.P.Ivanova, Yu.V.Palchikov, T.M.Shneidman, A.Andreev, W.Scheid Nuclear Molecules
doi: 10.1142/S0218301307006472
2007AD24 Phys.Atomic Nuclei 70, 1350 (2007) G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, T.M.Shneidman, W.Scheid Nuclear structure in the dinuclear model with rotating clusters NUCLEAR STRUCTURE 238U; calculated level energies, J, π using the dinuclear-system model.
doi: 10.1134/S1063778807080054
2007JO07 Phys.Atomic Nuclei 70, 812 (2007) Pseudospin Symmetry and Structure of Nuclei with Z ≥ 100 NUCLEAR STRUCTURE Z > 99; calculated level energies, J, π in the framework of the relativistic mean field approach including a pseudospin dependence of the residual forces in nuclei.
doi: 10.1134/S106377880705002X
2007JO11 Phys.Rev. C 76, 024309 (2007) Bohr Hamiltonian with different mass coefficients for the ground- and γ bands from experimental data
doi: 10.1103/PhysRevC.76.024309
2007MI01 J.Phys.(London) G34, 299 (2007) N.Minkov, P.Yotov, R.V.Jolos, W.Scheid Intrinsic origin of the high order angular momentum terms in an nuclear rotation Hamiltonian
doi: 10.1088/0954-3899/34/2/010
2007PE29 Phys.Rev. C 76, 044318 (2007); Erratum Phys.Rev. C 77, 019902 (2008) P.Petkov, P.von Brentano, J.Jolie, R.V.Jolos Doublet structure of the negative-parity states in 195Pt supported by particle-rotor calculations NUCLEAR STRUCTURE 195Pt; calculated levels, J, π, B(E2). Compared with experimental values. Particle-rotor model.
doi: 10.1103/PhysRevC.76.044318
2007SH30 Phys.Atomic Nuclei 70, 1452 (2007) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, R.V.Jolos Cluster approach to the structure of nuclei with Z ≥ 96 NUCLEAR STRUCTURE Z>95; Th, U, Pu, cm, Cf, Fm, No, Rf, Sg; calculated energies of the states of yrast rotational bands within the dinuclear-system model. Compared results to available data.
doi: 10.1134/S1063778807080212
2006JO06 Eur.Phys.J. A 29, 147 (2006) R.V.Jolos, N.Yu.Shirikova, V.V.Voronov On neutron number dependence of B(E1;0+1 → 1-1) reduced transition probability NUCLEAR STRUCTURE 124,126,128,130,132,134,136Xe, 106,108,110,112,115,116Cd, 116,118,120,122,124Sn; calculated B(E1), neutron and proton contributions to transition matrix elements.
doi: 10.1140/epja/i2006-10086-8
2006JO12 Phys.Rev.C 74, 064307 (2006) Mass coefficient and Grodzins relation for the ground-state band and gamma band NUCLEAR STRUCTURE 156,158,160Gd, 158,160,164Dy, 162,164,166,168Er, 168,170Yb; analyzed ground-state band and γ-band level energies, B(E2), K-mixing parameters, mass coefficients.
doi: 10.1103/PhysRevC.74.064307
2006SH19 Phys.Rev. C 74, 034316 (2006) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, R.V.Jolos Possible alternative parity bands in the heaviest nuclei NUCLEAR STRUCTURE 239,240U, 241,242,243,244,245Pu, 243,244,245,246,247,248Cm, 245,246,247,248,249,250Cf, 247,248,249,250,251,252Fm, 249,250,251,252,253,254No, 253,254,255,256Rf, 258Sg; calculated levels, J, π, rotational bands, transition dipole and quadrupole moments. Cluster model.
doi: 10.1103/PhysRevC.74.034316
2005JO09 Phys.Rev. C 71, 044305 (2005) R.V.Jolos, P.von Brentano, N.Pietralla Generalized Grodzins relation
doi: 10.1103/PhysRevC.71.044305
2005JO14 Phys.Rev. C 72, 024310 (2005) R.V.Jolos, P.von Brentano, A.Dewald, N.Pietralla Spin dependence of intrinsic and transition quadrupole moments
doi: 10.1103/PhysRevC.72.024310
2005JO25 Phys.Rev. C 72, 064312 (2005) Inversion of parity splitting in alternating parity bands at high angular momenta NUCLEAR STRUCTURE 220Ra; calculated parity splitting, odd-even staggering, inversion in alternating-parity rotational bands; deduced role of barrier penetration and angular momentum alignment.
doi: 10.1103/PhysRevC.72.064312
2005SH49 Eur.Phys.J. A 25, 387 (2005) T.M.Shneidman, R.V.Jolos, R.Krucken, A.Aprahamian, D.Cline, J.R.Cooper, M.Cromaz, R.M.Clark, C.Hutter, A.O.Macchiavelli, W.Scheid, M.A.Stoyer, C.Y.Wu E2 transitions between positive- and negative-parity states of the ground-state alternating-parity bands RADIOACTIVITY 252Cf(SF); measured Doppler-shifted Eγ, Iγ, γγ-, (fragment)γ-coin. 144Ba deduced transitions T1/2, B(E2), transition dipole, quadrupole, and octupole moments for alternating-parity band. Gammasphere array, cluster-model analysis.
doi: 10.1140/epja/i2005-10134-y
2004AD15 Nucl.Phys. A734, 433 (2004) G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman Manifestation of cluster effects in the structure of medium mass and heavy nuclei NUCLEAR STRUCTURE 144,146,148Ba, 146Ce; calculated alternating parity bands levels, J, π. 60Zn; calculated superdeformed band transitions branching ratios. 220,222,224,226Ra, 222,224,226,228,230,232Th, 234,236,238U; calculated dipole and quadrupole transition moments. Cluster model, comparisons with data.
doi: 10.1016/j.nuclphysa.2004.01.079
2004AD19 Phys.Rev. C 69, 054310 (2004) G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman Decay out of superdeformed bands in the mass region A ≈ 190 within a cluster approach NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196Pb; calculated superdeformed rotational band energies, decay-out probabilities. Cluster model.
doi: 10.1103/PhysRevC.69.054310
2004AD30 Yad.Fiz. 67, 1729 (2004); Phys.Atomic Nuclei 67, 1701 (2004) G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman Nuclear Structure with the Dinuclear Model NUCLEAR STRUCTURE 232,234,236,238U, 223Ra; calculated rotational bands level energies. 226Ra; calculated B(E2). 60Zn; calculated ground-state band and superdeformed band levels, J, π. Dinuclear system approach.
doi: 10.1134/1.1806910
2004AD31 Yad.Fiz. 67, 1737 (2004); Phys.Atomic Nuclei 67, 1709 (2004) G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman Superdeformation as Cluster State NUCLEAR STRUCTURE 190,192,194Hg; calculated normal-deformed and superdeformed bands levels, J, π, decay-out probabilities. Cluster approach.
doi: 10.1134/1.1806911
2004AD41 Phys.Rev. C 70, 064318 (2004) G.G.Adamian, N.V.Antonenko, R.V.Jolos, T.M.Shneidman Cluster interpretation of parity doublet rotational bands in odd-mass nuclei NUCLEAR STRUCTURE 151,153Pm, 153,155Eu, 221,223,225,227Ra, 223,225,227Ac, 223,229,231Th, 231Pa, 233U; calculated rotational bands level energies; 221,223,225,227Ra, 223,225,227Ac, 223,225Th, 229Pa; calculated dipole and quadrupole moments; deduced cluster features. Cluster model, comparisons with data.
doi: 10.1103/PhysRevC.70.064318
2004DO12 Phys.Rev. C 70, 044308 (2004) Interacting boson model study of the spin evolution of the yrast E2 transition probabilities in 162Yb NUCLEAR STRUCTURE 162Yb; calculated levels, J, π, B(E2). Interacting boson model, comparison with data.
doi: 10.1103/PhysRevC.70.044308
2004JO08 Fiz.Elem.Chastits At.Yadra 35, 408 (2004); Physics of Part.and Nuclei 35, 225 (2004) Triple Point in the Phase Transition Diagram of a Cold Nucleus NUCLEAR STRUCTURE 134Ba; analyzed level energies, B(E2); deduced symmetry and phase transition features. Interacting boson model.
2004JO09 Yad.Fiz. 67, 955 (2004); Phys.Atomic Nuclei 67, 931 (2004) Phase Transitions between Axisymmetric and Nonaxial Nuclear Shapes NUCLEAR STRUCTURE 134Ba; analyzed level energy and B(E2) ratios; deduced phase transition features.
doi: 10.1134/1.1755385
2004JO16 Phys.Rev. C 70, 054303 (2004) R.V.Jolos, N.Yu.Shirikova, V.V.Voronov Q-phonon description of the low lying 1- two-phonon states in spherical nuclei NUCLEAR STRUCTURE 116,118,120,122,124Sn, 134,136,138,140,142Ba, 140,142,144,146Ce, 142,144,146,148Nd, 144,146,148,150Sm; calculated electric dipole transition matrix elements. Q-phonon approach, comparison with data.
doi: 10.1103/PhysRevC.70.054303
2003AD10 Phys.Rev. C 67, 054303 (2003) G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid Cluster effects in the structure of the ground state and superdeformed bands of 60Zn NUCLEAR STRUCTURE 60Zn; calculated superdeformed band moment of inertia, transition quadrupole moment, related features. Dinuclear system model, comparison with data.
doi: 10.1103/PhysRevC.67.054303
2003AD31 Acta Phys.Pol. B34, 2147 (2003) G.G.Adamian, A.V.Andreev, N.V.Antonenko, S.P.Ivanova, R.V.Jolos, W.Scheid, T.M.Shneidman Dinuclear system phenomena in nuclear structure and nuclear reactions NUCLEAR STRUCTURE 146Ba, 148Nd, 222Ra, 242Pu; calculated level energies for alternating-parity states. 194Hg, 194Pb, 234,236,238U, 236,239,240Pu, 240Am, 230,231,233Th; calculated cluster states quadrupole moments, related features. Dinuclear system approach, comparison with data.
2003AD32 Acta Phys.Pol. B34, 1729 (2003) G.G.Adamian, N.V.Antonenko, R.V.Jolos, W.Scheid, T.M.Shneidman Cluster features in reactions and structure of heavy nuclei NUCLEAR STRUCTURE 220,222,224,226Ra, 222,224,226,228,230,232Th, 236,238U; calculated levels, J, π, transition moments; deduced cluster effects. Comparison with data.
2003JO14 Yad.Fiz. 66, 1945 (2003); Phys.Atomic Nuclei 66, 1897 (2003) Potential Barrier in the Problem of the Evolution of a Dinuclear System NUCLEAR STRUCTURE 272Hs; calculated dinuclear system potential energy.
doi: 10.1134/1.1619501
2003SH02 Phys.Rev. C 67, 014313 (2003) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, R.V.Jolos, W.Scheid Cluster interpretation of properties of alternating parity bands in heavy nuclei NUCLEAR STRUCTURE 222,224,226,228,230,232Th, 220,222,224,226Ra, 240,242Pu, 232,234,236,238U, 144,146,148Ba, 146,148Ce, 146,148Nd; calculated alternating parity bands levels, J, π, electric multipole transition moments. Cluster model, comparison with data.
doi: 10.1103/PhysRevC.67.014313
2003SH04 Yad.Fiz. 66, 230 (2003); Phys.Atomic Nuclei 66, 206 (2003) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, S.P.Ivanova, R.V.Jolos, W.Scheid Generation of Angular Momentum of Fission Fragments in a Cluster Model RADIOACTIVITY 252Cf(SF); calculated fission fragments angular momentum for different decay channels. Dinuclear system concept, comparisons with data.
doi: 10.1134/1.1553492
2002GE20 Prog.Theor.Phys.(Kyoto), Suppl. 146, 553 (2002) A.Gelberg, A.F.Lisetskiy, R.V.Jolos, P.von Brentano, T.Otsuka, T.Sebe, Y.Utsuno M1 Transitions in Odd-Odd Deformed N = Z Nuclei NUCLEAR STRUCTURE 46V, 50Mn, 54Co; calculated transitions B(M1). RADIOACTIVITY 46Cr(EC); calculated B(GT), log ft.
doi: 10.1143/PTPS.146.553
2002JO17 Phys.Rev. C66, 044303 (2002) Cluster interpretation of enhanced electric dipole transitions in nuclei with strong collective multipole correlations NUCLEAR STRUCTURE 108,110,112,114,116Cd, 116,118,120,122,124Sn, 134,136,138Ba, 140,142Ce, 142,144,146,148,150Nd, 144,148,150Sm; calculated electric dipole transition moments. Cluster model, comparison with data.
doi: 10.1103/PhysRevC.66.044303
2002KL02 Phys.Lett. 524B, 252 (2002) T.Klug, A.Dewald, R.V.Jolos, B.Saha, P.von Brentano, J.Jolie Supersymmetry of Identical Bands in 171, 172Yb Supported by Lifetime Data NUCLEAR REACTIONS 171Yb(32S, 32S'), E=105 MeV; measured Eγ, Iγ, Doppler shifts following Coulomb excitation. 171Yb levels deduced T1/2, transition quadrupole moments, B(E2). 171,172Yb analyzed transition quadrupole moments in identical bands; deduced weakly broken supersymmetry. Recoil distance technique.
doi: 10.1016/S0370-2693(01)01383-1
2002SH20 Phys.Rev. C65, 064302 (2002) T.M.Shneidman, G.G.Adamian, N.V.Antonenko, S.P.Ivanova, R.V.Jolos, W.Scheid Role of Bending Mode in Generation of Angular Momentum of Fission Fragments RADIOACTIVITY 252Cf(SF); calculated fission fragments angular momenta vs neutron multiplicity, role of bending vibrations. Dinuclear system concept, comparison with data.
doi: 10.1103/PhysRevC.65.064302
2002VO07 Phys.Lett. 534B, 63 (2002) P.von Brentano, R.V.Jolos, H.A.Weidenmuller Mixing of Bound and Unbound Levels
doi: 10.1016/S0370-2693(02)01551-4
2002VO12 Nucl.Phys. A704, 115c (2002) P.von Brentano, C.Friessner, R.V.Jolos, A.F.Lisetskiy, A.Schmidt, I.Schneider, N.Pietralla, T.Sebe, T.Otsuka Low Spin Structure of Odd-Odd N = Z Nuclei 54Co and 50Mn NUCLEAR REACTIONS 54Fe(p, n), E=13 MeV; 50Cr(p, n), E=15 MeV; measured Eγ, Iγ. 54Co, 50Mn deduced levels, J, π, B(E2), B(M1). Comparison with shell model predictions.
doi: 10.1016/S0375-9474(02)00772-8
2001JO01 Phys.Rev. C63, 024304 (2001) Partial Supersymmetry in the Particle-Rotor Model NUCLEAR STRUCTURE 173Hf, 181Pt; calculated rotational bands levels, J, π; 174,175,176Hf, 182Pt, 174,175Lu; analyzed rotational bands levels; deduced symmetry features. Particle-rotor model.
doi: 10.1103/PhysRevC.63.024304
2001JO07 Yad.Fiz. 64, No 3, 520 (2001); Phys.Atomic Nuclei 64, 465 (2001) Q-Phonon Scheme in the Collective Nuclear Model
doi: 10.1134/1.1358470
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