NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = V.G.Solovev Found 168 matches. Showing 1 to 100. [Next]2001SO17 Yad.Fiz. 64, No 7, 1275 (2001); Phys.Atomic Nuclei 64, 1199 (2001) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Gamma Deexcitation of the 180mTa Isomer NUCLEAR STRUCTURE 180Ta; calculated B(E2), B(M1) for transitions between vibrational bands built on ground and isomeric states. Quasiparticle-phonon model. NUCLEAR REACTIONS 180mTa(γ, γ'), E not given; calculated probability for isomer deexcitation. Three-step process.
doi: 10.1134/1.1389542
2000SO12 Fiz.Elem.Chastits At.Yadra 31, 786 (2000); Phys.Part.Nucl. 31, 385 (2000) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Dipole Excitations in Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 166,168Er, 172,174Yb, 178Hf, 238U; calculated levels B(M1), B(E1), B(E2). Quaisparticle-phonon model, RPA, comparisons with data.
1999BU25 Nucl.Phys. A656, 287 (1999) D.G.Burke, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Nuclear Structure of 172Yb NUCLEAR REACTIONS 173Yb(d, t), E=15 MeV; measured σ(E(t), θ). 171Yb(t, d), E=15 MeV; measured σ(E(d), θ). 172Yb deduced levels, J, π, spectroscopic strengths. Enriched targets, magnetic spectrograph. Comparison with quasiparticle-phonon model predictions with Coriolis mixing.
doi: 10.1016/S0375-9474(99)00318-8
1999SO15 J.Phys.(London) G25, 1023 (1999) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova, N.Lo Iudice Dipole Strength Distribution in Doubly Even Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 168Er, 178Hf, 238U; calculated E1, M1 strength distributions; deduced orbital, spin contributions. RPA. Comparisons with data.
doi: 10.1088/0954-3899/25/5/307
1998SO06 Nucl.Phys. A633, 247 (1998) Vibrational States on the Isomers in Deformed Nuclei NUCLEAR STRUCTURE 178,179Hf, 180Ta; calculated levels, J, π of vibrational states built on isomers, transitions B(Eλ), B(M1). Quasiparticle-phonon model.
doi: 10.1016/S0375-9474(98)00136-5
1998WE13 Eur.Phys.J. A 3, 25 (1998) T.Weber, J.de Boer, K.Freitag, J.Groger, C.Gunther, P.Herzog, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Nuclear Levels in 228Th Populated in the Decay of 228Pa (II) RADIOACTIVITY 228Pa(EC); measured Eγ, Iγ, γγ-coin. 228Th deduced levels, J, π, δ, B(E2), rotational bands. NUCLEAR STRUCTURE 228Th; calculated levels J, π, transition strengths. Quasiparticle-phonon model.
doi: 10.1007/s100500050146
1997DI09 Phys.Rev. C56, 1350 (1997) N.Dinh Dang, A.Arima, V.G.Soloviev, S.Yamaji Possible Deviation of the Sum of Strengths for the Double Giant Dipole Resonance from the Harmonic Oscillator Limit
doi: 10.1103/PhysRevC.56.1350
1997SO02 Nucl.Phys. A613, 45 (1997) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova, N.Lo Iudice Low-Lying Magnetic and Electric Dipole Transitions in Odd-Mass Deformed Nuclei: A microscopic approach NUCLEAR STRUCTURE 157,159Tb, 161,163Dy, 167Er; calculated levels, B(λ), reduced widths. Quasiparticle-phonon model, separable Hamiltonian.
doi: 10.1016/S0375-9474(96)00426-5
1997SO12 Phys.Rev. C56, R603 (1997) V.G.Soloviev, A.Arima, Nguyen Dinh Dang Possible Enhancement of the E1 Decay Rates of Double Giant Dipole States
doi: 10.1103/PhysRevC.56.R603
1997SO18 Z.Phys. A358, 287 (1997) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Dipole γ-ray Transition Rates in 238U NUCLEAR STRUCTURE 238U; calculated levels, B(λ), configuration, decay rates. Quasiparticle-phonon nuclear model.
doi: 10.1007/s002180050332
1997SO21 Z.Phys. A358, 117 (1997) V.G.Soloviev, A.V.Sushkov, N.Y.Shirikova Dipole Strength Distribution and Specific Properties of Excitations in the Second Minimum in Actinide Nuclei NUCLEAR STRUCTURE 238U, 240Pu; calculated vibrational levels, configurations, B(λ) at first, second minima. Quasiparticle-phonon nuclear model.
doi: 10.1007/s002180050284
1997SO24 Phys.Rev. C56, 2528 (1997) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Low-Energy Dipole γ-Ray Transition Rates in Even-Even Deformed Nuclei NUCLEAR STRUCTURE 168Er, 174Yb; calculated K(π)=1+ levels, B(M1), B(E2); 168Er; calculated K(π)=0-, 1- levels, B(E1), B(E3); 154Sm, 166Er, 172,174Yb, 178Hf; calculated M1, E1 strength distributions; 156,158,160Gd, 160,162,164Dy, 166,168Er, 172,174Yb, 178Hf; calculated summed M1, E1 strengths; deduced configurations. Quasiparticle-phonon nuclear model. Other models, data compared.
doi: 10.1103/PhysRevC.56.2528
1997SO25 Yad.Fiz. 60, No 10, 1754 (1997); Phys.Atomic Nuclei 60, 1599 (1997) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Vibrational States in 178Hf NUCLEAR STRUCTURE 178Hf; calculated vibrational levels, B(λ); deduced 0+ states dominant component. Comparisons with data. Quasiparticle-phonon model.
1997SO26 Int.J.Mod.Phys. E6, 437 (1997) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Quadrupole and Hexadecapole Vibrational Excitations in Deformed Nuclei NUCLEAR STRUCTURE 156,158,160Gd, 160,162,164Dy, 166,168Er; calculated levels, configurations, B(λ); deduced quasiparticle-phonon, one-, two-phonon coupling roles. Quasiparticle-phonon nuclear model.
doi: 10.1142/S0218301397000251
1996SO02 Phys.Rev. C53, 1022 (1996) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Low-Lying Magnetic Dipole Strength in 163Dy NUCLEAR STRUCTURE 162,163Dy; calculated B(M1), transition strength distribution, fragmentation strength differences. Quasiparticle-phonon model.
doi: 10.1103/PhysRevC.53.1022
1996SO04 Yad.Fiz. 59, No 1, 57 (1996); Phys.Atomic Nuclei 59, 51 (1996) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Description of Nonrotational States in 160Dy NUCLEAR STRUCTURE 160Dy; calculated levels, B(λ) ratios. Quasiparticle-phonon model.
1996SO05 Nucl.Phys. A600, 155 (1996) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova, N.Lo Iudice Effect of Two RPA Phonons on the Spectrum of the Low-Lying Magnetic Dipole Transitions in Deformed Nuclei NUCLEAR STRUCTURE 160,162,164Dy, 156,158,160Gd; calculated levels, B(M1) distribution; deduced two RPA phonons effect. Quasiparticle-phonon nuclear model, one-, two-RPA phonon states.
doi: 10.1016/0375-9474(96)00020-6
1996SO18 Pisma Zh.Eksp.Teor.Fiz. 63, 575 (1996); JETP Lett. 63, 607 (1996) Vibrational State in Odd Deformed Nuclei NUCLEAR STRUCTURE 163Dy; calculated nonrotational levels. Quasiparticle plus phonon model.
doi: 10.1134/1.567074
1996SO19 Fiz.Elem.Chastits At.Yadra 27, 1643 (1996); Phys.Part.Nucl. 27, 667 (1996) V.G.Solovev, A.V.Sushkov, N.Yu.Shirikova Low-Lying Nonrotational States in Strongly Deformed Even-Even Nuclei of the Rare-Earth Region NUCLEAR STRUCTURE 156,158,160Gd, 160,162,164Dy, 166,168Er; calculated low-lying nonrotational levels E, π, transitions B(λ). Quasiparticle-phonon model.
1995BE02 Nucl.Phys. A584, 413 (1995) J.Berzins, P.Prokofev, R.Georgii, R.Hucke, T.von Egidy, G.Hlawatsch, J.Klora, H.Lindner, U.Mayerhofer, H.H.Schmidt, A.Walter, V.G.Soloviev, N.Yu.Shirikova, A.V.Sushkov 162Dy Studied with (n, γ), (n, n'γ), (d, p) and (d, t) Reactions NUCLEAR REACTIONS 161Dy(n, γ), 162Dy(n, n'γ), E=fast, thermal; measured γ-spectra. 161Dy(d, p), E=15, 22 MeV; 163Dy(d, t), E=22 MeV; measured spectra. 162Dy deduced levels, configurations. Quasiparticle-phonon nuclear model. NUCLEAR STRUCTURE 162Dy; calculated levels, B(λ). Quasiparticle-phonon nuclear model.
doi: 10.1016/0375-9474(94)00522-O
1995SO01 Phys.Rev. C51, 551 (1995) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Description of Low-Lying Vibrational and Two-Quasiparticle States in 166Er NUCLEAR STRUCTURE 166Er; calculated levels, B(λ), γ-branching ratios. Quasiparticle phonon model.
doi: 10.1103/PhysRevC.51.551
1995SO06 Nucl.Phys. A586, 265 (1995) Order Against Chaos in Nuclei NUCLEAR STRUCTURE 166Er; calculated nonrotational (K, π)=2-, 3+, 4- states. Quasiparticle-phonon model.
doi: 10.1016/0375-9474(94)00534-T
1995SO09 Phys.Rev. C51, R2885 (1995) Fast γ-Ray Transitions between Excited States as Evidence of Order in Deformed Nuclei NUCLEAR STRUCTURE 160Gd, 160,162,164Dy; calculated levels decay rates. Quasiparticle-phonon nuclear model.
doi: 10.1103/PhysRevC.51.R2885
1995SO22 Phys.Scr. T56, 192 (1995) Gamma Decays of High Spin Isomers in the Vicinity of Closed Shells as a Key for Studying Order to Chaos Transitions in Nuclei NUCLEAR STRUCTURE 162Dy, 168Er, 160Gd; calculated levels γ-transitions, B(λ). 166Er; calculated, γ-transitions, levels; deduced chaos transitions related features. Quasiparticle-phonon model.
1995SO24 J.Phys.(London) G21, 1217 (1995) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Correlation between E1 and E3 Transition Strengths and Influence of the Fragmentation of One-Phonon States on the E1 Strength Distribution in Well-Deformed Nuclei NUCLEAR STRUCTURE 160Gd, 160,162,164Dy; calculated B(E1), B(E3); deduced correlation, K, π dependence, one-phonon states fragmentation features. Quasiparticle-phonon model.
doi: 10.1088/0954-3899/21/9/007
1994SO01 J.Phys.(London) G20, 113 (1994) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Gamma-Ray Transitions between Excited States in 168Er NUCLEAR STRUCTURE 168Er; calculated levels, B(λ), ratios. Quasiparticle phonon model.
doi: 10.1088/0954-3899/20/1/012
1994SO02 Nucl.Phys. A568, 244 (1994) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Description of Low-Lying Vibrational States and Gamma-Ray Transitions between Excited States in 156Gd and 158Gd NUCLEAR STRUCTURE 156,158Gd; calculated levels, B(λ); deduced dominant configuration. Quasiparticle-phonon model.
doi: 10.1016/0375-9474(94)90200-3
1994SO19 Yad.Fiz. 57, No 8, 1375 (1994); Phys.Atomic Nuclei 57, 1304 (1994) The Origin and Distribution of the E1 Strength Over Low-Lying States in Well-Deformed Nuclei NUCLEAR STRUCTURE 158Gd, 162,164Dy, 168Er; calculated levels, B(λ). RPA, quasiparticle approach.
1994SO22 Fiz.Elem.Chastits At.Yadra 25, 377 (1994); Sov.J.Part.Nucl 25, 157 (1994) V.G.Solovev, A.V.Sushkov, N.Yu.Shirikova A Version of the Quasiparticle-Phonon Nuclear MOdel for Even-Even Deformed Nuclei NUCLEAR STRUCTURE 168Er; calculated model functions U. Quasiparticle phonon model, density dependent separable interactions.
1994SO28 Int.J.Mod.Phys. E3, 1227 (1994) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Description of E1 Transition in Doubly Even Well-Deformed Nuclei NUCLEAR STRUCTURE 168,166Er, 164,162,160Dy, 158,156,160Gd; calculated levels, B(λ). Quasiparticle-phonon model.
doi: 10.1142/S0218301394000395
1993PI06 Nucl.Phys. A559, 1 (1993) M.Pignanelli, N.Blasi, J.A.Bordewijk, R.De Leo, M.N.Harakeh, M.A.Hofstee, S.Micheletti, R.Perrino, V.Yu.Ponomarev, V.G.Soloviev, A.V.Sushkov, S.Y.van der Werf Strength Distribution in Neodymium Isotopes: A test of collective nuclear models NUCLEAR REACTIONS 142,144,146,148,150Nd(p, p'), E=30.5 MeV; 144Nd(p, p'), E=51 MeV; 142,144,146,148,150Nd(d, d'), E=50.8 MeV; measured σ(Ep, θ), σ(Ed, θ). 142,144,146,148,150Nd deduced levels, J, π, B(λ). Enriched targets.
doi: 10.1016/0375-9474(93)90178-Z
1993SO05 Z.Phys. A345, 155 (1993) Description of Low-Lying Vibrational and Two-Quasiparticle States in 164Dy NUCLEAR STRUCTURE 164Dy, 168Er; calculated levels, B(λ). Two-phonon vibrational plus two-quasiparticle states, deformed Woods-Saxon potential.
1993SO12 Phys.Lett. 317B, 501 (1993) On the K-Dependence in the Gamma-Decay of Neutron Resonances in 168Er NUCLEAR STRUCTURE 168Er; analyzed Iγ from (n, γ) reaction data for thermal neutron capture; deduced K-mixing features in resonance region.
doi: 10.1016/0370-2693(93)91362-Q
1993SO20 Bull.Rus.Acad.Sci.Phys. 57, 1668 (1993) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova γ-Transitions between Excited States of Even-Even Deformed Nuclei NUCLEAR STRUCTURE 168Er, 162Dy, 156,158Gd; calculated B(λ). Quasiparticle phonon model.
1993SO21 Pisma Zh.Eksp.Teor.Fiz. 58, 403 (1993); JETP Lett.(USSR) 58, 413 (1993) Decisive Role of Fragmentation of Quasiparticle-Phonon Configurations in the Transition from Order to Chaos in Nuclei NUCLEAR STRUCTURE 181,179,177,178Hf, 175,177Lu, 212,213Fr, 177,179,180Ta; analyzed data; deduced multi-quasiparticle configuration fragmentation.
1992SO07 Nucl.Phys. A542, 410 (1992) Microscopic Description of the M3 Strength Distribution in Deformed Nuclei NUCLEAR STRUCTURE 164Dy, 168Er; calculated levels, B(M3). Modified RPA.
doi: 10.1016/0375-9474(92)90104-R
1992SO14 Yad.Fiz. 55, 2359 (1992); Sov.J.Nucl.Phys. 55, 1310 (1992) Distribution of the Magnetic M2 Strength in Deformed Nuclei NUCLEAR STRUCTURE 168Er, 164Dy; calculated levels, B(λ). RPA, multipole, spin-multipole interactions.
1992SO22 Bull.Rus.Acad.Sci.Phys. 56, 658 (1992) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Octupole Strength Distribution in Deformed Nuclei with Energy Below 6 MeV NUCLEAR STRUCTURE 168Er, 170,172,174Yb, 178Hf, 238U, 250Cf, 256Fm; calculated B(λ). 158Gd; calculated levels, B(λ), energy weighted sum rule percentages. Octupole transitions, quasiparticle phonon model.
1991KU22 Czech.J.Phys. B41, 1109 (1991) Description of the Gamow-Teller β+-Decays and (n, p) Transitions in Spherical Nuclei RADIOACTIVITY 94Ru, 96,98Pd, 100,102,104Cd, 104,106,108Sn, 142,144,146,148,150Dy; calculated Gamow-Teller β+-decay log ft; deduced (gA/gV) value limits. NUCLEAR REACTIONS 54Fe, 90Zr, 120Sn(n, p), E not given; calculated Gamow-Teller transition strength function.
doi: 10.1007/BF01598987
1991SO05 Yad.Fiz. 53, 101 (1991); Sov.J.Nucl.Phys. 53, 65 (1991) V.G.Solovev, A.V.Sushkov, N.Yu.Shirikova Description of Nonrotational States and Eλ-Strength Distribution in Deformed Nuclei in the Actinide Region NUCLEAR STRUCTURE 238U, 240Pu; calculated levels, B(λ). Quasiparticle-phonon model.
1991SO11 Phys.Lett. 262B, 189 (1991) Electric-Dipole Transitions in Doubly Even Deformed Nuclei NUCLEAR STRUCTURE 172Yb; calculated levels, B(λ). Quasiparticle-phonon nuclear model.
doi: 10.1016/0370-2693(91)91552-7
1991SO15 Yad.Fiz. 54, 1232 (1991); Sov.J.Nucl.Phys. 54, 748 (1991) V.G.Solovev, A.V.Sushkov, N.Yu.Shirikova Description of Nonrotational States of 250Cf and 256Fm NUCLEAR STRUCTURE 250Cf, 250,256Fm, 254No, 260Rf; calculated levels; deduced band structure, configuration. Quasiparticle-phonon nuclear model.
1990SO01 J.Phys.(London) G16, L57 (1990) On the Role of High-Multipolarity Interactions in Deformed Nuclei NUCLEAR STRUCTURE 178,176Hf, 174Yb, 168Er, 158Gd; analyzed data. Two-quasinucleon states, high multipolarity interactions.
doi: 10.1088/0954-3899/16/3/004
1990SO09 Fizika(Zagreb) 22, 19 (1990) Description of Vibrational States of Deformed Nuclei within the Quasiparticle-Phonon Nuclear Model NUCLEAR STRUCTURE 168Er; calculated levels, B(λ). Quasiparticle-phonon model.
1990SO12 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 818 (1990); Bull.Acad.Sci.Ussr, Phys.Ser. 54, No.5, 1 (1990) Description of Nonrotational States of 170,174Yb NUCLEAR STRUCTURE 170,174Yb; calculated levels, B(λ). Quasiparticle phonon model, nonrotational states.
1990SO16 Fiz.Elem.Chastits At.Yadra 21, 1360 (1990); Sov.J.Part.Nucl. 21, 579 (1990) Description of Deformed Nuclei in the Quasiparticle-Phonon and Interacting-Boson Models NUCLEAR STRUCTURE 168Er, 174,178Hf, 170,172,174Yb, 158Gd; calculated levels, B(λ). Quasiparticle-phonon, interacting boson models comparison.
1989KA47 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 2150 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.11, 90 (1989) D.Karadzhov, V.G.Solovev, A.V.Sushkov Influence of Quadrupole Pairing on the Energy of the Two-Quasi-Particle States of Deformed Nuclei NUCLEAR STRUCTURE 168Er, 172Yb, 173,180Hf; calculated levels; deduced quadrupole pairing role. Quasiparticle model.
1989SO01 Phys.Lett. 216B, 259 (1989) Gamow-Teller β+ Decay of Neutron-Deficit Deformed Nuclei RADIOACTIVITY 162,164,166Yb, 164,166Hf(β+); calculated log ft, partial β-decay strength.
doi: 10.1016/0370-2693(89)91111-8
1989SO11 Z.Phys. A334, 149 (1989) Description of Low-Lying Vibrational Kπ not Equal to 0+ States of Deformed Nuclei in the Quasiparticle-Phonon Nuclear Model NUCLEAR STRUCTURE 168Er, 172Yb, 178Hf; calculated levels, B(λ). Quasiparticle-Phonon nuclear model.
1989SO16 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 2066 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.11, 1 (1989) Low-Lying Vibrational States in Deformed Nuclei NUCLEAR STRUCTURE 168Er; calculated levels; deduced structure. Qusiparticle model.
1988KU19 Pisma Zh.Eksp.Teor.Fiz. 47, 68 (1988); JETP Lett.(USSR) 47, 79 (1988) Effect of Interaction in the Particle-Particle Channel on Gamow-Teller β+ Decay in Spherical Nuclei RADIOACTIVITY 152Yb, 150Er, 148,146Dy, 96Pd(β+); calculated Gamow-Teller β-decay log ft.
1988KU20 Nucl.Phys. A486, 118 (1988) Gamow-Teller β+ Decays and Strength Functions of (n, p) Transitions in Spherical Nuclei NUCLEAR STRUCTURE 152Yb, 152,150Er, 146,148Dy, 96Pd, 126Ba, 120Xe; calculated β+-decay log ft. 90Zr, 54Fe, 120Sn, 140Ce; calculated (n, p) transition strength functions. RPA.
doi: 10.1016/0375-9474(88)90042-5
1988SO01 J.Phys.(London) G14, Supplement S39 (1988) Comparison of the Quasiparticle-Phonon Nuclear Model with the Interacting Boson Model in Describing Deformed Nuclei NUCLEAR STRUCTURE 168Er; analyzed predicted levels; deduced model comparison.
doi: 10.1088/0305-4616/14/S/004
1988SO02 Yad.Fiz. 47, 332 (1988) Comparison of the of Interacting Boson Model with Quasiparticle-Phonon Nuclear Model NUCLEAR STRUCTURE 168Er; calculated levels, B(λ). Quasiparticle-Phonon model.
1988SO12 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2095 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 14 (1988) Influence of Particle-Particle Interaction on the Properties of States with Kπ = 2+ of Deformed Nuclei NUCLEAR STRUCTURE 168Er; calculated levels, B(λ); deduced parameter dependence. RPA.
1987PO02 Phys.Lett. 183B, 237 (1987) V.Yu.Ponomarev, V.G.Soloviev, A.I.Vdovin, Ch.Stoyanov The Role of ' Quasiparticle x Phonon ' Components in Gamma-Decay of High-Lying States NUCLEAR STRUCTURE 111Sn; calculated transition intensities, B(M1). Microscopic approach. NUCLEAR REACTIONS 112Sn(3He, αγ), E=3-6 MeV; calculated (θα, θγ). Microscopic approach.
doi: 10.1016/0370-2693(87)90955-5
1987SO18 Prog.Part.Nucl.Phys. 19, 107 (1987) Fragmentation of single-particle and collective motions in the quasiparticle-phonon nuclear model
doi: 10.1016/0146-6410(87)90004-4
1986NE06 Yad.Fiz. 44, 1443 (1986) V.O.Nesterenko, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Hexadecapole States in Deformed Nuclei NUCLEAR STRUCTURE 158,160Gd, 158,160,162,164Dy, 166,168,170Er, 168,170,172,174Yb, 174,176,178Hf, 184W, 186,188Os; calculated hexadecapole states, B(E4), wave functions. 168Er; calculated B(E2).
1986NG01 Yad.Fiz. 43, 1162 (1986) Nguyen Dinh Vinh, V.G.Soloviev Description of Subshell Fragmentation in Tungsten Isotopes NUCLEAR STRUCTURE 183,185,187W; calculated 3p3/2, 3p1/2 fragmentation, single nucleon transfer reaction spectroscopic factors. 182Re; calculated single nucleon transfer reaction spectroscopic factors.
1986SO09 Z.Phys. A324, 393 (1986) Confrontation between the Quasiparticle-Phonon Nuclear Model and the Interacting Boson Model for Deformed Nuclei NUCLEAR STRUCTURE 158Gd, 158,160,162Dy, 168,170Er, 172Yb, 178Hf; calculated levels, (β-), (γ) vibrational state structure. Quasiparticle phonon nuclear model.
1985KU07 J.Phys.(London) G11, 603 (1985) Fragmentation of Spin-Dipole Charge-Exchange States in Spherical Nuclei NUCLEAR STRUCTURE 90Zr, 120,124Sn, 124Te, 208Pb; calculated spin dipole charge exchange state fragmentation. Quasiparticle-phonon model, central forces.
doi: 10.1088/0305-4616/11/5/007
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
1984KU19 J.Phys.(London) G10, 1507 (1984) Fragmentation of the Gamow-Teller Resonance in Spherical Nuclei NUCLEAR STRUCTURE 90Zr, 120,124Sn, 124Te, 140Ce, 208Pb; calculated Gamow-Teller resonance fragmentation, transition strength distribution. Quasiparticle-phonon model.
doi: 10.1088/0305-4616/10/11/007
1984KU24 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 1801 (1984) Description of the Charge-Exchange Resonance Fragmentation in Spherical Nuclei NUCLEAR STRUCTURE 90Zr, 120Sn; calculated Gamow-Teller, spin-dipole transition strength distribution. RPA, charge-exchange process.
1984NG01 J.Phys.(London) G10, 517 (1984) Nguyen Dinh Thao, V.G.Soloviev, Ch.Stoyanov, A.I.Vdovin Fragmentation of the 1f Neutron-Hole Strength in 89Zr and 91Mo NUCLEAR STRUCTURE 89Zr, 91Mo; calculated 1f7/2, 1f5/2 neutron-hole state fragmentation. Quasiparticle-phonon model.
doi: 10.1088/0305-4616/10/4/012
1984SO04 Z.Phys. A316, 65 (1984) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Despcription of Charge-Exchange Resonances in Deformed Nuclei NUCLEAR REACTIONS 156,158,160Gd, 160,162,164Dy, 164,166,168Er, 168Yb, 236,238U, 238,240Pu(p, n), (n, p), E not given; calculated l=1 transition strength functions, Gamow-Teller, E1, spin-dipole resonance centroids. RPA.
1984SO15 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 1798 (1984) Description of T(>)-Giant Dipole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 156Gd, 166Er, 238U; calculated E1 transition strength distribution, GDR T(>) component energies. 156,158,160Gd, 160,162,164Dy, 164,166,168Er, 168Yb, 236,238U, 238,240Pu; calculated T(>) GDR characteristics.
1984SO16 Yad.Fiz. 40, 1163 (1984) Improvement of Description of Fragmentation of Collective Nuclear States NUCLEAR STRUCTURE 61Ni; calculated M1 transition strength fragmentation. 118Sn; calculated collective 2+ giant resonance strength fragmentation.
1984SO17 Pisma Zh.Eksp.Teor.Fiz. 40, 398 (1984); JETP Lett.(USSR) 40, 1216 (1984) Structure of Nonrotational States of Deformed Nuclei NUCLEAR STRUCTURE 158Gd; calculated levels, B(λ). 168Er; calculated levels; deduced nonrotational level structure. Quasiparticle-phonon model.
1984SO19 J.Phys.(Paris), Colloq.C-4, 69 (1984) Deep Hole and High-Lying Particle Strength Functions NUCLEAR STRUCTURE 115Sn, 145Eu; calculated neutron, proton hole states fragmentations. 75Co, 89Zr, 115Sn; calculated spectroscopic factors. 94Mo, 111,114,119Sn, 145Sm, 206Pb; calculated (p, n) reaction strength distributions. Quasiparticle-phonon model. NUCLEAR REACTIONS 238U(p, n), (n, p), E ≤ 32 MeV; 166Er(p, n), E ≤ 40 MeV; 124Te(p, n), E ≤ 25 MeV; calculated Gamow-Teller transition strength functions. Quasiparticle-phonon model.
1984VO14 Yad.Fiz. 40, 683 (1984) V.V.Voronov, Nguyen Dinh Dang, V.Yu.Ponomarev, V.G.Soloviev, Ch.Stoyanov Description of Giant Multipole Resonances in Spherical Nuclei NUCLEAR STRUCTURE 116,118Sn, 146Nd, 208Pb; calculated giant multipole resonance characteristics, B(λ). Quasiparticle-phonon model.
1983SO01 Z.Phys. A309, 353 (1983) V.G.Soloviev, V.O.Nesterenko, S.I.Bastrukov On Vibrational States in Deformed Odd-A Nuclei NUCLEAR STRUCTURE 155Sm, 161Tb, 159,165Ho, 167Er, 169Yb, 179Hf, 233Th, 233,235,237,239U, 237Np, 239Pu; calculated levels, Pauli effect significance. 155,159,161Gd, 169Er, 179Hf, 233,237,239U, 239Pu; calculated Pauli principle violation in levels. Quasiparticle-phonon model.
1983SO03 Nucl.Phys. A399, 141 (1983) V.G.Soloviev, Ch.Stoyanov, V.V.Voronov Nuclear Properties in the Lead Region within the Quasiparticle-Phonon Nuclear Model NUCLEAR REACTIONS 206,207Pb(n, n), E=thermal, resonance; calculated s-, p-, d-wave strength functions. 206,208Pb(γ, X), E not given: calculated photoabsorption σ(E). NUCLEAR STRUCTURE 206Pb; calculated GDR characteristics, B(E1) strength distribution. 208Pb; calculated, B(λ), B(E1), B(E2) strength functions, giant quadrupole, octuople resonances, EWSR, GDR characteristics. 207Pb, 203,205,207Tl; calculated deep hole-state fragmentation. Quasiparticle-phonon model.
doi: 10.1016/0375-9474(83)90599-7
1983SO11 Pisma Zh.Eksp.Teor.Fiz. 38, 151 (1983); JETP Lett.(USSR) 38, 179 (1983) V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Description of Gamow-Teller Resonances in Deformed Nuclei NUCLEAR REACTIONS 166,168Er, 162Dy, 238U(n, p), (p, n), E not given; calculated 1+, K=0, 1 residual state excitation strength function; deduced Gamow-Teller resonance, strength contribution. RPA.
1983SO12 Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2082 (1983) V.G.Soloviev, Ch.Stoyanov, R.Nikolaeva Estimate of the Pauli Principle Role in Two Phonon States of Spherical Nuclei NUCLEAR STRUCTURE 114,116Sn, 142,144,146,148Sm; calculated levels. Proximity model, Pauli effect.
1983VD01 Yad.Fiz. 37, 43 (1983) A.I.Vdovin, Nguyen Din Tkhao, V.G.Soloviev, Ch.Stoyanov Fragmentation of Neutron Hole States in 111,115Sn NUCLEAR STRUCTURE 111,115Sn; calculated neutron hole state fragmentation, C2S. Quasiparticle-phonon model.
1983VD02 Fiz.Elem.Chastits At.Yadra 14, 237 (1983); Sov.J.Part.Nucl. 14, 99 (1983) Quasiparticle-Phonon Model of the Nucleus. III. Single-Phonon States in Spherical Nuclei NUCLEAR STRUCTURE A=66-150; calculated B(E2). Isoscalar, isovector multipole-multipole interactions. 140Ce; calculated isoscalar, isovector B(E3), charge, neutron transition densities, B(M2). 208Pb; calculated B(E1), current, charge transition densities. 58Ni; calculated charge, current transition densities. 90Zr; calculated B(M2), B(E1), current transition densities. 124Te; calculated B(M2), B(E2). Quasiparticle-phonon model.
1982BA74 Izv.Akad.Nauk SSSR, Ser.Fiz. 46, 2144 (1982); Bull.Acad.Sci.USSR, Phys.Ser. 46, No.11, 80 (1982) S.I.Bastrukov, V.O.Nesterenko, V.G.Soloviev The Role of the Pauli Principle in Describing the Nonrotational States of Odd Deformed Nuclei NUCLEAR STRUCTURE 166,168Er; analyzed one-phonon state characteristics. 167,169Er; analyzed quasiparticle plus phonon state characteristics; deduced Pauli principle violation, vibrational state existence correlation.
1982KU10 Yad.Fiz. 35, 620 (1982) Description of T (>) Giant Resonances in Spherical Nuclei NUCLEAR STRUCTURE 88Sr, 90Zr, 92Mo, 116,120,124Sn; calculated B(λ), T(>), T(<) giant resonances, σ(T>)/σ(T<). Quasiparticle-phonon model.
1982SO10 Nucl.Phys. A382, 206 (1982) Radiative Strength Functions in Odd-A Spherical Nuclei NUCLEAR STRUCTURE 55Fe, 59,61Ni; calculated levels, E1, M1 strength functions, spectroscopic factors. Quasiparticle phonon model.
doi: 10.1016/0375-9474(82)90132-4
1982SO11 Yad.Fiz. 36, 1376 (1982) Collective Two-Phonon States in Deformed Nuclei NUCLEAR STRUCTURE 158Gd, 160Dy, 232U, 168Er, 228Th; calculated two phonon collective levels, fragmentation. Quasiparticle-phonon model, Pauli principle.
1981KH01 J.Phys.(London) G7, 151 (1981) C.Z.Khuong, V.G.Soloviev, V.V.Voronov The Effect of the Pauli Principle on the Fragmentation of One-Quasiparticle States in Spherical Nuclei NUCLEAR STRUCTURE 59Ni, 119Sn; calculated one quasiparticle state fragmentation. Quasiparticle-phonon model, Pauli effect.
doi: 10.1088/0305-4616/7/2/007
1981SO05 Z.Phys. A301, 263 (1981) On Collective Two-Phonon States in Deformed Nuclei NUCLEAR STRUCTURE 160Dy, 168Er, 240Pu, 154Gd, 230Th; calculated two-phonon state centroid energies; deduced strong fragmentation of two-phonon collective states. Quasiparticle-phonon model, Pauli principle.
1981SO07 Nucl.Phys. A370, 13 (1981) V.G.Soloviev, O.Stoyanova, V.V.Voronov Fragmentation of Two-Quasiparticle States in Spherical Nuclei NUCLEAR STRUCTURE 92Zr, 110,112,114,116,118,120,122,124Sn, 112Cd, 122Te; calculated fragmentation of two-quasiparticle states. Quasiparticle-phonon model.
doi: 10.1016/0375-9474(81)90752-1
1981SO11 Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1834 (1981) V.G.Soloviev, N.Yu.Shirikova, S.I.Serdyukova, F.Meliev, V.O.Nesterenko Role of Pauli Principle in the Description of Nonrotational Collective States in Deformed Nuclei NUCLEAR STRUCTURE 145Gd, 160,164Dy, 168Er, 230,232Th, 238U, 240Pu; calculated levels, B(λ). RPA with, without Pauli effect.
1980JO05 Z.Phys. A295, 147 (1980) R.V.Jolos, J.L.Molina, V.G.Soloviev Effect of the Pauli Principle on the Excited States of Doubly-Even Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 166Er; calculated two-phonon pole energies. Quasiparticle-phonon model, Pauli effect.
doi: 10.1007/BF01413072
1980NE09 Yad.Fiz. 32, 1209 (1980) V.O.Nesterenko, V.G.Soloviev, A.V.Khalkin Study of Correlations in Ground States of Deformed Nuclei NUCLEAR STRUCTURE 152,154Sm, 238U, 166Er; calculated average ground state quasiparticle number, B(λ). 228Th; calculated average ground state quasiparticle number. RPA.
1980SO04 Nucl.Phys. A342, 261 (1980) V.G.Soloviev, C.Stoyanov, A.I.Vdovin The Description of the Fragmentation of One-Quasiparticle States in Spherical Nuclei NUCLEAR STRUCTURE 57Ni, 115,117,119Sn, 123Te, 143Pm; calculated fragmentation of hole states. Quasiparticle-phonon model.
doi: 10.1016/0375-9474(80)90254-7
1980SO07 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 1938 (1980) V.G.Solovev, O.Stoyanova, Ch.Stoyanov Quasiparticle Numbers in Ground States of Spherical and Transitional Nuclei NUCLEAR STRUCTURE 144,146,148,150Sm, 126Te, 118Sn; calculated B(E2), B(E3). Quasiparticle formalism, ground state correlations.
1980VO01 Yad.Fiz. 31, 327 (1980); Sov.J.Nucl.Phys. 31, 173 (1980) V.V.Voronov, V.G.Solovev, O.Stoyanova Calculation of Neutron Strength Functions of Even-Even Spherical Nuclei NUCLEAR REACTIONS 53Cr, 61Ni, 72Ge, 87Sr, 91Zr, 95,97Mo, 143Nd(n, n), E not given; calculated s-, p-wave strength functions. Quasiparticle-phonon nuclear model.
1979KH02 J.Phys.(London) G5, L79 (1979) C.Z.Khuong, V.G.Soloviev, V.V.Voronov Description of the Substructure in the Radiative Strength Function of 117Sn and 119Sn NUCLEAR STRUCTURE 117,119Sn; calculated total E1, M1 photo-absorption σ. Quasiparticle-phonon nuclear model; deduced giant M1 around 8 MeV.
doi: 10.1088/0305-4616/5/4/007
1979PO11 Nucl.Phys. A323, 446 (1979) V.Y.Ponomarev, V.G.Soloviev, C.Stoyanov, A.I.Vdovin Magnetic Quadrupole Resonance in Spherical Nuclei NUCLEAR STRUCTURE 58Ni, 90Zr, 208Pb; calculated M2 strength distribution. Quasiparticle phonon nuclear model.
doi: 10.1016/0375-9474(79)90119-2
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.
1978SO05 Nucl.Phys. A304, 503 (1978) V.G.Soloviev, C.Stoyanov, V.V.Voronov The Influence of the Giant Dipole Resonance on Radiative Strength Functions in Spherical Nuclei NUCLEAR STRUCTURE 56Fe, 90Zr, Sn, 136,138Ba, 140Ce; calculated radiative strength functions. NUCLEAR REACTIONS 90Zr(γ, X), E=8-15 MeV; calculated total σ(E). 124Te, 140,142Ce(γ, X), E=8-18 MeV; calculated σ(E).
doi: 10.1016/0375-9474(78)90247-6
1978SO08 Phys.Lett. 79B, 187 (1978) V.G.Soloviev, C.Stoyanov, V.V.Voronov On the Enhancement of M1-Transitions from Neutron Resonances in the Ba and Ce Isotopes NUCLEAR STRUCTURE 136,138Ba, 140Ce; calculated M1 strength functions. Quasiparticle-phonon nuclear model.
doi: 10.1016/0370-2693(78)90218-6
1978SO12 Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 1991 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.9, 168 (1978) Description of the Characteristics of Nuclear States in a Wide Range of Excitation Energies NUCLEAR STRUCTURE 124Te; calculated E1 distribution. Quasiparticle phonon model. NUCLEAR REACTIONS 140Ce(γ, n), (γ, p), E=6-9 MeV; calculated σ(E). Quasiparticle phonon model.
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.
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