NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.I.Bastrukov Found 26 matches. 2012BA25 Phys.Scr. 85, 065204 (2012) S.I.Bastrukov, I.V.Molodtsova, J.W.Yu, R.X.Xu On Alfven's hypothesis about nuclear hydromagnetic resonances
doi: 10.1088/0031-8949/85/06/065204
2004IS06 Nucl.Phys. A734, E112 (2004) A.A.Isayev, S.I.Bastrukov, J.Yang Pairing effects in low density domain of nuclear matter
doi: 10.1016/j.nuclphysa.2004.03.033
2004IS15 Yad.Fiz. 67, 1867 (2004); Phys.Atomic Nuclei 67, 1840 (2004) A.A.Isayev, S.I.Bastrukov, J.Yang np Pairing Correlations in Low-Density Region of Nuclear Matter
doi: 10.1134/1.1811188
2002MI16 Eur.Phys.J. A 13, 399 (2002) The Low-Lying Isoscalar Giant Dipole Resonance NUCLEAR STRUCTURE 90Zr, 116Sn, 208Pb; analyzed isoscalar GDR energies. Microscopic and hydrodynamical model results compared with data.
doi: 10.1007/s10050-002-8768-3
1999BA74 Fiz.Elem.Chastits At.Yadra 30, 992 (1999); Phys.Part.Nucl. 30, 436 (1999) S.I.Bastrukov, I.V.Molodtsova, D.V.Podgainy, F.Weber, V.V.Papoyan Elastodynamical Properties of Nuclear Matter from the Observed Activity of Neutron Stars
1998BA05 J.Phys.(London) G24, L1 (1998) S.I.Bastrukov, D.V.Podgainy, I.V.Molodtsova, G.I.Kosenko Macroscopic Calculus for the Fission Barrier Height of Superheavy Elements NUCLEAR STRUCTURE 265Hs, 269,271,275,276Ds, 272Rg, 275,277,281,282Cn, 276Nh, 283,287,288Fl, 291,292Lv; calculated elastic deformation energy, fission barrier height. Elastic globe, liquid drop models.
doi: 10.1088/0954-3899/24/1/002
1997BA50 Int.J.Mod.Phys. E6, 89 (1997) S.I.Bastrukov, J.Libert, I.V.Molodtsova Elastodynamic Features of Nuclear Matter from Macroscopic Model of Giant Magnetic Resonances NUCLEAR STRUCTURE A=40-220; calculated torsional moment of inertia, stiffness magnetic dipole resonances energy vs mass, B(M1). 208Pb calculated M1 resonance form factors. Macroscopic approach, collective model.
doi: 10.1142/S0218301397000068
1996BB27 Dok.Akad.Nauk 350, 321 (1996); Phys.Doklady 41, 388 (1996) On the Stability of the Transverse-Shear Elastic Response of a Heavy Spherical Nucleus
1995BA15 Phys.Scr. 51, 54 (1995) S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov Torsional Multipole Magnetic Response of a Heavy Spherical Nucleus NUCLEAR STRUCTURE 28Si, 90Zr, 140Ce, 208Pb; calculated B(λ). 140Ce; calculated collective transition current density. Distorted Fermi sphere model. NUCLEAR REACTIONS 140Ce(e, e'), E=20-120 MeV; calculated σ(θ) vs E, θ=165°. Distorted Fermi sphere model.
doi: 10.1088/0031-8949/51/1/008
1995BA56 Phys.Rev. C52, 1114 (1995) S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov Integral Characteristic Parameters of the Giant M1 Resonance NUCLEAR STRUCTURE 90Zr, 120Sn, 140Ce, 206,208Pb; calculated giant M1 resonance energy, B(λ), Γ. Semi-classical model.
doi: 10.1103/PhysRevC.52.1114
1995BA91 Yad.Fiz. 58, No 6, 989 (1995); Phys.Atomic Nuclei 58, 916 (1995) S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov Macroscopic Mechanism of the Excitation of Mλ, T = 0 Resonances in Inelastic Electron Scattering NUCLEAR STRUCTURE 90Zr, 28Si, 140Ce, 208Pb; calculated collective magnetic torsional excitations, B(λ), energy for M2, M3 resonances. Nuclear fluid dynamics model. NUCLEAR REACTIONS 90Zr(e, e'), E not given; calculated torsional, magnetic quadrupole modes associated form factors. Nuclear fluid dynamics model.
1995BA93 Fiz.Elem.Chastits At.Yadra 26, 415 (1995); Sov.J.Part.Nucl 26, 180 (1995) Macroscopic Model for Magnetic Resonances in Spherical Nuclei NUCLEAR REACTIONS 90Zr(e, e'), E not given; calculated collective form factors. 140Ce(e, e'), E=20-120 MeV; 208Pb(e, e'), E=25-155 MeV; calculated magnetic quadrupole resonance σ(θ).
1995BB10 Pisma Zh.Eksp.Teor.Fiz. 61, 705 (1995); JETP Lett. 61, 717 (1995) Macroscopic Model of Magnetic Dipole Resonance in Spherical Nuclei NUCLEAR STRUCTURE 90Zr, 120Sn, 140Ce, 206,208Pb; calculated giant M1 resonance energy, B(λ); deduced branching ratio Z-, mass number dependences. Macroscopic model.
1994BA94 Yad.Fiz. 57, No 7, 1245 (1994); Phys.Atomic Nuclei 57, 1177 (1994) S.I.Bastrukov, I.V.Molodtsova, E.Kh.Yuldashbaeva The Effect of Elastic Properties of Nuclear Matter on Nuclear Fission
1993BA41 Nucl.Phys. A562, 191 (1993) S.I.Bastrukov, S.Misicu, A.V.Sushkov Dipole Torus Mode in Nuclear Fluid-Dynamics NUCLEAR STRUCTURE 90Zr, 208Pb; calculated transition current density. Nuclear fluid dynamics, dipole torus mode. NUCLEAR REACTIONS 90Zr, 208Pb(γ, X), E not given; calculated photoabsorption dipole electric form factor, σ. Nuclear fluid dynamics, dipole torus mode.
doi: 10.1016/0375-9474(93)90195-4
1993BA67 Europhys.Lett. 22, 85 (1993) Magnetic Form Factors for Nuclear Twist Modes NUCLEAR REACTIONS 90Zr, 40Ca, 208Pb(e, e'), E not given; calculated magnetic multipole form factors; deduced photoexcitation σ. Twist resonances, plane wave Born approximation.
doi: 10.1209/0295-5075/22/2/002
1993BA77 Bull.Rus.Acad.Sci.Phys. 57, 1796 (1993) S.I.Bastrukov, I.V.Molodtsova, V.M.Shilov Widths of Magnetic Twist Resonances
1992BA14 J.Phys.(London) G18, L37 (1992) Fluid-Dynamical Description of Low-Energy Resonances with (λ) ≥ 3 NUCLEAR STRUCTURE A ≤ 250; calculated low energy octupole, hexadecapole resonances energies. Fluid dynamical theory.
doi: 10.1088/0954-3899/18/2/004
1992BA34 Z.Phys. A341, 395 (1992) The Twist M(λ), T = 0 Giant Modes in Spherical Nuclei NUCLEAR STRUCTURE A=20-210; calculated twisting mode energies, B(λ). High multipole extension of Holzwarth-Eckart model, inertia, stiffness against multipolarity parameters from distorted Fermi-surface model.
doi: 10.1007/BF01301382
1991BA32 Z.Phys. A338, 455 (1991) S.I.Bastrukov, A.Bonasera, M.Di Toro, A.Sushkov The Low-Energy Isoscalar Dipole Resonance in Sperical Nuclei NUCLEAR STRUCTURE 90Zr, 208Pb; calculated low energy isoscalar dipole resonance; deduced soleniodal component role. Compressional Fermi-drop model.
doi: 10.1007/BF01295774
1991BA58 Yad.Fiz. 54, 927 (1991); Sov.J.Nucl.Phys. 54, 561 (1991) S.I.Bastrukov, E.B.Balbutsev, I.V.Molodtsova, M.L.Bobryshev, A.V.Papykin Isosclar 4- and 5- Giant Resonances in Spherical Nuclei NUCLEAR STRUCTURE A ≤ 230; calculated 4-, 5- giant resonances, excitation probabilities. Moments method.
1990BA04 Z.Phys. A335, 139 (1990) Fluid-Dynamics of the Nuclear Surface Fermi-Layer NUCLEAR STRUCTURE A=50-250; calculated quantum-capillary 2+ state energy vs mass. Long mean free path approach, fluid dynamical model.
1989BA77 Yad.Fiz. 50, 1264 (1989) E.B.Balbutsev, S.I.Bastrukov, I.N.Mikhailov, V.P.Sinichkin, L.Sh.Shekhter Vibrational 1+, 2+, 3+, and 4+ Excitations in Spherical Nuclei NUCLEAR STRUCTURE A=38-208; calculated collective state energies, giant resonance EWSR. Incompressible nucleus, sharp edge.
1984BA37 ATOMKI Kozlem. 26, 90 (1984) Description of the Low-Lying States in Deformed Nuclei within the Quasiparticle-Phonon Nuclear Model NUCLEAR STRUCTURE 163Dy, 165Ho; A=155-175; calculated B(E2). 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.
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.
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