NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = Dao Tien Khoa Found 14 matches. 1990DA12 J.Phys.(London) G16, 1253 (1990) T.K.Dao, A.Faessler, N.Ohtsuka Exchange Part of the Real Heavy-Ion Optical Potential within the Double-Folding Model and the Nuclear Matter Approach NUCLEAR REACTIONS 28Si(16O, 16O), E=49.7-215 MeV; 12C(12C, 12C), E=60-1200 MeV; 12C(16O, 16O), E=30-1510 MeV; calculated model potential parameters vs nucleus-nucleus separation. Double folding model.
doi: 10.1088/0954-3899/16/8/021
1990DA23 Fiz.Elem.Chastits At.Yadra 21, 1456 (1990); Sov.J.Part.Nucl. 21, 623 (1990) Exchange Effects in Nucleus-Nucleus Potentials and Nuclear Rainbow Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=40-1080 MeV; 208Pb(16O, 16O), E=80-1440 MeV; 90Zr(α, α), E=40-118 MeV; 58Ni(α, α), E=139.5, 172.5 MeV; 12C, 40Ca(α, α), E=104, 139 MeV; 40Ca, 12C(6Li, 6Li), E=156 MeV; calculated potentials; deduced exchange effects role. Semi-classical approach.
1990FA12 Phys.Rev.Lett. 65, 2978 (1990) A.Faessler, T.K.Dao, M.Grigorescu, R.Nojarov Low-Lying Magnetic Dipole Excitations in Actinide Nuclei NUCLEAR STRUCTURE 232Th, 238U; calculated B(M1). Quasiparticle RPA. NUCLEAR REACTIONS 232Th, 238U(e, e'), E not given; calculated form factors. Quasiparticle RPA transition densities.
doi: 10.1103/PhysRevLett.65.2978
1989DA17 Yad.Fiz. 50, 80 (1989) T.K.Dao, O.M.Knyazkov, I.N.Kukhtina, G.A.Feofilov Unified Semimicroscopic Description of Low-Energy p and α Scattering of Nuclei NUCLEAR REACTIONS 90Zr(p, p'), (p, p), E=25.05 MeV; 90Zr(α, α), (α, α'), E=104 MeV; analyzed σ(θ). 90Zr deduced neutron, proton distribution differences. Unified semi-microscopic description.
1988DA13 Yad.Fiz. 47, 1246 (1988) To a Unified Description of Elastic and Inelastic Scattering of Nucleons and Composite Particles on Nuclei NUCLEAR REACTIONS 58Ni(α, α), (α, α'), E=139 MeV; 90Zr(α, α), (α, α'), E=99.5 MeV; calculated σ(θ); deduced potential parameters, inelastic form factors.
1988DA24 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2256 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 178 (1988) Dao Tien Khoa, O.M.Knyazkov, I.N.Kukhtina, G.A.Feofilov Calculation of Nuclear Transition Densities in Quasi-Particle-Phonon Model and Semimicroscopic Analysis of the Scattering of 25-MeV Protons and 104-MeV α Particles at the 90Zr Nucleus NUCLEAR REACTIONS 90Zr(α, α'), E=104 MeV; 90Zr(p, p'), E=25 MeV; analyzed σ(θ). Quasiparticle-phonon model transition densities.
1988NE02 J.Phys.(London) G14, 725 (1988) V.O.Nesterenko, I.N.Kukhtina, A.V.Sushkov, Dao Tien Khoa On the Role of Hexadecapole Forces in Describing γ-Band States in the Rare-Earth Region NUCLEAR REACTIONS 168Er(polarized p, p'), E=65 MeV; calculated σ(θ), analyzing power vs θ; deduced hexadecapole force role. RPA isoscalar transition rates, coupled-channels model.
doi: 10.1088/0305-4616/14/6/012
1987DA23 Z.Phys. A328, 67 (1987) Exchange Effects in Elastic and Inelastic Alpha- and Heavy-Ion Scattering NUCLEAR REACTIONS 58Ni(α, α), E=172.5 MeV; 58Ni(α, α), (α, α'), E=139 MeV; 90Zr(α, α), E=40-118 MeV; 90Zr(α, α'), E=99.5 MeV; calculated σ(θ). 208Pb(α, α), E=27.6-166 MeV; 208Pb(16O, 16O), E=86-600 MeV; 208Pb(16O, 16O'), E=104 MeV; 40Ca(40Ca, 40Ca), E=129.6-240 MeV; 40Ca(16O, 16O), E=40-214 MeV; calculated potential parameters. 208Pb(16O, 16O'), E=104 MeV; calculated inelastic form factors, σ(θ). 208Pb(16O, 16O'), E=104 MeV; calculated σ(θ). Semi-microscopic model.
1987DA26 Rev.Roum.Phys. 32, 569 (1987) Exchange Effects in Elastic and Inelastic Alpha- and Heavy-Ion Scattering NUCLEAR REACTIONS 58Ni(α, α), (α, α'), E=139, 172.5 MeV; 90Zr(α, α), (α, α'), E=40-118 MeV; 208Pb(α, α), (α, α'), E=27.6-166 MeV; calculated σ(θ); deduced optical potentials.
1986DA23 Yad.Fiz. 44, 906 (1986) Dao Tien Khoa, I.N.Kukhtina, V.Yu.Ponomarev The Description of the Low-Lying One- and Two-Phonon Excitations in Spherical Nuclei Induced by Low-Energy Protons NUCLEAR REACTIONS 58Ni, 90Zr, 208Pb(p, p), (p, p'), E=40, 61.2 MeV; calculated σ(θ). Quasiparticle-phonon nuclear model.
1985DA12 Yad.Fiz. 41, 1166 (1985) A Microscopic Approach to the Description of Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=22.8, 50.6 MeV; 124Sn, 208Pb(6Li, 6Li), E=50.6 MeV; 90Zr(6Li, 6Li), E=34 MeV; 142,144,146Nd(12C, 12C), E=70.4 MeV; 208Pb(12C, 12C), E=96 MeV; 90Zr(12C, 12C), E=98 MeV; 60Ni(16O, 16O), E=61.4, 141.7 MeV; 208Pb(16O, 16O), E=104 MeV; calculated σ(θ). Microscopic model.
1985VO14 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2168 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 78 (1985) V.V.Voronov, Dao Tien Khoa, V.Yu.Ponomarev Microscopic Description of Elastic Scattering of γ-Quanta on Spherical Nuclei and Giant Dipole Resonance Excitation NUCLEAR REACTIONS 60Ni, 56Fe, 92Mo(γ, γ), E=14-22 MeV; calculated σ(θ) vs E, GDR strength functions. Quasiparticle-phonon model.
1984VO16 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 2008 (1984) Dipole Photon Scattering by Nuclei in the Lead Region NUCLEAR STRUCTURE 207,209Pb; 209Bi, 207Tl; calculated levels, spectroscopic factors. Quasiparticle-phonon model. NUCLEAR REACTIONS 208Pb(γ, γ), E=5-8 MeV; 206,207Pb, 205Tl, 209Bi(γ, γ), E ≈ 4.5-8 MeV; calculated dipole σ(θ) vs E. Quasiparticle-phonon model.
1984VO17 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 1846 (1984) V.V.Voronov, Dao Tien Khoa, V.Yu.Ponomarev Lowlying Dipole States in Spherical Nuclei NUCLEAR STRUCTURE 58Fe, 60Ni, 62Zn; N=80-86; calculated B(E1). Quasiparticle-phonon model.
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