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NSR database version of April 27, 2024.

Search: Author = T.K.Dao

Found 14 matches.

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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
Citations: PlumX Metrics

1990DA23      Fiz.Elem.Chastits At.Yadra 21, 1456 (1990); Sov.J.Part.Nucl. 21, 623 (1990)

T.K.Dao, O.M.Knyazkov

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
Citations: PlumX Metrics

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)

Dao Tien Khoa, O.M.Knyazkov

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
Citations: PlumX Metrics

1987DA23      Z.Phys. A328, 67 (1987)

Dao Tien Khoa, O.M.Knyazkov

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)

Dao Tien Khoa

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)

Dao Tien Khoa, K.V.Shitikova

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)

V.V.Voronov, Dao Tien Khoa

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.

Note: The following list of authors and aliases matches the search parameter T.K.Dao: , T.K.DAO