NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = D.Khoa Found 75 matches. 2022KH02 Phys.Rev. C 105, 065802 (2022) Spin symmetry energy and equation of state of spin-polarized neutron star matter
doi: 10.1103/PhysRevC.105.065802
2021AN01 Nucl.Phys. A1006, 122078 (2021) N.L.Anh, N.H.Phuc, D.T.Khoa, L.H.Chien, N.T.T.Phuc Folding model approach to the elastic p+12, 13C scattering at low energies and radiative capture 12, 13C(p, γ) reactions NUCLEAR REACTIONS 12,13C(p, γ), (p, p), E<5 MeV; calculated σ; deduced optical model potential, S-factors in the folding model, using a realistic density dependent nucleon-nucleon interaction.
doi: 10.1016/j.nuclphysa.2020.122078
2021PH01 Eur.Phys.J. A 57, 7 (2021) N.H.Phuc, Dao T.Khoa, N.T.T.Phuc Elastic α transfer in the 16O+12C scattering and its impact on the nuclear rainbow NUCLEAR REACTIONS 12C(16O, 16O), E=100-200 MeV; analyzed available data; deduced σ, S-matrix elements in the two-channel CRC analysis.
doi: 10.1140/epja/s10050-020-00325-3
2021PH02 Eur.Phys.J. A 57, 75 (2021) N.H.Phuc, D.T.Khoa, N.T.T.Phuc, D.C.Cuong Suppression of the nuclear rainbow in the inelastic nucleus-nucleus scattering NUCLEAR REACTIONS 12C(12C, 12C'), E=240 MeV; 12C(16O, 16O'), E=200, 260 MeV; analyzed available data; calculated σ(θ), σ.
doi: 10.1140/epja/s10050-021-00397-9
2021TA14 Eur.Phys.J. A 57, 153 (2021) Equation of state of asymmetric nuclear matter and the tidal deformability of neutron star
doi: 10.1140/epja/s10050-021-00467-y
2020CU03 Phys.Rev. C 102, 024622 (2020) D.C.Cuong, P.Descouvemont, D.T.Khoa, N.H.Phuc Coupled-reaction-channel study of the 12C(α, 8Be) reaction and the 8Be + 8Be optical potential NUCLEAR REACTIONS 8Be(8Be, 8Be), E(cm)=41.3 MeV; 8Be(α, α), E(cm)=43.3 MeV; 8Be(α, α), E=65 MeV; calculated differential σ(θ) using three- and four-body continuum-discretized coupled-channel (CDCC) methods, with realistic α + α interaction, and explicit accounting of the breakup effect; deduced local equivalent optical potential parameters. 12C(α, 8Be)8Be, E=65 MeV; calculated differential σ(θ) using the coupled-reaction channel (CRC) calculation with optical potentials from the CDCC calculations, and α spectroscopic factors from the complex scaling method (CSM) cluster model calculation; deduced cluster structure of 12C. Comparison with experimental data for elastic 12+α scattering.
doi: 10.1103/PhysRevC.102.024622
2020LO13 J.Phys.(London) G47, 035106 (2020) Rearrangement term in the folding model of the nucleon optical potential NUCLEAR REACTIONS 40,48Ca, 90Zr, 208Pb(n, n), E<40 MeV; calculated σ(θ), σ. Comparison with available data.
doi: 10.1088/1361-6471/ab5f54
2020TA18 Phys.Rev. C 102, 045809 (2020) Spin-polarized β-stable neutron star matter: The nuclear symmetry energy and GW170817 constraint
doi: 10.1103/PhysRevC.102.045809
2019PH03 Phys.Rev. C 100, 054615 (2019) N.T.T.Phuc, R.S.Mackintosh, N.H.Phuc, D.T.Khoa Elastic transfer and parity dependence of the nucleus-nucleus optical potential NUCLEAR REACTIONS 12C(16O, 16O), (16O, X), E=132, 300 MeV; calculated σ(θ, E) for ground-state channels of 16O and 12C using coupled reaction channel (CRC) approach with two- and ten-channel model space calculated parity-dependent core exchange potential (CEP) from S-matrix using inversion method; deduced strong contribution by the complex Majorana term in the total optical potential (OP).
doi: 10.1103/PhysRevC.100.054615
2018CH57 Phys.Rev. C 98, 064604 (2018) L.H.Chien, D.T.Khoa, D.C.Cuong, N.H.Phuc Consistent mean-field description of the 12C + 12C optical potential at low energies and the astrophysical S factor NUCLEAR REACTIONS 12C(12C, 12C), E=16, 18, 20, 35, 45, 74.2, 78.8, 83.3, 102.1, 117.1 MeV; analyzed differential σ(θ, E) experimental data, fusion σ(E); deduced optical model parameters, astrophysical S factor and reaction rate for T=0.8-2.0 GK using optical, double-folding (DFM) with CDM3Y3 density dependent nucleon-nucleon (NN) interaction, and barrier penetration models.
doi: 10.1103/PhysRevC.98.064604
2018PH02 Phys.Rev. C 98, 024613 (2018) N.T.T.Phuc, N.H.Phuc, D.T.Khoa Direct and indirect α transfer in elastic 16O + 12C scattering NUCLEAR REACTIONS 12C(16O, 16O), (16O, X), E=100, 159.9, 124, 132, 300 MeV; calculated σ(θ) for ground state channels of 16O and 12C, direct and indirect (multistep) transitions using form factors from double-folding model with CDM3Y3 interaction, with α spectroscopic factors (Sα) taken from large-scale shell model. Systematic optical model and coupled reaction channel (CRC) calculation including up to ten channels of excited and elastic transferred states. Comparison with experimental data. Discussed large-angle contributions associated with different transfer routes.
doi: 10.1103/PhysRevC.98.024613
2017CH45 Phys.Lett. B 774, 559 (2017) L.X.Chung, C.A.Bertulani, P.Egelhof, S.Ilieva, D.T.Khoa, O.A.Kiselev The dominance of the ν(0d5/2)2 configuration in the N = 8 shell in 12Be from the breakup reaction on a proton target at intermediate energy NUCLEAR REACTIONS 1H(12Be, X)11Be, E=700.5 MeV/nucleon; measured reaction products; deduced σ(p). Distorted wave impulse approximation (DWIA) analysis.
doi: 10.1016/j.physletb.2017.09.068
2017LO07 Phys.Rev. C 96, 014311 (2017) Single-charge-exchange reactions and the neutron density at the surface of the nucleus NUCLEAR STRUCTURE 58Ni, 90Zr, 120Sn, 208Pb; calculated nuclear densities calculated using the Skyrme HF-BCS calculation. NUCLEAR REACTIONS 58Ni, 90Zr, 208Pb(3He, t), E=420 MeV; 120Sn(p, n), E=170 MeV; calculated differential σ(θ) for the population of the isobaric analog state (IAS) using the DWBA approach with the single-charge-exchange (SCX) form factors obtained from nuclear density calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.014311
2016KH09 Phys.Rev. C 94, 034612 (2016) D.T.Khoa, N.H.Phuc, D.T.Loan, B.M.Loc Nuclear mean field and double-folding model of the nucleus-nucleus optical potential NUCLEAR REACTIONS 12C(12C, 12C), E=139.5, 158.8, 240, 288.6, 360, 1016 MeV; 12C(16O, 16O), E=132, 170, 200, 230, 260, 281, 330, 608, 1503 MeV; analyzed σ(θ, E) data using realistic density dependent CDM3Yn versions of the M3Y interaction in an extended Hartree-Fock (HF) calculation of nuclear matter (NM), and double-folding model of the nucleus-nucleus optical potential.
doi: 10.1103/PhysRevC.94.034612
2016TA05 Phys.Rev. C 93, 035806 (2016) N.H.Tan, D.T.Loan, D.T.Khoa, J.Margueron Mean-field study of hot β-stable protoneutron star matter: Impact of the symmetry energy and nucleon effective mass
doi: 10.1103/PhysRevC.93.035806
2015CH51 Phys.Rev. C 92, 034608 (2015) L.X.Chung, O.A.Kiselev, D.T.Khoa, P.Egelhof Elastic proton scattering at intermediate energies as a probe of the 6, 8He nuclear matter densities NUCLEAR REACTIONS 1H(6He, p), E=717 MeV/nucleon; 1H(8He, p), E=674 MeV/nucleon; 4He(p, p), E=702 MeV; analyzed σ(θ) data from GSI experiments using Glauber multiple scattering model (GMSM) and several phenomenological parametrizations of the nuclear matter density. 6,8He; deduced nuclear matter radii and densities, structure of 6He in terms of the core and dineutron halo radii.
doi: 10.1103/PhysRevC.92.034608
2015LO09 Phys.Rev. C 92, 034304 (2015) Extended Hartree-Fock study of the single-particle potential: The nuclear symmetry energy, nucleon effective mass, and folding model of the nucleon optical potential NUCLEAR STRUCTURE 1n, 1H; calculated neutron and proton single-particle (SP) optical potentials (OP) and the symmetry energy in nuclear matter, neutron and proton, effective mass and their splittings. Consistent Hartree-Fock (HF) study of the asymmetric nuclear matter using CDM3Y3 and CDM3Y6 density dependent interactions. NUCLEAR REACTIONS 208Pb(n, n), E=30.4, 40 MeV; calculated σ(θ) by folding model of the neutron optical potential. Consistent inclusion of rearrangement terms (RT) into the HF-type folding model calculation of the nucleon OP in the mean-field approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.034304
2014KH02 Eur.Phys.J. A 50, 34 (2014) Folding model study of the charge-exchange scattering to the isobaric analog state and implication for the nuclear symmetry energy NUCLEAR REACTIONS 208Pb(n, n), E=30.4 MeV;48Ca, 90Zr, 120Sn, 208Pb(p, p), E=35, 45 MeV;90Zr, 120Sn(p, p), E=40 MeV;208Pb(p, p), E=45 MeV; calculated σ(θ), σ using complex folded optical potential and hybrid optical potential; deduced model parameters. 48Ca, 90Zr, 120Sn(p, n), E=35, 45 MeV; calculated σ(θ), σ(θ) to IAS using CC with complex folded or hybrid optical potential; deduced symmetry energy. 14C, 48Ca(3He, t), E=72, 82 MeV; calculated σ, σ(θ) to IAS using CC with complex folded or hybrid optical potential. Results compared with data.
doi: 10.1140/epja/i2014-14034-9
2014LO02 Phys.Rev. C 89, 024317 (2014) B.M.Loc, D.T.Khoa, R.G.T.Zegers Charge-exchange scattering to the isobaric analog state at medium energies as a probe of the neutron skin NUCLEAR REACTIONS 90Zr, 208Pb(3He, t), E=420 MeV; analyzed σ(θ) data in distorted wave Born approximation (DWBA) using double folded charge-exchange form factor for scattering to the isobaric analog state (IAS). deduced neutron skin value.
doi: 10.1103/PhysRevC.89.024317
2013CU05 Phys.Rev. C 88, 064317 (2013) D.C.Cuong, D.T.Khoa, Y.Kanada-Enyo Folding-model analysis of inelastic α+12C scattering at medium energies, and the isoscalar transition strengths of the cluster states of 12C NUCLEAR REACTIONS 12C(α, α), (α, α'), E=240, 386 MeV; analyzed σ(E, θ) data for first 1-, 2+ and 3- states, second 2+ (Hoyle state), excited first and second 0+ states using DWBA and coupled channel methods; deduced best-fit M(E0), B(E1), B(E2), B(E3), distribution of isoscalar transition strength for second excited 0+ and second 2+. Folding model+coupled-channels analysis.
doi: 10.1103/PhysRevC.88.064317
2012DE03 Phys.Rev. C 85, 024619 (2012) R.P.DeVito, D.T.Khoa, S.M.Austin, U.E.P.Berg, B.M.Loc Neutron scattering from 208Pb at 30.4 and 40.0 MeV and isospin dependence of the nucleon optical potential NUCLEAR REACTIONS 208Pb(n, n), E=30.4, 40.0 MeV; measured neutron spectra using time-of-flight system at NSCL, MSU, σ(E, θ); comparison with σ(E, θ) data for 208Pb(p, p), E=45.0, 47.3, 49.4, 54.2 MeV, and optical model calculations; deduced optical model parameters using the Woods-Saxon geometry given by the CH89 systematics. Diffractive structure in σ(θ) distributions. 208Pb(p, n), E=45 MeV; analyzed σ(θ); deduced isovector term (isospin impurity) of the optical potential. Relevance to data for IAS.
doi: 10.1103/PhysRevC.85.024619
2011LO16 Phys.Rev. C 83, 065809 (2011) D.T.Loan, N.H.Tan, Dao T.Khoa, J.Margueron Equation of state of neutron star matter, and the nuclear symmetry energy
doi: 10.1103/PhysRevC.83.065809
2010CU01 Nucl.Phys. A836, 11 (2010) Microscopic study of the isoscalar giant resonances in 208Pb induced by inelastic α scattering NUCLEAR REACTIONS 208Pb(α, α'), E=240, 386 MeV; analyzed σ(θ), σ(θ, E) using a microscopic double-folding model within DWBA; deduced isoscalar GDR, GQR strength distributions using RPA and DWBA. Comparison with other models and experimental data.
doi: 10.1016/j.nuclphysa.2009.12.009
2009NG02 Phys.Rev. C 79, 034314 (2009) Neutron transition strengths of 2+1 states in the neutron-rich oxygen isotopes determined from inelastic proton scattering NUCLEAR REACTIONS 18O(polarized p, p), (polarized p, p'), E=24.5, 43 MeV; 20O(p, p), (p, p'), E=43 MeV; 22O(p, p), (p, p'), E=46.6 MeV; analyzed σ(θ) and analyzing powers data for 2+ states using coupled-channel analysis with microscopic optical potential and inelastic form factor in the folding model; deduced isoscalar and isovector deformation lengths, deformation ratios. 16,18,20,22,24O; systematics of levels and deformation lengths for first 2+ states.
doi: 10.1103/PhysRevC.79.034314
2009TH03 Phys.Rev. C 80, 064312 (2009) H.S.Than, D.T.Khoa, N.Van Giai Neutron star cooling: A challenge to the nuclear mean field
doi: 10.1103/PhysRevC.80.064312
2008KH02 Phys.Lett. B 660, 331 (2008) Missing monopole strength of the Hoyle state in the inelastic α + 12C scattering NUCLEAR REACTIONS 12C(α, α), E=104, 172.5, 240 MeV; 12C(α, α'), E=104, 139, 172.5, 240 MeV; analyzed σ(θ) using a fully microscopic folding model. Missing monopole strength of the Hoyle state discussed.
doi: 10.1016/j.physletb.2007.12.059
2008KH14 Int.J.Mod.Phys. E17, 2055 (2008) Probing the isoscalar excitations of 12C with inelastic alpha scattering NUCLEAR REACTIONS 12C(α, α), E=240 MeV; calculated energy levels, J, π, B(Eλ), σ(θ), form factors. DWBA, comparison with experiment.
doi: 10.1142/S0218301308011082
2007GR23 Phys.Rev. C 76, 054608 (2007) D.E.Groh, J.S.Pinter, P.F.Mantica, T.J.Mertzimekis, A.E.Stuchbery, D.T.Khoa Nuclear spin polarization following intermediate-energy heavy-ion reactions NUCLEAR REACTIONS 197Au(14N, X)12B, E=39.4 MeV/nucleon; 197Au(15N, X)13B, E=68, 109.6 MeV/nucleon; 93Nb(15N, X)13B, E=67.3 MeV/nucleon; 27Al(15N, X)13B, E=68 MeV/nucleon; 9Be(36Ar, X)37K, E=150.0 MeV/nucleon; 9Be(36S, X)34Al, E=77.6 MeV/nucleon; 9Be, 184W(58Ni, X)55Ni, E=140 MeV/nucleon; calculated polarization coefficients.
doi: 10.1103/PhysRevC.76.054608
2007KH02 J.Phys.(London) G34, R111 (2007) D.T.Khoa, W.von Oertzen, H.G.Bohlen, S.Ohkubo Nuclear rainbow scattering and nucleus-nucleus potential
doi: 10.1088/0954-3899/34/3/R01
2007KH09 Phys.Rev. C 76, 014603 (2007) Folding model study of the isobaric analog excitation: Isovector density dependence, Lane potential, and nuclear symmetry energy NUCLEAR REACTIONS 48Ca, 90Zr, 120Sn(p, n), E=35, 24 MeV; analyzed σ and angular distributions data using a folding model.
doi: 10.1103/PhysRevC.76.014603
2007KH20 Eur.Phys.J. Special Topics 150, 31 (2007) Isovector deformation and its link to the neutron shell closure NUCLEAR REACTIONS 1H(38S, 38S), E=39 MeV/nucleon; 1H(22O, 22O), e=46.6 MeV/nucleon; calculated elastic and inelastic σ(θ) using the DWBA formalism with folded form factors. Compared results to data.
doi: 10.1140/epjst/e2007-00258-8
2006BE04 Phys.Rev.Lett. 96, 012501 (2006) E.Becheva, Y.Blumenfeld, E.Khan, D.Beaumel, J.M.Daugas, F.Delaunay, Ch.-E.Demonchy, A.Drouart, M.Fallot, A.Gillibert, L.Giot, M.Grasso, N.Keeley, K.W.Kemper, D.T.Khoa, V.Lapoux, V.Lima, A.Musumarra, L.Nalpas, E.C.Pollacco, O.Roig, P.Roussel-Chomaz, J.E.Sauvestre, J.A.Scarpaci, F.Skaza, H.S.Than N = 14 Shell Closure in 22O Viewed through a Neutron Sensitive Probe NUCLEAR REACTIONS 1H(22O, 22O), (22O, 22O'), E=46.6 MeV/nucleon; measured particle spectra, σ(E, θ). 22O level deduced deformation parameter, shell closure features. MUST detector array.
doi: 10.1103/PhysRevLett.96.012501
2005KH09 Phys.Rev. C 71, 044601 (2005) Isospin dependence of 6He+p optical potential and the symmetry energy NUCLEAR REACTIONS 1H(6He, 6He), (6He, 6Li), E=41.6 MeV/nucleon; analyzed σ(θ); deduced optical potential, symmetry energy, halo features. Folding analysis, coupled-channels formalism, Hartree-Fock calculation of nuclear matter symmetry energy.
doi: 10.1103/PhysRevC.71.044601
2005KH13 Nucl.Phys. A759, 3 (2005) D.T.Khoa, H.G.Bohlen, W.von Oertzen, G.Bartnitzky, A.Blazevic, F.Nuoffer, B.Gebauer, W.Mittig, P.Roussel-Chomaz Study of refractive structure in the inelastic 16O + 16O Image scattering at the incident energies of 250 to 1120 MeV NUCLEAR REACTIONS 16O(16O, 16O'), E=250, 350, 480, 704, 1120 MeV; measured σ(E, θ); deduced refractive features. DWBA and folding-model analysis, nuclear rainbow.
doi: 10.1016/j.nuclphysa.2005.04.027
2004KH06 Phys.Rev. C 69, 044605 (2004) D.T.Khoa, H.S.Than, T.H.Nam, M.Grasso, N.Van Giai Microscopic calculation of the interaction cross section for stable and unstable nuclei based on the nonrelativistic nucleon-nucleon t matrix NUCLEAR REACTIONS 12C(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), (12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), (20C, X), (16O, X), (17O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), E ≈ 740-1050 MeV/nucleon; calculated reaction and interaction σ. DWIA, microscopic complex optical potential, folding model.
doi: 10.1103/PhysRevC.69.044605
2004KH09 Phys.Lett. B 595, 193 (2004) Di-neutron elastic transfer in the 4He(6He, 6He)4He reaction NUCLEAR REACTIONS 4He(6He, 6He), E(cm)=11.6, 15.9, 60.3 MeV; analyzed σ(θ); deduced role of two-neutron elastic transfer. Coupled reaction channels analysis.
doi: 10.1016/j.physletb.2004.05.063
2003CO20 Nucl.Phys. A722, 111c (2003) G.Colo, P.F.Bortignon, D.Sarchi, D.T.Khoa, E.Khan, N.Van Giai Excited states of neutron-rich nuclei: mean field theory and beyond NUCLEAR STRUCTURE 132Sn; calculated GDR transition densities, dipole strength distribution. 120,122,124,126,128,130,132,134Sn; calculated level energies, B(E2), B(E3). Quasiparticle RPA. NUCLEAR REACTIONS 32S(p, p'), E=53 MeV; 38S(p, p'), E=39 MeV; calculated σ(θ), isoscalar and isovector components. Comparison with data.
doi: 10.1016/S0375-9474(03)01345-9
2003KE10 Nucl.Phys. A726, 159 (2003) N.Keeley, K.W.Kemper, D.T.Khoa DWBA analysis of the 13C(6Li, d)17O reaction at 10 MeV/nucleon and its astrophysical implications NUCLEAR REACTIONS 13C(6Li, d), E=60 MeV; analyzed σ(E, θ). 17O deduced spectroscopic factors. DWBA and coupled reaction channels analysis, comparison with previous results, astrophysical implications discussed.
doi: 10.1016/S0375-9474(03)01622-1
2003KH05 Phys.Rev. C 68, 011601 (2003) Probing the isovector transition strength of the low-lying nuclear excitations induced by inverse kinematics proton scattering NUCLEAR REACTIONS 1H(18O, 18O'), (20O, 20O'), E=30, 43 MeV/nucleon; analyzed σ(E, θ). 18O, 20O deduced deformation parameters, isoscalar and isovector transition matrix elements. DWBA analysis, folding model.
doi: 10.1103/PhysRevC.68.011601
2003KH10 Nucl.Phys. A722, 92c (2003) Microscopic study of interaction cross sections measured at relativistic energies for stable and unstable nuclei NUCLEAR REACTIONS 12C(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), (12C, X), (14C, X), (16C, X), (18C, X), (19C, X), (20C, X), (16O, X), (18O, X), (20O, X), (22O, X), (24O, X), E ≈ 790-1050 MeV/nucleon; calculated reaction, interaction σ. Parameter-free folding approach, comparisons with data.
doi: 10.1016/S0375-9474(03)01342-3
2003VO19 Nucl.Phys. A722, 202c (2003) W.von Oertzen, H.G.Bohlen, D.T.Khoa Nuclear rainbow and the EOS of cold nuclear matter NUCLEAR REACTIONS 16O(16O, 16O), E=124-1120 MeV; analyzed σ(θ); deduced density-dependent interaction, equation of state for cold nuclear matter.
doi: 10.1016/S0375-9474(03)01359-9
2002BO20 Nucl.Phys. A703, 573 (2002) H.G.Bohlen, D.T.Khoa, W.von Oertzen, B.Gebauer, F.Nuoffer, G.Bartnitzky, A.Blazevic, W.Mittig, P.Roussel-Chomaz One-Neutron Transfer Reaction and Refractive Effects in the 16O + 16O System NUCLEAR REACTIONS 16O(16O, 17O), E=250-1120 MeV; measured σ(E, θ); deduced spectroscopic factors. Optical potential, DWBA analysis.
doi: 10.1016/S0375-9474(01)01676-1
2002KH01 Phys.Rev. C65, 024611 (2002) D.T.Khoa, G.R.Satchler, D.T.Nguyen Do 1.37 GeV α Particles Find Nuclei Attractive or Repulsive ? NUCLEAR REACTIONS 12C, 40Ca(α, α), E=1370 MeV; analyzed σ(θ); deduced optical potential features.
doi: 10.1103/PhysRevC.65.024611
2002KH05 Nucl.Phys. A706, 61 (2002) D.T.Khoa, E.Khan, G.Colo, N.Van Giai Folding Model Analysis of Elastic and Inelastic Proton Scattering on Sulfur Isotopes NUCLEAR REACTIONS 30,32,34,36,38,40S(p, p), (p, p'), E ≈ 28-53 MeV/nucleon; calculated σ(θ). Folding-plus-DWBA approach, comparison with data.
doi: 10.1016/S0375-9474(02)00866-7
2002KH13 Prog.Theor.Phys.(Kyoto), Suppl. 146, 452 (2002) Isovector Mixing in Inelastic Scattering Induced by the Radioactive Beams NUCLEAR REACTIONS 1H(20O, 20O), E=43 MeV/nucleon; analyzed elastic and inelastic σ(θ); deduced transition moments, isovector mixing.
doi: 10.1143/PTPS.146.452
2002LA20 Phys.Rev. C66, 034608 (2002) V.Lapoux, N.Alamanos, F.Auger, V.Fekou-Youmbi, A.Gillibert, F.Marie, S.Ottini-Hustache, J.-L.Sida, D.T.Khoa, Y.Blumenfeld, F.Marechal, J.-A.Scarpaci, T.Suomijarvi, J.H.Kelley, J.-M.Casandjian, M.Chartier, M.D.Cortina-Gil, M.Mac Cormick, W.Mittig, F.de Oliveira Santos, A.N.Ostrowski, P.Roussel-Chomaz, K.W.Kemper, N.Orr, J.S.Winfield Coupling Effects in the Elastic Scattering of 6He on 12C NUCLEAR REACTIONS 12C(6He, 6He), E=38.3 MeV/nucleon; measured σ(θ); deduced optical model parameters, coupling effects. 12C(α, α), E=104, 139, 172.5 MeV; 12C(6Li, 6Li), E=99-318 MeV; analyzed σ(θ); deduced polarization potential. Folding model analysis with density-dependent effective interactions.
doi: 10.1103/PhysRevC.66.034608
2002VO02 Acta Phys.Pol. B33, 93 (2002) W.von Oertzen, H.G.Bohlen, V.Subotin, D.T.Khoa Nuclear Rainbows, Nucleus-Nucleus Potentials and the EOS of Nuclear Matter
2002VO09 Yad.Fiz. 65, 710 (2002); Phys.Atomic Nuclei 65, 678 (2002) W.von Oertzen, A.Blazevic, H.G.Bohlen, D.T.Khoa, F.Nuoffer, P.Roussel-Chomaz, W.Mittig, J.M.Casandjian Nuclear-Rainbow Scattering and Nucleus-Nucleus Potentials at Short Distances NUCLEAR REACTIONS 16O(16O, X), E=7-70 MeV/nucleon; analyzed σ(θ); deduced potential features. Double-folding model.
doi: 10.1134/1.1471273
2001KH02 Phys.Rev. C63, 034007 (2001) α-Nucleus Optical Potential in the Double-Folding Model NUCLEAR REACTIONS 12C, 16O, 58Ni, 90Zr(α, α), E=54-173 MeV; calculated optical potential parameters, σ(θ). Double-folding model, exchange effects, comparison with data.
doi: 10.1103/PhysRevC.63.034007
2000IN07 Nucl.Phys. A676, 3 (2000) A.Ingemarsson, J.Nyberg, P.U.Renberg, O.Sundberg, R.F.Carlson, A.J.Cox, A.Auce, R.Johansson, G.Tibell, D.T.Khoa, R.E.Warner New Results for Reaction Cross Sections of Intermediate Energy α-Particles on Targets from 9Be to 208Pb NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(α, X), E=69.6-192.4 MeV; measured reaction σ(θ), non-elastic σ(θ); deduced reduced interaction radius. Comparison with Optical model and Glauber model calculations. 58Ni(α, p), (α, 3He), (α, d), (α, t), E=80-160 MeV; calculated breakup σ(θ) from fragment spectra.
doi: 10.1016/S0375-9474(00)00200-1
2000KH06 Nucl.Phys. A668, 3 (2000) Generalized Folding Model for Elastic and Inelastic Nucleus-Nucleus Scattering using Realistic Density Dependent Nucleon-Nucleon Interaction NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=112, 121.6, 240, 300 MeV; 58,60Ni(α, α), (α, α'), E=172.5 MeV; calculated σ(θ), σ(E, θ). Generalized double-folding model. Comparison with data, other models.
doi: 10.1016/S0375-9474(99)00680-6
2000KH13 Nucl.Phys. A672, 387 (2000) D.T.Khoa, W.von Oertzen, H.G.Bohlen, F.Nuoffer Study of Diffractive and Refractive Structure in the Elastic 16O + 16O Scattering at Incident Energies Ranging from 124 to 1120 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=124-1120 MeV; analyzed elastic σ(θ); deduced refractive features. Optical model.
doi: 10.1016/S0375-9474(99)00856-8
2000OG06 Phys.Rev. C62, 044601 (2000) A.A.Ogloblin, Yu.A.Glukhov, W.H.Trzaska, A.S.Demyanova, S.A.Goncharov, R.Julin, S.V.Klebnikov, M.Mutterer, M.V.Rozhkov, V.P.Rudakov, G.P.Tiorin, D.T.Khoa, G.R.Satchler New Measurement of the Refractive, Elastic 16O + 12C Scattering at 132, 170, 200, 230, and 260 MeV Incident Energies NUCLEAR REACTIONS 12C(16O, 16O), E=132, 170, 200, 230, 260 MeV; measured σ(θ); deduced rainbow scattering features, optical model parameters.
doi: 10.1103/PhysRevC.62.044601
1998OG02 Phys.Rev. C57, 1797 (1998) A.A.Ogloblin, D.T.Khoa, Y.Kondo, Yu.A.Glukhov, A.S.Demyanova, M.V.Rozhkov, G.R.Satchler, S.A.Goncharov Pronounced Airy Structure in Elastic 16O + 12C Scattering at E(lab) = 132 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=132 MeV; measured σ(θ); deduced Airy minimum, refractive scattering features. Optical model analysis.
doi: 10.1103/PhysRevC.57.1797
1997KH04 Phys.Rev. C56, 954 (1997) D.T.Khoa, G.R.Satchler, W.von Oertzen Nuclear Incompressibility and Density Dependent NN Interactions in the Folding Model for Nucleus-Nucleus Potentials NUCLEAR REACTIONS 58Ni, 12C(α, α), E=104-172.5 MeV; 40Ca(α, α), E=80-141.7 MeV; 90Zr(α, α), E=79.5-141.7 MeV; 208Pb(α, α), E=104-139 MeV; 16O(16O, 16O), E=250, 350, 480 MeV; 12C(12C, 12C), E=126.7, 300, 1016, 1503 MeV; analyzed σ(θ); deduced optical model parameters, density dependence, incompressibility. M3Y effective interaction.
doi: 10.1103/PhysRevC.56.954
1997SA03 Phys.Rev. C55, 285 (1997) Missing Monopole Strength in 58Ni and Uncertainties in the Analysis of α-Particle Scattering NUCLEAR REACTIONS 58Ni(α, α'), E=140-340 MeV; calculated σ(θ) vs E. 58Ni deduced multipole transition strengths, dependence on model parameters. Folding model.
doi: 10.1103/PhysRevC.55.285
1996BA14 Phys.Lett. 365B, 23 (1996) G.Bartnitzky, A.Blazevic, H.G.Bohlen, J.M.Casandjian, M.Chartier, H.Clement, B.Gebauer, A.Gillibert, Th.Kirchner, D.T.Khoa, A.Lepine-Szily, W.Mittig, W.von Oertzen, A.N.Ostrowski, P.Roussel-Chomaz, J.Siegler, M.Wilpert, Th.Wilpert Model-Unrestricted Nucleus-Nucleus Scattering Potentials from Measurement and Analysis of 16O + 16O Scattering NUCLEAR REACTIONS 16O(16O, 16O), E=250-704 MeV; measured σ(θ); deduced model parameters, potential characteristics. Model-unrestricted analysis.
doi: 10.1016/0370-2693(95)01292-3
1996KH03 Nucl.Phys. A602, 98 (1996) D.T.Khoa, W.von Oertzen, A.A.Ogloblin Study of the Equation of State for Asymmetric Nuclear Matter and Interaction Potential between Neutron-Rich Nuclei using the Density-Dependent M3Y Interaction NUCLEAR REACTIONS 14C(11Li, 11Li), E=30, 60 MeV/nucleon; 12C(11Li, 11Li), E=57.9 MeV/nucleon; 14C(8He, 8He), E=30 MeV/nucleon; calculated differential σ; deduced neutron halo role. Nonrelativistic Hartree-Fock scheme, realistic M3Y effective NN-interaction.
doi: 10.1016/0375-9474(96)00091-7
1995KH03 Phys.Rev. C51, 2069 (1995) D.T.Khoa, G.R.Satchler, W.von Oertzen Folding Analysis of the Elastic 6Li + 12C Scattering: Knock-on exchange effects, energy dependence, and dynamical polarization potential NUCLEAR REACTIONS 12C(6Li, 6Li), E=99-318 MeV; analyzed σ(θ). Folded potential, density-dependent interactions.
doi: 10.1103/PhysRevC.51.2069
1995KH04 Nucl.Phys. A583, 353c (1995) D.T.Khoa, A.Faessler, N.Ohtsuka, D.H.E.Gross Thermalization Effects in Heavy-Ion Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=100, 400 MeV/nucleon; calculated average matter density, temperature, one-body entropy time evolution; deduced thermalization process related features. Quantum molecular dynamics approach.
doi: 10.1016/0375-9474(94)00686-H
1995KH05 Phys.Rev.Lett. 74, 34 (1995) D.T.Khoa, W.von Oertzen, H.G.Bohlen, G.Bartnitzky, H.Clement, Y.Sugiyama, B.Gebauer, A.N.Ostrowski, Th.Wilpert, M.Wilpert, C.Langner Equation of State of Cold Nuclear Matter from Refractive 16O + 16O Elastic Scattering NUCLEAR REACTIONS 16O(16O, 16O), E=145-480 MeV; measured σ(θ); deduced cold nuclear matter equation of state features. Folding analysis, effective density dependent interaction, refractive scattering.
doi: 10.1103/PhysRevLett.74.34
1995KH07 Phys.Lett. 342B, 6 (1995) Refractive Alpha-Nucleus Scattering: A probe for the incompressibility of cold nuclear matter NUCLEAR REACTIONS 40Ca, 12C, 90Zr(α, α), E=59.1-118 MeV; analyzed σ(θ) data; deduced nuclear incompressibility. Effective density dependent NN-interaction, folding analysis.
doi: 10.1016/0370-2693(94)01393-Q
1995KH11 Phys.Lett. 358B, 14 (1995) D.T.Khoa, G.R.Satchler, W.von Oertzen Realistic Scenario for the Quasielastic Scattering of 11Li, 11C + 12C at E/A ≈ 60 MeV NUCLEAR REACTIONS 12C(11C, 11C), (11C, 11C'), (11Li, 11Li), (11Li, 11Li'), E=56.3-87 MeV/nucleon; analyzed total, elastic, inelastic σ(θ) data; deduced model parameters. Semi-Microscopic optical model.
doi: 10.1016/0370-2693(95)00999-2
1994KH02 Phys.Rev. C49, 1652 (1994) D.T.Khoa, W.von Oertzen, H.G.Bohlen Double-Folding Model for Heavy-Ion Optical Potential: Revised and applied to study 12C and 16O elastic scattering NUCLEAR REACTIONS 12C(12C, 12C), E=112-1016 MeV; 16O(16O, 16O), E=145-480 MeV; 12C(16O, 16O), E=608, 1503 MeV; 28Si(16O, 16O), E=1503 MeV; analyzed σ(θ); deduced model parameters. Generalized double-folding model, density dependent interaction based optical potentials.
doi: 10.1103/PhysRevC.49.1652
1994PU03 Nucl.Phys. A575, 733 (1994) R.K.Puri, N.Ohtsuka, E.Lehmann, A.Faessler, M.A.Matin, D.T.Khoa, G.Batko, S.W.Huang Temperature-Dependent Mean Field and Its Effect on Heavy-Ion Reactions NUCLEAR REACTIONS 40Ca(40Ca, X), 93Nb(93Nb, X), E=400 MeV/nucleon; calculated maximum, average densities, transverse flow time evolution. Temperature dependent mean field nucleon potentials.
doi: 10.1016/0375-9474(94)90164-3
1993BO28 Z.Phys. A346, 189 (1993) H.G.Bohlen, E.Stiliaris, B.Gebauer, W.von Oertzen, M.Wilpert, Th.Wilpert, A.Ostrowski, D.T.Khoa, A.S.Demyanova, A.A.Ogloblin Refractive Scattering and Reactions, Comparison of Two Systems: 16O + 16O and 20Ne + 12C NUCLEAR REACTIONS 12C(20Ne, 20Ne), E=390 MeV; 16O(16O, 17O), (16O, 16O), E=350 MeV; measured σ(θ); deduced model parameters. DWBA analysis.
doi: 10.1007/BF01306079
1993CE01 Phys.Rev. C47, 1091 (1993) M.Centelles, X.Vinas, M.Barranco, N.Ohtsuka, A.Faessler, D.T.Khoa, H.Muther Relativistic Extended Thomas-Fermi Calculations of Finite Nuclei with Realistic Nucleon-Nucleon Interactions NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 56Ni, 90Zr, 114,118Sn, 140Ce, 208Pb; calculated binding energy, charge radius. 52Fe, 118Sn, 152Dy, 186Os, 207Bi, 240Pu; calculated fission barrier, saddle point quadrupole moment, critical angular momentum, equidensity lines. Relativistic extended Thomas-Fermi calculations, realistic interactions. NUCLEAR REACTIONS 12C(12C, 12C), E=2.4 GeV; 28Si, 12C(16O, 16O), E=1.503 GeV; calculated σ(θ). Relativistic extended Thomas-Fermi calculations, realistic interactions.
doi: 10.1103/PhysRevC.47.1091
1993KH03 Phys.Lett. 304B, 8 (1993) A Nuclear Matter Study using the Density Dependent M3Y Interaction NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; calculated σ(θ). Standard Hartree-Fock scheme, density-dependent M3Y interaction.
doi: 10.1016/0370-2693(93)91391-Y
1992KH02 Nucl.Phys. A542, 671 (1992) D.T.Khoa, N.Ohtsuka, A.Faessler, M.A.Matin, S.W.Huang, E.Lehmann, Y.Lofty Microscopic Study of Thermal Properties of the Nuclear Matter Formed in Heavy-Ion Collisions NUCLEAR REACTIONS 20Ne(20Ne, X), 40Ca(40Ca, X), 93Nb(93Nb, X), E=100-400 MeV/nucleon; calculated central region nucleon density, temperature, local entropy per nucleon vs evolution time. Generalized hot Thomas-Fermi formalism.
doi: 10.1016/0375-9474(92)90263-J
1992KH03 Nucl.Phys. A548, 102 (1992) D.T.Khoa, N.Ohtsuka, M.A.Matin, A.Faessler, S.W.Huang, E.Lehmann, R.K.Puri In-Medium Effects in the Description of Heavy-Ion Collisions with Realistic NN Interactions NUCLEAR REACTIONS 40Ca(40Ca, X), 93Nb(93Nb, X), E=400 MeV/nucleon; calculated temperature, nuclear matter density time evolution. Quantum molecular dynamical approach, phenomenological Skyrme forces, Brueckner G-matrix potential.
doi: 10.1016/0375-9474(92)90079-Y
1991CE09 J.Phys.(London) G17, L193 (1991) M.Centelles, X.Vinas, M.Barranco, N.Ohtsuka, A.Faessler, D.T.Khoa, H.Muther Relativistic Extended Thomas-Fermi Calculations of Finite Nuclei NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 56Ni, 90Zr, 114,118Sn, 140Ce, 208Pb; calculated binding energy, charge radii. 240Pu; calculated fission barrier angular momentum dependence vs quadrupole moment. Relativistic extended Thomas-Fermi model. NUCLEAR REACTIONS 12C(12C, 12C), E=1.016 GeV; calculated σ(θ). Microscopic optical potential. Relativistic extended Thomas-Fermi model.
doi: 10.1088/0954-3899/17/11/005
1991KH05 Nucl.Phys. A529, 363 (1991) D.T.Khoa, N.Ohtsuka, S.W.Huang, M.Ismail, A.Faessler, M.El-Shabshiry, J.Aichelin Photon Production in Heavy-Ion Collisions and Nuclear Equation of State NUCLEAR REACTIONS 12C(12C, X), 40Ca(40Ca, X), 93Nb(93Nb, X), E=84, 200 MeV/nucleon; calculated γ production σ. Quantum molecular dynamics model.
doi: 10.1016/0375-9474(91)90799-C
1991KH08 Phys.Lett. 260B, 278 (1991) D.T.Khoa, W.von Oertzen, A.Faessler, M.Ermer, H.Clement Pauli Exchange Effects in the Elastic Scattering of 16O + 16O NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; calculated σ(θ); deduced model parameters. Generalized double folding model.
doi: 10.1016/0370-2693(91)91612-Y
1991LI33 Nucl.Phys. A534, 697 (1991) G.Li, D.T.Khoa, T.Maruyama, S.W.Huang, N.Ohtsuka, A.Faessler, J.Aichelin Subthreshold Pion Production in Nucleus-Nucleus Collisions within the Quantum Molecular Dynamics Approach NUCLEAR REACTIONS 12C(12C, X), Ca(Ca, X), 93Nb(93Nb, X), E=200 MeV/nucleon; 20Ne(20Ne, X), E=183 MeV/nucleon; 64Cu(20Ne, X), E=250 MeV/nucleon; calculated pion production σ(θ, E(π)). Quantum molecular dynamics model.
doi: 10.1016/0375-9474(91)90467-K
1988KH08 Nucl.Phys. A484, 376 (1988) Exchange Effects in Nuclear Rainbow Scattering NUCLEAR REACTIONS 12C(α, α), E=139 MeV; 40Ca(α, α), E=104 MeV; 58Ni(α, α), E=139, 172.5 MeV; 90Zr(α, α), E=40-118 MeV; 40Ca, 12C(6Li, 6Li), E=156 MeV; 12C, 16O(9Be, 9Be), E ≈ 158 MeV; analyzed σ(θ); deduced potential parameters, exchange effects role. Microscopic model.
doi: 10.1016/0375-9474(88)90077-2
Back to query form Note: The following list of authors and aliases matches the search parameter D.Khoa: , D.T.KHOA |