NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Liang Found 92 matches. 2024NA07 Nuovo Cim. C 47, 52 (2024) T.Naito, G.Colo, T.Hatsuda, H.Liang, X.Roca-Maza, H.Sagawa Possible inconsistency between phenomenological and theoretical determinations of charge symmetry breaking in nuclear energy density functionals NUCLEAR STRUCTURE 10Be, 10C; calculated mass difference with the Green's function Monte Carlo (GFMC) with the Argonne v18 (AV18) and Urbana X (UX) interactions.
doi: 10.1393/ncc/i2024-24052-9
2024XI05 Phys.Rev. C 109, 034309 (2024) Extraction of higher-order radial moments of nuclear charge density from muonic atom spectroscopy
doi: 10.1103/PhysRevC.109.034309
2024YI03 Chin.Phys.C 48, 024102 (2024) Nuclear mass predictions based on a deep neural network and finite-range droplet model (2012) NUCLEAR STRUCTURE N=65-105; analyzed available data; deduced atomic masses using a neural network with two hidden layers for nuclear mass prediction, based on the finite-range droplet model (FRDM12).
doi: 10.1088/1674-1137/ad021c
2023HO11 Phys.Rev. C 108, 054312 (2023) D.S.Hou, A.Takamine, M.Rosenbusch, W.D.Xian, S.Iimura, S.D.Chen, M.Wada, H.Ishiyama, P.Schury, Z.M.Niu, H.Z.Liang, S.X.Yan, P.Doornenbal, Y.Hirayama, Y.Ito, S.Kimura, T.M.Kojima, W.Korten, J.Lee, J.J.Liu, Z.Liu, S.Michimasa, H.Miyatake, J.Y.Moon, S.Naimi, S.Nishimura, T.Niwase, T.Sonoda, D.Suzuki, Y.X.Watanabe, K.Wimmer, H.Wollnik First direct mass measurement for neutron-rich 112Mo with the new ZD-MRTOF mass spectrograph system
doi: 10.1103/PhysRevC.108.054312
2023NA16 Phys.Rev. C 107, 064302 (2023) T.Naito, G.Colo, H.Liang, X.Roca-Maza, H.Sagawa Effects of Coulomb and isospin symmetry breaking interactions on neutron-skin thickness NUCLEAR STRUCTURE 16O, 40,48Ca, 48Ni, 208Pb; calculated neutron-skin-thickness. 40,48Ca; calculated charge radii difference between 40Ca and 48Ca. 48Ca, 48Ni; calculated mass difference of mirror nuclei.Investigated the influence of the corrections to the Hartree-Fock-Slater approximation by the Coulomb interaction and charge-symmetry breaking term originating from the strong interaction. Comparison to experimental values.
doi: 10.1103/PhysRevC.107.064302
2023NI11 Nucl.Instrum.Methods Phys.Res. A1057, 168703 (2023) M.Niu, Z.Long, R.Fan, W.Jiang, J.Liu, Q.Xiu, R.Xu, H.Wang, Zh.Zhou, K.Sun, Zh.Zhang, H.Zhang, H.Yi, Y.Chen, D.Wang, X.Xia, H.Liang Research on the performance of a diamond detector for the cross-section measurements at CSNS Back-n NUCLEAR REACTIONS 12C, 6Li(n, α), 12C(n, n'), E=0.00001-100 MeV; measured reaction products, En, In, TOF; deduced the bi-parametric contour plot facilitated the identification of event bands in a bi-parameter experiment (neutron time of flight and deposited energy). Comparison with MATLAB simulations. The Back-n white neutron facility located within the China Spallation Neutron Source (CSNS).
doi: 10.1016/j.nima.2023.168703
2023XI10 Phys.Lett. B 846, 138232 (2023) H.H.Xie, T.Naito, J.Li, H.Liang Revisiting the extraction of charge radii of 40Ca and 208Pb with muonic atom spectroscopy NUCLEAR STRUCTURE 40Ca, 208Pb; calculated charge densities, together with the corresponding muonic transition energies using the covariant density functional theory as a benchmark; deduced nuclear charge radii from muonic atom spectroscopy.
doi: 10.1016/j.physletb.2023.138232
2023YA26 Phys.Rev. C 108, 034315 (2023) Z.-X.Yang, X.-H.Fan, T.Naito, Z.-M.Niu, Z.-Pa.Li, H.Liang Calibration of nuclear charge density distribution by back-propagation neural networks
doi: 10.1103/PhysRevC.108.034315
2022GU02 Phys.Rev. C 105, 024317 (2022) Cooper quartet correlations in infinite symmetric nuclear matter
doi: 10.1103/PhysRevC.105.024317
2022MI14 Phys.Rev. C 106, 024306 (2022) Calculation of β-decay half-lives within a Skyrme-Hartree-Fock-Bogoliubov energy density functional with the proton-neutron quasiparticle random-phase approximation and isoscalar pairing strengths optimized by a Bayesian method RADIOACTIVITY 87,88,89,90,91,92,93,94,95,96,97,98,99,100Kr, 88,89,90,91,92,93,94,95,96,97,98,99,100,101Rb, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137Mo, 102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138Tc(β-); 113,115,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143Cd, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144In(β-); 155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192Sm, 156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193Eu(β-); Z=8-110(β-); A=20-368(β-); calculated β--decay T1/2, partial T1/2 for Gamow-Teller decays, Q values, isoscalar spin-triplet strength for neutron-rich nuclei using proton-neutron quasiparticle random-phase approximation (pnQRPA), proton-neutron quasiparticle Tamm-Dancoff approximation (pnQTDA), with Skryme energy density functional, and Bayesian neural network (BNN), the last for isoscalar spin-triplet strength. Calculated T1/2, Q values, isoscalar spin-triplet strength for 5580 neutron-rich nuclei spanning Z=8-110, N=12-258 and A=20-368 are listed in Supplemental Material of the paper. Comparison with available experimental T1/2 in NUBASE2016.
doi: 10.1103/PhysRevC.106.024306
2022NA10 Phys.Rev. C 105, L021304 (2022) T.Naito, G.Colo, H.Liang, X.Roca-Maza, H.Sagawa Toward ab initio charge symmetry breaking in nuclear energy density functionals NUCLEAR STRUCTURE 48Ca, 208Pb; calculated neutron skin thickness, mass difference for mirror nuclei 48Ca-48Ni, dependence of neutron-skin thickness on the charge symmetry breaking strength s0. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.L021304
2022NA38 Phys.Rev. C 106, L061306 (2022) T.Naito, X.Roca-Maza, G.Colo, H.Liang, H.Sagawa Isospin symmetry breaking in the charge radius difference of mirror nuclei NUCLEAR STRUCTURE 48Ca, 48Ni; calculated charge radius difference of mirror nuclei. Discussed the connection of obtained values with the nuclear equation of state and effect of isospin symmetry breaking on such relation. Hartree-Fock calculations with SAMi-J family of energy density functionals.
doi: 10.1103/PhysRevC.106.L061306
2022NI10 Phys.Rev. C 106, L021303 (2022) Nuclear mass predictions with machine learning reaching the accuracy required by r-process studies ATOMIC MASSES 159,160,161,162,163,164,165,166Nd, 160,161,162,163,164,165,166,167Pm, 161,162,163,164,165,166,167,168Sm, 162,163,164,165,166,167,168,169Eu, 163,164,165,166,167,168,169,170Gd, 164,165,166,167,168,169,170,171Tb; calculated S(2n). Machine learning algorithm. Bayesian neural networks by learning the mass surface of even-even nuclei and the correlation energies to their neighboring nuclei. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.L021303
2021AC04 Phys.Rev. C 103, 044304 (2021) G.Accorto, T.Naito, H.Liang, T.Niksic, D.Vretenar Nuclear energy density functionals from empirical ground-state densities NUCLEAR STRUCTURE 16O, 40Ca, 56Ni, 100Sn; calculated sum of neutron vector and scalar potentials for 16O (N=Z=8 system) as a function of the radial coordinate, vector densities of four symmetric systems: 16O (N=Z=8), 40Ca (N=Z=20), 56Ni (N=Z=28) and 100Sn (N=Z=50) using density functional perturbation theory and the inverse Kohn-Sham method, with the improved relativistic energy density functional (EDF) DD-PC1 determined by empirical exact ground-state densities of finite systems.
doi: 10.1103/PhysRevC.103.044304
2021NA16 Phys.Rev. C 104, 024316 (2021) T.Naito, G.Colo, H.Liang, X.Roca-Maza Second and fourth moments of the charge density and neutron-skin thickness of atomic nuclei NUCLEAR STRUCTURE 36,38,40,42,44,46,48,50,52,54Ca, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Sn; calculated second r2 and fourth r4 moments of the proton, neutron, and charge density distributions as function of mass number, correlation of proton second and fourth moments for 44,46Ca, 110,112Sn. Skyrme Hartree-Fock-Bogoliubov calculation with the assumption of axial symmetry using the code HFBTHO and SLy4 energy density functional. Comparison with experimental data. Relevance to extraction of neutron radius using the experimentally measured second and fourth moments of the charge distribution.
doi: 10.1103/PhysRevC.104.024316
2021WA30 Chin.Phys.C 45, 064103 (2021) Z.Wang, T.Naito, H.Liang, W.H.Long Exploring effects of tensor force and its strength via neutron drops
doi: 10.1088/1674-1137/abf036
2021WA32 Phys.Rev. C 103, 064326 (2021) Tensor-force effects on shell-structure evolution in N=82 isotones and Z=50 isotopes in the relativistic Hartree-Fock theory NUCLEAR STRUCTURE 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb, 154Hf; 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated energy differences of ν1i13/2 and ν1h9/2 orbitals with respect to 140Ce for N=82 nuclei, and for π1h11/2 and π1g7/2 orbitals with respect to 108Sn for Z=50 nuclei using relativistic Hartree-Fock (RHF) theory with PKA1, PKO1, PKO2 and PKO3 effective interactions, with and without tensor-force contributions, the former with covariant density functional theory (CDFT), and compared with experimental data. 16,24O, 36S, 40,48,52,54Ca, 56,68,72Ni, 86Kr, 90Zr, 94Ru, 100,116,124,132Sn, 136Xe, 140Ce, 146Gd, 182,194,200,204,208,214Pb, 210Po, 214Ra, 218U; calculated binding energies and charge radii using the 'New' interaction and compared with results using PKO1 interaction, and with experimental data.
doi: 10.1103/PhysRevC.103.064326
2021XU07 Chin.Phys.C 45, 114103 (2021) Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai Description of elastic scattering induced by the unstable nuclei 9, 10, 11, 13, 14C NUCLEAR REACTIONS 208Pb(9C, 9C), (11C, 11C), E=222-227 MeV; 27Al, 58Ni, 208Pb(10C, 10C), E=29.1-256 MeV; 28Si, 208Pb(9C, 9C), E<500 MeV; 28Si, 208Pb(11C, 11C), E<500 MeV; 28Si(13C, 13C), E=25-60 MeV; 40Ca, 56Fe, 60Ni, 66Zn, 88Sr(14C, 14C), E=51 MeV; 92,100Mo(14C, 14C), E=71 MeV; 28Si(14C, 14C), E<500 MeV; analyzed available data; deduced σ, σ(θ), global optical model potentials.
doi: 10.1088/1674-1137/ac1fe1
2020GU02 Phys.Rev. C 101, 024304 (2020) Nonrelativistic expansion of the Dirac equation with spherical scalar and vector potentials by a reconstituted Foldy-Wouthuysen transformation NUCLEAR STRUCTURE 208Pb; calculated neutron density, neutron scalar density, and comparisons with exact density and various models using the reconstituted similarity renormalization group (SRG) method, as reconstituted Foldy-Wouthuysen (FW) transformation.
doi: 10.1103/PhysRevC.101.024304
2020NA19 Phys.Rev. C 101, 064311 (2020) T.Naito, X.Roca-Maza, G.Colo, H.Liang Effects of finite nucleon size, vacuum polarization, and electromagnetic spin-orbit interaction on nuclear binding energies and radii in spherical nuclei NUCLEAR STRUCTURE 4He, 14,16,24O, 40,48Ca, 48Ni, 100,124,132,162Sn, 208Pb, 310126; calculated total energies, Coulomb energies, and charge radii, ratios of the Coulomb direct and exchange energies, mirror nuclei mass difference between 48Ca and 48Ni using self-consistent Skyrme Hartree-Fock method with generalized gradient approximation (GGA), and including electromagnetic effects of nucleon finite size, vacuum polarization, and electromagnetic spin-orbit interaction. Comparison with other theoretical predictions.
doi: 10.1103/PhysRevC.101.064311
2020WA17 Phys.Rev. C 101, 064306 (2020) Z.Wang, T.Naito, H.Liang, W.H.Long Self-consistent random-phase approximation based on the relativistic Hartree-Fock theory: Role of ρ-tensor coupling NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated energies and transition probabilities of isobaric analog states (IAS) and Gamow-Teller resonances, neutron and proton single-particle spectra. Random-phase approximation (RPA) based on the relativistic Hartree-Fock theory, extended with self-consistent ρ-meson tensor coupling. Comparison with experimental data for excitation energies and transition strength distributions.
doi: 10.1103/PhysRevC.101.064306
2020XU03 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 12C, 27Al, 28Si, 58Ni, 208Pb(8B, 8B), 9Be, 12C, 16O, 28Si, 58Ni, 120Sn, 208Pb(10B, 10B), 12C, 28Si, 58Ni, 208Pb, 209Bi(11B, 11B), E<50 MeV; analyzed available data. 8,10,11B; calculated σ; deduced global phenomenological optical model potentials.
doi: 10.1088/1674-1137/44/3/034101
2020XU04 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 27Al, 58Ni, 208Pb, 12C, 28Si(8B, 8B), E<100 MeV; 27Al, 28Si, 58Ni, 120Sn, 16O, 9Be, 208Pb(10B, 10B), E<100 MeV; 28Si, 58Ni, 209Bi, 12C, 209Bi(11B, 11B), E<100 MeV; analyzed available data. 9Be; deduced optical model potential parameters, σ, σ(θ).
doi: 10.1088/1674-1137/44/3/034101
2020XU10 Chin.Phys.C 44, 124103 (2020) Y.-L.Xu, Y.-L.Han, X.-W.Su, X.-J.Sun, H.-Y.Liang, H.-R.Guo, C.-H.Cai Global optical model potential describing 12C-nucleus elastic scattering NUCLEAR REACTIONS 24Mg, 28Si, 32S, 39K, 40,42,48Ca, 50Cr, 56Fe, Fe, 58,64Ni, Ni, 90,91,92,94,96Zr, 92Mo, 116,117,118,119,120,122,124Sn, 194,198Pt, 208Pb, 209Bi(12C, 12C), E<200 MeV; analyzed available data; deduced a new global optical model potential parameters.
doi: 10.1088/1674-1137/abb4d0
2019GU12 Phys.Rev. C 99, 054324 (2019) Nonrelativistic expansion of Dirac equation with spherical scalar and vector potentials by similarity renormalization group
doi: 10.1103/PhysRevC.99.054324
2019MA56 Phys.Rev. C 100, 024330 (2019) C.Ma, Z.Li, Z.M.Niu, H.Z.Liang Influence of nuclear mass uncertainties on radiative neutron-capture rates NUCLEAR REACTIONS 124Mo, 126Ru, 194Er, 196Yb(n, γ), T9=0.0001-10; Sb, Zr(n, γ), T9=1; calculated radiative n-capture rates with TALYS using ten mass models to determine the uncertainties. Z=5-100, N=10-230; analyzed uncertainties of radiative neutron-capture rates from nuclear mass uncertainties at different temperatures.
doi: 10.1103/PhysRevC.100.024330
2019NA03 Phys.Rev. C 99, 024309 (2019) T.Naito, X.Roca-Maza, G.Colo, H.Liang Coulomb exchange functional with generalized gradient approximation for self-consistent Skyrme Hartree-Fock calculations NUCLEAR STRUCTURE 4He, 14,16,24O, 40,48Ca, 100,124,132,162Sn, 208Pb, 310126; calculated Coulomb exchange energies with the LDA and PBE-GGA Coulomb exchange functionals and compared with the exact-Fock energies, radial Coulomb exchange potential, proton and neutron density distributions, and proton single-particle energies in 208Pb using self-consistent Skyrme Hartree-Fock calculations with Coulomb exchange functional and generalized gradient approximation (GGA). Comparison with values calculated by local density approximation.
doi: 10.1103/PhysRevC.99.024309
2019NI07 Phys.Rev. C 99, 064307 (2019) Z.M.Niu, H.Z.Liang, B.H.Sun, W.H.Long, Y.F.Niu Predictions of nuclear β-decay half-lives with machine learning and their impact on r-process nucleosynthesis RADIOACTIVITY 67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89Ni, 122Zr, 123Nb, 124Mo, 125Tc, 126Ru, 127Rh, 128Pd, 129Ag, 130Cd, 131In, 132Sn, 133Sb, 134Te, 187Pm, 188Sm, 189Eu, 190Gd, 191Tb, 192Dy, 193Ho, 194Er, 195Tm, 196Yb, 197Lu, 198Hf, 199Ta, 200W, 201Re, 202Os, 203Ir, 204Pt, 205Au, 206Hg, 207Tl(β-); calculated T1/2, and uncertainties using machine-learning approach based on Bayesian neural network (BNN). Comparison with experimental values, and with other theoretical predictions. A=90-210; discussed impact on r-process nucleosynthesis calculations.
doi: 10.1103/PhysRevC.99.064307
2019SH24 Chin.Phys.C 43, 074104 (2019) Mass predictions of the relativistic continuum Hartree-Bogoliubov model with radial basis function approach ATOMIC MASSES N=0-160; analyzed available data; calculated nuclear masses using radial basis function (RBF) approach.
doi: 10.1088/1674-1137/43/7/074104
2019SH41 Prog.Part.Nucl.Phys. 109, 103713 (2019) S.Shen, H.Liang, W.H.Long, J.Meng, P.Ring Towards an ab initio covariant density functional theory for nuclear structure
doi: 10.1016/j.ppnp.2019.103713
2019XU05 Phys.Rev. C 99, 034618 (2019) Y.Xu, Y.Han, H.Liang, Z.Wu, H.Guo, C.Cai Global optical model potential for the weakly bound projectile 9Be NUCLEAR REACTIONS Mg(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 27Al(9Be, 9Be), E=12.0, 14.0, 18.0, 20.0, 22.0, 25.0, 28.0, 32.0, 33.0, 35.0.40.0, 47.5 MeV; 28Si(9Be, 9Be), E=12.0, 13.0, 14.0, 17.0, 20.0, 23.0, 26.0, 30.0, 45.0, 50.0, 60.0 MeV; 40Ca(9Be, 9Be), E=14.0, 20.0, 26.0, 45.0.50.0, 60.0 MeV; 58Ni(9Be, 9Be), E=20.0, 26.0 MeV; 64Zn(9Be, 9Be), E=17.0, 19.0, 21.0, 23.0, 26.0, 28.0, 28.4, 28.97 MeV; 89Y(9Be, 9Be), E=18.6, 20.6, 22.7, 24.7, 26.7, 28.7, 33.2 MeV; Ag(9Be, 9Be), E=26.0 MeV; 144Sm(9Be, 9Be), E=30.0, 31.5, 33.0, 34.0, 35.0, 37.0, 39.0, 41.0, 44.0, 48.0 MeV; 208Pb(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 9.5, 40.0, 41.0, 42.0, 44.0, 46.0, 47.2, 48.0, 50.0, 60.0, 68.0, 75.0 MeV; 209Bi(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 39.5, 40.0, 41.0, 42.0, 44.0, 46.0, 48.0 MeV; analyzed elastic σ(θ, E) data for global phenomenological energy-dependent optical model potential parameters for 9Be. 9Be, 12,13C, 27Al, 64Zn, 89Y, 144Sm(9Be, X), E=10-300 MeV; 28Si, Cu(9Be, X), E=10-500 MeV; 89Y(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (9Be, X), (11B, X); calculated reaction σ(E) using optical model and compared with experimental data. 9Be(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 12C(9Be, 9Be), E=13.0, 14.0, 14.5, 17.3, 19.0, 20.0, 21.0, 26.0, 153.8 MeV; 13C(9Be, 9Be), E=19.46, 25.05 MeV; 16O(9Be, 9Be), E=20.0, 25.94 MeV; calculated elastic σ(θ, E) using optical model parameters and compared with experimental data.
doi: 10.1103/PhysRevC.99.034618
2018DI08 Phys.Rev. C 98, 014316 (2018) K.-M.Ding, M.Shi, J.-Y.Guo, Z.-M.Niu, H.Liang Resonant-continuum relativistic mean-field plus BCS in complex momentum representation NUCLEAR STRUCTURE 120,122,124,126,128,130,132,134,136,138,140Zr; calculated neutron single particle energies and widths, occupation probabilities of neutron single particle levels, and neutron single particle spectra and density distributions in 124Zr. 80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Zr; calculated S(2n), rms neutron radii. Resonant-continuum relativistic mean-field plus BCS in complex momentum representation with the BCS approximation for pairing correlations. Comparison with available experimental values.
doi: 10.1103/PhysRevC.98.014316
2018LI32 Phys.Rev. C 98, 014311 (2018) H.Z.Liang, H.Sagawa, M.Sasano, T.Suzuki, M.Honma Gamow-Teller transitions from high-spin isomers in N = Z nuclei RADIOACTIVITY 52Fe, 94Ag(β-); calculated Gamow-Teller transition strength distributions from 12+ isomeric state and g.s. in 52Fe and 21+ isomeric state and g.s. in 94Ag using sum-rule approach and shell model calculations; deduced stronger Gamow-Teller strengths from the high-spin states as compared to those from the low-spin ground states.
doi: 10.1103/PhysRevC.98.014311
2018NA10 Phys.Rev. C 97, 044319 (2018) Application of a Coulomb energy density functional for atomic nuclei: Case studies of local density approximation and generalized gradient approximation NUCLEAR STRUCTURE 4He, 12C, 16O, 40,48Ca, 58Ni, 116,124Sn, 206,208Pb; calculated direct, exchange, and correlation Coulomb energies, exchange energy densities weighted with charge-density distributions as a function of radius by the local density approximation (LDA), and by the generalized gradient approximation (GGA) using B88, PW91, PBE, and PBEsol energy density functionals; deduced deviation between LDA and generalized gradient approximation (GGA) exchange energies.
doi: 10.1103/PhysRevC.97.044319
2018SH20 Phys.Rev. C 97, 054312 (2018) S.Shen, H.Liang, J.Meng, P.Ring, S.Zhang Relativistic Brueckner-Hartree-Fock theory for neutron drops NUCLEAR STRUCTURE N=4-50; calculated ground-state energies, radii, neutron skin thickness, two-neutron energy difference, density distributions, single-particle energies, and neutron spin-orbit and pseudospin-orbit splittings of neutron drops for even numbers of neutrons from N=4 to N=50 using Relativistic Brueckner-Hartree-Fock (RBHF) theory with bare nucleon-nucleon interaction. Comparison with results from other nonrelativistic ab initio calculations, and from relativistic density functional theory.
doi: 10.1103/PhysRevC.97.054312
2018SH21 Phys.Rev. C 97, 064301 (2018) Combination of complex momentum representation and Green's function methods in relativistic mean-field theory NUCLEAR STRUCTURE 74Ca; calculated single particle resonance for g7/2 orbital, level density distribution, and density of continuum states for the 1g7/2 orbital, continuum level density (CLD) for all the resonance states, density distributions for the 1g7/2, 2d3/2, 3s1/2, 2d5/2 and 1g9/2 orbitals, single-particle levels, and wave function of the 2d3/2 resonant state. Combined complex momentum representation method with Green's function method in the relativistic mean-field framework (RMF-CMR-GF); discussed single-particle wave functions and densities for halo structure in 74Ca.
doi: 10.1103/PhysRevC.97.064301
2018WA26 Phys.Rev. C 98, 034313 (2018) Z.Wang, Q.Zhao, H.Liang, W.H.Long Quantitative analysis of tensor effects in the relativistic Hartree-Fock theory NUCLEAR STRUCTURE 40,48,52,54Ca, 208Pb, 16,22O, 14C, 34,42Si, 36,44S, 56,60,66,68,78Ni; calculated contributions to the total energy from the tensor forces in different couplings, proton and neutron gap energies with and without tensor force in each meson-nucleon coupling using relativistic Hartree-Fock theory with PKA1 effective interaction. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.034313
2018XI02 At.Data Nucl.Data Tables 121-122, 1 (2018) X.W.Xia, Y.Lim, P.W.Zhao, H.Z.Liang, X.Y.Qu, Y.Chen, H.Liu, L.F.Zhang, S.Q.Zhang, Y.Kim, J.Meng The limits of the nuclear landscape explored by the relativistic continuum Hartree-Bogoliubov theory NUCLEAR STRUCTURE Z=8-120; calculated ground-state properties using the spherical relativistic continuum Hartree-Bogoliubov (RCHB) theory with the relativistic density functional PC-PK1.
doi: 10.1016/j.adt.2017.09.001
2018XU01 Phys.Rev. C 97, 014615 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai Global phenomenological optical model potential for the 7Li projectile nucleus NUCLEAR REACTIONS 9Be(7Li, 7Li), E=15.75, 24.0, 30.0, 63.0, 130.0 MeV; 12C(7Li, 7Li), E=7.5, 9.0, 12.0, 15.0, 36.0, 131.8 MeV; 16O(7Li, 7Li), E=26.0, 36.0, 42.0, 50.0 MeV; 11B, 12,13C, 24Mg(7Li, 7Li), E=34.0 MeV; 24,26Mg(7Li, 7Li), E=88.7 MeV; 27Al(7Li, 7Li), E=6.0, 7.0, 8.0, 9.0, 10.0, 11.0, 12.0, 13.0, 14.0, 16.0, 18.0, 19.0, 24.0 MeV; 28Si(7Li, 7Li), E=8.0, 8.5, 9.0, 10.0, 11.0, 11.5, 13.0, 15.0, 16.0, 21.0, 26.0, 36.0, 177.8 MeV; 40,44,48Ca(7Li, 7Li), E=34.0; 40Ca(7Li, 7Li), E=88.7 MeV; 46,48Ti(7Li, 7Li), E=17.0 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe, 65Cu, 90Zr(7Li, 7Li), E=34.0 MeV; 58Ni(7Li, 7Li), E=14.22, 16.25.18.28, 19.0, 20.31.34.0, 42.0 MeV; 60,62Ni, 64,68Zn(7Li, 7Li), E=34.0 MeV; 80Se(7Li, 7Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 23.0, 26.0 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 116Sn(7Li, 7Li), E=18.0, 19.0, 20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0 MeV; 120Sn(7Li, 7Li), E=19.5, 20.0, 20.5, 22.0, 24.0, 25.0, 26.0, 28.0, 30.044.0 MeV; 138Ba(7Li, 7Li), E=21.0, 22.0, 23.0, 24.0, 28.0, 30.0, 32.0, 52.0 MeV; 140Ce, 142Nd(7Li, 7Li), E=52.0 MeV; 144Sm(7Li, 7Li), E=21.6, 22.1, 22.6.23.0, 25.0, 27.0, 29.0, 30.0, 32.0, 35.0, 40.8, 52.0 MeV; 208Pb(7Li, 7Li), E=27.0, 29.0, 33.0, 39.0, 42.0, 52.0 MeV; 232Th(7Li, 7Li), E=24.0, 26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed σ(θ, E) experimental data by global phenomenological optical model potential. 13C, 27Al, 64Zn, 116Sn, 138Ba, (7Li, X), E<300 MeV; 28Si, Cu, 208Pb(7Li, X), E<400 MeV; calculated reaction σ(E) using optical model, and compared with experimental data.
doi: 10.1103/PhysRevC.97.014615
2018XU10 Phys.Rev. C 98, 024619 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai 6Li global phenomenological optical model potential NUCLEAR REACTIONS 24Mg, 48Ca(6Li, 6Li), E=240.0 MeV; 25,26Mg, 39K, 91Zr(6Li, 6Li), E=34.0 MeV; 27Al(6Li, 6Li), E=7.0, 8.0, 10.0, 12.0, 18.0, 34.0 MeV; 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 16.0, 20.0, 21.0, 25.0, 27.0, 34.0, 46.0, 99.0, 135.0, 154.0, 210.0, 240.0, 318.0, 350.0 MeV; 40Ca(6Li, 6Li), E=50.6, 99.0, 156.0, 210.0, 240.0 MeV; 54Fe(6Li, 6Li), E=38.0, 44.0, 50.0 MeV; 59Co(6Li, 6Li), E=12.0, 18.0, 26.0, 30.0 MeV; 58Ni(6Li, 6Li), E=9.85, 11.21, 12.13, 13.04, 14.04, 34.0, 50.6, 73.7, 90.0, 99.0, 210.0, 240.0 MeV; 65Cu(6Li, 6Li), E=25.0 MeV; 64Zn(6Li, 6Li), E=10.77, 11.69, 12.0, 12.43, 13.0, 13.54, 13.8, 14.92, 15.0, 16.30, 16.5, 18.0, 18.14, 19.98, 22.0 MeV; 72,74,76Ge(6Li, 6Li), E=28.0 MeV; 80Se(6Li, 6Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 22.19, 23.0, 26.0 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=11.0, 12.0, 13.0, 15.0, 17.0, 19.0, 21.0, 25.0, 30.0, 34.0, 60.0, 70.0, 73.7, 99.0, 156.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 112Sn(6Li, 6Li), E=21.0, 22.0, 23.0, 25.0, 30.0, 35.0 MeV; 116Sn(6Li, 6Li), E=20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0, 40.0 MeV; 118Sn(6Li, 6Li), E=42.0 MeV; 120Sn(6Li, 6Li), E=30.0, 44.0, 90.0 MeV; 124Sn(6Li, 6Li), E=73.7 MeV; 138Ba(6Li, 6Li), E=21.0, 22.0, 23.0, 24.0, 26.0, 28.0 MeV; 144Sm(6Li, 6Li), E=21.0, 22.1, 22.6, 24.1, 26.0, 28.0, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25.0, 29.0, 31.0, 33.0, 35.0, 36.0, 37.0, 39.0, 42.0, 43.0, 46.0, 48.0, 50.6, 73.7, 88.0, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=24.0, 26.0, 28.0, 29.9, 30.0, 32.0, 32.8, 34.0, 36.0, 40.0, 44.0, 50.0 MeV; 232Th(6Li, 6Li), E=26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed differential σ(θ, E) data; deduced a new set of 6Li global phenomenological energy-dependent optical potential parameters based on the form of the Woods-Saxon potential within the optical model. 63,65Cu, 64Zn, 112,116Sn, 138Ba, 208Pb(6Li, X), E<400 MeV; calculated reaction σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.98.024619
2017FA02 Phys.Rev. C 95, 024311 (2017) Z.Fang, M.Shi, J.-Y.Guo, Z.-M.Niu, H.Liang, S.-S.Zhang Probing resonances in the Dirac equation with quadrupole-deformed potentials with the complex momentum representation method NUCLEAR STRUCTURE 37Mg; calculated levels, resonances, single-particle resonances, J, π, single-particle energies for deformation (Nilsson orbitals) for the bound and resonant states concerned, radial-momentum probability distributions for the bound and resonant deformed states by solving the Dirac equation in complex momentum representation, and a set of coupled differential equations by the coupled-channel method.
doi: 10.1103/PhysRevC.95.024311
2017GU06 Phys.Rev. C 95, 034614 (2017) H.Guo, H.Liang, Y.Xu, Y.Han, Q.Shen, C.Cai, T.Ye Microscopic optical potential for 6He NUCLEAR REACTIONS 12C(6He, 6He), E=8.79, 9.18, 9.9, 18, 230, 250 MeV; 27Al(6He, 6He), E=9.54, 11.0, 12.0, 13.4 MeV; 51V(6He, 6He), E=15.4, 23.0 MeV; 58Ni(6He, 6He), E=9.0, 10.0, 12.2, 16.5, 21.7 MeV; 64Zn(6He, 6He), E=10.0, 13.6 MeV; 65Cu(6He, 6He), E=19.56, 22.6, 30.05 MeV; 120Sn(6He, 6He), E=17.4, 18.05, 19.8, 20.05 MeV; 197Au(6He, 6He), E=10.1, 27.0 MeV; 209Bi(6He, 6He), E=14.71, 16.26, 17.8, 19.0, 19.14, 22.02, 22.5 MeV; 208Pb(6He, 6He), E=14.0, 16, 18, 22, 27, 56.6 MeV; 9Be(6He, 6He), E=16.2, 16.8, 21.3, 150 MeV; calculated differential σ(θ, E) relative to Rutherford cross section using microscopic optical potential (MOP) and global phenomenological 6He optical potential (GOP) based on experimental data. 28Si(6He, X), E<330 MeV; calculated total σ(E) using MOP and GOP. Comparison with experimental data. Isospin-dependent nucleon microscopic optical potential derived by using Green's function method through the nuclear matter approximation and the local density approximation based on the Skyrme nucleon-nucleon effective interaction.
doi: 10.1103/PhysRevC.95.034614
2017LI21 Nucl.Sci.Eng. 187, 107 (2017) H.Liang, Z.Wu, Z.Zhang, Y.Han, X.Jiao Calculations and Analysis of n+93Nb Reaction NUCLEAR REACTIONS 93Nb(n, X), E<200 MeV; calculated σ, σ(E), σ(θ), σ(θ, E) using theoretical models. Comparison with ENDF/B-VII, JENDL-4, TENDL-2015 libraries, experimental data.
doi: 10.1080/00295639.2017.1295699
2017NI07 Phys.Rev. C 95, 044301 (2017) Z.M.Niu, Y.F.Niu, H.Z.Liang, W.H.Long, J.Meng Self-consistent relativistic quasiparticle random-phase approximation and its applications to charge-exchange excitations NUCLEAR STRUCTURE 36,38,40,42,44,46,48,50,52,54,56,58,60Ca, 54,56,58,60,62,64,68,70,72,74,76,78,80,82,84,86,88Ni, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148Sn; calculated nuclear masses, S(2n), Q(β) values for Ca, Ni and Sn isotopes, neutron-skin thicknesses, IAS and GT excitation energies for Sn isotopes using the RHFB theory with PKO1 interaction and the RHB theory with DD-ME2 effective interaction. 118Sn; calculated running sum of the GT transition probabilities, and GT strength distribution using RHFB+QRPA approach with PKO1 interaction. 114Sn; calculated transition probabilities for the IAS by RHFB+QRPA, RHF+RPA, RHFB+RPA, RHFB+QRPA* with PKO1 interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.044301
2017SH20 Phys.Rev. C 96, 014316 (2017) S.Shen, H.Liang, J.Meng, P.Ring, S.Zhang Fully self-consistent relativistic Brueckner-Hartree-Fock theory for finite nuclei NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground state energies, charge and matter radii, single-particle spectra, binding energy per nucleon by relativistic ab initio approach. Solution of full relativistic Brueckner-Hartree-Fock (RBHF) equations with the relativistic form of the Bonn potential as a bare nucleon-nucleon interaction. Comparison with available experimental data.
doi: 10.1103/PhysRevC.96.014316
2017SU16 Phys.Rev. C 95, 054606 (2017) X.W.Su, Y.L.Han, H.Y.Liang, Z.D.Wu, H.R.Guo, C.H.Cai Global phenomenological optical model potential for 8Li projectile NUCLEAR REACTIONS 9Be(8Li, 8Li), E=14, 19.6, 27 MeV; 12C(8Li, 8Li), E=14, 23.9 MeV; 13C, 14N, 27Al, 197Au(8Li, 8Li), E=14 MeV; 51V(8Li, 8Li), E=18.5, 26 MeV; 58Ni(8Li, 8Li), E=14, 19.6, 20.2, 22 MeV; 208Pb(8Li, 8Li), E=24.4, 27.9, 28.9, 30.6, 33.1 MeV; calculated σ(θ, E) by optical potential model, and compared with experimental data; deduced global phenomenological optical model parameters (OMPs) for 8Li. 9Be(8Li, X), E=19.6 MeV; 12C(8Li, X), E=14 MeV; 51V(8Li, X), E=18.5, 26.0 MeV; 208Pb(8Li, X), E=24.4, 27.6, 28.89, 30.57, 33.13 MeV; calculated total σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.95.054606
2016LI35 Phys.Rev.Lett. 117, 062502 (2016) N.Li, M.Shi, J.-Y.Guo, Z.-M.Niu, H.Liang Probing Resonances of the Dirac Equation with Complex Momentum Representation NUCLEAR STRUCTURE 120Sn; calculated energies and widths of single neutron state resonances. Relativistic mean-field (RMF) theory.
doi: 10.1103/PhysRevLett.117.062502
2016NI16 Phys.Rev. C 94, 054315 (2016) Z.M.Niu, B.H.Sun, H.Z.Liang, Y.F.Niu, J.Y.Guo Improved radial basis function approach with odd-even corrections ATOMIC MASSES Z=8-100, N=8-160, A=16-260; calculated masses using relativistic mean-field (RMF) with radial basis function (RBF) approach, and RMF with RBF considering odd-even effects (RBFoe). Z=31, 32, N=31-53; calculated S(n) with RMF+RBF, and RMF+RBFoe approaches. Comparison with experimental data taken form AME-2012.
doi: 10.1103/PhysRevC.94.054315
2016SH34 Chin.Phys.Lett. 33, 102103 (2016) S.-H.Shen, J.-N.Hu, H.-Z.Liang, J.Meng, P.Ring, S.-Q.Zhang Relativistic Brueckner-Hartree-Fock Theory for Finite Nuclei NUCLEAR STRUCTURE 16O; calculated total energy, charge radius, single-particle spectra for protons and neutrons. Brueckner-Hartree-Fock equations solved for finite nuclei in a Dirac-Woods-Saxon basis.
doi: 10.1088/0256-307X/33/10/102103
2016SU13 Int.J.Mod.Phys. E25, 1650033 (2016) X.-W.Su, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Global 6He optical model potential NUCLEAR REACTIONS 6,7Li, 9Be, 12C, 27Al, 28Si, 51V, 48Ti, 58Ni, 63,65Cu, 64Zn, 120Sn, 197Au, 206,208Pb, 209Bi(6He, X), (6He, 6He), E<300 MeV; analyzed available data; deduced optical potential; calculated σ, σ(θ).
doi: 10.1142/S0218301316500336
2015TA16 Prog.Theor.Exp.Phys. 2015, 073D01 (2015) Y.Tanimura, K.Hagino, H.Z.Liang 3D mesh calculations for covariant density functional theory NUCLEAR STRUCTURE 16O, 24Mg, 28Si; calculated binding and single-particle energies, hexadecapole deformation parameters, potential energy surfaces.
doi: 10.1093/ptep/ptv083
2014GU01 Nucl.Phys. A922, 84 (2014) H.Guo, Y.Xu, H.Liang, Y.Han, Q.Shen Microscopic optical model potential for triton NUCLEAR REACTIONS A=6-232(t, t), (t, X), E=threshold-60 MeV/nucleon; calculated triton microscopic optical model potential, reaction σ, elastic scattering σ(θ). Compared with some data.
doi: 10.1016/j.nuclphysa.2013.11.007
2014HA17 Nucl.Data Sheets 118, 132 (2014) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculation of Actinide Nuclear Reaction Data
doi: 10.1016/j.nds.2014.04.018
2014LI10 Ann.Nucl.Energy 69, 301 (2014) The energy spectra and double-differential cross-sections for p+92, 94, 95, 96, 97, 98, 100Mo reactions at the incident energies from threshold to 200 MeV NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, xn), (p, xp), (p, xd), (p, xα), (p, xt), E<160 MeV; calculated σ(E), σ(E, θ). Exciton model including the improved Iwamoto-Harada model, comparison with experimental data.
doi: 10.1016/j.anucene.2014.02.008
2014LI14 Phys.Scr. 89, 054018 (2014) H.Liang, T.Nakatsukasa, Z.Niu, J.Meng Finite-amplitude method: an extension to the covariant density functionals NUCLEAR STRUCTURE 208Pb; calculated isoscalar giant monopole resonances. The finite-amplitude method for optimizing the computational performance of the random-phase approximation.
doi: 10.1088/0031-8949/89/5/054018
2014VA16 Phys.Scr. 89, 054008 (2014) N.Van Giai, H.Liang, H.-Q.Gu, W.Long, J.Meng Treating Coulomb exchange contributions in relativistic mean field calculations: why and how NUCLEAR STRUCTURE Pb; calculated Coulomb exchange energy for A=180-272 using relativistic HFB using Slater approximation with relativistic local density approximation.
doi: 10.1088/0031-8949/89/5/054008
2014WU07 Ann.Nucl.Energy 73, 17 (2014) Z.Wu, H.Liang, J.Li, Z.Zhang, Y.Han Theoretical calculations and evaluations of n + 32, 33, 34, 36, nat.S reactions NUCLEAR REACTIONS 32,33,34,36S, S(n, n), (n, n'), (n, X), (n, p), (n, t), (n, xn), (n, xp), E<200 MeV; calculated σ, σ(θ, E), σ(θ). APMN nuclear model code, comparison ENDF/B-VII, JENDL-4, and TENDL-2012 libraries.
doi: 10.1016/j.anucene.2014.05.032
2013GU14 Phys.Rev. C 87, 041301 (2013) H.-Q.Gu, H.Liang, W.H.Long, N.Van Giai, J.Meng Slater approximation for Coulomb exchange effects in nuclear covariant density functional theory NUCLEAR STRUCTURE Z=20, A=36-76; Z=28, A=56-96; Z=40, A=80-136; Z=50, A=100-180; Z=82, A=180-270; calculated Coulomb exchange energies, relative deviation of Coulomb exchange energies using self-consistent relativistic and non-relativistic local density approximations (RLDA, NRLDA) for even-even nuclei. 188,208,228, 248Pb; calculated proton density distributions using relativistic Hartree-Fock-Bogoliubov (RHFB) with PKA1 interaction. 208Pb; calculated proton single-particle energy shifts. Implementation of the Coulomb exchange effects in the relativistic Hartree (RH) theory.
doi: 10.1103/PhysRevC.87.041301
2013LI06 Phys.Rev. C 87, 014334 (2013) H.Liang, S.Shen, P.Zhao, J.Meng Pseudospin symmetry in supersymmetric quantum mechanics: Schrodinger equations NUCLEAR STRUCTURE 132Sn; calculated discrete eigenstates for neutrons, pseudospin-orbit splittings. Supersymmetry (SUSY) quantum mechanics, perturbation theory, and similarity renormalization group (SRG) method. Pseudospin symmetry (PSS) and its breaking mechanism.
doi: 10.1103/PhysRevC.87.014334
2013LI20 Phys.Rev. C 87, 054310 (2013) H.Liang, T.Nakatsukasa, Z.Niu, J.Meng Feasibility of the finite-amplitude method in covariant density functional theory NUCLEAR STRUCTURE 16O; calculated unperturbed 0+ excitation strengths. 132Sn, 208Pb; calculated isoscalar giant monopole resonance (ISGMR). Self-consistent relativistic random-phase approximation (RPA) and finite-amplitude method (FAM) based on RMF theory. Comparison with experimental data. Discussed effects of the Dirac sea in the matrix-FAM scheme.
doi: 10.1103/PhysRevC.87.054310
2013ME08 Phys.Scr. T154, 014010 (2013) J.Meng, Y.Chen, H.Z.Liang, Y.F.Niu, Z.M.Niu, L.S.Song, W.Zhao, Z.Li, B.Sun, X.D.Xu, Z.P.Li, J.M.Yao, W.H.Long, T.Niksic, D.Vretenar Mass and lifetime of unstable nuclei in covariant density functional theory NUCLEAR STRUCTURE A=80-195; calculated masses, binding energies, β-decay T1/2. Finite-range droplet model and Weizsacker-Skyrme models, comparison with available data.
doi: 10.1088/0031-8949/2013/T154/014010
2013NI09 Phys.Rev. C 87, 051303 (2013) Z.M.Niu, Y.F.Niu, Q.Liu, H.Z.Liang, J.Y.Guo Nuclear β+/EC decays in covariant density functional theory and the impact of isoscalar proton-neutron pairing RADIOACTIVITY 32,34Ar, 36,38Ca, 40,42Ti, 46,48,50Fe, 50,52,54Ni, 56,58Zn, 96,98,100Cd, 100,102,104Sn(β+), (EC); calculated half-lives, B(GT). Self-consistent proton-neutron QRPA with relativistic Hartree-Bogoliubov (QRPA+RHB) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.051303
2013NI12 Phys.Lett. B 723, 172 (2013) Z.M.Niu, Y.F.Niu, H.Z.Liang, W.H.Long, T.Niksic, D.Vretenar, J.Meng β-decay half-lives of neutron-rich nuclei and matter flow in the r-process RADIOACTIVITY Fe, Cd, 124Mo, 126Ru, 128Pd, 130Cd, 134Sn(β-); calculated T1/2, solar r-process abundances. Fully self-consistent proton-neutron quasiparticle random phase approximation (QRPA), based on the spherical relativistic Hartree-Fock-Bogoliubov (RHFB) framework.
doi: 10.1016/j.physletb.2013.04.048
2013SH31 Phys.Rev. C 88, 024311 (2013) S.Shen, H.Liang, P.Zhao, S.Zhang, J.Meng Pseudospin symmetry in supersymmetric quantum mechanics. II. Spin-orbit effects
doi: 10.1103/PhysRevC.88.024311
2012CH26 Phys.Rev. C 85, 067301 (2012) Density-dependent deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE 38Mg; calculated proton, neutron and matter rms radii, total ground state energy, quadrupole deformation, single particle energies of neutrons. Deformed relativistic continuum Hartree-Bogoliubov (RCHB) calculations, density-dependent meson-nucleon couplings. Comparison with spherical RCHB calculations.
doi: 10.1103/PhysRevC.85.067301
2012HA16 Ann.Nucl.Energy 46, 179 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen The analysis of n+237Np reactions for energies up to 200 MeV NUCLEAR REACTIONS 237Np(n, γ), (n, F), (n, 2n), (n, xn), (n, xp), (n, xd), (n, xt), (n, xα) E<200 MeV; calculated σ, σ(θ, E), σ(θ), σ(E). Optical model, the intra-nuclear cascade model, the unified Hauser-Feshbach theory, comparison with ENDF/B-VII and JENDL-3 libraries and available data.
doi: 10.1016/j.anucene.2012.03.013
2012HA24 Nucl.Sci.Eng. 172, 102 (2012) Y.Han, Y.Xu, H.Liang, H.Guo, C.Cai, Q.Shen Theoretical Calculations and Analysis of n + 27Al Reaction NUCLEAR REACTIONS 27Al(n, X), (n, n), (n, n'), (n, p), (n, γ), (n, d), (n, t), (n, α), (n, 2n), (n, xn), (n, xp), (n, xα), E<200 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Comparison with ENDF/B-VII and JENDL-3 evaluated nuclear libraries.
doi: 10.13182/NSE11-28
2012LI27 Phys.Rev. C 85, 064302 (2012) Fine structure of charge-exchange spin-dipole excitations in 16O NUCLEAR REACTIONS 16O(polarized p, n), (n, p), E not given; analyzed fine structure of charge-exchange spin-dipole (SD) excitations using fully self-consistent random phase approximation based on the covariant density functional theory. Balance between the s- and ω-meson fields via the exchange terms.
doi: 10.1103/PhysRevC.85.064302
2012LI36 Phys.Rev. C 86, 021302 (2012) H.Liang, P.Zhao, P.Ring, X.Roca-Maza, J.Meng Localized form of Fock terms in nuclear covariant density functional theory NUCLEAR STRUCTURE 90Zr, 208Pb; calculated Gamow-Teller resonance (GTR) and spin-dipole resonance (SDR) strength distributions. Relativistic Hartree-Fock (RHF) covariant density functional. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.021302
2012ZH18 Phys.Rev. C 85, 054310 (2012) P.W.Zhao, J.Peng, H.Z.Liang, P.Ring, J.Meng Covariant density functional theory for antimagnetic rotation NUCLEAR STRUCTURE 105Cd; calculated total Routhians, energy spectrum, total angular momenta, kinetic and dynamic moments of inertia, B(E2) values, alignments, Dirac currents, density distribution contours for antimagnetic rotational (AMR) band using tilted-axis cranking and relativistic mean field (TAC-RMF), and TAC with covariant density functional theory (CDFT). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054310
2011GU15 Phys.Rev. C 83, 064618 (2011) H.Guo, Y.Xu, H.Liang, Y.Han, Q.Shen 4He microscopic optical model potential NUCLEAR REACTIONS 12C, 58Ni, 116Sn, 208Pb(α, X), E=20-300 MeV; calculated radial dependence of real and imaginary parts of the potential, volume integral and rms radii. 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb, 209Bi(α, X), E=5-200 MeV; calculated reaction σ(E). 62,64Ni, 63,65Cu, 64,66,68,70Zn, 70,72Ge(α, α), E=25.0 MeV; 94Mo, 107Ag, 116,122,124Sn(α, α), E=25.2 MeV; 20,22Ne, 24,26Mg, 28Si, 40Ar, 40,42,44,48Ca, 56Fe, 56,58,60,62Ni, 90Zr, 124Sn, 208Pb(α, α), E=104 MeV; 16O, 46,48Ti, 58Ni, 116Sn, 197Au(α, α), E=240 MeV; 12C, 58Ni, 90Zr, 116Sn, 144Sm, 208Pb(α, α), E=386.0 MeV; calculated σ(θ). 12C(α, α), E=120.0-400 MeV; 58Ni(α, α), E=29.0-386 MeV; 24Mg(α, α), E=39.0-172.5 MeV; 107Ag(α, α), E=15.0-43.0 MeV; 116Sn(α, α), E=23.3-386 MeV; 124Sn(α, α), E=23.3-104 MeV; 208Pb(α, α), E=23.6-386.0 MeV; 209Bi(α, α), E=19.0-104 MeV; calculated σ(E, θ); deduced 4He microscopic optical model potential by Greens function method. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064618
2011HA28 Ann.Nucl.Energy 38, 1852 (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Calculation and evaluations for n + 63, 65, nat.Cu reactions NUCLEAR REACTIONS Cu, 63,65Cu(n, X), (n, n), (n, n'), (n, γ), (n, p), (n, d), (n, α), (n, 2n), (n, 3n), E<250 MeV; calculated σ, σ(θ). Optical model, preequilibrium theory, comparison with ENDF/B-VII.0, JENDL-3.3 evaluated nuclear libraries and experimental data.
doi: 10.1016/j.anucene.2011.05.016
2011HA29 Ann.Nucl.Energy 38, 1950 (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Double differential cross sections of n + 63, 65, nat.Cu reactions NUCLEAR REACTIONS Cu, 63,65Cu(n, X), (n, xn), (n, xp), (n, xα), (n, xd), (n, xt), E<200 MeV; calculated σ(θ, E). Optical model, unified Hauser-Feshbach and exciton model, comparison with ENDF/B-VII.0, JENDL-3.3 evaluated nuclear libraries and experimental data.
doi: 10.1016/j.anucene.2011.05.001
2011HA44 J.Korean Phys.Soc. 59, 855s (2011) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen, C.Cai The Theoretical Calculation of Cross Section and Spectrum for n+238U Reaction up to 150 MeV NUCLEAR REACTIONS 238U(n, f), (n, xn), (n, d), (n, t), (n, p), (n, α), E=0-200 MeV; calculated σ, dσ(E, θ) using different reaction models.
doi: 10.3938/jkps.59.855
2011LI03 Phys.Rev. C 83, 011302 (2011) Spin-orbit and orbit-orbit strengths for the radioactive neutron-rich doubly magic nucleus 132Sn in relativistic mean-field theory NUCLEAR STRUCTURE 132Sn; Z=50, N=62-86; N=82, Z=50-74; calculated S(2n), S(2p), Nilsson model spin-orbit parameter and orbit-orbit parameter using Relativistic mean-field theory with the PC-PK1, NL3*, DD-ME2, PK1, and PK-DD effective interactions for even-even Z=50 isotopes and N=82 isotones. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.011302
2011LI05 Nucl.Instrum.Methods Phys.Res. B269, 597 (2011) Calculation and analysis of p + 40, 42, 43, 44, 46, 48, natCa reaction cross sections at incident energies from threshold to 250 MeV NUCLEAR REACTIONS 40,42,43,44,46,48Ca, Ca(p, p), (p, p'), (p, n), (p, 2n), (p, X), (p, 3He), (p, 2p), (p, xn), (p, xd), (p, x3He), (p, xα), E<250 MeV; calculated σ, σ(θ). Optical model calculations.
doi: 10.1016/j.nimb.2011.01.015
2011LI09 Phys.Rev. C 83, 041301 (2011) H.Liang, P.Zhao, Y.Zhang, J.Meng, N.Van Giai Perturbative interpretation of relativistic symmetries in nuclei
doi: 10.1103/PhysRevC.83.041301
2011LI27 Nucl.Instrum.Methods Phys.Res. B269, 1899 (2011) Theoretical calculation and analysis of the p+59Co reaction NUCLEAR REACTIONS 59Co(p, X)57Co/58Co/56Co/56Mn/55Co/55Fe/54Mn/52Mn/51Cr, 59Co(p, n), (p, np), (p, 3n), (p, 4n), (p, xn), (p, xp), (p, xα), (p, xd), (p, xt), (p, x3He), E<200 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Optical model, comparison with experimental data.
doi: 10.1016/j.nimb.2011.05.014
2011ZH28 Phys.Rev.Lett. 107, 122501 (2011) P.W.Zhao, J.Peng, H.Z.Liang, P.Ring, J.Meng Antimagnetic Rotation Band in Nuclei: A Microscopic Description NUCLEAR STRUCTURE 105Cd; calculated angular momentum, energy and rotational frequency, B(E2). Covariant density functional theory.
doi: 10.1103/PhysRevLett.107.122501
2011ZH57 Phys.Lett. B 699, 181 (2011) P.W.Zhao, S.Q.Zhang, J.Peng, H.Z.Liang, P.Ring, J.Meng Novel structure for magnetic rotation bands in 60Ni NUCLEAR STRUCTURE 60Ni; calculated energy spectra, total angular momenta, evolution of deformation parameters, B(M1), B(E2), B(M1)/B(E2) ratios; deduced systematics of the newly observed shears bands. The self-consistent tilted axis cranking relativistic mean-field theory based on a point-coupling interaction.
doi: 10.1016/j.physletb.2011.03.068
2010HA06 Phys.Rev. C 81, 024616 (2010) Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen Global phenomenological optical model potential for nucleon-actinide reactions at energies up to 300 MeV NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np, 239,240,242Pu, 241Am(n, X), E=0.01-300 MeV; calculated total σ. 235,238U(n, n), E=0.01-300 MeV; calculated σ. 232Th, 235,238U, 239Pu(n, n'), E=0.1-300 MeV; calculated non-inelastic σ. 232Th, 235,238U, 239Pu(n, n), (n, n'), E=0.14-15.2 MeV; 238U(n, n), E=96 MeV; calculated σ(θ) for elastic σ, inelastic σ and elastic+inelastic σ. 232Th, 238U(p, X), E=0-300 MeV; calculated σ. 232Th, 235,238U(p, p), (p, p'), E=16-95 MeV; calculated σ(θ). global phenomenological optical model potential. Deduced of neutron and proton global optical model potential parameters. Comparison and analysis with experimental data.
doi: 10.1103/PhysRevC.81.024616
2010LI30 Eur.Phys.J. A 44, 119 (2010) H.Liang, W.H.Long, J.Meng, N.Van Giai Spin symmetry in Dirac negative-energy spectrum in density-dependent relativistic Hartree-Fock theory NUCLEAR STRUCTURE 16O; calculated single-particle energies, spin-orbit splitting, associated features of the negative-energy spectrum. Density-dependent relativistic Hartree-Fock theory.
doi: 10.1140/epja/i2010-10938-6
2010LI52 J.Phys.:Conf.Ser. 205, 012028 (2010) Isospin symmetry-breaking corrections for superallowed β decay in relativistic RPA approaches RADIOACTIVITY 10C, 14O, 18Ne, 26Al, 26Si, 30S, 34Cl, 34Ar, 38K, 38Ca, 42Sc, 42Ti, 54Co, 66As, 70Br, 74Br(EC), (β+); calculated ft, matrix elements, isospin symmetry-breaking corrections Δδc using self-consistent relativistic RPA.
doi: 10.1088/1742-6596/205/1/012028
2010ME09 Nucl.Phys. A834, 436c (2010) J.Meng, Z.P.Li, H.Z.Liang, Z.M.Niu, J.Peng, B.Qi, B.Sun, S.Y.Wang, J.M.Yao, S.Q.Zhang Covariant Density Functional Theory for Nuclear Structure and Application in Astrophysics NUCLEAR STRUCTURE 144,146,148,150,152,154,156Nd; calculated levels, J, π, B(E2), mass excess using covariant density functional theory. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.058
2010MO12 Phys.Rev. C 81, 064327 (2010) M.Moreno Torres, M.Grasso, H.Liang, V.De Donno, M.Anguiano, N.Van Giai Tensor effects in shell evolution at Z, N=8, 20, and 28 using nonrelativistic and relativistic mean-field theory NUCLEAR STRUCTURE 14C, 16,22O, 40,48,52,54Ca, 34,42Si, 36,44S, 56,60,66,68,78Ni; analyzed effects of the tensor force on the neutron and proton gaps. Hartree-Fock calculations with Skyrme and Gogny interactions. Non-relativistic and relativistic mean-field approaches. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.064327
2010SU15 Nucl.Instrum.Methods Phys.Res. B268, 2585 (2010) X.Su, H.Liang, Y.Han, C.Cai, Q.Shen The theoretical calculation of p+232Th reaction for energies up to 250 MeV NUCLEAR REACTIONS 232Th(p, n), (p, 2n), (p, 3n), (p, 6n), (p, xn), (p, xα), (p, xt), (p, F), (p, X), E<250 MeV; calculated σ, σ(θ), σ(E), σ(θ, E). Optical and Iwamoto-Harada models.
doi: 10.1016/j.nimb.2010.07.003
2010ZH35 Chin.Phys.Lett. 27, 102103 (2010) W.Zhang, H.-Z.Liang, S.-Q.Zhang, J.Meng Search for Ring-Like Nuclei under Extreme Conditions NUCLEAR STRUCTURE 24Mg; calculated potential energy surfaces, configurations, total and excitation energies, deformation parameters, rms radii. Adiabatic and diabatic constrained RMF approaches.
doi: 10.1088/0256-307X/27/10/102103
2009LI22 Phys.Rev. C 79, 064316 (2009) Isospin corrections for superallowed Fermi β decay in self-consistent relativistic random-phase approximation approaches RADIOACTIVITY 10C, 14O, 18Ne, 26Si, 26Al, 30S, 34Ar, 34Cl, 38Ca, 38K, 42Ti, 42Sc, 54Co, 66As, 70Br, 74Rb(β+); calculated excitation energies, nucleus independent Ft values, and isospin symmetry-breaking corrections for superallowed 0+ to 0+ β transitions using self-consistent random phase approximation (RPA) in the relativistic framework. Comparison with experimental data. Discussed Vud matrix element and unitarity of the Cabibbo-Kobayashi-Maskawa matrix element.
doi: 10.1103/PhysRevC.79.064316
2009NI01 Chin.Phys.Lett. 26, 032103 (2009) Stability of Strutinsky Shell Correction Energy in Relativistic Mean Field Theory NUCLEAR STRUCTURE 208Pb; calculated neutron shell correction energies using a RMF approach.
doi: 10.1088/0256-307X/26/3/032103
2009ZH47 Chin.Phys.C 33, Supplement 1, 113 (2009) First attempt to overcome the disaster of Dirac sea in imaginary time step method
doi: 10.1088/1674-1137/33/S1/036
2008LI38 Phys.Rev.Lett. 101, 122502 (2008) Spin-Isospin Resonances: A Self-Consistent Covariant Description NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated GTR and SDR strength distributions using a RHF+RPA appraoch.
doi: 10.1103/PhysRevLett.101.122502
2008TA12 Phys.Rev. C 77, 054316 (2008) D.Tarpanov, H.Liang, N.Van Giai, C.Stoyanov Mean-field study of single-particle spectra evolution in Z = 14 and N = 28 chains NUCLEAR STRUCTURE 34,36,38,40,42Si, 44S, 46Ar, 48Ca; calculated spin-orbit splitting, subshell closure, single-particle levels. Skyrme-Hartree-Fock and relativistic Hartree-Fock mean field models.
doi: 10.1103/PhysRevC.77.054316
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