NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.Hu Found 103 matches. Showing 1 to 100. [Next]2024WU03 Phys.Rev. C 109, 024310 (2024) X.H.Wu, C.Pan, K.Y.Zhang, J.Hu Nuclear mass predictions of the relativistic continuum Hartree-Bogoliubov theory with the kernel ridge regression
doi: 10.1103/PhysRevC.109.024310
2023HU04 Phys.Rev. C 107, 024915 (2023) Cross effects in spin hydrodynamics: Entropy analysis and statistical operator
doi: 10.1103/PhysRevC.107.024915
2023TH01 Phys.Rev. C 107, 015803 (2023) V.Thakur, R.Kumar, P.Kumar, M.Kumar, C.Mondal, K.Huang, J.Hu, B.K.Agrawal, S.K.Dhiman Relativistic approach for the determination of nuclear and neutron star properties in consideration of PREX-II results NUCLEAR STRUCTURE A=20-220; calculated charge rms radii, binding energy. 48Ca, 208Pb; calculated neutron skin thickness. Obtained properties of nonrotating neutron star. New parametrization of the relativistic mean-field (RMF) model obtained by fit to the available experimental data on binding energy, charge rms radii and taking into account recent PREX-II results on neutron skin thickness. Comparison to results obtained with different parametrizations - NL3, IOPB-I, FSUGarnet, Big Apple.
doi: 10.1103/PhysRevC.107.015803
2023WA35 Eur.Phys.J. A 59, 224 (2023) J.Wang, J.Ren, W.Jiang, X.Ruan, Q.Sun, J.Hu, B.Jiang, J.Bao, Q.Zhang, G.Luan, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, J.Bai, P.Cao, Q.Chen, Y.Chen, Z.Chen, Z.Cui, A.Fan, R.Fan, C.Feng, F.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, W.Jia, H.Jiang, Z.Jiang, Z.Jin, L.Kang, B.Li, C.Li, G.Li, J.Li, Q.Li, Y.Li, J.Liu, R.Liu, S.Liu, C.Ning, B.Qi, Z.Ren, Z.Song, K.Sun, Z.Tan, J.Tang, S.Tang, L.Wang, P.Wang, Z.Wang, Z.Wen, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, Y.Yu, G.Zhang, L.Zhang, M.Zhang, X.Zhang, Y.Zhang, Y.Zhang, Z.Zhang, M.Zhao, L.Zhou, K.Zhu, J.Zhang Determination of the 232Th(n, γ) cross section from 10 to 200 keV at the Back-n facility at CSNS NUCLEAR REACTIONS 232Th, 197Au(n, γ), E=10-200 keV; measured reaction products, En, In, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, CENDL-3.2, JENDL-5 libraries and TALYS 1.96 calculations. The back-streaming white neutron beam-line (Back-n) of China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-023-01126-0
2023YI06 Phys.Rev. C 108, 034002 (2023) P.Yin, X.L.Shang, J.N.Hu, J.Y.Fu, E.Epelbaum, W.Zuo Pairing properties of semilocal coordinate- and momentum-space regularized chiral interactions
doi: 10.1103/PhysRevC.108.034002
2023ZH43 Phys.Rev. C 108, 025809 (2023) Equation of state of nuclear matter and neutron stars: Quark mean-field model versus relativistic mean-field model
doi: 10.1103/PhysRevC.108.025809
2022HU03 J.Phys.(London) G49, 25104 (2022) The Ξ-nuclear potential constrained by recent Ξ-hypernuclei experiments NUCLEAR STRUCTURE 15C, 14N; analyzed available data; deduced nuclear potential in the quark mean-field (QMF) model.
doi: 10.1088/1361-6471/ac4469
2022HU16 Int.J.Mod.Phys. E31, 2250072 (2022) J.Hu, S.Wang, X.Sun, Y.Han, J.Zhang Effects of energy levels of the compound nucleus on particle emission for the 6Li(n, t), 3He(n p), and 7Be(n, p) reactions NUCLEAR REACTIONS 6Li(n, t), 3He(n, p), 7Be(n, p), E<10 MeV; calculated σ using the improved knockout model. Comparison with ENDF/B-VIII.0, JENDL-4.0, EAF-2010 libraries and experimental data.
doi: 10.1142/S0218301322500720
2022HU18 Phys.Rev. C 106, 045802 (2022) J.Hu, N.Tian, Y.Y.Li, S.Q.Hou, S.W.Xu, J.B.Liu, J.F.Lv R-matrix analyses for the 7Li(t, n)9Be and 7Li (3He, p) reactions and their improved thermonuclear reaction rates NUCLEAR REACTIONS 7Li(t, n), E<1.5 MeV; 7Li(3He, p), E<3.3 MeV; analyzed available experimental data on energy levels, particle widths, σ(E); calculated thermonuclear reaction rates, resonance energies and widths (from R-matrix fit). R-matrix analysis with code AZURE2. Comparison with previously published results. Analysis of the thermonuclear reaction rates relevant to the primordial 9Be abundance.
doi: 10.1103/PhysRevC.106.045802
2022LI72 Phys.Rev. C 106, 065804 (2022) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, D.X.Wang, S.Y.Zhang, G.L.Yang, X.K.Li, Z.D.An, J.J.He, W.Luo, X.G.Cao, L.L.Song, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, Y.D.Liu, C.W.Ma, Y.T.Wang, J.Su, L.Y.Zhang, Y.X.Yang, S.Feng, W.B.Liu, W.Q.Su, S.Jin, K.J.Chen Experimental determination of the neutron resonance peak of 162Er at 67.8 eV NUCLEAR REACTIONS 162Er(n, γ), E=20-100 eV; measured Eγ, Iγ; deduced neutron-capture yield, resonances, decay widths. Resonance parameters at 67.8 eV are extracted for the first time. R-matrix analysis. Comparison to other experimental results and ENDF/B-VIII.0 data. 4 C6D6 detectors. Neutron beam from Back-n Facility of the CSNS.
doi: 10.1103/PhysRevC.106.065804
2022ZH62 Phys.Rev. C 106, L051303 (2022) Resolving the spurious-state problem in the Dirac equation with the finite-difference method NUCLEAR STRUCTURE 132Sn; calculated neutron energy levels, neutron wave functions. Solved spurious-state problem appearing while solving Dirac equations with finite-difference method, by replacing the central difference formula with the asymmetric difference formula.
doi: 10.1103/PhysRevC.106.L051303
2021BA06 Phys.Rev. C 103, 015804 (2021) Impact of strong magnetic fields on the inner crust of neutron stars
doi: 10.1103/PhysRevC.103.015804
2021DI06 Nucl.Phys. A1014, 122237 (2021) Neutron drop trapped in axially deformed external fields NUCLEAR STRUCTURE N=28; calculated energy levels, J, π using an axially symmetric harmonic oscillator (ASHO) potential within the Skyrme HFB model.
doi: 10.1016/j.nuclphysa.2021.122237
2021HA53 Astrophys.J. 915, L13 (2021) S.Hayakawa, M.La Cognata, L.Lamia, H.Yamaguchi, D.Kahl, K.Abe, H.Shimizu, L.Yang, O.Beliuskina, S.M.Cha, K.Y.Chae, S.Cherubini, P.Figuera, Z.Ge, M.Gulino, J.Hu, A.Inoue, N.Iwasa, A.Kim, D.Kim, G.Kiss, S.Kubono, M.La Commara, M.Lattuada, E.J.Lee, J.Y.Moon, S.Palmerini, C.Parascandolo, S.Y.Park, V.H.Phong, D.Pierroutsakou, R.G.Pizzone, G.G.Rapisarda, S.Romano, C.Spitaleri, X.D.Tang, O.Trippella, A.Tumino, N.T.Zhang Constraining the Primordial Lithium Abundance: New Cross Section Measurement of the 7Be + n Reactions Updates the Total 7Be Destruction Rate NUCLEAR REACTIONS 2H(7Be, p7Li)1H, E=3.16 MeV/nucleon; measured reaction products. 8Be; deduced σ, low-lying resonance parameters, astrophysical reaction rates for 7Be(n, p) and 7Be(n, α) reactions. Comparison with available data. the Trojan Horse Method (THM), Center-for-Nuclear-Study RI Beam separator (CRIB), the University of Tokyo, located atthe RI Beam Factory, RIKEN.
doi: 10.3847/2041-8213/ac061f
2021HU11 Phys.Rev. C 103, 044611 (2021) J.Hu, S.Wang, X.Sun, Y.Han, J.Zhang Model calculation of the differential cross sections and angle-integrated cross sections of the emitted triton for neutron-induced 6Li reactions at low incident energies NUCLEAR REACTIONS 6Li(n, t), E=1 eV-3 MeV; calculated differential and angle-integrated σ(E, θ) using Knock-out model based on zero-range DWBA theory, and Hauser-Feshbach model. Comparison with experimental and evaluated (JEFF-3.3 and ENDF/B-VIII-0) data.
doi: 10.1103/PhysRevC.103.044611
2021HU23 Phys.Rev.Lett. 127, 172701 (2021) J.Hu, H.Yamaguchi, Y.H.Lam, A.Heger, D.Kahl, A.M.Jacobs, Z.Johnston, S.W.Xu, N.T.Zhang, S.B.Ma, L.H.Ru, E.Q.Liu, T.Liu, S.Hayakawa, L.Yang, H.Shimizu, C.B.Hamill, A.St J.Murphy, J.Su, X.Fang, K.Y.Chae, M.S.Kwag, S.M.Cha, N.N.Duy, N.K.Uyen, D.H.Kim, R.G.Pizzone, M.La Cognata, S.Cherubini, S.Romano, A.Tumino, J.Liang, A.Psaltis, M.Sferrazza, D.Kim, Y.Y.Li, S.Kubono Advancement of Photospheric Radius Expansion and Clocked Type-I X-Ray Burst Models with the New 22Mg(α, p)25Al Reaction Rate Determined at the Gamow Energy NUCLEAR REACTIONS 1H(25Al, p), (25Al, p'), (25Al, X), E=142 MeV; measured reaction products, Ep, Ip, Eγ, Iγ. 26Si; deduced σ(θ), level energies, J, π, resonance parameters, astrophysical reaction rates. Comparison with available data.
doi: 10.1103/physrevlett.127.172701
2021JI06 Phys.Rev. C 103, 055802 (2021) Nuclear pasta and symmetry energy in the relativistic point-coupling model NUCLEAR STRUCTURE 208Pb; calculated binding energy per nucleon versus symmetry energy based on PC-PK1 parameterization. Investigated influence of nuclear symmetry energy and its density dependence on pasta structures in neutron-rich nuclei by a coupling term between the isoscalar-vector and isovector-vector interactions using three-dimensional calculations based on Thomas-Fermi approximation, with the nuclear interaction from relativistic mean-field approach with the point-coupling interaction; deduced shapes as droplets, rods, slabs, tubes, and bubbles, and intermediate pasta structures in cold stellar matter with relatively large proton fractions. Relevance to inner crust of neutron stars and in core-collapse supernova explosions and neutron-star mergers.
doi: 10.1103/PhysRevC.103.055802
2021JI10 Nucl.Instrum.Methods Phys.Res. A1013, 165677 (2021) B.Jiang, J.Han, W.Jiang, J.Hu, X.Wang, J.Chen, X.Cai Monte-Carlo calculations of the energy resolution function with Geant4 for analyzing the neutron capture cross section of 232Th measured at CSNS Back-n NUCLEAR REACTIONS 232Th, 197Au(n, γ), E<20 MeV; analyzed available data; calculated Energy Resolution Function (ERF) for the Back-n facility at the China Spallation Neutron Source (CSNS Back-n facility) a newly-built time-of-flight (TOF) spectrometer.
doi: 10.1016/j.nima.2021.165677
2021JU01 Phys.Rev. C 103, 025809 (2021) M.Ju, X.Wu, F.Ji, J.Hu, H.Shen Hadron-quark mixed phase in the quark-meson coupling model
doi: 10.1103/PhysRevC.103.025809
2021LI61 Phys.Rev. C 104, 054302 (2021) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, X.G.Cao, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, J.C.Wang, D.X.Wang, S.Y.Zhang, Y.D.Liu, X.Ma, C.W.Ma, Y.T.Wang, Z.D.An, J.J.He, J.Su, L.Y.Zhang, Y.X.Yang, W.B.Liu, W.Q.Su New experimental measurement of natEr(n, γ) cross sections between 1 and 100 eV NUCLEAR REACTIONS 162,164,166,167,168,170Er, 12,13C, 197Au(n, γ), E=0.001-100 keV; measured E(n), I(n), Eγ, Iγ using C6D6 liquid scintillator and a silicon monitor and natural Er, C and Au targets at the China spallation neutron source (CSNS) facility; deduced neutron-capture σ(E), capture yields as function of E(n), neutron resonances in Er isotopes in the 1-100 eV region. 162,164,166,167,168Er; deduced energies of 43 neutron resonances (nine for 162Er, five for 164Er, three for 166Er, 25 for 167Er, one for 168Er), cross sections, widths Γγ and Γn by R-matrix analysis. Comparison with previous experimental data, and with data in evaluated databases ENDF/B-VIII.0, ENDF/B-VII.1, JENDL-4.0, and ROSFOND-2010.
doi: 10.1103/PhysRevC.104.054302
2020GE07 Phys.Rev. C 102, 044304 (2020) Origin of the evolution of spin-orbit and pseudospin-orbit splittings in neutron drops NUCLEAR STRUCTURE N=6-50; calculated total energies of neutron drops, spin-orbit (SO) splittings of 1p and 1d partners, pseudospin-orbit (PSO) splittings 1p and 1d pseudo-partners, neutron densities, staggering patterns. Skyrme EDF theory with SLy5 and SAMi-T parametrizations. Comparison with results from RBHF theory with the Bonn A potential.
doi: 10.1103/PhysRevC.102.044304
2020GU11 Phys.Lett. B 806, 135473 (2020) Y.K.Gupta, B.K.Nayak, U.Garg, K.Hagino, K.B.Howard, N.Sensharma, M.Senyigit, W.P.Tan, P.D.O'Malley, M.Smith, R.Gandhi, T.Anderson, R.J.deBoer, B.Frentz, A.Gyurjinyan, O.Hall, M.R.Hall, J.Hu, E.Lamere, Q.Liu, A.Long, W.Lu, S.Lyons, K.Ostdiek, C.Seymour, M.Skulski, B.Vande Kolk Determination of hexadecapole (β4) deformation of the light-mass nucleus 24Mg using quasi-elastic scattering measurements NUCLEAR REACTIONS 90Zr(16O, 16O), (24Mg, 24Mg), E=61 MeV; measured reaction products. 24Mg; deduced deformation parameters, σ, B(Eλ). CCFULL calculations.
doi: 10.1016/j.physletb.2020.135473
2020HA03 Phys.Rev. C 101, 015804 (2020) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu γ-ray spectroscopy of astrophysically important states in 39Ca NUCLEAR REACTIONS 40Ca(3He, αγ)39Ca, E=30 MeV; Measured Eγ, Iγ, Eα, Iα, αγ-coin, reaction products using the GODDESS array (Gammasphere for γ detection and ORRUBA for particle detection) at the ATLAS-ANL facility. 39Ca; deduced levels, J, π, γ-branching ratios. 38K(p, γ)39Ca, T=0.1-0.4 GK; deduced resonance parameters, astrophysical reaction rates. Discussed impact on abundances of isotopes created at the endpoint of nova nucleosynthesis.
doi: 10.1103/PhysRevC.101.015804
2020HA31 Phys.Rev. C 102, 045802 (2020) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu 19Ne level structure for explosive nucleosynthesis NUCLEAR REACTIONS 19F(3He, t)19Ne, E=30 MeV; measured reaction products, E(t), I(t), Eγ, Iγ, (triton)γ-, and (triton)γγ-coin using ORRUBA array with Micron QQQ5 telescopes for tritons and Gammasphere array for γ rays at ATLAS-ANL facility. 19Ne; deduced levels, J, π, γ-branching ratios. Comparison with earlier experimental results and with evaluated data. 18F(p, α)15O, E(cm)<0.9 MeV; calculated astrophysical S factors, and reaction rates at temperature of 0.06 to 0.4 GK.
doi: 10.1103/PhysRevC.102.045802
2020HU05 Phys.Rev. C 101, 034616 (2020) J.Hu, X.Sun, J.Zhang, S.Wang, Y.Han Theoretical analysis of double-differential cross sections of proton, deuteron, and triton emission in thee p + 7Li reaction at 14 MeV NUCLEAR REACTIONS 7Li(p, p'), (p, d), (p, t), (p, pd), (p, pt), (p, 2d), (p, 3He), (p, α), (p, pα), (p, dα), (p, 5He), E=14 MeV; calculated double differential σ(θ) using statistical theory of light nucleus reactions (STLN), including the sequential and simultaneous emission processes. Comparison with available experimental data.
doi: 10.1103/PhysRevC.101.034616
2020JI09 Phys.Rev. C 102, 015806 (2020) Nuclear pasta in hot and dense matter and its influence on the equation of state for astrophysical simulations
doi: 10.1103/PhysRevC.102.015806
2020WA27 J.Phys.(London) G47, 105108 (2020) Properties of nuclear matter in relativistic Brueckner-Hartree-Fock model with high-precision charge-dependent potentials
doi: 10.1088/1361-6471/aba423
2020WU02 Phys.Rev. C 101, 024303 (2020) Single-Λ+c hypernuclei within a quark mean-field model NUCLEAR STRUCTURE 16O, 40Ca, 51V, 89Y, 139La, 208Pb; calculated binding energies, charge, proton and neutron radii for core nuclei of hypernuclei. 17O, 41Ca, 52V, 90Y, 140La, 209Pb; calculated energy levels, binding energies, charge, proton and neutron radii of single-Λ+c hypernuclei within the quark mean-field (QMF) model.
doi: 10.1103/PhysRevC.101.024303
2020ZH14 Astrophys.J. 893, 126 (2020) Q.Zhang, Z.Huang, J.Hu, B.Chen, S.Hou, T.Wang, K.Fang Astrophysical S(E) for the 9Be(p, d)8Be and 9Be(p, α)6Li Reactions by Direct Measurement NUCLEAR REACTIONS 9Be(p, d), (p, α), E=34-100 KeV/nucleon; measured reaction products, Eα, Iα; deduced yields, S-factors, resonance parameters, reaction rates. Comparison with available data.
doi: 10.3847/1538-4357/ab8222
2019HA08 Phys.Rev.Lett. 122, 052701 (2019) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu Key 19Ne States Identified Affecting γ-Ray Emission from 18F in Novae NUCLEAR REACTIONS 19F(3He, t)19Ne, E=30 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, S-factor, reaction rates, resonance energies. Comparison with available data.
doi: 10.1103/PhysRevLett.122.052701
2019HA14 Phys.Rev. C 99, 035805 (2019) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu New γ-ray transitions observed in 19Ne with implications for the 15O(α, γ)19Ne reaction rate NUCLEAR REACTIONS 19F(3He, t), E=30 MeV; measured triton spectra, Eγ, Iγ, tγ- and γγ-coin using Gammasphere array for γ detection with the silicon detector array ORRUBA Dual Detectors for Experimental Structure Studies (GODDESS) at ATLAS-ANL facility. 19Ne; deduced levels, J, π, and γ-branching ratios for the decay of 4.14- and 4.20-MeV states. 15O(α, γ)19Ne, E≈18-180 keV; calculated fractional contribution of the corrected branching ratios for the 4.14 MeV, 7/2- and 4.20 MeV, 9/2- states in 19Ne to astrophysical reaction rate, which is of significance in breakout from the hot CNO cycle in type I x-ray bursts. Comparison with previous experimental values.
doi: 10.1103/PhysRevC.99.035805
2019HU09 J.Phys.(London) G46, 045101 (2019) A unified description of nuclear structures in shape phase transitions NUCLEAR STRUCTURE 150Nd, 156Dy, 158Er, 160Yb, 126,128Xe, 108Pd, 62Zn; analyzed available data; calculated B(E2), J, π. T(4) critical point symmetry (CPS).
doi: 10.1088/1361-6471/ab046b
2019JI06 Phys.Rev. C 100, 045801 (2019) Effects of nuclear symmetry energy and equation of state on neutron star properties
doi: 10.1103/PhysRevC.100.045801
2019RU05 J.Phys.(London) G46, 125108 (2019) X.H.Ruan, J.T.Hu, T.Rong, X.Bao Yields distribution of induced fission with improved scission point model NUCLEAR REACTIONS 230,231,232,233,234U, 206,207,208,209,210,211,212Fr, 214,215,216,217,218,219,220,221,222,223,224,225,226Ac, 220,221,222,223,224,225,226,227,228,229Th(n, F), E not given; calculated charge distributions using an improved scission point model. Comparison with available data.
doi: 10.1088/1361-6471/ab4820
2019ZH02 Nucl.Instrum.Methods Phys.Res. B438, 48 (2019) L.Zhang, S.Xu, J.He, S.Wang, H.Chen, J.Hu, S.Ma, N.Zhang, S.Hou, W.Liu Properties of fluorine targets and their application on the astrophysically important 19F(p, α)16O reaction NUCLEAR REACTIONS 19F(p, α), E < 270 keV; measured reaction products, Eγ, Iγ; deduced γ-ray yields.
doi: 10.1016/j.nimb.2018.10.024
2019ZH10 Phys.Rev. C 99, 025804 (2019) Z.-Y.Zhu, A.Li, J.-N.Hu, H.Shen Quark mean-field model for nuclear matter with or without bag
doi: 10.1103/PhysRevC.99.025804
2018FA09 Phys.Lett. B 785, 262 (2018) K.Fang, Q.Zhang, B.Chen, Z.Zhang, Q.Wang, T.Wang, J.Kasagi, J.Hu, S.Xu Direct measurement of astrophysical factor S(E) and screening potential for 9Be (p, α)6Li reaction at low energy NUCLEAR REACTIONS 9Be(p, α), E=18-100 keV; measured reaction products, Eα, Iα; deduced yields, S-factor. Comparison with available data.
doi: 10.1016/j.physletb.2018.08.066
2018HU09 Nucl.Sci.Eng. 191, 262 (2018) Calculation and Evaluations for n+64, 66, 67, 68, 70, natZn Reactions NUCLEAR REACTIONS 64,66,67,68,70Zn, Zn(n, X), E<200 MeV; calculated σ(θ), σ(E), σ(θ, E). Comparison with experimental data, JEFF-3.2 and JENDL-4.0 evaluated nuclear data libraries.
doi: 10.1080/00295639.2018.1469334
2018LI25 Phys.Rev. C 97, 054313 (2018) Nucleon properties in the Polyakov quark-meson model
doi: 10.1103/PhysRevC.97.054313
2018LI43 Phys.Rev. C 98, 024316 (2018) Z.-X.Liu, C.-J.Xia, W.-L.Lu, Y.-X.Li, J.N.Hu, T.-T.Sun Relativistic mean-field approach for Λ, Ξ and Σ Hypernuclei NUCLEAR STRUCTURE 17O, 17N, 17F, 41Ca, 41K, 41Sc, 91Zr, 91Nb, 91Y, 209Pb, 209Tl, 209Bi; calculated mean-field potentials, single-particle levels, density distributions, energies, radii, tensor potentials, and binding energies for hyperons (Λ, Ξ and Σ) in the hypernuclei, starting with the core nuclei of 16O, 40Ca and 208Pb. Relativistic mean-field model. Comparison with available experimental data.
doi: 10.1103/PhysRevC.98.024316
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
2018YU01 Chin.Phys.C 42, 034103 (2018) X.-R.Yu, J.Hu, X.-X.Li, S.-Y.An, Y.Zhang Effects of single particle on shape phase transitions and phase coexistence in odd-even nuclei
doi: 10.1088/1674-1137/42/3/034103
2018ZH07 Phys.Rev. C 97, 015805 (2018) Massive neutron star with strangeness in a relativistic mean-field model with a high-density cutoff NUCLEAR STRUCTURE 16O, 90Zr, 208Pb; calculated total energies and charge radii, mass-radius and mass-density relations for neutron star with the original TM1, and with and without hyperons. Relativistic mean-field (RMF) model by including logarithmic interaction as a function of the scalar meson field with TM1 parameter set and σ-cut potential.
doi: 10.1103/PhysRevC.97.015805
2017HU02 Phys.Rev. C 95, 025804 (2017) Neutron stars within a relativistic central variational method
doi: 10.1103/PhysRevC.95.025804
2017HU11 Phys.Rev. C 96, 034307 (2017) J.Hu, Y.Zhang, E.Epelbaum, U.-G.Meissner, J.Meng Nuclear matter properties with nucleon-nucleon forces up to fifth order in the chiral expansion
doi: 10.1103/PhysRevC.96.034307
2017HU18 Phys.Rev. C 96, 054304 (2017) Single-Ξ- hypernuclei within a quark mean-field model NUCLEAR STRUCTURE 12Be, 15C, 17N, 41K, 89Sr, 139Ba, 208Tl; calculated binding energies and potentials of single-Ξ- hypernuclei for different orbital states of the hyperons in different quark mean-field model (QMF) interactions. Comparison with experimental values.
doi: 10.1103/PhysRevC.96.054304
2017LI28 Nucl.Instrum.Methods Phys.Res. B410, 158 (2017) L.X.Liu, H.W.Wang, Y.G.Ma, X.G.Cao, X.Z.Cai, J.G.Chen, G.L.Zhang, J.L.Han, G.Q.Zhang, J.F.Hu, X.H.Wang, W.J.Li, Z.Yan, H.J.Fu Measurements of the total cross section of natBe with thermal neutrons from a photo-neutron source NUCLEAR REACTIONS 9Be(n, X), E=0.007-0.1 eV; measured reaction products, En, In, time-of-flight; deduced σ. Comparison with available data.
doi: 10.1016/j.nimb.2017.08.022
2017XI08 Phys.Rev. C 95, 054310 (2017) Quark mean field model with pion and gluon corrections for Λ and Ξ0 hypernuclei and neutron stars NUCLEAR STRUCTURE 40Ca, 89Y, 208Pb; calculated energy levels of Λ and Ξ0 hyperons for hypernuclei by QMF-NK1S, QMF-NK2S, and QMF-NK3S, and compared with experimental data and previous QMF model calculations without pion and gluon effects. 40Ca, 51V, 89Y, 139La, 208Pb; calculated binding energies of Λ hypernuclei with the QMF-NK3S parameters, and compared with experimental data. Fractions of leptons and baryons in neutron star matter as functions of total baryon density, and masses of neutron stars as functions of density and radius using QMF-NK1S, QMF-NK2S, and QMF-NK3S parameter sets.
doi: 10.1103/PhysRevC.95.054310
2016BR01 Phys.Rev. C 93, 025503 (2016) M.Brodeur, C.Nicoloff, T.Ahn, J.Allen, D.W.Bardayan, F.D.Becchetti, Y.K.Gupta, M.R.Hall, O.Hall, J.Hu, J.M.Kelly, J.J.Kolata, J.Long, P.O'Malley, B.E.Schultz Precision half-life measurement of 17F RADIOACTIVITY 17F(β+)[from 2H(16O, X), E not given]; measured β radiation, half-life of 17F decay at the University of Notre Dame β-decay counting station; deduced mixing ratio ρ for the mixed transition between mirror nuclei and the correlation parameters based on Standard Model validity. Discussed uncertainty estimates. Comparison with previous experimental measurements. NUCLEAR REACTIONS 2H(16O, X)12C/13C/14N/15O/16O/17O/17F, E not given; measured yields of reaction products at Notre Dame TwinSol facility.
doi: 10.1103/PhysRevC.93.025503
2016HE05 Phys.Rev. C 93, 055804 (2016) J.J.He, B.L.Jia, S.W.Xu, S.Z.Chen, S.B.Ma, S.Q.Hou, J.Hu, L.Y.Zhang, X.Q.Yu Direct measurement of 11B(p, γ)12C astrophysical S factors at low energies NUCLEAR REACTIONS 11B(p, γ)12C, E(cm)=130-257 keV; measured Eγ, Iγ, excitation functions, cross section at IMP-Lanzhou; deduced astrophysical S factors. Comparison with previous experimental results and with data in NACREII database.
doi: 10.1103/PhysRevC.93.055804
2016HU20 Phys.Rev. C 94, 054325 (2016) Phase transition in hot Λ hypernuclei within the relativistic Thomas-Fermi approximation NUCLEAR STRUCTURE 40Ca, 208Pb; calculated density distributions of Λ hyperon, rms radii of neutrons, protons, and Λ hyperon, specific heat as a function of temperature in hypernuclei. 16O, 28Si, 40Ca, 51V, 89Y, 139La, 208Pb; calculated single-Λ binding energies of hypernuclei as function of temperature. Relativistic Thomas-Fermi approximation for hot single-Λ hypernuclei. Comparison with available experimental data.
doi: 10.1103/PhysRevC.94.054325
2016LI06 Phys.Rev. C 93, 015803 (2016); Publisher's Note: Phys.Rev. C 102, 019907 (2020) A.Li, J.N.Hu, X.L.Shang, W.Zuo Nonrelativistic nucleon effective masses in nuclear matter: Brueckner-Hartree-Fock model versus relativistic Hartree-Fock model
doi: 10.1103/PhysRevC.93.015803
2016LI54 Ann.Nucl.Energy 96, 181 (2016) Z.Lin, Y.Nie, X.Cai, G.Kang, J.Hu, X.Wang, J.Ren, X.Ruan, J.Chen Benchmarking of 232Th evaluation by a 14.8 MeV neutron leakage spectra experiment with slab samples
doi: 10.1016/j.anucene.2016.05.019
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
2016SU10 Phys.Lett. B 756, 323 (2016) J.Su, W.P.Liu, N.T.Zhang, Y.P.Shen, Y.H.Lam, N.A.Smirnova, M.MacCormick, J.S.Wang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, Z.C.Gao, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li, G.Audi Revalidation of the isobaric multiplet mass equation at A = 53, T = 3/2 RADIOACTIVITY 53Ni(EC), (ECp) [from Be(58Ni, X)53Ni, E=68.3 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced T1/2, level scheme, J, π, isobaric analog state, mass excess, explanation of unexpected deviation from the isobaric multiplet mass equation (IMME) at A=53, T=3/2.
doi: 10.1016/j.physletb.2016.03.024
2016XI13 Phys.Rev. C 94, 044308 (2016) Quark mean field model with pion and gluon corrections NUCLEAR STRUCTURE 40,48Ca, 90Zr, 208Pb; calculated binding energies, rms charge radii, spin-orbit splittings and charge density distributions. Quark mean field (QMF) model with quark confinement potentials QMF-NK1, QMF-NK2, and QMF-NK3. Comparison with experimental values.
doi: 10.1103/PhysRevC.94.044308
2016ZH45 Phys.Rev. C 94, 045803 (2016); Erratum Phys.Rev. C 102, 019905 (2020) Z.-Y.Zhu, A.Li, J.-N.Hu, H.Sagawa Δ(1232) effects in density-dependent relativistic Hartree-Fock theory and neutron stars
doi: 10.1103/PhysRevC.94.045803
2015SH16 Phys.Rev. C 91, 047304 (2015) Y.P.Shen, W.P.Liu, J.Su, N.T.Zhang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, J.S.Wang, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li Measurement of the 52Fe mass via the precise proton-decay energy of 53Com RADIOACTIVITY 53mCo(p)[from 9Be(58Ni, X), E=68.3 MeV/nucleon]; 41Ti(β+p); measured Ep, Ip, at RIBLL-HIRFL-Lanzhou facility; deduced mass excess of 52Fe and compared with AME-2012 evaluation. 51Fe, 52Co(β+); measured half-lives and compared with evaluated data in ENSDF. ATOMIC MASSES 52Fe; deduced mass excess from Q value of proton decay of 3174.1 keV, 19/2- isomer in 53Co determined from measured proton energy. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.047304
2015SH19 Eur.Phys.J. A 51, 40 (2015) An effective formula for nuclear charge radii COMPILATION A=40-214; compiled experimental charge radii; deduced effective five-parameter formula considering Casten factor and odd-even staggering.
doi: 10.1140/epja/i2015-15040-1
2014BA45 Phys.Rev. C 90, 045802 (2014) S.S.Bao, J.N.Hu, Z.W.Zhang, H.Shen Effects of the symmetry energy on properties of neutron star crusts near the neutron drip density
doi: 10.1103/PhysRevC.90.045802
2014HU01 Prog.Theor.Exp.Phys. 2014, 013D02 (2014) Quark mean-field model for single and double Λ and Ξ hypernuclei NUCLEAR STRUCTURE 40Ca, 89Y, 208Pb; calculated hypernuclei single-particle, binding and bond energies.
doi: 10.1093/ptep/ptt119
2014HU03 Phys.Rev. C 89, 025802 (2014) Extended quark mean-field model for neutron stars
doi: 10.1103/PhysRevC.89.025802
2014HU13 Phys.Rev. C 90, 014309 (2014) Effective ΛN potential from relativistic Brueckner-Hartree-Fock theory NUCLEAR STRUCTURE 16O, 28Si, 40Ca, 51V, 89Y, 139La, 208Pb; calculated total and single binding energies of hypernuclei, effective ΛN potentials. Density-dependent relativistic mean-field (DDRMF) approach through the relativistic Brueckner-Hartree-Fock (RBHF) theory with Jul94 potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.014309
2014HU16 Phys.Rev. C 90, 025803 (2014) J.Hu, J.J.He, A.Parikh, S.W.Xu, H.Yamaguchi, D.Kahl, P.Ma, J.Su, H.W.Wang, T.Nakao, Y.Wakabayashi, T.Teranishi, K.I.Hahn, J.Y.Moon, H.S.Jung, T.Hashimoto, A.A.Chen, D.Irvine, C.S.Lee, S.Kubono Examination of the role of the 14O(α, p)17F reaction rate in type-I x-ray bursts NUCLEAR REACTIONS 1H(17F, p), E=3.6 MeV/nucleon, [17F secondary beam from 2H(16O, n), E=6.6 MeV/nucleon primary reaction]; measured Ep, Ip, angular distribution using radioactive ion beam separator (CRIB) at CNS-RIKEN facility. 18Ne; deduced levels, resonances, J, π, L-transfers, widths, proton partial widths, resonance strengths. R-matrix analysis of experimental data. Comparison with previous experimental results. 14O(α, p)17F, at T9=0.25-3.0; deduced reaction rates and compared with other studies. Relevance to hot-CNO cycle of the rp-process in type-I x-ray bursts (XRBs).
doi: 10.1103/PhysRevC.90.025803
2014ME18 Phys.Scr. 89, 054029 (2014) J.Meng, P.W.Zhao, S.Q.Zhang, J.N.Hu, J.Li Nuclear moments in covariant density functional theory
doi: 10.1088/0031-8949/89/5/054029
2014SU21 Phys.Rev. C 90, 054321 (2014) T.T.Sun, S.Q.Zhang, Y.Zhang, J.N.Hu, J.Meng Green's function method for single-particle resonant states in relativistic mean field theory NUCLEAR STRUCTURE 120Sn; calculated density of neutron states, single-neutron energies for positive and negative-parity bound states, energies and widths of single-neutron resonant states. Relativistic mean field theory formulated with Green's function method.
doi: 10.1103/PhysRevC.90.054321
2014ZH05 Phys.Rev. C 89, 015804 (2014) L.Y.Zhang, J.J.He, A.Parikh, S.W.Xu, H.Yamaguchi, D.Kahl, S.Kubono, P.Mohr, J.Hu, P.Ma, S.Z.Chen, Y.Wakabayashi, H.W.Wang, W.D.Tian, R.F.Chen, B.Guo, T.Hashimoto, Y.Togano, S.Hayakawa, T.Teranishi, N.Iwasa, T.Yamada, T.Komatsubara, Y.H.Zhang, X.H.Zhou Investigation of the thermonuclear 18Ne(α, p)21Na reaction rate via resonant elastic scattering of 21Na + p NUCLEAR REACTIONS 1H(21Na, p), E=89 MeV, [21Na secondary beam from 2H(20Ne, X), E=8.2 MeV/nucleon primary reaction]; measured particle spectra, Ep, Ip, σ using CNS Radioactive Ion Beam Separator at RIKEN facility. 22Mg; deduced levels, resonances, J, π, proton widths, resonance parameters by R-matrix analysis. comparison with previous experimental results. 18Ne(α, p)21Na; deduced thermonuclear reaction rates. One-zone postprocessing x-ray burst calculations, and effect on peak nuclear energy generation rate, reaction fluxes, and onset temperature of breakout reaction from hot CNO cycles to rp process in type I x-ray bursts.
doi: 10.1103/PhysRevC.89.015804
2014ZH36 Phys.Rev. C 90, 054302 (2014) Z.W.Zhang, S.S.Bao, J.N.Hu, H.Shen Symmetry energy of hot nuclei in the relativistic Thomas-Fermi approximation NUCLEAR STRUCTURE 56Fe, 208Pb; calculated proton and neutron density distributions and rms radii, neutron skin thickness. 56Ti, 56Cr, 56Fe, 56Ni, 208Pb, 208Po, 208Rn, 208Ra, 208Th; calculated symmetry energy coefficient asym as a function of Z. 56Fe, 112Sn, 150Sm, 208Pb; calculated temperature as a function of the excitation energy per particle, temperature dependence of asym. Relativistic Thomas-Fermi approximation using the relativistic mean-field model for four parameterization NL3, TM1, FSU and IUFSU.
doi: 10.1103/PhysRevC.90.054302
2013DU09 Nucl.Instrum.Methods Phys.Res. A723, 99 (2013) N.N.Duy, S.Kubono, H.Yamaguchi, D.Kahl, Y.Wakabayashi, T.Teranishi, N.Iwasa, Y.K.Kwon, L.H.Khiem, Y.H.Kim, J.S.Song, J.Hu, Y.Ayyad Low-energy radioactive ion beam production of 22Mg NUCLEAR REACTIONS 3He(20Ne, n), E=6.2 MeV/nucleon; measured reaction products; deduced yields.
doi: 10.1016/j.nima.2013.05.026
2013GU04 Phys.Rev. C 87, 015803 (2013) B.Guo, J.Su, Z.H.Li, Y.B.Wang, S.Q.Yan, Y.J.Li, N.C.Shu, Y.L.Han, X.X.Bai, Y.S.Chen, W.P.Liu, H.Yamaguchi, D.N.Binh, T.Hashimoto, S.Hayakawa, D.Kahl, S.Kubono, J.J.He, J.Hu, S.W.Xu, N.Iwasa, N.Kume, Z.H.Li Determination of the astrophysical 12N(p, γ)13O reaction rate from the 2H(12N, 13O)n reaction and its astrophysical implications NUCLEAR REACTIONS 2H(12N, 13O)1n, E=59 MeV; measured reaction products, energy loss, time-of-flight, differential σ(θ); deduced ANC, astrophysical S factors. 12N(p, γ)13O, at T9=0.3-3.0; deduced stellar reaction rate. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.87.015803
2013HE16 Phys.Rev. C 88, 012801 (2013) J.J.He, L.Y.Zhang, A.Parikh, S.W.Xu, H.Yamaguchi, D.Kahl, S.Kubono, J.Hu, P.Ma, S.Z.Chen, Y.Wakabayashi, B.H.Sun, H.W.Wang, W.D.Tian, R.F.Chen, B.Guo, T.Hashimoto, Y.Togano, S.Hayakawa, T.Teranishi, N.Iwasa, T.Yamada, T.Komatsubara The 18Ne(α, p)21Na breakout reaction in x-ray bursts: Experimental determination of spin-parities for α resonances in 22Mg via resonant elastic scattering of 21Na+p NUCLEAR REACTIONS 1H(21Na, p), [21Na secondary beam from 20Ne(d, n), E=8.2 MeV/nucleon primary reaction], E=89.4 MeV; measured E(p), I(p) σ(E) at CRIB-CNS-RIKEN facility. 22Mg; deduced levels, resonances, J, π. R-matrix analysis. 18Ne(α, p)21Na; deduced α-widths, resonance strengths, reaction rates using a narrow resonance formalism. Comparison of reaction rates with previous experimental studies and statistical model calculations. Discussed impact of new rates for 18Ne(α, p)21Na reaction on x-ray burst (XRB) calculations.
doi: 10.1103/PhysRevC.88.012801
2013HE21 Phys.Lett. B 725, 287 (2013) J.J.He, S.Z.Chen, C.E.Rolfs, S.W.Xu, J.Hu, X.W.Ma, M.Wiescher, R.J.de Boer, T.Kajino, M.Kusakabe, L.Y.Zhang, S.Q.Hou, X.Q.Yu, N.T.Zhang, G.Lian, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan A drop in the 6Li(p, γ)7Be reaction at low energies NUCLEAR REACTIONS 6Li(p, γ), E(cm)<1 MeV; measured reaction products, Eγ, Iγ; deduced S-factors, positive-parity resonance. Comparison with available data, SUSY assisted Big-bang Nucleosynthesis models.
doi: 10.1016/j.physletb.2013.07.044
2013JI13 Phys.Rev. C 88, 035801 (2013) S.J.Jin, Y.B.Wang, J.Su, S.Q.Yan, Y.J.Li, B.Guo, Z.H.Li, S.Zeng, G.Lian, X.X.Bai, W.P.Liu, H.Yamaguchi, S.Kubono, J.Hu, D.Kahl, H.S.Jung, J.Y.Moon, C.S.Lee, T.Teranishi, H.W.Wang, H.Ishiyama, N.Iwasa, T.Komatsubara, B.A.Brown Resonant scattering of 22Na+p studied by the thick-target inverse-kinematic method NUCLEAR REACTIONS 1H(22Na, 22Na), E<37.1 MeV, [22Na secondary beam from 1H(22Ne, 22Na), E=6.0 MeV/nucleon primary reaction]; measured back-angle recoil-proton spectra, TOF, differential σ(E) using thick target technique at RIBF-RIKEN facility. R-matrix analysis of resonance spectra. 23Mg; deduced levels, resonances, J, π, Γp, Γγ, resonance strengths, two s-wave resonances. Comparison with previous experimental data, and with shell-model calculations. 22Na(p, γ)23Mg, T9=0.01-10; deduced astrophysical reaction rates. Comparison with previous experimental data and NACRE evaluation. NUCLEAR STRUCTURE 23Mg; calculated levels, J, π, s-wave resonances, their spectroscopic factors and γ widths using shell model with usda and usdb interactions. Comparison with experimental data, and with structure of 23Na mirror nucleus.
doi: 10.1103/PhysRevC.88.035801
2013LI55 Phys.Rev. C 88, 064307 (2013) J.Li, J.X.Wei, J.N.Hu, P.Ring, J.Meng Relativistic description of magnetic moments in nuclei with doubly closed shells plus or minus one nucleon NUCLEAR MOMENTS 207,209Pb, 207Tl, 209Bi; calculated magnetic moments using relativistic mean field point-coupling model with the density functional PC-PK1. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.064307
2013SU07 Phys.Rev. C 87, 024312 (2013) J.Su, W.P.Liu, N.C.Shu, S.Q.Yan, Z.H.Li, B.Guo, W.Z.Huang, S.Zeng, E.T.Li, S.J.Jin, X.Liu, Y.B.Wang, G.Lian, Y.J.Li, Y.S.Chen, X.X.Bai, J.S.Wang, Y.Y.Yang, R.F.Chen, S.W.Xu, J.Hu, S.Z.Chen, S.B.Ma, J.L.Han, P.Ma, Q.Hu, J.B.Ma, X.G.Cao, S.L.Jin, Z.Bai, K.Yang, F.D.Shi, W.Zhang, Z.Chen, L.X.Liu, Q.Y.Lin, X.S.Yan, X.H.Zhang, F.Fu, J.J.He, X.Q.Li, C.He, M.S.Smith Reexamining the β decay of 53, 54Ni, 52, 53Co, 51Fe, and 50Mn RADIOACTIVITY 50Mn, 50Cr, 51Fe, 52,53Co, 53,54Ni(β+), (EC), (β+p)[from (58Ni, X), E=68.6 MeV/nucleon]; measured β-delayed protons, (proton)γ-coin, Eγ, Iγ, T1/2 at HIRFL facility in Lanzhou. Implications for r process. Comparison with previous experimental studies.
doi: 10.1103/PhysRevC.87.024312
2013YA06 Phys.Rev. C 87, 044613 (2013), Pub.Note Phys.Rev. C 88, 019901 (2013) Y.Y.Yang, J.S.Wang, Q.Wang, D.Y.Pang, J.B.Ma, M.R.Huang, J.L.Han, P.Ma, S.L.Jin, Z.Bai, Q.Hu, L.Jin, J.B.Chen, N.Keeley, R.Rusek, R.Wada, S.Mukherjee, Z.Y.Sun, R.F.Chen, X.Y.Zhang, Z.G.Hu, X.H.Yuan, X.G.Cao, Z.G.Xu, S.W.Xu, C.Zhen, Z.Q.Chen, Z.Chen, S.Z.Chen, C.M.Du, L.M.Duan, F.Fu, B.X.Gou, J.Hu, J.J.He, X.G.Lei, S.L.Li, Y.Li, Q.Y.Lin, L.X.Liu, F.D.Shi, S.W.Tang, G.Xu, X.Xu, L.Y.Zhang, X.H.Zhang, W.Zhang, M.H.Zhao, Z.Y.Guo, Y.H.Zhang, H.S.Xu, G.Q.Xiao Elastic scattering of the proton drip-line nucleus 8B off a natPb target at 170.3 MeV NUCLEAR REACTIONS Pb(8B, 8B), E=170.3 MeV, [secondary 8B beam from 9Be(12C, X), E=54.2 MeV/nucleon primary reaction]; measured reaction products, energy loss, time of flight, magnetic rigidity, σ(θ) at RIBLL-HRIFL facility in Lanzhou. Analysis of σ(θ) data by optical model using a single-folding-type potential, and by continuum discretized coupled-channels (CDCC) method. Effect of breakup-channel couplings. Comparison with previous experimental σ(θ) data for Pb(7Be, 7Be), E=125 MeV, and 208Pb(6Li, 6Li), E=99 MeV.
doi: 10.1103/PhysRevC.87.044613
2013YA24 Nucl.Instrum.Methods Phys.Res. A 701, 1 (2013) Y.Y.Yang, J.S.Wang, Q.Wang, J.B.Ma, M.R.Huang, J.L.Han, P.Ma, S.L.Jin, Z.Bai, Q.Hu, L.Jin, J.B.Chen, R.Wada, Z.Y.Sun, R.F.Chen, X.Y.Zhang, Z.G.Hu, X.H.Yuan, X.G.Cao, Z.G.Xu, S.W.Xu, C.Zhen, Z.Q.Chen, Z.Chen, S.Z.Chen, C.M.Du, L.M.Duan, F.Fu, B.X.Gou, J.Hu, J.J.He, X.G.Lei, S.L.Li, Y.Li, Q.Y.Lin, L.X.Liu, F.D.Shi, S.W.Tang, G.Xu, X.Xu, L.Y.Zhang, X.H.Zhang, W.Zhang, M.H.Zhao, Y.H.Zhang, H.S.Xu A method for the measurement of elastic scattering angular distribution at HIRFL-RIBLL NUCLEAR REACTIONS Pb(7Be, 7Be), E=125.3 MeV; measured products, Pb; deduced σ(θ). Data were imported from EXFOR entry S0076.
doi: 10.1016/j.nima.2012.10.088
2012WA11 Prog.Theor.Phys.(Kyoto) 127, 739 (2012) Skyrme-Hartree-Fock plus Tensor Correction for Nuclear Matter
doi: 10.1143/PTP.127.739
2011HE07 Int.J.Mod.Phys. E20, 747 (2011) J.J.He, L.Li, J.Hu, L.Y.Zhang, S.W.Xu, X.Q.Yu, M.L.Liu Development of a Lorentzian-Function approximation utilizing in the charge-particle-induced nonresonant reaction rate
doi: 10.1142/S0218301311018204
2011HE09 Eur.Phys.J. A 47, 67 (2011) J.J.He, J.Hu, S.W.Xu, Z.Q.Chen, X.Y.Zhang, J.S.Wang, H.W.Wang, W.D.Tian, X.Q.Yu, L.Y.Zhang, L.Li, Y.Y.Yang, P.Ma, X.H.Zhang, J.Su, E.T.Li, Z.G.Hu, Z.Y.Guo, X.Xu, X.H.Yuan, W.Lu, Y.H.Yu, Y.D.Zang, S.W.Ye, R.P.Ye, J.D.Chen, S.L.Jin, C.M.Du, S.T.Wang, J.B.Ma, L.X.Liu, Z.Bai, X.Q.Li, X.G.Lei, Z.Y.Sun, Y.H.Zhang, X.H.Zhou, H.S.Xu Study of proton resonances in 18Ne via resonant elastic scattering of 17F + p and its astrophysical implication in the stellar reaction of 14O(α, p)17F NUCLEAR REACTIONS 1H, 12C(17F, X), E=4.22 MeV/nucleon; measured E(particle), I(particle, θ); deduced σ(θ), R-matrix resonance parameters; calculated σ(θ), α spectroscopic factors, resonant reaction rates using multichannel R-matrix.
doi: 10.1140/epja/i2011-11067-6
2011WA25 Phys.Rev. C 84, 037303 (2011) S.T.Wang, X.H.Zhou, Y.H.Zhang, Z.Y.Sun, Y.Zheng, M.L.Liu, L.Chen, N.T.Zhang, J.Hu, F.Ma, W.Hua, S.Guo, Y.H.Qiang, L.Ma, Y.D.Fang, G.S.Li, H.B.Zhou, B.Ding, H.X.Wang, X.G.Lei, Y.X.Guo, Y.X.Liu, Y.Shi, F.R.Xu, L.H.Zhu, X.G.Wu Identification of the γ -vibrational band built on the 11/2-[505] orbital in 165Er NUCLEAR REACTIONS 160Gd(9Be, 4n), E=42, 45 MeV; measured Eγ, Iγ, γγ-coin. 165Er; deduced levels, J, π, bands, 3-qp state.
doi: 10.1103/PhysRevC.84.037303
2010HU10 Eur.Phys.J. A 43, 323 (2010) The role of the form factor and short-range correlation in the relativistic Hartree-Fock model for nuclear matter
doi: 10.1140/epja/i2010-10917-y
2010WE03 Prog.Theor.Phys.(Kyoto) 123, 811 (2010) Role of Form Factor in Relativistic Hartree-Fock Approach for Finite Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energy per nucleon, single-particle energies. Relativistic Hartree-Fock (RHF) approach.
doi: 10.1143/PTP.123.811
2009HE12 Phys.Rev. C 80, 015801 (2009) J.J.He, S.Kubono, T.Teranishi, J.Hu, M.Notani, H.Baba, S.Nishimura, J.Y.Moon, M.Nishimura, H.Iwasaki, Y.Yanagisawa, N.Hokoiwa, M.Kibe, J.H.Lee, S.Kato, Y.Gono, C.S.Lee Investigation of excited states in 22Mg via resonant elastic scattering of 21Na+p and its astrophysical implications NUCLEAR REACTIONS p(21Na, p)22Mg, E=4.0 MeV/nucleon; measured Ep, σ(θ).22Mg; deduced levels, J, π, resonances, widths and resonance parameters. R-matrix analysis of σ(θ) data with SAMMY-M6-BETA code. 18Ne(α, p)21Na, E not given; deduced astrophysical resonance reaction rates.22Mg, 22Ne; comparison of level systematics of mirror nuclei.
doi: 10.1103/PhysRevC.80.015801
2009HU02 Phys.Rev. C 79, 024305 (2009) J.Hu, Y.Ogawa, H.Toki, A.Hosaka, H.Shen Extended relativistic chiral mean field model for nuclear matter
doi: 10.1103/PhysRevC.79.024305
2009WA23 Chin.Phys.C 33, 629 (2009) S.-T.Wang, X.-H.Zhou, Y.-H.Zhang, Y.zheng, M.-L.Liu, F.Ma, J.Hu, L.Chen, X.Zhang, N.-T.Zhang, L.-H.Zhu, x.-G.Wu, G.-S.Li Electric-dipole transitions in 165Er NUCLEAR REACTIONS 160Gd(9Be, 4n), E=42, 45 MeV; measured Eγ, Iγ, γγ-coin; 165Er; deduced levels, J, π, bands, B(E1), octupole deformation.
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2001ZH07 Phys.Rev. C63, 047305 (2001) Configuration Dependence of Moments of Inertia in the Odd-A Nucleus from BCS Theory NUCLEAR STRUCTURE 170Yb, 171Lu; calculated rotational bands moments of inertia; deduced role of blocking effect. BCS theory.
doi: 10.1103/PhysRevC.63.047305
1999BR06 Phys.Rev. C59, 767 (1999) U.Brosa, H.-H.Knitter, T.-S.Fan, J.-M.Hu, S.-L.Bao Systematics of Fission-Channel Probabilities NUCLEAR STRUCTURE 234,236,239U, 232,233Th, 238Np, 240,242Pu; analyzed fission channel probabilities; deduced barrier parameters.
doi: 10.1103/PhysRevC.59.767
1997BA23 Phys.Lett. 395B, 151 (1997) Neutron Halo in Light Nuclei NUCLEAR STRUCTURE 4,5,6,7,8He, 4,5,6,7,8,9,10,11Li, 8,9,10,11,12,13,14Be; calculated binding energies, nucleon distributions rms radii, other properties. Mean-field approximation with Skyrme force.
doi: 10.1016/S0370-2693(97)00070-1
1997BA54 Phys.Rev. C56, 1410 (1997) Microscopic Study of the Ground State Properties of Light Nuclei NUCLEAR STRUCTURE 3,4,5,6,7,8He, 4,5,6,7,8,9,10,11Li, 6,7,8,9,10,11,12,13,14Be, 7,8,9,10,11,12,13,14,15,16,17,18,19B, 8,9,10,11,12,13,14,15,16,17,18,19,20,21,22C, 10,11N; calulated binding energies, neutron separation energies, odd-even mass difference. 4,6,8,10Li, 8,10,12,14,16,18B, 10,12,14,16,18,20,22N; calculated ground-state J, π. 6,7,8,9,10,11Li, 7,8,9,10,11,12,13Be, 8,9,10,11,12,13,14,15,16B, 12,13,14,15,16,17,18,19,20,21,22C; calculated nucleon distribution rms radii. 9,10,11Li, 11,12,13,14Be; calculated nucleon density distributions. Skyrme Hartree-Fock model with pairing.
doi: 10.1103/PhysRevC.56.1410
1997ZH04 Nucl.Phys. A615, 229 (1997) S.-G.Zhou, C.Zheng, F.Xu, J.Hu Study of the Superdeformed Nuclei in A = 190 Region with the Cranking Bohr-Mottelson Hamiltonian NUCLEAR STRUCTURE 189,191,190,192,193,194Hg, 192,194,196,198,193,195Pb, 191,193,195,192,194Tl, 196Bi, 191Au, 198Po; analyzed superdeformed bands transition energies; deduced mass, rigidity parameters. Cranking Bohr-Mottelson Hamiltonian.
doi: 10.1016/S0375-9474(96)00490-3
1996AN02 Nucl.Phys. A598, 1 (1996) Trial Densities for the Extended Thomas-Fermi Model NUCLEAR STRUCTURE 16O, 40,48Ca, 58Ni, 90Zr, 116,124,132Sn, 140Ce, 208Pb; calculated binding energies, charge radii, neutron skin thickness. Extended Thomas-Fermi method.
doi: 10.1016/0375-9474(95)00461-0
1995FA14 Nucl.Phys. A591, 161 (1995); Erratum Nucl.Phys. A606, 607 (1996) Study of Multichannel Theory for the Neutron Induced Fissions of Actinide Nuclei NUCLEAR REACTIONS 235U(n, F), E=thermal, 0.5-6 MeV; 232Th(n, F), E=1.38-5.6 MeV; 233U(n, F), E=thermal, 0.45=5.5 MeV; 238U(n, F), E=1.3-5.3 MeV; 237Np(n, F), E=0.8, 5.5 MeV; 239Pu(n, F), E=thermal, 5.5 MeV; 240Pu(n, F), E=0.85, 4.9 MeV; 241Pu(n, F), E=0.3-5 MeV; 242Pu(n, F), E=0.7, 4.9 MeV; analyzed fission fragment mass yield distributions, total kinetic energy, neutron multiplicities; deduced channel probability incident energy dependence.
doi: 10.1016/0375-9474(95)00193-5
1995HU07 Phys.Rev. C51, 2504 (1995) Cranking Bohr-Mottelson Hamiltonian Applied to Normal Bands of Odd-A Nuclei NUCLEAR STRUCTURE A=155-185; A ≥ 231; analyzed rotational bands data. Cranking Bohr-Mottelson Hamiltonian.
doi: 10.1103/PhysRevC.51.2504
1995XU01 Phys.Rev. C52, 431 (1995) Cranking Bohr-Mottelson Hamiltonian Applied to Superdeformed Bands in the A ≈ 150 Region NUCLEAR STRUCTURE 143Eu, 152Dy; calculated superdeformed band states transition energies. 146,147,148,149,150Gd, 150,151Tb, 151,152,153Dy; deduced superdeformed state spin assignments. Cranking Bohr-Mottelson Hamiltonian.
doi: 10.1103/PhysRevC.52.431
1994XU03 Phys.Rev. C49, 1449 (1994) Cranking Bohr-Mottelson Hamiltonian Applied to Superdeformed Bands in A ≈ 190 Region NUCLEAR STRUCTURE 189,191,192Hg; A ≈ 160; analyzed superdeformed bands data. Cranking Bohr-Mottelson Hamiltonian.
doi: 10.1103/PhysRevC.49.1449
1993HU06 Chin.J.Nucl.Phys. 15, No 1, 45 (1993) Spin Determination of Superdeformed Bands, A - 190 and A - 150 Regions NUCLEAR STRUCTURE 190,191,192,193,194Hg, 193,194Tl, 194,196,198Pb, 146,147,148,149,150Gd, 150,151Tb, 151,152,153Dy; analyzed level spectra, Eγ; deduced superdeformed band states spin. Different methods.
1993HU09 Phys.Rev. C48, 2270 (1993) Coupling between Rotational and Vibrational Motions with the Cranking Bohr-Mottelson Hamiltonian NUCLEAR STRUCTURE 234U, 232Th, 176Hf, 164Er; calculated rotational spectra; deduced mass parameters. Cranking Bohr-Mottelson Hamiltonian, rare earth nuclei also studied.
doi: 10.1103/PhysRevC.48.2270
1991CH47 Chin.J.Nucl.Phys. 13, No 4, 297 (1991) A Macroscopic Model for Fast Rotating Nuclei NUCLEAR STRUCTURE 154Sm; calculated potential energy surfaces, fission barrier vs spin, nucleon densities contours. 152Dy; calculated proton density contours. Fast rotating nuclei, macroscopic model.
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