NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = C.W.Ma Found 81 matches. 2023MA48 Phys.Rev. C 108, 044606 (2023) C.-W.Ma, X.-X.Chen, X.-B.Wei, D.Peng, H.-L.Wei, Y.-T.Wang, J.Pu, K.-X.Cheng, Y.-F.Guo, C.-Y.Qiao Systematic behavior of fragments in Bayesian neural network models for projectile fragmentation reactions
doi: 10.1103/PhysRevC.108.044606
2023WA08 Phys.Rev. C 107, L041601 (2023) Y.Wang, F.Guan, X.Diao, M.Wan, Y.Qin, Z.Qin, Q.Wu, D.Guo, D.Si, S.Xiao, B.Zhang, Y.Zhang, B.Tian, X.Wei, H.Yang, P.Ma, R.J.Hu, L.Duan, F.Duan, Q.Hu, J.Ma, S.Xu, Z.Bai, Y.Yang, J.Wang, W.Liu, W.Su, X.Wei, C.-W.Ma, X.Li, H.Wang, F.Wang, Y.Zhang, M.Warda, A.Dobrowolski, B.Nerlo-Pomorska, K.Pomorski, L.Ou, Z.Xiao Observing the ping-pong modality of the isospin degree of freedom in cluster emission from heavy-ion reactions NUCLEAR REACTIONS 208Pb(86Kr, X), E=25 MeV/nucleon; measured reaction products, A=3 isobars in coincidence with the intermediate mass fragments of A=6-11; deduced velocity spectra of 3H and 3He, yields ratios of 3H/3He correlate reversely to the neutron-to-proton ratio N/Z of the intermediate mass fragments. Comparison with ImQMD transport model. Yield ratio 3H/3He exhibits evident anticorrelation with the N/Z of the latter, suggesting the ping-pong modality of the N/Z of the emitted particles. Anti-correlation shows dependence on the slope of the symmetry energy at saturation density. Compact Spectrometer for Heavy IoN Experiment (CSHINE) at the final focal plane of the Radioactive Ion Beam Line at Lanzhou (RIBLL-I).
doi: 10.1103/PhysRevC.107.L041601
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
2022MA39 Chin.Phys.C 46, 074104 (2022) C.-W.Ma, X.-B.Wei, X.-X.Chen, D.Peng, Y.-T.Wang, J.Pu, K.-X.Cheng, Y.-F.Guo, H.-L.Wei Precise machine learning models for fragment production in projectile fragmentation reactions using Bayesian neural networks
doi: 10.1088/1674-1137/ac5efb
2022PE09 J.Phys.(London) G49, 085102 (2022) D.Peng, H.-L.Wei, X.-X.Chen, X.-B.Wei, Y.-T.Wang, J.Pu, K.-X.Cheng, C.-W.Ma Bayesian evaluation of residual production cross sections in proton-induced nuclear spallation reactions NUCLEAR REACTIONS 1H(36Ar, X), (40Ar, X), (40Ca, X), (56Fe, X), (93Nb, X), (93Zr, X), (107Pd, X), (90Sr, X), (136Xe, X), (137Cs, X), (138Ba, X), (197Au, X), E<2.6 GeV/nucleon; analyzed available data; deduced accurate and complete energy-dependent residual σ using a simplified EPAX formula (sEPAX), the Bayesian neural network (BNN) technique.
doi: 10.1088/1361-6471/ac7069
2022ZH15 Phys.Rev. C 105, 034611 (2022) X.Zhang, X.Liu, Y.Huang, W.Lin, H.Zheng, R.Wada, A.Bonasera, Z.Chen, L.Chen, J.Han, R.Han, M.Huang, Q.Hu, Q.Leng, C.W.Ma, G.Qu, P.Ren, G.Tian, Z.Xu, Z.Yang, L.Zhang Determining impact parameters of heavy-ion collisions at low-intermediate incident energies using deep learning with convolutional neural networks NUCLEAR REACTIONS 124Sn(124Sn, X), E=50, 70, 100 MeV/nucleon; calculated absolute transverse and longitudinal momentum per nucleon of all possible charged particles in exit channel with constrained molecular dynamics (CoMD) model, impact parameter values by convolutional neural network (CNN). Events generated by CoMD are used as input for CNN training. Comparison to impact parameter values obtained using the conventional methods with the impact-parameter sensitive observables.
doi: 10.1103/PhysRevC.105.034611
2021HU24 Phys.Rev. C 104, 044611 (2021) Y.Huang, W.Lin, H.Zheng, R.Wada, A.Bonasera, Z.Chen, J.Han, R.Han, M.Huang, K.Hagel, T.Keutgen, X.Liu, Y.G.Ma, C.W.Ma, Z.Majka, G.Qu, L.Qin, P.Ren, G.Tian, J.Wang, Z.Yang, J.B.Natowitz Experimental investigation of abnormal transverse flow enhancement of α particles in heavy-ion collisions NUCLEAR REACTIONS 27Al, 48Ti, 58Ni(40Ar, X), E=47 MeV/nucleon from Texas A and M K500 cyclotron facility; measured reaction products, σ(θ) using 4π array NIMROD-ISiS, consisting of a charged particle array and Neutron Ball; deduced normalized charged particle multiplicity distributions, reduced impact parameters, average in-plane fragment transverse momentum for Z=1-5 fragments as function of rapidity, flow as a function of atomic number, two-particle azimuthal correlation functions, relative flow magnitude as function of atomic number, monotonically increasing trend as a function of fragment charge number, evidences for the non-existence of the abnormal α flow behavior in the heavy-ion collisions. Comparison with improved antisymmetrized molecular dynamics model calculations with Fermi motion (AMD-FM).
doi: 10.1103/PhysRevC.104.044611
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
2021MA60 Prog.Part.Nucl.Phys. 121, 103911 (2021) C.-W.Ma, H.-L.Wei, X.-Q.Liu, J.Su, H.Zheng, W.P.Lin, Y.-X.Zhang Nuclear fragments in projectile fragmentation reactions
doi: 10.1016/j.ppnp.2021.103911
2020MA01 Chin.Phys.C 44, 014104 (2020) C.-W.Ma, D.Peng, H.-L.Wei, Z.-M.Niu, Y.-T.Wang, R.Wada Isotopic cross-sections in proton induced spallation reactions based on the Bayesian neural network method NUCLEAR REACTIONS 36,40Ar, 40Ca, 56Fe, 136Xe, 197Au, 208Pb, 238U(p, X), E=200-1500 MeV/nucleon; analyzed available data; deduced σ using the Bayesian neural network (BNN) method.
doi: 10.1088/1674-1137/44/1/014104
2020MA61 Chin.Phys.C 44, 124107 (2020) C.-W.Ma, D.Peng, H.-L.Wei, Y.-T.Wang, J.Pu A Bayesian-neural-network prediction for fragment production in proton induced spallation reaction NUCLEAR REACTIONS 36,40Ar, 40Ca, 56Fe, 136Xe, 197Au, 208Pb, 238U(p, X), E<1000 MeV/nucleon; analyzed available data; deduced fragment production in spallation reactions yields key infrastructure data, σ, parameters using the empirical SPACS parameterizations, a Bayesian-neural-network (BNN) approach.
doi: 10.1088/1674-1137/abb657
2020WA25 Phys.Rev. C 102, 024620 (2020) S.S.Wang, Y.G.Ma, X.G.Cao, D.Q.Fang, C.W.Ma Hard-photon production and its correlation with intermediate-mass fragments in a framework of a quantum molecular dynamics model NUCLEAR REACTIONS 40Ca(40Ca, X), E=60 MeV/nucleon; calculated differential σ from inclusive events with and without Pauli blocking for hard photons, separation time between direct photons and thermal photons as a function of impact parameter, production probabilities of photons and IMFs and multiplicity correlation as function of time, hard-photon (Eγ=20-130 MeV) energy spectra, temperatures as a function of incident energy. 40Ca(40Ca, X), E=40-120 MeV/nucleon; calculated multiplicities of direct and thermal photons, multiplicity of intermediate-mass fragments (IMFs), and multiplicity correlations between the direct photons or thermal photons and the IMFs as function of incident energy and centrality. 12C(14N, X), E=20, 30, 40 MeV/nucleon; calculated high-energy photon spectra and compared with experimental data. Isospin-dependent quantum molecular dynamics (IQMD) model by embedding incoherent neutron-proton bremsstrahlung photon production channel to investigate high-energy photon production and correlation with fragments.
doi: 10.1103/PhysRevC.102.024620
2020WA30 Eur.Phys.J. A 56, 254 (2020) S.S.Wang, Y.G.Ma, X.G.Cao, D.Q.Fang, C.W.Ma Azimuthal anisotropy and multiplicities of hard photons and free nucleons in intermediate-energy heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=60 MeV/nucleon; analyzed available data; calculated average density, hard photon production probability, directed flows, scale-invariant momentum vs scale-invariant rapidity using a framework of isospin-dependent quantum molecular dynamics (IQMD) model.
doi: 10.1140/epja/s10050-020-00264-z
2019WE10 Chin.Phys.C 43, 074103 (2019) H.-L.Wei, Y.-D.Song, C.-W.Ma, Z.-H.Li, J.Su Cross-section prediction for isotopes near neutron drip line in 70, 80Zn projectile fragmentation reactions NUCLEAR REACTIONS 9Be(70Zn, X)59Ca/60Ca, E=345 MeV/nucleon; analyzed available data. 66,70Ca; deduced parameters, σ for production of very neutron rich calcium nuclei.
doi: 10.1088/1674-1137/43/7/074103
2018HU04 Phys.Rev. C 97, 034909 (2018) Investigating the quark flavor dependence of the chiral magnetic effect with a multiphase transport model
doi: 10.1103/PhysRevC.97.034909
2018MA02 J.Phys.(London) G45, 015102 (2018) Mass dependence of temperature for intermediate mass fragment in heavy-ion reactions NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), E=140 MeV/nucleon; analyzed available data; deduced mass and temperature dependence in fragment distributions.
doi: 10.1088/1361-6471/aa8a24
2018MA10 Prog.Part.Nucl.Phys. 99, 120 (2018) Shannon information entropy in heavy-ion collisions
doi: 10.1016/j.ppnp.2018.01.002
2018NI02 Chin.Phys.C 42, 034102 (2018) Pairing-energy coefficients of neutron-rich fragments in spallation reactions NUCLEAR REACTIONS 208Pb, 238U, 136Xe, 56Fe(p, X), E<1 GeV/nucleon; analyzed available data; deduced the ratio of pairing-energy coefficient to temperature of neutron-rich fragments.
doi: 10.1088/1674-1137/42/3/034102
2018NI05 Phys.Rev. C 97, 034609 (2018) F.Niu, P.-H.Chen, Y.-F.Guo, C.-W.Ma, Z.-Q.Feng Effect of isospin diffusion on the production of neutron-rich nuclei in multinucleon transfer reactions NUCLEAR REACTIONS 208Pb(58Ni, X), E=256 MeV; 208Pb(64Ni, X), E=268 MeV; 198Pt(78Kr, X), E=307 MeV; 198Pt(86Kr, X), E=302 MeV; 198Pt(91Kr, X), E=294 MeV; calculated potential energy surface for 58Ni+208Pb reaction as functions of the protons and neutrons of the projectile-like and target-like fragments, yields for projectile-like Z=22-27, N=24-42 and for target-like fragments Z=79-81, 83-85, N=104-130 fragments, charge and mass distributions of fragments in multinucleon transfers (MNT) in 58Ni+208Pb and 64Ni+208Pb reactions, yields of Z=71-78, N=90-130 fragments and N=126 isotonic distributions in 78,86,91Kr+198Pt reactions. Dinuclear system model for production cross sections of neutron-rich isotopes. Comparison with available experimental data.
doi: 10.1103/PhysRevC.97.034609
2018SO08 Chin.Phys.C 42, 074102 (2018) Predictions for cross sections of light proton-rich isotopes in the 40Ca + 9Be reaction NUCLEAR REACTIONS 9Be(40Ca, X), E=140 MeV/nucleon; calculated σ for Z = 10-19; deduced empirical formula to predict σ using binding energies in AME16 evaluation.
doi: 10.1088/1674-1137/42/7/074102
2018SO17 Phys.Rev. C 98, 024620 (2018) Fragmentation binding energies and cross sections of isotopes near the proton dripline NUCLEAR REACTIONS 9Be(58Ni, X)39Ti/40Ti/41Ti/42Ti/39Sc/40V/41V/42V/43V/42Cr/43Cr/44Cr/45Cr/44Mn/45Mn/46Mn/47Mn/45Fe/46Fe/47Fe/48Fe/49Fe/47Co/48Co/49Co/50Co/51Co/48Ni/49Ni/50Ni/51Ni/52Ni/53Ni, E=140, 650 MeV/nucleon; calculated production σ(E); deduced exponential empirical correlation between the cross section σ and the average binding energies of proton-rich nuclei, the latter taken from AME-2016 evaluation. Scaling phenomenon in mirror nuclei.
doi: 10.1103/PhysRevC.98.024620
2017MA09 Phys.Rev. C 95, 024612 (2017) Scaling phenomena of isobaric yields in projectile fragmentation, spallation, and fission reactions NUCLEAR REACTIONS 9Be, 181Ta(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; 1,2H(136Xe, X), E=500 MeV/nucleon; Pb(124Xe, X), (136Xe, X), 1H(136Xe, X), (238U, X), (56Fe, X), (208Pb, X), 2H(208Pb, X), (238U, X), E=1 GeV/nucleon; analyzed experimental yields of fragments with A=10-160 produced in projectile fragmentation, spallation, and fission reactions; deduced isobaric ratio difference scaling parameter SΔ ln R21 to investigate properties of the equilibrium system at the time of fragment formation.
doi: 10.1103/PhysRevC.95.024612
2017MA70 J.Phys.(London) G44, 125101 (2017) An empirical formula for isotopic yield in Fe + p spallation reactions NUCLEAR REACTIONS 56Fe(p, X)23Na/24Na/25Na/26Na/35Cl/36Cl/37Cl/38Cl/45V/46V/52V/53V, E=300, 500, 750, 1000, 1500 MeV; measured reaction fragments; deduced σ and formula.
doi: 10.1088/1361-6471/aa90e6
2017NI17 Phys.Rev. C 96, 064622 (2017) F.Niu, P.-H.Chen, Y.-F.Guo, C.-W.Ma, Z.-Q.Feng Multinucleon transfer dynamics in heavy-ion collisions near Coulomb-barrier energies NUCLEAR REACTIONS 124Sn(48Ca, X), (40Ca, X), E(cm)/VC=1.12; 232Th(40Ca, X), (40Ar, X), (58Ni, X), E(cm)/VC=1; 248Cm(40Ca, X), (40Ar, X), (58Ni, X), E(cm)/VC=1, 1.02, 1.11; calculated σ for projectile-like (PLF) and target-like fragment (TLF) production. 248Cm(58Ni, X), E(cm)/VC=0.90, 1.01, 1.20; calculated σ for target-like fragment (TLF) production. Multistep model based on dinuclear system (DNS) concept for multinucleon transfer reactions near the Coulomb barrier energies.
doi: 10.1103/PhysRevC.96.064622
2017WA15 Phys.Rev. C 95, 054615 (2017) S.S.Wang, Y.G.Ma, X.G.Cao, W.B.He, H.Y.Kong, C.W.Ma Investigation of giant dipole resonances in heavy deformed nuclei with an extended quantum molecular dynamics model NUCLEAR STRUCTURE 130,132,134,142,144,146,148,150Nd, 134,136,138,144,148,150,152,154Sm; calculated β2, energies, dipole strengths, spectra of giant dipole resonances (GDR), dependence of GDR spectra on symmetry energy coefficient for 150Nd. Deformation evolution of giant dipole resonance. Extended quantum molecular dynamics model. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.054615
2017YU05 Chin.Phys.C 41, 094001 (2017) M.Yu, H.-L.Wei, Y.-D.Song, C.-W.Ma Experimental determination of one- and two-neutron separation energies for neutron-rich copper isotopes NUCLEAR REACTIONS 9Be(86Kr, X)65Cu/66Cu/67Cu/68Cu/69Cu/70Cu/71Cu/72Cu/73Cu/74Cu/75Cu/76Cu, E=64 MeV/nucleon; analyzed available data; deduced the one-neutron or two-neutron separation energy of neutron-rich isotopes.
doi: 10.1088/1674-1137/41/9/094001
2016MA15 J.Phys.(London) G43, 045102 (2016) C.-W.Ma, Y.-D.Song, C.-Y.Qiao, S.-S.Wang, H.-L.Wei, Y.-G.Ma, X.-G.Cao A scaling phenomenon in the difference of Shannon information uncertainty of fragments in heavy-ion collisions NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; analyzed available data using Shannon's information-entropy uncertainty; calculated scaling phenomenon in the manner of canonical ensemble theory. Antisymmetric molecular dynamics (AMD) and AMD + GEMINI models.
doi: 10.1088/0954-3899/43/4/045102
2016MA51 Phys.Rev. C 94, 024615 (2016) C.-W.Ma, F.Niu, C.-Y.Qiao, Y.-F.Niu, T.-Z.Yan Pairing energy of fragments produced in intermediate-energy heavy-ion collisions NUCLEAR REACTIONS 9Be, 181Ta(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; analyzed experimental data for isobaric yield ratios to obtain ratio of the pairing-energy coefficient for fragments to the temperature. AMD+GEMINI models in the framework of modified Fisher model (MFM).
doi: 10.1103/PhysRevC.94.024615
2015MA04 Phys.Rev. C 91, 014615 (2015) C.-W.Ma, Y.-L.Zhang, C.-Y.Qiao, S.-S.Wang Target effects in isobaric yield ratio differences between projectile fragmentation reactions NUCLEAR REACTIONS 9Be, 181Ta(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; analyzed experimental data to investigate target effects on the isobaric yield ratios (IYR) and isobaric yield ratio differences (IBD) in different reactions. Proposed as a probe to study the difference between the neutron and proton densities of the reaction systems.
doi: 10.1103/PhysRevC.91.014615
2015MA40 Chin.Phys.Lett. 32, 072501 (2015) C.-W.Ma, Y.-L.Zhang, S.-S.Wang, C.-Y.Qiao A Model Comparison Study of Fragment Production in 140 A MeV 58, 64Ni+9Be Reactions NUCLEAR REACTIONS 9Be(58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated σ for fragments production using the AMD and AMD+GEMINI models. Comparison with available data.
doi: 10.1088/0256-307X/32/7/072501
2015MA64 Phys.Rev. C 92, 064601 (2015) C.-W.Ma, T.-T.Ding, C.-Y.Qiao, X.-G.Cao Improved thermometer for intermediate-mass fragments in heavy-ion collisions with isobaric yield ratio difference NUCLEAR REACTIONS 9Be, 181Ta(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; Pb(124Xe, X), (136Xe, X), E=1 GeV/nucleon; 112,124Sn(112Sn, X), (124Sn, X), E=1 GeV/nucleon; analyzed experimental isobaric yield ratios (IYR) for intermediate mass fragments (IMFs) using residual binding energies; deduced improved isobaric ratio thermometer (TIB) for IMFs in heavy-ion collisions.
doi: 10.1103/PhysRevC.92.064601
2015QI06 Phys.Rev. C 92, 014612 (2015) C.Y.Qiao, H.L.Wei, C.W.Ma, Y.L.Zhang, S.S.Wang Isobaric yield ratio difference between the 140 A MeV 58Ni + 9Be and 64Ni + 9Be reactions studied by the antisymmetric molecular dynamics model NUCLEAR REACTIONS 58,64Ni(9Be, X), E=140 MeV/nucleon; calculated cross-sectional distributions of fragments, and isobaric yield ratios (IYRs) for large-A, N-Z=0-3 fragments. Isobaric yield ratio difference (IBD) method. Antisymmetric molecular dynamics (AMD) model plus the sequential decay model GEMINI. Comparison with experimental data, and with other theoretical calculations.
doi: 10.1103/PhysRevC.92.014612
2014MA31 Phys.Rev. C 89, 057602 (2014) C.W.Ma, J.Yu, X.M.Bai, Y.L.Zhang, H.L.Wei, S.S.Wang Isobaric yield ratio difference and neutron density difference in calcium isotopes NUCLEAR REACTIONS 40Ca(38Ca, X), (42Ca, X), (44Ca, X), (46Ca, X), (48Ca, X), (50Ca, X), (52Ca, X), E=80 MeV/nucleon; 9Be(40Ca, X), (48Ca, X), E=140 MeV/nucleon; calculated isobaric yield ratio difference, ratio of chemical potential difference between neutrons and protons to temperature (IB-(Δμ21/T)) for prefragments and final fragments. Modified statistical abrasion-ablation (SAA) model, assuming Fermi type neutron density distribution. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.057602
2014MA75 Eur.Phys.J. A 50, 139 (2014) C.-W.Ma, X.-M.Bai, J.Yu, H.-L.Wei Neutron density distributions of neutron-rich nuclei studied with the isobaric yield ratio difference
doi: 10.1140/epja/i2014-14139-1
2014MA78 Chin.Phys.C 38, 104101 (2014) C.-W.Ma, R.-Y.Jing, X.Feng, X.-G.Cao, C.J.Lu, H.-W.Wang Investigation of neutron induced reactions on 23Na by using Talys1.4 NUCLEAR REACTIONS 23Na(n, n), (n, 2n), (n, X), (n, γ), (n, np), 22Na(n, X), E<40 MeV; calculated σ, yields. Talys-1.4 nuclear model code, comparison with experimental data.
doi: 10.1088/1674-1137/38/10/104101
2013MA07 Chin.Phys.C 37, 024102 (2013) C.-W.Ma, H.-L.Song, J.Pu, T.-L.Zhang, S.Zhang, S.-S.Wang Symmetry energy from neutron-rich fragments in heavy-ion collisions, and its dependence on incident energy, and impact parameters NUCLEAR REACTIONS 12C(60Ni, X), E=80, 140 MeV/nucleon; calculated fragments yield, σ, isobaric yield ratios. Comparison with available data.
doi: 10.1088/1674-1137/37/2/024102
2013MA24 Phys.Rev. C 87, 034618 (2013) C.-W.Ma, S.-S.Wang, Y.-L.Zhang, H.-L.Wei Isobaric yield ratio difference in heavy-ion collisions, and comparison to isoscaling NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; analyzed isotopic (Z=6-19) and isotonic (N=8-21) yield ratio, IB-Δμ/Temp and IS-Δμ/Temp distributions. Isobaric yield ratio difference (IBD) method in heavy-ion collisions.
doi: 10.1103/PhysRevC.87.034618
2013MA56 Phys.Rev. C 88, 014609 (2013) C.-W.Ma, X.-L.Zhao, J.Pu, S.-S.Wang, C.-Y.Qiao, X.Feng, R.Wada, Y.-G.Ma Temperature determined by isobaric yield ratios in a grand-canonical ensemble theory
doi: 10.1103/PhysRevC.88.014609
2013MA75 Phys.Rev. C 88, 044612 (2013) Neutron-skin effects in isobaric yield ratios for mirror nuclei in a statistical abrasion-ablation model NUCLEAR REACTIONS 9Be(36Ca, X), (40Ca, X), (44Ca, X), (48Ca, X), (56Ca, X), (45Si, X), (45S, X), (45Ar, X), (45Ca, X), (45Ti, X), (45Cr, X), (24F, X), (30F, X), (25Na, X), (40Mg, X), (34Al, X), (35P, X), (50S, X), (44Cl, X), (60K, X), (54Sc, X), (70Ti, X), (64Mn, X), (80Fe, X), (65Cu, X), (74Cu, X), (85As, X), (85Sr, X), E=140 MeV/nucleon; calculated isobaric yield ratios for mirror nuclei (IYR-m) as function of impact parameter, dependence on neutron-skin thickness of projectile, projectile isospin dependence. Neutron skin effects. Modified statistical abrasion-ablation model.
doi: 10.1103/PhysRevC.88.044612
2013MA79 J.Phys.(London) G40, 125106 (2013) C.-W.Ma, S.-S.Wang, Y.-L.Zhang, H.-L.Wei Chemical properties of colliding sources in 124, 136Xe and 112, 124Sn induced collisions in isobaric yield ratio difference and isoscaling method NUCLEAR REACTIONS 124Sn(124Sn, X), 112Sn(112Sn, X), Pb(124Xe, X), (136Xe, X), E=1 GeV/nucleon; calculated isocaling phenomena and parameters between fragments, isoscaling and isobaric yield ratio difference. Comparison with available data.
doi: 10.1088/0954-3899/40/12/125106
2013PU01 Phys.Rev. C 87, 047603 (2013) J.Pu, J.H.Chen, S.Kumar, Y.G.Ma, C.W.Ma, G.Q.Zhang Influence of the symmetry energy on isospin ratios from projectile and target fragmentations in intermediate-energy heavy-ion collisions NUCLEAR REACTIONS 58,64Ni(40Ca, X), (48Ca, X), E=50, 600 MeV/nucleon; calculated single and double ratios of neutrons to protons as a function of kinetic energy, sensitivity factor of the symmetry energy. Isospin-dependent quantum molecular dynamics (IQMD) model.
doi: 10.1103/PhysRevC.87.047603
2012MA17 Chin.Phys.Lett. 29, 062101 (2012) C.-W.Ma, J.Pu, S.-S.Wang, H.-L.Wei The Symmetry Energy from the Neutron-Rich Nucleus Produced in the Intermediate-Energy 40, 48Ca and 58, 64Ni Projectile Fragmentation NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated isobaric yield ratios, production of neutron-rich isobars. Modified Fisher model.
doi: 10.1088/0256-307X/29/6/062101
2012MA28 Eur.Phys.J. A 48, 78 (2012) C.-W.Ma, J.Pu, H.-L.Wei, S.-S.Wang, H.-Li.Song, S.Zhang, L.Chen Symmetry energy extracted from fragments in relativistic energy heavy-ion collisions induced by 124, 136Xe NUCLEAR REACTIONS Pb(124Xe, X), E=1 GeV/nucleon;H, Pb(136Xe, X), E=1 GeV/nucleon; calculated, analyzed fragment yields; deduced symmetry energy coefficient vs mass for different isospin.
doi: 10.1140/epja/i2012-12078-5
2012MA38 Chin.Phys.Lett. 29, 092101 (2012) C.-W.Ma, J.-B.Yang, M.Yu, J.Pu, S.-S.Wang, H.-L.Wei Surface and Volume Symmetry Energy Coefficients of a Neutron-Rich Nucleus
doi: 10.1088/0256-307X/29/9/092101
2012MA52 Phys.Rev. C 86, 054611 (2012) C.W.Ma, J.Pu, Y.G.Ma, R.Wada, S.S.Wang Temperature determined by isobaric yield ratios in heavy-ion collisions NUCLEAR REACTIONS 9Be(64Ni, X), E=140 MeV/nucleon; 208Pb(136Xe, X), E=1 GeV/nucleon; analyzed σ, temperature (T) of fragments, and ratio of difference between the chemical potential of neutron and proton and temperature in heavy ion collisions using isobaric yield ratio (IYR) method. Modified statistical abrasion-ablation (SAA) model.
doi: 10.1103/PhysRevC.86.054611
2011FU11 Phys.Rev. C 84, 037603 (2011) Y.Fu, D.Q.Fang, Y.G.Ma, X.Z.Cai, W.D.Tian, H.W.Wang, W.Guo, G.H.Liu, C.W.Ma, R.R.Fan, F.Fu, H.Gao, Q.Gao, W.T.Guo, J.L.Han, Z.G.Hu, T.H.Huang, F.Jia, B.Li, X.G.Lei, Z.Y.Sun, M.Wang, J.S.Wang, Z.G.Xiao, Z.G.Xu, X.W.Yao, H.B.Zhang, X.H.Zhang, C.Zheng, H.S.Xu, G.Q.Xiao, W.L.Zhan Measurement of the longitudinal momentum distribution of 30S after one-proton removal from 31Cl NUCLEAR REACTIONS 12C(31Cl, 30S), E=44 MeV/nucleon; measured particle, spectra, TOF at RIBLL facility. 30S; deduced longitudinal fragment momentum distribution. 31Cl; calculated proton density distributions; deduced configuration of valence proton Few-body Glauber model analysis.
doi: 10.1103/PhysRevC.84.037603
2011MA41 Phys.Rev. C 83, 064620 (2011) C.-W.Ma, F.Wang, Y.-G.Ma, C.Jin Isobaric yield ratios in heavy-ion reactions, and symmetry energy of neutron-rich nuclei at intermediate energies NUCLEAR REACTIONS 9Be(48Ca, X), (64Ni, X), E=140 MeV/nucleon; calculated isobaric yield ratios of the fragments using a modified Fisher model. Correlations between the isobaric yield ratios and the energy coefficients in the Weiszacker-Bethe semiclassical mass formula.
doi: 10.1103/PhysRevC.83.064620
2011MA61 Chin.Phys.C 35, 1017 (2011) Isospin dependence of projectile fragmentation and neutron-skin thickness of neutron-rich nuclei NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), E=140 MeV/nucleon; Pb(124Xe, X), (136Xe, X), E=1 GeV/nucleon; measured reaction products; deduced fragments σ. Comparison with statistical abrasion-ablation model calculations.
doi: 10.1088/1674-1137/35/11/007
2010MA01 J.Phys.(London) G37, 015104 (2010) C.-W.Ma, H.-L.Wei, G.-J.Liu, J.-Y.Wang Systematic behavior in the isospin dependence of projectile fragmentation of mirror nuclei with A = 20-60 NUCLEAR REACTIONS 12C(20Mg, X), (20O, X), (24Si, X), (24Ar, X), (36Ca, X), (36S, X), (40Ti, X), (40Ar, X), (44Ca, X), (44Cr, X), (60Ni, X), (60Ge, X), E=80 MeV/nucleon; calculated fragment cross section distribution; deduced isospin dependence of projectile fragmentation.
doi: 10.1088/0954-3899/37/1/015104
2010MA47 Nucl.Phys. A834, 581c (2010) C.-W.Ma, H.-L.Wei, H.-Y.Wang, W.-F.Li, Y.-Q.Li The isospin dependence of the projectile fragmentation of mirror nuclei at intermediate energy NUCLEAR REACTIONS 12C(20O, X)Be/B/C/N/O, (20Mg, X)Be/B/C/N/O, E=80 MeV/nucleon; measured isotope yields; deduced σ. 12C(60Ni, X)N/Ne/Al/S/K/Ti/Mn/Ni, (60Ge, X)N/Ne/Al/S/K/Ti/Mn/Ni, E=80 MeV/nucleon; measured isotope yields; deduced σ; analyzed effect of mirror nuclei systems using statistical abrasion-ablation model.
doi: 10.1016/j.nuclphysa.2010.01.097
2010MA63 Phys.Rev. C 82, 057602 (2010) Reexamination of the neutron skin thickness using neutron removal cross sections NUCLEAR REACTIONS 12C(44Ca, X), (46Ca, X), (48Ca, X), (50Ca, X), (52Ca, X), E=1 GeV/nucleon; calculated σ as function of fragment mass and charge, correlations between σ for different fragment isotopes and corresponding S(n) values for finite neutron-rich nuclei. Statistical abrasion-ablation model.
doi: 10.1103/PhysRevC.82.057602
2010TI03 Int.J.Mod.Phys. E19, 1076 (2010) W.D.Tian, H.W.Wang, Y.G.Ma, G.H.Liu, C.W.Ma, Q.M.Su, T.Z.Yan, Y.Shi, X.Z.Cai, D.Q.Fang, J.G.Chen, W.Guo, K.Wang, H.S.Xu, Z.G.Hu, Z.G.Xiao, Z.Y.Sun, Z.Y.Guo, G.Q.Xiao, X.G.Lei, B.Li, X.H.Yuan, H.B.Zhang, X.W.Yao, W.T.Guo, X.H.Zhang, Q.Gao, C.Zheng, H.Gao, Z.G.Xu, F.Fu, J.L.Han, R.R.Fan Projectile fragmentation of 36, 40Ar induced reactions NUCLEAR REACTIONS 64Ni(36Ar, X), (40Ar, X), E=50 MeV/nucleon; measured reaction products; deduced fragment yields, σ(θ), isoscaling parameters. Comparison with empirical models.
doi: 10.1142/S0218301310015515
2010TI05 Int.J.Mod.Phys. E19, 1815 (2010) W.D.Tian, Y.G.Ma, H.W.Wang, G.H.Liu, C.W.Ma, Q.M.Su, T.Z.Yan, X.Z.Cai, D.Q.Fang, J.G.Chen, W.Guo, Y.Shi, K.Wang, H.S.Xu, Z.G.Hu, Z.G.Xiao, Z.Y.Sun, Z.Y.Guo, G.Q.Xiao, X.G.Lei, B.Li, X.H.Yuan, H.B.Zhang, X.W.Yao, W.T.Guo, X.H.Zhang, Q.Gao, C.Zheng, H.Gao, Z.G.Xu, F.Fu, J.L.Han, R.R.Fan Projectile fragmentation of 36-40Ar induced reactions NUCLEAR REACTIONS 64Ni(36Ar, X), (40Ar, X), E=50 MeV/nucleon; measured reaction products; deduced fragment yields, σ. Comparison with EPAX and SAA models.
doi: 10.1142/S0218301310016247
2009FU19 Chin.Phys.C 33, Supplement 1, 126 (2009) Y.Fu, D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, W.Guo, C.-W.Ma, W.-D.Tian, H.-W.Wang, K.Wang Isoscaling behavior studied by HIPSE model NUCLEAR REACTIONS 9Be(58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated isotopic distribution, yield ratios; deduced HIPSE parameters dependence of isoscaling parameters. Heavy-ion phase-space exploration (HIPSE) model.
doi: 10.1088/1674-1137/33/S1/040
2009MA13 Phys.Rev. C 79, 034606 (2009) C.-W.Ma, H.-L.Wei, J.-Y.Wang, G.-J.Liu, D.-Q.Fang, W.-D.Tian, X.-Z.Cai, H.-W.Wang, Y.-G.Ma Isospin dependence of projectile-like fragment production at intermediate energies NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; calculated σ. Discussed isospin dependence of projectile fragmentation, shapes of fragment isotopic and isotonic distributions of different asymmetric projectiles. Statistical abration-ablation model. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.034606
2008MA13 Chinese Physics B 17, 1216 (2008) C.-W.Ma, Y.Fu, D.-Q.Fang, Y.-G.Ma, X.-Z.Cai, W.Guo, W.-D.Tian, H.-W.Wang A possible experimental observable for the determination of neutron skin thickness
doi: 10.1088/1674-1056/17/4/011
2008MA47 Int.J.Mod.Phys. E17, 1669 (2008) C.W.Ma, Y.Fu, D.Q.Fang, Y.G.Ma, X.Z.Cai, W.D.Tian, K.Wang, C.Zhong Isospin effect and isoscaling phenomenon in projectile fragmentation
doi: 10.1142/S0218301308010684
2008TI10 Int.J.Mod.Phys. E17, 1705 (2008) W.D.Tian, Y.G.Ma, X.Z.Cai, D.Q.Fang, W.Guo, C.W.Ma, G.H.Liu, W.Q.Shen, Y.Shi, H.W.Wang, K.Wang, T.Z.Yan Dynamical and sequential decay effects on isoscaling and density dependence of the symmetry energy
doi: 10.1142/S0218301308010714
2007FA14 J.Phys.(London) G34, 2173 (2007) D.Q.Fang, Y.G.Ma, C.Zhong, C.W.Ma, X.Z.Cai, J.G.Chen, W.Guo, Q.M.Su, W.D.Tian, K.Wang, T.Z.Yan, W.Q.Shen Systematic study of isoscaling behavior in projectile fragmentation by the statistical abrasion-ablation model NUCLEAR REACTIONS 27Al(86Kr, X), E=44 MeV/nucleon; 27Al(129Xe, X), E=790 MeV/nucleon; 112Sn(112Sn, X), (124Sn, X), E=60 MeV/nucleon; calculated calculated fragment yields and isotopic distributions using a modified statistical abrasion-ablation model. Compared results to available data.
doi: 10.1088/0954-3899/34/10/007
2007FA16 Phys.Rev. C 76, 031601 (2007) D.Q.Fang, W.Guo, C.W.Ma, K.Wang, T.Z.Yan, Y.G.Ma, X.Z.Cai, W.Q.Shen, Z.Z.Ren, Z.Y.Sun, J.G.Chen, W.D.Tian, C.Zhong, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, A.Ozawa, T.Suda, K.Sugawara, T.Suzuki, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata Examining the exotic structure of the proton-rich nucleus 23Al NUCLEAR REACTIONS 12C(23Al, p), E=74 MeV/nucleon; measured fragment longitudinal momentum distributions. 12C(23Al, X), (24Al, X), (24Al, X), E=74 MeV/nucleon; measured reaction cross sections. Compared results to model calculations.
doi: 10.1103/PhysRevC.76.031601
2007MA53 Nucl.Phys. A790, 299c (2007) Y.G.Ma, X.Z.Cai, J.G.Chen, D.Q.Fang, W.Guo, G.H.Liu, C.W.Ma, E.J.Ma, W.Q.Shen, Y.Shi, Q.M.Su, W.D.Tian, H.W.Wang, K.Wang, Y.B.Wei, T.Z.Yan Nucleon-nucleon momentum correlation function for light nuclei NUCLEAR STRUCTURE 11Li; calculated binding energies, neutron-neutron correlation functions. 6,7,8,9,11Li, 13,14,15,16,17,18,19C, 14,15,16,17N; calculated binding energies, proton-neutron correlation functions. 27,28,29,30S; calculated binding energies, proton-proton correlation functions. Isospin-dependent quantum molecular dynamics.
doi: 10.1016/j.nuclphysa.2007.03.146
2007MA56 Nucl.Phys. A787, 611c (2007) Y.G.Ma, T.Z.Yan, X.Z.Cai, J.G.Chen, D.Q.Fang, W.Guo, G.H.Liu, C.W.Ma, E.J.Ma, W.Q.Shen, Y.Shi, Q.M.Su, W.D.Tian, H.W.Wang, K.Wang Scaling of anisotropy flows in intermediate energy heavy ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), 58Ni, 124Sn(86Kr, X), E=25 MeV/nucleon; calculated directed flow vs rapidity, elliptic flow and 4th momentum anisotropy vs transverse momentum. Quantum molecular dynamics model. Nucleonic coalescence and reaction mechanism features discussed.
doi: 10.1016/j.nuclphysa.2006.12.091
2007TI01 Chin.Phys.Lett. 24, 385 (2007) W.-D.Tian, Yu.-G.Ma, X.-Z.Cai, D.-Q.Fang, W.Guo, C.-W.Ma, G.-H.Liu, W.-Q.Shen, Yu.Shi, Q.-M.Su, H.-W.Wang, K.Wang, T.-Z.Yan Isoscaling in Statistical Sequential Decay Model NUCLEAR STRUCTURE 150,168Re; calculated isotope yield ratios, isoscaling parameters from decay of excited nuclides. Sequential decay model.
doi: 10.1088/0256-307X/24/2/023
2006GU28 Int.J.Mod.Phys. E15, 1523 (2006) W.Guo, D.Q.Fang, Y.G.Ma, C.W.Ma, K.Wang, T.Z.Yan, X.Z.Cai, W.Q.Shen, Z.Y.Sun, Z.Z.Ren, J.G.Chen, J.H.Chen, G.H.Liu, E.J.Ma, G.L.Ma, Y.Shi, Q.M.Su, W.D.Tian, H.W.Wang, C.Zhong, J.X.Zuo, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, A.Ozawa, T.Suda, K.Sugawara, T.Suzuki, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata Measurements of reaction cross section and fragment momentum distribution for N=10 proton-rich isotones NUCLEAR REACTIONS 12C(23Al, 22MgX), (24Al, 23MgX), (22Mg, 21NaX), (21Na, 20NeX), E not given; measured fragment parallel momentum distribution following one-proton removal. 12C(23Al, X), (24Al, X), E not given; measured reaction σ.
doi: 10.1142/S0218301306005101
2006MA05 Phys.Rev. C 73, 014604 (2006) Y.G.Ma, Y.B.Wei, W.Q.Shen, X.Z.Cai, J.G.Chen, J.H.Chen, D.Q.Fang, W.Guo, C.W.Ma, G.L.Ma, Q.M.Su, W.D.Tian, K.Wang, T.Z.Yan, C.Zhong, J.X.Zuo Surveying the nucleon-nucleon momentum correlation function in the framework of quantum molecular dynamics model NUCLEAR REACTIONS 12C(13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), E=800 MeV/nucleon; 12C(18C, X), E=100 MeV/nucleon; calculated two-nucleon momentum correlation functions. Isospin-dependent quantum molecular dynamics model.
doi: 10.1103/PhysRevC.73.014604
2006MA62 Chin.Phys.Lett. 23, 2695 (2006) E.-J.Ma, Yu.-G.Ma, J.-G.Chen, X.-Z.Cai, D.-Q.Fang, W.Guo, G.-H.Liu, C.-W.Ma, W.-Q.Shen, Yu.Shi, Q.-M.Su, W.-D.Tian, H.W.Wang, K.Wang, T.-Z.Yan Cross Sections of Elastic Electron and Positron Scattering from Proton-Rich Nuclei NUCLEAR REACTIONS 12C, 208Pb(e, e), (e+, e+), E=450 MeV; 12C, 16O(e, e), (e+, e+), E=374.5, 750 MeV; 28,32S(e, e), (e+, e+), E=250, 500 MeV; calculated σ(θ). Relativistic partial-wave expansion method, comparison with data.
doi: 10.1088/0256-307X/23/10/020
2006MA96 High Energy Phys. and Nucl.Phys. (China), Supplement 2, 30, 186 (2006) C.-W.Ma, D.-Q.Fang, W.Guo, K.Wang, T.-Z.Yan, Y.-G.Ma, X.-Z.Cai, W.-Q.Shen, Z.-Y.Sun, Z.-Z.Ren, J.-G.Chen, W.-D.Tian, H.-W.Wang, E.-J.Ma, G.-H.Liu, Y.Shi, Q.-M.Su, C.Zhong, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, T.Suda, K.Sugawara, T.Suzuki, A.Ozawa, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata Study of Exoticness of Proton-Rich Nuclei 23Al and it's Neighboring Nuclei
2006SU22 Int.J.Mod.Phys. E15, 1803 (2006) Q.M.Su, D.Q.Fang, Y.G.Ma, C.Zhong, C.W.Ma, K.Wang, T.Z.Yan, X.Z.Cai, W.Q.Shen Study of isoscaling phenomena for projectile-like fragments NUCLEAR REACTIONS 112Sn(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), (78Kr, X), (86Kr, X), (112Sn, X), (124Sn, X), (129Xe, X), (136Xe, X), E=60 MeV/nucleon; calculated fragment yields; deduced isoscaling parameters. Statistical abrasion-ablation model.
doi: 10.1142/S021830130600537X
2006YA09 Phys.Lett. B 638, 50 (2006) T.Z.Yan, Y.G.Ma, X.Z.Cai, J.G.Chen, D.Q.Fang, W.Guo, C.W.Ma, E.J.Ma, W.Q.Shen, W.D.Tian, K.Wang Scaling of anisotropic flow and momentum-space densities for light particles in intermediate energy heavy ion collisions NUCLEAR REACTIONS 124Sn(86Kr, X), E=25 MeV/nucleon; calculated elliptic and higher order flows vs transverse momentum, related quantities. Isospin dependent quantum molecular dynamics model.
doi: 10.1016/j.physletb.2006.05.018
2005CH71 Chinese Physics 14, 2444 (2005) J.-G.Chen, X.-Z.Cai, T.-T.Wang, Yu.-G.Ma, Z.-Z.Ren, D.-Q.Fang, C.Zhong, Yi.-B.Wei, W.Guo, X.-F.Zhou, K.Wang, G.-L.Ma, W.-D.Tian, J.-H.Chen, T.-Z.Yan, J.-X.Zuo, C.-W.Ma, W.-Q.Shen Investigation on the deformation of Ne and Mg isotope chains within relativistic mean-field model NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36Ne, 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44Mg; calculated deformations, binding energies, shape coexistence features. Relativistic mean-field model, comparison with data.
doi: 10.1088/1009-1963/14/12/013
2005MA37 J.Phys.(London) G31, S1179 (2005) Y.G.Ma, G.L.Ma, X.Z.Cai, J.G.Chen, J.H.Chen, D.Q.Fang, W.Guo, Z.J.He, H.Z.Huang, J.L.Long, C.W.Ma, B.H.Sa, W.Q.Shen, Q.M.Su, K.Wang, Y.B.Wei, T.Z.Yan, C.Zhong, J.X .Zuo Δ-scaling and heat capacity in relativistic ion collisions NUCLEAR REACTIONS 1H(p, X), C(C, X), Pb(Pb, X), E=20-200 GeV/nucleon; calculated particle multiplicities, heat capacity, Δ-scaling features.
doi: 10.1088/0954-3899/31/6/082
2005MB06 Phys.Rev. C 72, 064603 (2005) Y.G.Ma, K.Wang, X.Z.Cai, J.G.Chen, J.H.Chen, D.Q.Fang, W.Guo, C.W.Ma, G.L.Ma, W.Q.Shen, Q.M.Su, W.D.Tian, Y.B.Wei, T.Z.Yan, C.Zhong, X.F.Zhou, J.X.Zuo Isoscaling behavior in fission dynamics NUCLEAR REACTIONS 112Sn(112Sn, X), 116Sn(116Sn, X), E ≈ 7-10 MeV/nucleon; calculated fission fragment isotopic yields, mean temperature; deduced isoscaling behavior. Langevin model.
doi: 10.1103/PhysRevC.72.064603
2005TI01 Chin.Phys.Lett. 22, 306 (2005) W.-D.Tian, Yu.-G.Ma, X.-Z.Cai, J.G.Chen, J.-H.Chen, D.-Q.Fang, W.Guo, C.-W.Ma, G.-L.Ma, W.-Q.Shen, K.Wang, Y.-B.Wei, T.-Z.Yan, C.Zhong, J.-X.Zuo Isoscaling Behaviour in the Isospin-Dependent Quantum Molecular Dynamics Model NUCLEAR REACTIONS 40Ca(40Ca, X), 48Ca(48Ca, X), E=25-70 MeV/nucleon; calculated fragment yield ratios, isoscaling parameters. Isospin-dependent quantum molecular dynamics.
doi: 10.1088/0256-307X/22/2/011
2004CH60 Chin.Phys.Lett. 21, 2140 (2004) J.-G.Chen, X.-Z.Cai, T.-T.Wang, Y.-G.Ma, Z.-Z.Ren, D.-Q.Fang, C.Zhong, Y.-B.Wei, W.Guo, X.-F.Zhou, K.Wang, G.-L.Ma, W.-D.Tian, J.-X.Zuo, C.-W.Ma, J.-H.Chen, T.-Z.Yan, W.-Q.Shen Investigation of Exotic Structure of the Largely Deformed Nucleus 23Al in the Relativistic-Mean-Field Model NUCLEAR STRUCTURE 23Al; calculated ground-state binding energy, quadrupole deformation, radii, one- and two-proton separation energies, excited states energies, J, π, configurations. 20Ne, 21Na, 22Mg; calculated ground-state quadrupole deformations. Deformed relativistic mean field model.
doi: 10.1088/0256-307X/21/11/018
1977MA23 Phys.Rev. C16, 1179 (1977) Microscopic Calculations of High-Spin Rotational States NUCLEAR STRUCTURE 162Er, 168Yb, 174Hf, 238U; calculated high-spin rotational states. Diagonalization cranking model using BCS, fully particle-number-projection wave functions.
doi: 10.1103/PhysRevC.16.1179
1975MA01 Phys.Rev. C11, 213 (1975) Microscopic Study of the Variable-Moment-of-Inertia Model for Rare-Earth Model NUCLEAR STRUCTURE A=152-188; calculated force constant, moment of inertia parameter.
doi: 10.1103/PhysRevC.11.213
1974MA05 Phys.Rev. C9, 1083 (1974) Exponential Dependence of the Nuclear Moment of Inertia on Pairing Correlation and the Pairing Stretch Model for Nuclear Rotation NUCLEAR STRUCTURE 162Dy, 168Er, 172Yb, 178Hf, 182W; calculated levels.
doi: 10.1103/PhysRevC.9.1083
1974TR05 Phys.Rev. C9, 2275 (1974) Two-Step Shell-Model Calculation of 208Po NUCLEAR STRUCTURE 208Po; two-step shell model, calculated levels, J, π.
doi: 10.1103/PhysRevC.9.2275
1973MA42 Phys.Rev. C8, 2313 (1973) Shell Model in the Lead Region NUCLEAR STRUCTURE 206,210Pb, 210Po, 208,210Bi, 206,208Tl, 206Hg; calculated levels, J, π, binding energies, γ-branching, γ-mixing, S.
doi: 10.1103/PhysRevC.8.2313
1971TR04 Phys.Rev. C3, 2421 (1971) W.W.True, C.W.Ma, W.T.Pinkston Negative-Parity States in Pb208 NUCLEAR STRUCTURE 208Pb; calculated levels, T(El), S, isobaric analog.
doi: 10.1103/PhysRevC.3.2421
1970MA35 Phys.Rev. C2, 798 (1970) Nuclear Rotation: Cranking-Model Calculations and their Relation to Other Treatments NUCLEAR STRUCTURE 152,154Sm, 154,156,158,160Gd, 160,162,164Dy, 164,166,168,170Er, 168,170,172,174,176Yb, 174,176,178,180Hf, 180,182,184,186W, 184,186,188Os; calculated cranking, Coriolis-antipairing corrections to rotational spectra.
doi: 10.1103/PhysRevC.2.798
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