NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Y.Ma Found 68 matches. 2023HA08 Phys.Rev. A 107, L020803 (2023) P.Hao, K.Deng, F.F.Wu, Z.Y.Ma, W.Z.Wei, W.H.Yuan, Y.B.Du, H.L.Liu, H.X.Zhang, L.R.Pang, B.Wang, J.Zhang, Z.H.Lu Precision measurement of 25Mg+-ion D1 and D2 transition frequencies ATOMIC PHYSICS 25Mg; measured frequencies; deduced precise values of doublet transition frequencies using the decoherence-assisted spectroscopy method with the full use of spontaneous emission signals to improve the detection sensitivity.
doi: 10.1103/PhysRevA.107.L020803
2019ZH39 Nucl.Phys. A990, 1 (2019) Z.Zhang, R.R.Xu, Z.Y.Ma, Z.G.Ge, Y.Tian, D.Y.Pang, X.D.Sun, Y.L.Jin, X.Tao, Y.Zhang, J.M.Wang Global α-nucleus optical model based on an Dirac Brueckner Hartree Fock approach
doi: 10.1016/j.nuclphysa.2019.06.013
2018TI06 Phys.Rev. C 97, 064615 (2018) Effects of nonlocality of nuclear potentials on direct capture reactions NUCLEAR REACTIONS 48Ca(n, γ), E=0.01-0.4 MeV; 7Li(n, γ), E=0.01-2 MeV; 12C(p, γ), E=0-1.2 MeV; calculated local and non-local potential parameters, s-wave phase shifts of target nuclides as function of incident energy, and σ(E) with the Perey-Buck-type nonlocal potentials using a potential model; deduced effects of potential nonlocality in direct radiative capture reactions. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.064615
2013YA23 Chin.Phys.C 37, 124102 (2013) Collective multipole excitations of exotic nuclei in relativistic continuum random phase approximation NUCLEAR STRUCTURE 34,40,48,60Ca, 16,28O, 100,132Sn; calculated isoscalar and isovector collective multipole excitations, strength functions. Comparison with available data.
doi: 10.1088/1674-1137/37/12/124102
2011RU13 J.Korean Phys.Soc. 59, 1729s (2011) X.C.Ruan, G.C.Chen, H.X.Huang, X.Li, Y.B.Nie, B.Zhou, Z.Y.Ma, J.Bao, Q.P.Zhong, Z.Y.Zhou, H.Q.Tang, J.S.Zhang, C.L.Lan, Y.L.Zhang, Y.M.Li Measurement of the Secondary Neutron Emission Differential and Double-Differential Cross Sections between 20 and 30 MeV NUCLEAR REACTIONS 9Be(n, n), (n, xn), E=21.65 MeV; measured In, En using TOF and BC501A; deduced σ, σ(θ), σ(E, θ); calculated TOF neutron spectra using Monte Carlo code STREUER, σ by LUNF code. Compared with other data.
doi: 10.3938/jkps.59.1729
2010MA35 Nucl.Phys. A834, 50c (2010) Density functional theory with a separable pairing force in finite nuclei NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn; calculated E2, B(E2), pairing gap using separable and Gogny D1S forces. 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm; calculated deformation using RMF+BCS, HFB, RHB (relativistic Hartree-Bogoliubov). Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.015
2010NI06 Phys.Rev. C 81, 054318 (2010) T.Niksic, P.Ring, D.Vretenar, Y.Tian, Z.-y.Ma 3D relativistic Hartree-Bogoliubov model with a separable pairing interaction: Triaxial ground-state shapes NUCLEAR STRUCTURE 134,136,138,140,142,144,146,148,150,152,154,156Sm, 190,192,194,196,198,200Pt; calculated triaxial quadrupole binding-energy contour maps, neutron and proton pairing energy maps in β-γ plane, quadrupole deformations. 192Pt; calculated proton and neutron canonical single-particle energy levels. Relativistic Hartree-Bogoliubov (RHB) model.
doi: 10.1103/PhysRevC.81.054318
2010YA20 Phys.Rev. C 82, 054305 (2010) D.Yang, L.-G.Cao, Y.Tian, Z.-Y.Ma Importance of self-consistency in relativistic continuum random-phase approximation calculations NUCLEAR STRUCTURE 40Ca, 132Sn, 208Pb; calculated inverse energy-weighted moments and strength distributions of isoscalar giant-monopole resonances (ISGMR), isovector giant-monopole resonances (IVGMR), isoscalar giant-quadrupole resonances (ISGQR), isovector giant-quadrupole resonances (IVGQR) using relativistic continuum random phase approximation (RCRPA) method.
doi: 10.1103/PhysRevC.82.054305
2010ZH11 Phys.Rev. C 81, 044319 (2010) D.-D.Zhang, Z.-Y.Ma, B.-Q.Chen, S.-F.Shen α-decay half-lives of superheavy elements with the Dirac-Brueckner-Hartree-Fock (DBHF) nucleon effective interaction RADIOACTIVITY 261,263Sg, 264,267,272Bh, 264,265,275Hs, 268Mt, 270,279,281Ds, 272Rg, 283,285Cn, 283,284Nh, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Og; calculated half-lives using microscopic NN effective interaction based on the Dirac-Brueckner-Hartree-Fock (DBHF) approach and the M3Y effective interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044319
2010ZH19 Chin.Phys.C 34, 334 (2010) D.-D.Zhang, B.-Q.Chen, Z.-Y.Ma Systematic studies on α-decay half-lives for super heavy nuclei NUCLEAR STRUCTURE Z=102-120; calculated T1/2; deduced nucleus-nucleus potential. Performed cluster model (PCM).
doi: 10.1088/1674-1137/34/3/006
2010ZO02 Chin.Phys.C 34, 56 (2010) W.-H.Zou, Y.Tian, S.-F.Shen, J.-Z.Gu, B.-B.Peng, D.-D.Zhang, Z.-Y.Ma Nuclear structure around 80Zr NUCLEAR STRUCTURE 80,82,84Zr; calculated potential energy surfaces, ground state bands. Projected shell model (PSM) and relativistic Hartee-Bogoliubov (RHB) theory.
doi: 10.1088/1674-1137/34/1/010
2010ZO03 Phys.Rev. C 82, 024309 (2010) W.-h.Zou, Y.Tian, J.-z.Gu, S.-f.Shen, J.-m.Yao, B.-b.Peng, Z.-y.Ma Microscopic description of nuclear structure around 80Zr NUCLEAR STRUCTURE 80,82,84Zr; calculated ground-state total binding energies and angular momentum projected potential energy surfaces (AMPPES) using projected shell model with a quadrupole constrained relativistic Hartree-Bogoliubov (RHB) theory and NL3 effective interaction and Gogny D1S interaction for the pairing force. Shape coexistence and shape transitions, and decay out of superdeformed rotational bands.
doi: 10.1103/PhysRevC.82.024309
2009DO20 Chin.Phys.C 33, 532 (2009) Elastic scattering of 6He from 12C at 38.3 MeV/nucleon NUCLEAR REACTIONS 12C(6He, 6He), E=38.3 MeV/nucleon; analyzed elastic scattering data within standard optical model; calculated σ(θ). Comparison with theoretical models and experimental data.
doi: 10.1088/1674-1137/33/7/006
2009TI03 Phys.Lett. B 676, 44 (2009) A finite range pairing force for density functional theory in superfluid nuclei NUCLEAR STRUCTURE Sn, Pb; calculated pairing energy and associated matrix elements using the relativistic Hartree?Bogoliubov approach.
doi: 10.1016/j.physletb.2009.04.067
2009TI04 Phys.Rev. C 79, 064301 (2009) Separable pairing force for relativistic quasiparticle random-phase approximation NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn, 122Zr, 124Mo, 126Ru, 128Pd, 130Cd, 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb; calculated energies of first 2+, first and second 3-, B(E2), proton average gap, and isoscalar giant monopole resonance (ISGMR) using Relativistic Hartree-Bogoliubov (RHB) and relativistic quasiparticle random phase approximation (RQRPA). Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064301
2009TI07 Phys.Rev. C 80, 024313 (2009) Axially deformed relativistic Hartree Bogoliubov theory with a separable pairing force NUCLEAR STRUCTURE 164Er, 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm, 240Pu; calculated binding energies, neutron and proton pairing energies using axially symmetric relativistic Hartree-Bogoliubov calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024313
2009YA02 Chin.Phys.Lett. 26, 022101 (2009) Isoscalar Giant Monopole Resonance in Relativistic Continuum Random Phase Approximation NUCLEAR STRUCTURE 120Sn, 208Pb; calculated Isoscalar Giant Monopole resonance strength in the framework of relativistic continuum random phase approximation.
doi: 10.1088/0256-307X/26/2/022101
2008CA10 Chin.Phys.Lett. 25, 1625 (2008) Symmetry Energy and Isovector Giant Dipole Resonance in Finite Nuclei NUCLEAR STRUCTURE 90Zr, 132Sn, 144Sm, 208Pb; calculated IVGDR energies as a function of symmetry energy using relativistic mean field theory.
doi: 10.1088/0256-307X/25/5/028
2008ZO03 Phys.Rev. C 78, 064613 (2008) Microscopic optical potential for α-nucleus elastic scattering in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 12C(α, α), E=104, 120, 145, 166, 172.5 MeV; 16O(α, α), E=48.7, 54.1, 69.5, 80.7, 104 MeV; 28Si(α, α), E=104, 166, 240 MeV; 40Ca(α, α), E=40.05, 47, 53.9, 80, 104, 141.7 MeV; calculated density dependence of optical model potentials, normalization factors, σ(θ). DBHF calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.064613
2007GR21 Phys.Rev. C 76, 044319 (2007) M.Grasso, Z.Y.Ma, E.Khan, J.Margueron, N.Van Giai Evolution of the proton sd states in neutron-rich Ca isotopes NUCLEAR STRUCTURE 48,52,70,78Ca; calculated excitation energies. Skyrme-Hartree-Fock equations used.
doi: 10.1103/PhysRevC.76.044319
2007LI26 Phys.Rev. C 75, 054320 (2007) Pygmy and giant dipole resonances in Ni isotopes NUCLEAR STRUCTURE Ni; calculated properties of the isovector giant and pigmy dipole resonances for even-even Ni isotopes within the framework of a relativistic random phase approximation built on a relativistic mean field ground state.
doi: 10.1103/PhysRevC.75.054320
2007MA02 Chin.Phys.Lett. 24, 69 (2007) Influence of D-state in 4He on S Factor for the 2H(d, γ)4He Reaction NUCLEAR REACTIONS 2H(d, γ), E(cm)=10-1000 keV; calculated astrophysical S-factors; deduced sensitivity to 4He D-state.
doi: 10.1088/0256-307X/24/1/019
2006LI30 Chin.Phys.Lett. 23, 1719 (2006) Ground-State Properties of Ca Isotopes and the Density Dependence of the Symmetry Energy NUCLEAR STRUCTURE 52,54,60,70Ca; calculated neutron and proton density distributions, radii, single-particle energies. Relativistic mean field approach.
doi: 10.1088/0256-307X/23/7/018
2006MA82 Int.J.Mod.Phys. E15, 1347 (2006) Z.-Yu.Ma, B.-Q.Chen, J.Liang, L.-G.Cao Giant resonances and asymmetry energy NUCLEAR STRUCTURE 70,72,74,76,78,80,82,84,86,88,90,92,94,96Ni; calculated GDR energies. 132Sn, 208Pb; calculated asymmetry energy, giant resonance strength. Relativistic quasiparticle RPA.
doi: 10.1142/S0218301306004934
2006RO03 Phys.Rev. C 73, 014614 (2006) Isospin-dependent optical potentials in Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 40Ca, 208Pb(p, p), E=10-200 MeV; calculated σ(θ), Ay(θ), spin-rotation functions. Relativistic microscopic optical model, comparison with data.
doi: 10.1103/PhysRevC.73.014614
2006TI10 Chin.Phys.Lett. 23, 3226 (2006) A Separable Pairing Force in Nuclear Matter
doi: 10.1088/0256-307X/23/12/029
2006ZH15 Chin.Phys.Lett. 23, 1723 (2006) H.-F.Zhang, W.Zuo, J.-Q.Li, S.Im, Z.-Yu.Ma, B.-Q.Chen Anomaly in the Charge Radii and Nuclear Structure NUCLEAR STRUCTURE A=118-150; calculated isotope shifts, radii, quadrupole deformations for Pr isotopes. 139,140,141,142Pr; calculated single-particle energy levels, proton and neutron density distributions. Relativistic mean field approach.
doi: 10.1088/0256-307X/23/7/019
2006ZH16 Chin.Phys.Lett. 23, 1734 (2006) H.-F.Zhang, J.-Q.Li, W.Zuo, B.-Q.Chen, Z.-Yu.Ma, S.Im, G.Royer Alpha Decay Half-Lives of New Superheavy Elements through Quasimolecular Shapes RADIOACTIVITY 294Og, 290,291,292,293Lv, 286,287,288,289Fl, 283,285Cn, 279Ds, 275Hs, 271Sg(α); calculated T1/2. WKB approximation, comparison with data and other models.
doi: 10.1088/0256-307X/23/7/022
2005CA15 Phys.Rev. C 71, 034305 (2005) Low-lying dipole modes in 26, 28Ne in the quasiparticle relativistic random phase approximation NUCLEAR STRUCTURE 26,28Ne; calculated isovector dipole strength distributions, resonance features. Quasiparticle relativistic RPA.
doi: 10.1103/PhysRevC.71.034305
2005CH09 Chin.Phys.Lett. 22, 302 (2005) B.-Q.Chen, Z.Yu.Ma, Z.-Y.Zhu, H.-Q.Song, Y.-L.Zhao Deformed Potential Energy of Super Heavy Element Z = 120 in a Generalized Liquid Drop Model NUCLEAR REACTIONS 244Pu(58Fe, X), 208Pb(88Sr, X), (94Sr, X), 166Dy(136Xe, X), 252Fm(50Ca, X), E not given; calculated deformed potential energies for fusion reactions. Generalized liquid drop model.
doi: 10.1088/0256-307X/22/2/010
2004CA17 Chin.Phys.Lett. 21, 810 (2004) Isoscalar Giant Resonances of 120Sn in the Quasiparticle Relativistic Random Phase Approximation NUCLEAR STRUCTURE 120Sn; calculated giant resonance response functions. Quasiparticle relativistic RPA.
doi: 10.1088/0256-307X/21/5/013
2004CA44 Eur.Phys.J. A 22, 189 (2004) Effect of resonant continuum on pairing correlations in the relativistic approach NUCLEAR STRUCTURE 68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98Ni; calculated pairing energies, binding energies, two-neutron separation energies, radii. Relativistic approach, role of resonant continuum discussed.
doi: 10.1140/epja/i2004-10029-5
2004LI19 Phys.Rev. C 69, 034326 (2004) Z.H.Liu, M.Ruan, Y.L.Zhao, H.Q.Zhang, F.Yang, Z.Y.Ma, C.J.Lin, B.Q.Chen, Y.W.Wu, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, H.S.Xu, Z.Y.Sun, J.X.Li, Z.J.Chen Evidence for enhancement of the total reaction cross sections for 27, 28P with a 28Si target and examination of possibly relevant mechanisms NUCLEAR REACTIONS Si(23Na, X), (24Mg, X), (25Mg, X), (25Al, X), (26Al, X), (26Si, X), (27Si, X), (27P, X), (28P, X), E ≈ 20-40 MeV/nucleon; measured reaction σ; deduced reaction mechanism features. Secondary beams from 36Ar fragmentation. Modified Glauber model analysis.
doi: 10.1103/PhysRevC.69.034326
2004LI57 Chin.Phys.Lett. 21, 1711 (2004) Z.-H.Liu, M.Ruan, Y.-L.Zhao, H.-Q.Zhang, F.Yang, Z.-Y.Ma, C.-J.Lin, B.-Q.Chen, Y.-W.Wu, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, H.-S.Xu, Z.-Y.Sun, J.-X.Li, Z.-Q.Chen Possible Experimental Evidence of a Moderate Proton Halo in 29S NUCLEAR REACTIONS 28Si(29Si, X), (27Si, X), (28P, X), (27P, X), E ≈ 40 MeV/nucleon; measured reaction σ. 29S deduced proton halo features. Modified Glauber theory analysis.
doi: 10.1088/0256-307X/21/9/009
2004MA44 Eur.Phys.J. A 20, 429 (2004) Z.-Y.Ma, B.-Q.Chen, N.Van Giai, T.Suzuki The Gamow-Teller resonance in finite nuclei in the relativistic random phase approximation NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated Gamow-Teller response functions, resonance energies. Relativistic RPA.
doi: 10.1140/epja/i2003-10167-2
2004MA90 Phys.Lett. B 604, 170 (2004) Z.-Y.Ma, J.Rong, B.-Q.Chen, Z.-Y.Zhu, H.-Q.Song Isospin dependence of nucleon effective mass in Dirac Brueckner-Hartree-Fock approach
doi: 10.1016/j.physletb.2004.11.004
2003CA33 Chin.Phys.Lett. 20, 1459 (2003) Isovector Giant Dipole Resonance of Stable Nuclei in a Consistent Relativistic Random-phase Approximation NUCLEAR STRUCTURE 40Ca, 90Zr, 116Sn, 208Pb; A=10-250; calculated isovector GDR energies. Relativistic RPA, comparisons with data.
doi: 10.1088/0256-307X/20/9/314
2003CH81 Chin.Phys.Lett. 20, 1936 (2003) Deformed Potential Energy of 236Db in a Generalized Liquid Drop Model NUCLEAR REACTIONS 241Am(22Ne, 4n), E not given; calculated potential barrier, shape evolution in cold fusion reaction. Generalized liquid drop model, quasi-molecular shape. NUCLEAR STRUCTURE 263Db calculated deformed potential energy. Generalized liquid drop model, quasi-molecular shape.
doi: 10.1088/0256-307X/20/11/009
2003MA26 Chin.Phys.Lett. 20, 1025 (2003) Gamow-Teller Resonance of 90Zr in a Relativistic Approach NUCLEAR STRUCTURE 90Zr; calculated Gamow-Teller resonance response function. Relativistic RPA approach.
doi: 10.1088/0256-307X/20/7/315
2003ZH03 Chin.Phys.Lett. 20, 53 (2003) Y.-L.Zhao, Z.-Y.Ma, B.-Q.Chen, W.-Q.Shen Halo Structure of Nucleus 23Al NUCLEAR REACTIONS 12C(23Al, X), E ≈ 30 MeV/nucleon; calculated reaction σ vs projectile core radius, diffuseness parameter. Glauber model, comparison with data.
doi: 10.1088/0256-307X/20/1/316
2002LI09 Chin.Phys.Lett. 19, 190 (2002) A New Decomposition Approach of Dirac Brueckner Hartree-Fock G Matrix for Asymmetric Nuclear Matter
doi: 10.1088/0256-307X/19/2/315
2002MA27 Nucl.Phys. A703, 222 (2002) Z.-Y.Ma, A.Wandelt, V.G.Nguyen, D.Vretenar, P.Ring, L.-G.Cao Collective Multipole Excitations in a Microscopic Relativistic Approach NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated giant resonance strength distributions. 208Pb; calculated transitions B(Eλ). Relativistic RPA, comparisons with data.
doi: 10.1016/S0375-9474(01)01598-6
2002MA54 Phys.Rev. C66, 024321 (2002) Effective Dirac Brueckner-Hartree-Fock method for asymmetric nuclear matter and finite nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 48,56,68Ni, 90Zr, 100,132Sn, 208Pb; calculated binding energies, radii. 16O, 40,48Ca, 48Ni; calculated spin-orbit splitting. Dirac-Brueckner-Hartree-Fock approach.
doi: 10.1103/PhysRevC.66.024321
2001CH84 Chin.Phys.Lett. 18, 1561 (2001) One Neutron Halo in a 12B Excited State NUCLEAR STRUCTURE 11,12B; calculated single-particle energies, radii, density distributions. 12B; deduced excited state halo. Relativistic mean field approach.
doi: 10.1088/0256-307X/18/12/306
2001MA30 Nucl.Phys. A686, 173 (2001) Z.-Y.Ma, V.G.Nguyen, A.Wandelt, D.Vretenar, P.Ring Isoscalar Compression Modes in Relativistic Random Phase Approximation NUCLEAR STRUCTURE 144Sm, 208Pb; calculated isoscalar giant monopole and dipole resonance features. Fully consistent relativistic RPA.
doi: 10.1016/S0375-9474(00)00523-6
2001MA43 Nucl.Phys. A687, 64c (2001) Z.-Y.Ma, V.G.Nguyen, A.Wandelt, D.Vretenar, P.Ring A Consistent Approach in Relativistic Random Phase Approximation NUCLEAR STRUCTURE 208Pb; calculated isoscalar giant monopole resonance strength distribution. Relativistic Random Phase Approximation, comparison between different interaction potentials.
doi: 10.1016/S0375-9474(01)00602-9
2001RI17 Nucl.Phys. A694, 249 (2001) P.Ring, Z.-Y.Ma, V.G.Nguyen, D.Vretenar, A.Wandelt, L.-G.Cao The Time-Dependent Relativistic Mean-Field Theory and the Random Phase Approximation NUCLEAR STRUCTURE 116Sn; calculated isoscalar giant monopole resonance strength distribution. Relativistic RPA, time-dependent relativistic mean field theory.
doi: 10.1016/S0375-9474(01)00986-1
2001TA21 Chin.Phys.Lett. 18, 1030 (2001) Y.-H.Tan, Y.-A.Luo, P.-Z.Ning, Z.-Y.Ma Static Properties of Λ-Hypernuclei NUCLEAR STRUCTURE 12C, 16O, 51V, 89Y, 139La, 208Pb; calculated hyperon single-particle energies. 12C, 16O, 40Ca, 208Pb; calculated hypernucleus binding energies, radii. Self-consistent relativistic mean-field model, comparisons with data.
doi: 10.1088/0256-307X/18/8/311
2000NG05 Trans.Bulg.Nucl.Soc. 5, 151 (2000) The Giant Monopole Resonance in Relativistic Random Phase Approximation NUCLEAR STRUCTURE 208Pb; calculated giant monopole resonance strength distributions. RPA approach.
2000ZH08 Chin.Phys.Lett. 17, 185 (2000) Y.Zhou, Z.-Y.Ma, B.-Q.Chen, J.-Q.Li Ground-State Properties of Z = 59 Nuclei in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE Z=59, A=120-198; calculated ground-state deformation, related properties. 118,119,185,186Pr; calculated levels, J, π. Relativistic mean-field model, blocking approximation method.
doi: 10.1088/0256-307X/17/3/011
1999CH15 Phys.Lett. 455B, 13 (1999) B.Q.Chen, Z.Y.Ma, F.Grummer, S.Krewald Neutron Rich Nuclei in Density Dependent Relativistic Hartree-Fock Theory with Isovector Mesons NUCLEAR STRUCTURE Ca; calculated binding energies, radii for A=30-70. 40,70Ca; calculated neutron densities; deduced Fock exchange term effects, meson contributions. Density-dependent relativistic Hartree-Fock theory.
doi: 10.1016/S0370-2693(99)00428-1
1998CH01 J.Phys.(London) G24, 97 (1998) B.Q.Chen, Z.Y.Ma, F.Grummer, S.Krewald Relativistic Mean-Field Theory Study of Proton Halos in the 2s1d Shell NUCLEAR STRUCTURE 24,25,26,27,28,29P, 26,27,28,29,30,31S; calculated one-, two-proton separation energies, density distributions; 31P, 24,25,26,27,28,30Si; calculated density distributions; deduced proton halo candidates. Relativistic mean-field theory.
doi: 10.1088/0954-3899/24/1/013
1998CH30 Acta Phys.Pol. B29, 2223 (1998) B.Q.Chen, Z.Y.Ma, F.Grummer, S.Krewald The Role of Fock Terms and Isovector Mesons in Relativistic Hartree-Fock Calculations for Neutron Rich Nuclei NUCLEAR STRUCTURE Ca; calculated binding energies, proton, neutron radii for A=30-70; deduced Fock term, vector mesons contributions.
1998CH31 Chin.Phys.Lett. 15, 636 (1998) B.-Q.Chen, Z.Y.Ma, S.Krewald, F.Grummer Contribution of Fock Term to Properties of Exotic Nuclei NUCLEAR STRUCTURE Z=40; A=30-70; calculated binding energies, proton, neutron radii. 40,70Ca; calculated neutron density distributions; deduced Fock exchange term contributions for exotic nuclei. Density-dependent relativistic Hartree-Fock theory.
doi: 10.1088/0256-307X/15/9/005
1998LE23 Phys.Rev. C58, 1551 (1998) T.-S.H.Lee, Z.-Y.Ma, B.Saghai, H.Toki Photoproduction of a Λ on 12C NUCLEAR REACTIONS 12C(γ, K+), E=0.7-1.2 GeV; calculated hypernucleus production σ(θ); deduced dependence on pγ amplitudes, possible medium effects. Comparison with data.
doi: 10.1103/PhysRevC.58.1551
1997GR31 Bull.Rus.Acad.Sci.Phys. 61, 1925 (1997) F.Grummer, B.Q.Chen, Z.Y.Ma, S.Krewald Bulk Properties of Light Deformed Nuclei Derived from a Medium-Modified Meson-Exchange Interaction NUCLEAR STRUCTURE Z=6-12; calculated radii, charge density, deformations for even-even nuclei. Medium-modified meson-exchange interaction.
1996GR21 Phys.Lett. 387B, 673 (1996) F.Grummer, B.Q.Chen, Z.Y.Ma, S.Krewald Bulk Properties of Light Deformed Nuclei Derived from a Medium-Modified Meson-Exchange Interaction NUCLEAR STRUCTURE 8,10,12,14,16,18,20,22C, 16,18,20,22,24,26,28,30,32Ne, 12,14,16,18,20,22,24,26O, 20,22,24,26,28,30,32,34,36Mg; calculated energy per nucleon, nucleon charge densities rms radii, deformations in some cases. Deformed HFB, medium modified meson exchange interaction.
doi: 10.1016/0370-2693(96)01126-4
1996MA45 Nucl.Phys. A608, 305 (1996) Z.-Y.Ma, J.Speth, S.Krewald, B.-Q.Chen, A.Reuber Hypernuclei with Meson-Exchange Hyperon-Nucleon Interactions NUCLEAR STRUCTURE A=12-208; calculated Λ hypernuclei single particle levels, other aspects. Relativistic mean field theory.
doi: 10.1016/S0375-9474(96)00169-8
1995CH68 J.Phys.(London) G21, 1759 (1995) B.Q.Chen, Z.Y.Ma, S.Krewald, F.Grummer Properties of Proton and Neutron Rich Nuclei in the Vicinity of 100Sn in Relativistic Mean Field Theory NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 78Ni, 80Zn, 82Ge, 84Se, 86Kr, 88Sr, 90Zr, 92Mo, 94Ru, 96Pd, 98Cd; calculated binding energy per nucleon, nucleon rms radii. Relativistic mean field theory, effective interactions.
doi: 10.1088/0954-3899/21/12/011
1995MA18 J.Phys.(London) G21, 79 (1995) Z.Y.Ma, D.-C.Feng, B.-Q.Chen, W.-Q.Liu Does the Longitudinal Suppression of Quasielastic Electron Scattering Exist ( Question ) NUCLEAR REACTIONS 40Ca(e, e'X), E=407.8-840.7 MeV; calculated σ(θ) vs energy transfer. Relativistic mean field, nonrelativistic quasiparticle approaches.
doi: 10.1088/0954-3899/21/1/009
1995SH19 Phys.Rev. C52, 144 (1995) Relativistic Density-Dependent Hartree-Fock Approach for Finite Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energy per nucleon, charge radii. Relativistic density-dependent Hartree-Fock approach.
doi: 10.1103/PhysRevC.52.144
1991MA10 Phys.Lett. 256B, 1 (1991) Quasiparticle Properties of Protons in 208Pb NUCLEAR STRUCTURE 208Pb; calculated charge density, proton quasiparticle properties. Quasiparticle hamiltonian, phenomenological approach, correlations.
doi: 10.1016/0370-2693(91)90207-7
1988MA55 Nucl.Phys. A490, 619 (1988) Z.-Y.Ma, P.Zhu, Y.-Q.Gu, Y.-Z.Zhuo Optical Potentials in Relativistic Meson-Nucleon Model NUCLEAR REACTIONS 12C, 16O, 40Ca, 58Ni, 90Zr, 118Sn, 208Pb(polarized p, p), E=65 MeV; calculated σ(θ), analyzing power vs θ. Relativistic microscopic optical potentials.
doi: 10.1016/0375-9474(88)90017-6
1983MA01 Nucl.Phys. A394, 60 (1983) Perturbative Derivation of Realistic Energy-Independent Optical Potentials NUCLEAR REACTIONS 40Ca(n, n), E=30.5 MeV; calculated energy independent optical potentials. Empirical potential input, perturbative method.
doi: 10.1016/0375-9474(83)90161-6
1983MA25 Nucl.Phys. A402, 275 (1983) Implicatons of a Dynamical Effective Mass on the Nuclear Shell Model NUCLEAR REACTIONS 51V(e, e'), E not given; calculated transverse form factors, M7 multipole transition contribution. Shell model, dynamical effective mass. NUCLEAR STRUCTURE 40Ca, 208Pb; calculated single particle levels, ground state mass density distributions. Shell model, dynamical effective mass.
doi: 10.1016/0375-9474(83)90499-2
1983PR05 Phys.Lett. 128B, 141 (1983) Effective Mass in Nuclei and the Level Density Parameter NUCLEAR STRUCTURE A=20-260; calculated level density parameter vs mass; deduced volume, surface, curvature coefficients. Local quasiparticle effective mass, surface effects.
doi: 10.1016/0370-2693(83)90377-5
1981MA31 Phys.Lett. 106B, 159 (1981) Z.-Y.Ma, X.-Z.Wu, J.-S.Zhang, Y.-Z.Zhuo, J.O.Rasmussen Calculation of Muon Final Probabilities after Muon-Induced Fission in a Four-State basis NUCLEAR REACTIONS, Fission 238U(μ-, F), E at rest; calculated muon orbital occupation probability vs fragment separation energy. Four basis state calculation. ATOMIC PHYSICS, Mesic-Atoms 68Zn, 80Se, 88Sr, 98Mo, 108Pd, 120Sn, 132Xe, 142Ce, 152Sm, 164Dy; calculated 1s-, 2p-state muonic binding energies.
doi: 10.1016/0370-2693(81)90898-4
1980MA38 Nucl.Phys. A348, 446 (1980) Z.Y.Ma, X.Z.Wu, G.S.Zhang, Y.C.Cho, Y.S.Wang, J.H.Chiou, S.T.Sen, F.C.Yang, J.O.Rasmussen Calculation of Muon Final-State Probabilities after Muon-Induced Fission NUCLEAR REACTIONS, Fission 238U(μ-, F), E at rest; calculated muon-fragment binding probability. Time dependent perturbation, different fission asymmetries, fragment dynamical conditions.
doi: 10.1016/0375-9474(80)90264-X
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