NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = B.Chen Found 90 matches. 2024CH14 Phys.Rev. C 109, 024909 (2024) Difference between signal and background of the chiral magnetic effect relative to spectator and participant planes in isobar collisions at √ sNN=200 GeV
doi: 10.1103/PhysRevC.109.024909
2023CH37 Phys.Rev. C 108, 014901 (2023) Bottomonium transport in p-Pb and Pb-Pb collisions at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.108.014901
2023PA32 Phys.Rev. C 108, 034903 (2023) C.Pan, S.Zheng, M.Yang, Z.Liu, B.Chen Nonthermal distributions of charmed hadrons in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.108.034903
2023YA16 Phys.Rev. C 107, 054917 (2023) M.Yang, S.Zheng, B.Tong, J.Zhao, W.Ouyang, K.Zhou, B.Chen Bottom energy loss and nonprompt J/ψ production in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.107.054917
2023ZH16 Phys.Rev. C 107, 044909 (2023) Charmonium transport in the high-μB medium
doi: 10.1103/PhysRevC.107.044909
2022CH26 Phys.Rev. C 105, 054901 (2022) B.Chen, L.Jiang, X.-H.Liu, Y.Liu, J.Zhao X(3872) production in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.105.054901
2022TO08 Phys.Rev. C 106, 034911 (2022) Charmonium dissociation at high baryon chemical potential
doi: 10.1103/PhysRevC.106.034911
2022ZH16 Phys.Rev. C 105, 034902 (2022) Charmonium triangular flow in high energy nuclear collisions
doi: 10.1103/PhysRevC.105.034902
2021CH30 Phys.Rev. C 103, 064910 (2021) Hadronic effects on charmonium elliptic flows in heavy-ion collisions
doi: 10.1103/PhysRevC.103.064910
2021HU07 Chin.Phys.C 45, 024001 (2021) Z.Huang, B.Chen, L.Qin, Q.Zhang, F.Zhang, T.Wang, K.Fang Measurement of astrophysical S-factor for 9Be(d, α0)7Li and 9Be(d, α1)7Li* reactions at low energies NUCLEAR REACTIONS 9Be(d, α), E=66-94 keV; measured reaction products, Eα, Iα; deduced thick target yields, S-factors. Comparison with available data.
doi: 10.1088/1674-1137/abca1d
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
2019WA15 Appl.Radiat.Isot. 147, 144 (2019) Q.Wang, Y.Han, B.Chen, Z.Huang, S.Tamaki, Is.Murata, T.Wang, K.Fang Cross sections of (n, x) reactions on cerium isotopes induced by D-T neutrons NUCLEAR REACTIONS 136,138,140,142Ce(n, 2n), 140,142Ce(n, p), (n, α), 142Ce(n, γ), E ∼ 14 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VII.1, CENDL-3.1, JENDL-4.0 libraries, TALYS-1.8 code calculations.
doi: 10.1016/j.apradiso.2019.03.012
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
2018ZH01 Appl.Radiat.Isot. 132, 61 (2018) Z.Zhang, Q.Zhang, S.Chen, B.Chen, Q.Wang, C.Lai, K.Fang Measurement of cross-sections for 14 MeV neutron interaction with 175Lu NUCLEAR REACTIONS 175Lu(n, 2n), (n, p), (n, α), E=14.1, 14.5, 14.7 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VII.1, JEFF-3.2 and FENDL-3.1b evaluated nuclear data libraries.
doi: 10.1016/j.apradiso.2017.11.017
2017CH13 Phys.Rev. C 95, 034908 (2017) Elliptic flow as a probe for the ψ(2S) production mechanism in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.95.034908
2016CH16 Phys.Rev. C 93, 044917 (2016) Effects of quark-gluon plasma and hadron gas on charmonium production at energies available at the CERN Super Proton Synchrotron and the Facility for Antiproton and Ion Research
doi: 10.1103/PhysRevC.93.044917
2016CH19 Phys.Rev. C 93, 054905 (2016) Detailed rapidity dependence of J/ψ production at energies available at the Large Hadron Collider
doi: 10.1103/PhysRevC.93.054905
2015CH44 Eur.Phys.J. A 51, 82 (2015) Investigation of ΛQ and ΞQ baryons in the heavy quark-light diquark picture
doi: 10.1140/epja/i2015-15082-3
2013CH22 Phys.Rev. C 87, 054616 (2013) B.Chen, F.Sammarruca, C.A.Bertulani Microscopic in-medium nucleon-nucleon cross sections with improved Pauli blocking effects
doi: 10.1103/PhysRevC.87.054616
2012CH35 Phys.Rev. C 86, 034906 (2012) Mean field effect on J/ψ production in heavy ion collisions
doi: 10.1103/PhysRevC.86.034906
2012SA51 Phys.Rev. C 86, 054317 (2012) F.Sammarruca, B.Chen, L.Coraggio, N.Itaco, R.Machleidt Dirac-Brueckner-Hartree-Fock versus chiral effective field theory
doi: 10.1103/PhysRevC.86.054317
2012SA58 Eur.Phys.J. A 48, 181 (2012) The impact of charge symmetry and charge independence breaking on the properties of neutrons and protons in isospin-asymmetric nuclear matter
doi: 10.1140/epja/i2012-12181-7
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
2009LI43 Phys.Rev. C 80, 044329 (2009) Influence of the pairing interaction at ultrahigh spin NUCLEAR STRUCTURE 155Tb; analyzed proton alignments, moments of inertia, and influence of the pairing interaction near ultrahigh spins using the particle number-conserving (PNC) method of the cranked shell model.
doi: 10.1103/PhysRevC.80.044329
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
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
2006ZH41 Eur.Phys.J. A 30, 519 (2006) H.Zhang, S.Im, J.Li, W.Zuo, Z.Ma, B.Chen, W.Scheid Improved BCS-type pairing for the relativistic mean-field theory NUCLEAR STRUCTURE 74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sr; calculated neutron and proton shell gaps, total energy per nucleon, quadrupole deformation, isotope shifts, shape coexistence, two-neutron separation energies. Relativistic mean-field theory, density-dependent δ interaction.
doi: 10.1140/epja/i2006-10147-0
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
2005ZH18 Phys.Rev. C 71, 054312 (2005) H.Zhang, J.Li, W.Zuo, Z.Ma, B.Chen, S.Im Properties of the superheavy element 287115 and its α-decay time NUCLEAR STRUCTURE 287Mc, 283Nh, 279Rg, 275Mt, 271Bh; calculated binding energies, β2, single-particle level energies. RADIOACTIVITY 287Mc, 283Nh, 279Rg, 275Mt, 271Bh(α); calculated Qα, T1/2.
doi: 10.1103/PhysRevC.71.054312
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
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
2002LI36 Phys.Rev. C65, 064305 (2002) Ground-State and Pairing Properties of Pr Isotopes in Relativistic Mean-Field Theory NUCLEAR STRUCTURE Pr; calculated binding energies, quadrupole deformation, isotope shifts, radii, one-nucleon separation energies.
doi: 10.1103/PhysRevC.65.064305
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
2001LI26 Phys.Rev. C63, 054612 (2001) J.-Y.Liu, Y.-F.Yang, W.Zuo, S.-J.Wang, Q.Zhao, W.-J.Guo, B.Chen Isospin Effect on the Process of Multifragmentation and Dissipation at Intermediate Energy Heavy Ion Collisions NUCLEAR REACTIONS 76Kr, 120Xe(40Ca, X), 76Zn, 120Cd(40Ar, X), E ≈ 50-150 MeV/nucleon; calculated intermediate mass fragments multiplicity vs time, quadrupole of single particle momentum distributions; deduced isospin effect. Isospin-dependent quantum molecular dynamics.
doi: 10.1103/PhysRevC.63.054612
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
1999NG03 Nucl.Phys. A649, 37c (1999) V.G.Nguyen, Z.Ma, H.Toki, B.Chen Relativistic Calculations of Giant Resonances with Non-Linear Models NUCLEAR STRUCTURE 90Zr, 208Pb; calculated isoscalar, isovector giant monopole resonance response functions. 30,32,34,36,38,40,42,44,46,48,50,52Ar; calculated GDR response functions. Relativistic RPA.
doi: 10.1016/S0375-9474(99)00036-6
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
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.
1997LI05 Nucl.Phys. A616, 131c (1997) W.Liu, X.Bai, S.Zhou, Z.Ma, Z.Li, Y.Wang, A.Li, Z.Ma, B.Chen, X.Tang, Y.Han, Q.Shen, J.Xu Measurement of the Angular Distribution for the 7Be(d, n)8B Reaction and Determination of the Astrophysical S Factor for the 7Be(p, γ)8B Reaction NUCLEAR REACTIONS, ICPND 7Be(d, n), E(cm)=5.8 MeV; measured σ(θ), reaction σ; deduced 7Be(p, γ) reaction astrophysical S-factor, model parameters.
doi: 10.1016/S0375-9474(97)00082-1
1997MA77 Prog.Theor.Phys.(Kyoto) 98, 917 (1997) Z.Ma, H.Toki, B.Chen, V.G.Nguyen The Giant Dipole Resonance in Ar-Isotopes in the Relativistic RPA NUCLEAR STRUCTURE 30,32,34,36,38,40,42,44,46,48,50Ar; calculated rms radii, GDR response functions; deduced splitting near proton, neutron drip lines. Relativistic RPA.
doi: 10.1143/PTP.98.917
1997RE07 Z.Phys. A357, 137 (1997) Level Inversion of N = 9 Isotones in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 16,17O, 15,16N, 14,15C, 13,14B, 12,13Be; calculated binding energy, nucleon, charge radii, single particle level energies, density distributions in some cases. Relativistic mean-field theory.
doi: 10.1007/s002180050228
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
1996LI12 Phys.Rev.Lett. 77, 611 (1996) W.Liu, X.Bai, S.Zhou, Z.Ma, Z.Li, Y.Wang, A.Li, Z.Ma, B.Chen, X.Tang, Y.Han, Q.Shen Angular Distribution for the 7Be(d, n)8B Reaction at E(c.m.) = 5.8 MeV and the S17(0) Factor for the 7Be(p, γ)8B Reaction NUCLEAR REACTIONS, ICPND 2H(7Be, n), E(cm)=5.8 MeV; measured σ(θ); deduced astrophysical S-factor for 7Be(p, γ). DWBA analysis.
doi: 10.1103/PhysRevLett.77.611
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
1996RE02 Phys.Rev. C53, R572 (1996) One-Proton Halo in 26P and Two-Proton Halo in 27S NUCLEAR STRUCTURE 26P, 25Si, 27S; calculated binding energy, neutron, proton, single particle orbitals radii, nucleon, matter density distributions; deduced halo characteristics. Nonlinear relativistic mean field theory.
doi: 10.1103/PhysRevC.53.R572
1996RE03 Z.Phys. A353, 363 (1996) Z.Ren, W.Mittig, B.Chen, Z.Ma, G.Auger Relativistic Mean-Field Study of Light Proton-Rich Nuclei 18Ne, 20Mg and 22Si NUCLEAR STRUCTURE 18Ne, 20Mg, 22Si, 16O; calculated nucleon radii, binding energy, nucleon, matter density distributions. 18Ne, 20Mg, 22Si deduced proton halo features. Relativistic mean field theory.
doi: 10.1007/BF01285147
1996RE04 J.Phys.(London) G22, L1 (1996); Erratum J.Phys.(London) G22, 1115 (1996) Relativistic Mean-Field Study of Odd-A N and F Isotopes NUCLEAR STRUCTURE 15,17,19,21,23N, 17,19,21,23,25,27,29F; calculated binding energy, nucleon rms radii. 15,21,23N, 27,29,23,25F; calculated nucleon, matter, halo neutron density distribution. Non-linear relativistic mean field theory, effective interactions.
doi: 10.1088/0954-3899/22/1/001
1996RE13 J.Phys.(London) G22, 523 (1996) Z.Ren, B.Chen, Z.Ma, Z.Zhu, G.Xu One-Neutron Halos in 22N, 23O and 24F and Three-Neutron Halo in 26F NUCLEAR STRUCTURE 22N, 23O, 24,26F; calculated binding energy, neutron, proton, matter radii, density distributions, single particle energies. 22Ne, 23O, 26,24F deduced neutron halo characteristics. Nonlinear relativistic mean-field theory.
doi: 10.1088/0954-3899/22/4/013
1995CH36 Phys.Rev. C52, 878 (1995) Proton-Nucleus Scattering Based on the Relativistic Brueckner-Hartree-Fock Model NUCLEAR REACTIONS 40Ca, 16O, 90Zr, 208Pb(polarized p, p), E=160-500 MeV; analyzed σ(θ), polarization observables data. Optical potentials from relativistic Brueckner-Bethe-Goldstone equation.
doi: 10.1103/PhysRevC.52.878
1995CH55 Phys.Lett. 355B, 37 (1995) B.Chen, J.Dobaczewski, K.-L.Kratz, K.Langanke, B.Pfeiffer, F.-K.Thielemann, P.Vogel Influence of Shell-Quenching Far from Stability on the Astrophysical r-Process NUCLEAR STRUCTURE A=80-140; analyzed r-process paths, abundances data; deduced far from stability nuclear structure properties testing possibility.
doi: 10.1016/0370-2693(95)00737-6
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
1995CH75 Chin.J.Nucl.Phys. 17, No 1, 1 (1995) H.-Z.Chen, X.-Z.Zhang, W.-S.Han, B.-Q.Chen, X.-N.Jin Deuteron Photodisintegration Between 250 and 750 MeV NUCLEAR REACTIONS 2H(γ, p), E=250-750 MeV; calculated σ(θ), P(θ), σ(E). Relativistic framework, dynamical isobar propagator.
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
1995MA25 Chin.Phys.Lett. 12, 72 (1995) Finite-Nuclei Properties in Relativistic Density Dependent Hartree-Fock Approach NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energy per nucleon, charge rms radius.
1995RE09 Phys.Rev. C52, R20 (1995) Neutron Halos in O Isotopes NUCLEAR STRUCTURE 28,26,24,22,20,18,16O; calculated proton, neutron radii, spin-orbit splitting, other ground state features. Nonlinear relativistic mean field theory.
doi: 10.1103/PhysRevC.52.R20
1995RE10 J.Phys.(London) G21, 691 (1995) Ground-State Properties of the Nucleus 100Sn in Relativistic and Non-Relativistic Mean-Field Approaches NUCLEAR STRUCTURE 100,114,132Sn; calculated binding energy per nucleon, n-, p- radii, differences. Mean field approach, Skyrme interactions.
doi: 10.1088/0954-3899/21/5/013
1995RE13 Phys.Lett. 351B, 11 (1995) Z.Ren, G.Xu, B.Chen, Z.Ma, W.Mittig Structure of Halo Nuclei 14Be and 32Ne NUCLEAR STRUCTURE 12,14Be, 30,32Ne; calculated proton, neutron, matter density distribution, rms radii, binding energy, single particle levels energy; deduced halo neutron occupation related features. Density-dependent relativistic mean-field theory.
doi: 10.1016/0370-2693(95)00364-Q
1995RE16 Phys.Rev. C52, R1764 (1995) Z.Ren, W.Mittig, B.Chen, Z.Ma, G.Auger, G.Xu Neutron Halo and Spin-Orbit Splitting in Some Neutron-Rich Nuclei NUCLEAR STRUCTURE 12,14Be, 30,32Ne, 60,62Ca, 122,124Zr; calculated ground state energy. 14Be, 32Ne; calculated neutron, proton, halo radii, single particle energies. 40,48,60Ca; calculated spin-orbit splitting variation. Density-dependent relativistic mean-field theory.
doi: 10.1103/PhysRevC.52.R1764
1995RE20 J.Phys.(London) G21, 1269 (1995) Relativistic Mean-Field Study of Light Neutron-Rich Nuclei NUCLEAR STRUCTURE 12Be, 14C, 28,16O, 30Ne, 32Mg, 34Si, 36S, 38Ar, 40,60Ca, 42Ti, 64Cr, 66Fe, 68Ni; calculated binding energy, nucleon radii. Nonlinear relativistic mean field theory.
doi: 10.1088/0954-3899/21/9/012
1995RE23 J.Phys.(London) G21, L83 (1995) Z.Ren, B.Chen, Z.Ma, W.Mittig, G.Xu Spin-Orbit Splittings in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energy per nucleon, nucleon rms radii. 40,48,60Ca; calculated spin-orbit splittings vs tensor coupling strength. Relativistic mean-field theory.
doi: 10.1088/0954-3899/21/11/001
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
1994BO24 Nucl.Phys. A574, 185c (1994) P.Bonche, E.Chabanat, B.Q.Chen, J.Dobaczewski, H.Flocard, B.Gall, P.H.Heenen, J.Meyer, N.Tajima, M.S.Weiss Microscopic Approach to Collective Motion NUCLEAR STRUCTURE 192Hg, 194Pb; calculated superdeformed bands, energies, quadrupole moments, dynamical, rigid body moments of inertia, Eγ. 194,196,198,200,202,204,206,208,210,212,214,216,218,220Pb; calculated proton, neutron rms radii. Microscopic approach, collective motion.
doi: 10.1016/0375-9474(94)90045-0
1994CH54 Phys.Lett. 339B, 297 (1994) Suppression of Medium Effects in Quasielastic Electron Scattering at High Momentum Transfer NUCLEAR REACTIONS 56Fe(e, e), E not given; calculated longitudinal response functions. Momentum dependent nucleon self-energy.
doi: 10.1016/0370-2693(94)90621-1
1994CH75 Chin.J.Nucl.Phys. 16, No 4, 295 (1994) Relativistic Description of Proton Scattering on 16O, 40Ca and 208Pb at 800 MeV NUCLEAR REACTIONS 16O, 40Ca, 208Pb(polarized p, p), E=800 MeV; analyzed σ(θ), analyzing power vs θ. Relativistic, microscopic optical potential.
1994MA41 Phys.Rev. C50, 3170 (1994) Isovector Meson Contribution in the Relativistic Hartree-Fock Approach for Finite Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 90Zr; calculated binding energy per nucleon, rms charge radii. 90Zr; calculated charge distribution. Relativistic Hartree-Fock approach, isovector meson contribution.
doi: 10.1103/PhysRevC.50.3170
1993CH31 Phys.Rev. C48, 1392 (1993) Atomic Parity Nonconservation and Neutron Radii in Cesium Isotopes NUCLEAR STRUCTURE 125,127,129,131,133,135,137,139Cs; calculated binding energies, isotope shifts, neutron, charge radii; deduced relationship to weak charges uncertainity. Hartree-Fock method.
doi: 10.1103/PhysRevC.48.1392
1993FL04 Nucl.Phys. A557, 559c (1993) H.Flocard, B.Q.Chen, B.Gall, P.Bonche, J.Dobaczewski, P.H.Heenen, M.S.Weiss Hartree-Fock and Hartree-Fock-Bogoliubov Calculations of Superdeformed Bands NUCLEAR STRUCTURE 192,194Hg, 194Pb; calculated superdeformed bands quadrupole moments, dynamical, rigid body moments of inertia. Hartree-Fock, HFB calculations, limitations discussed.
doi: 10.1016/0375-9474(93)90569-J
1992CH12 Phys.Rev. C45, 2332 (1992) B.Chen, T.A.Armstrong, R.A.Lewis, R.Newton, G.A.Smith, J.P.Bocquet, F.Malek, H.Nifenecker, M.Maurel, E.Monnand, P.Perrin, C.Ristori, G.Ericsson, T.Johansson, G.Tibell, M.Rey-Campagnolle, S.Polikanov, T.Krogulski, J.Mougey Neutron Yields and Angular Distributions Produced in Antiproton Annihilation at Rest in Uranium NUCLEAR REACTIONS U(p-bar, F), E at rest; measured fission (fragment)n-coin, neutron yields; deduced fragment neutron emission mechanism.
doi: 10.1103/PhysRevC.45.2332
1992CH31 J.Phys.(London) G18, 1505 (1992) The Investigation of the Non-Orthogonal Basis Expansion Method for a Three-Fermion System NUCLEAR STRUCTURE A=3; calculated hypernucleus ground state energy rate of convergence. Nonorthogonal basis expansion method.
doi: 10.1088/0954-3899/18/9/012
1992CH32 Phys.Rev. C46, R1582 (1992) B.-Q.Chen, P.-H.Heenen, P.Bonche, M.S.Weiss, H.Flocard Observation of Identical Bands in Superdeformed Nuclei with the Cranked Hartree-Fock Method NUCLEAR STRUCTURE 194,192Hg, 194Pb; calculated superdeformed band level energies, quadrupole moments, dynamical, rigid moments of inertia; deduced twinning characteristics. Cranked Hartree-Fock, Skyrme effective interaction.
doi: 10.1103/PhysRevC.46.R1582
1992CH38 Chin.J.Nucl.Phys. 14, No 3, 258 (1992) Recent Development in Investigation of Nucleon-Nucleus Scattering at Medium Energy NUCLEAR REACTIONS 16O, 40Ca, 90Zr, 208Pb(p, p), (polarized p, p), E=160-800 MeV; analyzed σ(θ), spin observables data. Relativistic Brueckner Hartree-Fock approach.
1992MA60 Chin.J.Nucl.Phys. 14, No 4, 301 (1992) Effect of Tensor Coupling of ρ Meson in Relativistic Hartree Theory for Ca Isotopes NUCLEAR STRUCTURE 38,40,42,44,46,48,50,52,54,56,58,62,64,66,68,70Ca; calculated proton, neutron rms radii, binding energies per particle. Relativistic Hartree theory.
1990LU05 Phys.Rev. C42, 707 (1990) Z.-D.Lu, B.Chen, J.-S.Zhang, Y.-Z.Zhuo, H.-Y.Han Transient Behavior at Deformations Beyond Saddle Point and Neutron Multiplicity NUCLEAR REACTIONS 142Nd(16O, xn), E=207 MeV; analyzed neutron multiplicity data; deduced friction constant. NUCLEAR STRUCTURE 240Pu; calculated fission rates, evolution distribution, neutron multiplicity vs excitation energy.
doi: 10.1103/PhysRevC.42.707
1988CH46 Chin.J.Nucl.Phys. 10, 320 (1988) Chen Bin, Zhang Jingshang, Lu Zhongdao, Han Huiyi, Zhuo Yizhong Difference of Fission Behaviors at Saddle and Scission Points and the Neutron Multiplicity Prior to Fission NUCLEAR STRUCTURE 240Pu; calculated fission rates neutron multiplicity. Diffusion model.
1983CH52 Chin.J.Nucl.Phys. 5, 113 (1983) Chen Baoqiu, Jin Shizhao, Chen Jiafu, Tian Baoyin d + d Four-Body Break Up Process NUCLEAR REACTIONS 2H(d, 2p), E=80 MeV; calculated σ(θ1, θ2, E1, E2). PWBA, four-body breakup, two spectator quasifree scattering.
1983CH59 Chin.J.Nucl.Phys. 5, 63 (1983) Chen Baoqiu, Chen Jiafu, Tian Baoying, Jin Shizhao 6Li + 6Li → 3α Reaction NUCLEAR REACTIONS 6Li(6Li, 2α), E ≤ 24 MeV; calculated breakup yield vs E; deduced reaction mechanism.
1982CH28 Chin.J.Nucl.Phys. 4, 244 (1982) The Application of Diffraction Model to Quasi-Free Scattering NUCLEAR REACTIONS 6Li(α, 2α), E=18 MeV; 6Li(p, pα), E=56.5 MeV; 6Li(d, dα), E=52 MeV; analyzed data. Diffraction model, quasifree scattering.
1981JI05 Chin.J.Nucl.Phys. 3, 108 (1981) Jin Xingnan, Chen Baoqiu, Yao Jinzhang, Li Zhuxia Theoretical Analysis on the Quasifree Scattering of 6Li NUCLEAR REACTIONS 6Li(p, pd), E=100, 156, 590 MeV; 6Li(d, 2d), E=8, 9, 11 MeV; 6Li(α, 2α), (α, dα), E=18 MeV; analyzed σ(θ1, θ2, E1); deduced 6Li cluster formation charateristics. PWIA, DWIA analyses.
1980CH37 Chin.J.Nucl.Phys. 2, 131 (1980) On 6Li(p, pd)α and 6Li(d, 2d)α Analysis of Quasifree scattering NUCLEAR REACTIONS 6Li(p, pd), E=100 MeV; 6Li(d, 2d), E=10 MeV; calculated σ(θd, θp, Ep), σ(θd1, θd2, Ed1). Antisymmetrized cluster model, PWIA, spectactor influence.
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