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NSR database version of April 11, 2024.

Search: Author = B.Chen

Found 90 matches.

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2024CH14      Phys.Rev. C 109, 024909 (2024)

B.-X.Chen, X.-L.Zhao, G.-L.Ma

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
Citations: PlumX Metrics


2023CH37      Phys.Rev. C 108, 014901 (2023)

B.Chen, B.Tong

Bottomonium transport in p-Pb and Pb-Pb collisions at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.108.014901
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2023ZH16      Phys.Rev. C 107, 044909 (2023)

J.Zhao, B.Chen

Charmonium transport in the high-μB medium

doi: 10.1103/PhysRevC.107.044909
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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
Citations: PlumX Metrics


2022TO08      Phys.Rev. C 106, 034911 (2022)

B.Tong, B.Chen

Charmonium dissociation at high baryon chemical potential

doi: 10.1103/PhysRevC.106.034911
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2022ZH16      Phys.Rev. C 105, 034902 (2022)

J.Zhao, B.Chen, P.Zhuang

Charmonium triangular flow in high energy nuclear collisions

doi: 10.1103/PhysRevC.105.034902
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2021CH30      Phys.Rev. C 103, 064910 (2021)

B.Chen, L.Jiang, Y.Liu

Hadronic effects on charmonium elliptic flows in heavy-ion collisions

doi: 10.1103/PhysRevC.103.064910
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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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32768.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32773.


2017CH13      Phys.Rev. C 95, 034908 (2017)

B.Chen

Elliptic flow as a probe for the ψ(2S) production mechanism in relativistic heavy ion collisions

doi: 10.1103/PhysRevC.95.034908
Citations: PlumX Metrics


2016CH16      Phys.Rev. C 93, 044917 (2016)

B.Chen

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
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2016CH19      Phys.Rev. C 93, 054905 (2016)

B.Chen

Detailed rapidity dependence of J/ψ production at energies available at the Large Hadron Collider

doi: 10.1103/PhysRevC.93.054905
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2015CH44      Eur.Phys.J. A 51, 82 (2015)

B.Chen, K.-We.Wei, A.Zhang

Investigation of ΛQ and ΞQ baryons in the heavy quark-light diquark picture

doi: 10.1140/epja/i2015-15082-3
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2012CH35      Phys.Rev. C 86, 034906 (2012)

B.Chen, K.Zhou, P.Zhuang

Mean field effect on J/ψ production in heavy ion collisions

doi: 10.1103/PhysRevC.86.034906
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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
Citations: PlumX Metrics


2012SA58      Eur.Phys.J. A 48, 181 (2012)

F.Sammarruca, L.White, B.Chen

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
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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
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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
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2009LI43      Phys.Rev. C 80, 044329 (2009)

S.X.Liu, T.Li, B.R.Chen

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
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2006LI30      Chin.Phys.Lett. 23, 1719 (2006)

J.Liang, Z.-Yu.Ma, B.-Q.Chen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0802.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2003CH81      Chin.Phys.Lett. 20, 1936 (2003)

B.-Q.Chen, Z.-Y.Ma, Y.-L.Zhao

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
Citations: PlumX Metrics


2003MA26      Chin.Phys.Lett. 20, 1025 (2003)

Z.-Y.Ma, B.-Q.Chen

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
Citations: PlumX Metrics


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
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2002LI36      Phys.Rev. C65, 064305 (2002)

J.Li, Z.Ma, B.Chen, Y.Zhou

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
Citations: PlumX Metrics


2001CH84      Chin.Phys.Lett. 18, 1561 (2001)

B.-Q.Chen, Z.-Y.Ma

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0481.


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
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1997RE07      Z.Phys. A357, 137 (1997)

Z.Ren, B.Chen, Z.Ma, G.Xu

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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0745.


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
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1996RE02      Phys.Rev. C53, R572 (1996)

Z.Ren, B.Chen, Z.Ma, G.Xu

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
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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
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1996RE04      J.Phys.(London) G22, L1 (1996); Erratum J.Phys.(London) G22, 1115 (1996)

Z.Ren, B.Chen, Z.Ma, G.Xu

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
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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
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1995CH36      Phys.Rev. C52, 878 (1995)

B.Q.Chen, A.D.MacKellar

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
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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
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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
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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
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1995MA25      Chin.Phys.Lett. 12, 72 (1995)

Z.Ma, H.Shi, B.Chen

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)

Z.Ren, W.Mittig, B.Chen, Z.Ma

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
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1995RE10      J.Phys.(London) G21, 691 (1995)

Z.Ren, G.-O.Xu, B.Chen, Z.Ma

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
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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
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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
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1995RE20      J.Phys.(London) G21, 1269 (1995)

Z.Ren, B.Chen, Z.Ma, W.Mittig

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
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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
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1995SH19      Phys.Rev. C52, 144 (1995)

H.-L.Shi, B.-Q.Chen, Z.-Y.Ma

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
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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
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1994CH54      Phys.Lett. 339B, 297 (1994)

B.Chen, Z.Ma

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
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1994CH75      Chin.J.Nucl.Phys. 16, No 4, 295 (1994)

B.-Q.Chen

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)

Z.Ma, H.Shi, B.Chen

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
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1993CH31      Phys.Rev. C48, 1392 (1993)

B.Q.Chen, P.Vogel

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
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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
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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
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1992CH31      J.Phys.(London) G18, 1505 (1992)

B.Chen

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
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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
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1992CH38      Chin.J.Nucl.Phys. 14, No 3, 258 (1992)

B.Chen

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)

Z.Ma, B.Chen

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
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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)

Chen Baoqiu

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)

Chen Baoqiu

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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Note: The following list of authors and aliases matches the search parameter B.Chen: , B.Q.CHEN, B.R.CHEN, B.X.CHEN