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NSR database version of May 24, 2024.

Search: Author = C.L.Zhang

Found 18 matches.

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2024SU06      Eur.Phys.J. A 60, (2024)

Sh.Sun, R.-Q.Yu, L.-G.Cao, Ch.-L.Zhang, F.-Sh.Zhang

Application of relativistic continuum random phase approximation to giant dipole resonance of 208Pb and 132Sn

NUCLEAR STRUCTURE 132Sn, 208Pb; calculated the properties of isovector giant dipole resonances (IVGDR) using the relativistic continuum random phase approximation (RCRPA).

doi: 10.1140/epja/s10050-024-01288-5
Citations: PlumX Metrics

2020LI40      Phys.Rev. C 102, 044305 (2020)

T.Li, M.Z.Chen, C.L.Zhang, W.Nazarewicz, M.Kortelainen

Nucleon localization function in rotating nuclei

NUCLEAR STRUCTURE 152Dy; calculated single-particle neutron and proton Routhians as functions of angular frequency using Skyrme interaction SkM* and the cranked Hartree-Fock (CHF), and cranked harmonic oscillator (CHO) methods for the SD band, current, spin, spin-kinetic and spin-current tensor densities for the SD band using CHF method; used the concept of nucleon localization function (NLF) to interpret the results from CHF method for fast rotation in nuclei. Discussed oscillating pattern of the NLF in terms of interference between kinetic-energy and particle densities, and nodal pattern of the NLF in terms of direction of major axis of a rotating nucleus, and aligned angular momentum.

doi: 10.1103/PhysRevC.102.044305
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2016ZH52      Phys.Rev. C 94, 064323 (2016)

C.L.Zhang, B.Schuetrumpf, W.Nazarewicz

Nucleon localization and fragment formation in nuclear fission

NUCLEAR STRUCTURE 232Th, 240Pu, 264Fm; calculated nucleonic density and spatial localization distributions, potential energy curves along the fission pathways, neutron and proton nucleon localization function (NLF) profiles for 264Fm and two 132Sn nuclei, 232Th and 100Zr + 132Sn. 132Sn, 100Zr; calculated nucleonic densities and spatial localizations for the ground states. Self-consistent energy density functional method (EDFM) with a quantified energy density functional optimized for fission studies.

doi: 10.1103/PhysRevC.94.064323
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2015ZH33      Phys.Rev. C 92, 034307 (2015)

C.L.Zhang, G.H.Bhat, W.Nazarewicz, J.A.Sheikh, Y.Shi

Theoretical study of triaxial shapes of neutron-rich Mo and Ru nuclei

NUCLEAR STRUCTURE 106,108Mo, 108,110,112Ru; calculated levels, J, π, moments of inertia, shapes, and transition quadrupole moments, potential energy surfaces (PES) in (Q20, Q22) plane, Routhians, alignments for high-spin bands, equilibrium deformation plots, ground, γ and γγ bands. Triaxial shape deformations. Nuclear density functional theory (DFT) with the optimized energy density functional UNEDF0, and triaxial projected shell model (TPSM). Comparison with experimental data.

doi: 10.1103/PhysRevC.92.034307
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2013SH39      Phys.Rev. C 88, 034311 (2013)

Y.Shi, C.L.Zhang, J.Dobaczewski, W.Nazarewicz

Kerman-Onishi conditions in self-consistent tilted-axis-cranking mean-field calculations

NUCLEAR STRUCTURE 160Yb; calculated total Routhians as a function of tilting angle, triaxial strongly deformed bands (TSD), quadrupole moments. Tilted-axis-cranking (TAC) energy-density functional (EDF) theory. 110Mo, 158Er; calculated Routhians and other parameters for TSD band in 158Er and a triaxial band in 110Mo to test validity of Kerman-Onishi conditions through self-consistent Hartree-Fock (SHF), and self-consistent Hartree-Fock-Bogoliubov with pairing from Lipkin-Nogami formalism (SFHB-LN) calculations.

doi: 10.1103/PhysRevC.88.034311
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2012ZH21      Eur.Phys.J. A 48, 65 (2012)

G.L.Zhang, C.L.Zhang, H.Q.Zhang, C.J.Lin, D.Y.Pang, X.K.Wu, H.M.Jia, G.P.An, Z.D.Wu, X.X.Xu, F.Yang, Z.H.Liu, S.Kubono, H.Yamaguchi, S.Hayakawa, D.N.Binh, Y.K.Kwon, N.Iwasa, M.Mazzocco, M.La Commara, M.Romoli, C.Signorini

Quasi-elastic scattering of the proton drip line nucleus 17F on 12C at 60 MeV

NUCLEAR REACTIONS 12C(17F, 17F'), E=60 MeV; measured E(17F), I(17F, θ); deduced σ(θ), σ; calculated σ(θ) using optical model and CDCC; deduced parameters. Compared with data, also for nearby projectiles.

doi: 10.1140/epja/i2012-12065-x
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2377.

2010ZH06      Phys.Rev. C 81, 034611 (2010)

H.Q.Zhang, C.L.Zhang, C.J.Lin, Z.H.Liu, F.Yang, A.K.Nasirov, G.Mandaglio, M.Manganaro, G.Giardina

Competition between fusion-fission and quasifission processes in the 32S+184W reaction

NUCLEAR REACTIONS 184W(32S, X), E=140, 145, 150, 155, 160, 165, 170 MeV; measured capture σ, σ(θ) of fission fragments, fission excitation functions. 182,184(32S, X), E(cm)=120-220 MeV; analyzed fission excitation functions, comparison with previous experimental data and theoretical cross sections using dinuclear system (DNS) model for capture, complete fusion, quasifission, fast fission, and total evaporation residues.

doi: 10.1103/PhysRevC.81.034611
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1791.

2010ZH29      Nucl.Phys. A834, 201c (2010)

C.L.Zhang, H.Q.Zhang, C.J.Lin, A.K.Nasirov, G.Mandaglio, M.Manganaro, G.Giardina

Competition between fusion-fission and quasifission processes in 32S+184W reaction

NUCLEAR REACTIONS 184W(32S, F), E(cm)=118.8, 123.1, 127.3, 131.5, 135.8, 141.4, 144.4 MeV; measured fission fragment angular distributions; deduced fission, fusion σ, σ(θ), reaction mechanism features. Comparison with dinuclear system model.

doi: 10.1016/j.nuclphysa.2009.12.040
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0069.

2009JI02      Chin.Phys.Lett. 26, 032301 (2009)

F.Jia, C.-J.Lin, H.-Q.Zhang, F.Yang, H.-M.Jia, X.-X.Xu, Z.-D.Wu, Z.-H.Liu, G.-L.Zhang, C.-L.Zhang

Experimental Evidence of Two-Proton Emissions from 18Ne Excited State

NUCLEAR REACTIONS 197Au(18Ne, 18Ne'), E not given; measured Ep, Ip. 18Ne; deduced level energies. Two proton decay.

doi: 10.1088/0256-307X/26/3/032301
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Data from this article have been entered in the XUNDL database. For more information, click here.

2009WU01      Chin.Phys.Lett. 26, 022503 (2009)

Z.-D.Wu, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, G.-P.An, C.-L.Zhang, G.-L.Zhang, H.-M.Jia, X.-X.Xu, C.-L.Bai, N.Yu, F.Jia

Optical Potential Parameters for Halo Nucleus System 6He+12C from Transfer Reaction 11B(7Li, 6He)12C

NUCLEAR REACTIONS 11B(7Li, 6He), E=18.3, 28.3 MeV; analyzed σ(θ). 12C(6He, 7Li); deduced optical potential parameters.

doi: 10.1088/0256-307X/26/2/022503
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0056.

2008AN17      Chin.Phys.Lett. 25, 4237 (2008)

G.-P.An, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, G.-L.Zhang, C.-L.Zhang, Z.-D.Wu, F.Jia, H.-M.Jia, X.-X.Xu, C.-L.Bai, N.Yu

Optical Potential Parameters of Weakly Bound Nuclear System 17F+13C

NUCLEAR REACTIONS 16O(14N, 14N), (14N, 13C), E=76.2, 57.0 MeV; measured σ(θ). Compared results to model calculations.

doi: 10.1088/0256-307X/25/12/014
Citations: PlumX Metrics

2008JI03      Chin.Phys.Lett. 25, 2834 (2008)

H.-M.Jia, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, F.Jia, C.-L.Zhang, G.-P.An, Z.-D.Wu, X.-X.Xu, C.-L.Bai, N.Yu

Surface Diffuseness Anomaly in 16O+208Pb Quasi-elastic Scattering at Backward Angle

NUCLEAR REACTIONS 208Pb(16O, 16O'), E=40.50-80.25 MeV; measured quasi=elastic scattering excitation function at backward angles.

doi: 10.1088/0256-307X/25/8/028
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2008YA03      Phys.Rev. C 77, 014601 (2008)

F.Yang, C.J.Lin, X.K.Wu, H.Q.Zhang, C.L.Zhang, P.Zhou, Z.H.Liu

Barrier distributions from 32S+90,96Zr quasi-elastic scattering: Investigation of the role of neutron transfer in sub-barrier fusion reactions

NUCLEAR REACTIONS 90,96Zr(32S, X), E=60-90 MeV; measured cross sections, barrier distributions.

doi: 10.1103/PhysRevC.77.014601
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2007LI43      Nucl.Phys. A787, 281c (2007)

C.J.Lin, H.Q.Zhang, F.Yang, M.Ruan, Z.H.Liu, Y.W.Wu, X.K.Wu, P.Zhou, C.L.Zhang, G.L.Zhang, G.P.An, H.M.Jia, X.X.Xu

Effects of breakup of weakly bound projectile and neutron transfer on fusion reactions around Coulomb barrier

NUCLEAR REACTIONS 152Sm(16O, 16O), (16O, 16O'), (16O, X), E(cm)=45-70 MeV; measured σ(θ=156, θ=160, θ=164), evaporation residue σ for boron, carbon, nitrogen and oxygen isotopes; deduced reaction mechanism features. 208Pb(6Li, 6Li), (6Li, 6Li'), (6Li, X), (7Li, 7Li), (7Li, 7Li'), (7Li, X), E(cm)=18-42 MeV; 90,96Zr(32S, X), E(cm)=60-95 MeV; measured σ; deduced reaction mechanism features. 208Pb(6Li, 6Li), E(cm)=26-40 MeV; measured fusion σ; deduced reaction mechanism features. Comparison with coupled-channels model.

doi: 10.1016/j.nuclphysa.2006.12.044
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2007ZH02      Chin.Phys.Lett. 24, 397 (2007)

G.-L.Zhang, H.-Q.Zhang, Z-H.Liu, C.-L.Zhang, C.-J.Lin, F.Yang, G.-P.An, H.-M.Jia, Z.-D.Wu, X.-X.Xu, C.-L.Bai, N.Yu

Calculation of Interaction Potentials between Spherical and Deformed Nuclei

NUCLEAR REACTIONS 154Sm(32S, X), E(cm)=100-130 MeV; calculated interaction potentials, fusion σ, dependence on deformation and orientation. Double folding model.

doi: 10.1088/0256-307X/24/2/026
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2006ZH12      Chin.Phys.Lett. 23, 1146 (2006)

C.-L.Zhang, H.-Q.Zhang, C.-J.Lin, M.Ruan, Z.-H.Liu, F.Yang, X.-K.Wu, P.Zhou, G.-P.An, H.-M.Jia, Z.-D.Wu, X.-X.Xu.C.-L.Bai

Unusual Threshold Anomaly in the 6Li+208Pb System

NUCLEAR REACTIONS 208Pb(6Li, 6Li), E=25-46 MeV; measured elastic σ(θ); deduced optical potential parameters, effects of coupling to breakup channel.

doi: 10.1088/0256-307X/23/5/023
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0050.

2006ZH31      J.Phys.(London) G32, 2261 (2006)

C.L.Zhang, H.Q.Zhang, X.Z.Zhang, H.Sagawa, F.R.Xu

Polarization charge of O isotopes

NUCLEAR STRUCTURE 16,22,24O; calculated isoscalar, isovector, and charge quadrupole response functions, transition densities, polarization charge. Microscopic particle-vibration coupling model.

doi: 10.1088/0954-3899/32/11/017
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2005ZH28      Chin.Phys.Lett. 22, 1877 (2005)

C.-L.Zhang, H.-Q.Zhang, X.-Z.Zhang

Dynamical Structure of Nuclear Excitation in Continuum

NUCLEAR STRUCTURE 28O, 34Ca; calculated monopole and quadrupole strength functions, radial transition densities. Collective excitation in continuum.

doi: 10.1088/0256-307X/22/8/015
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