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NSR database version of April 24, 2024.

Search: Author = X.Z.Zhang

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2022LI28      Few-Body Systems 63, 43 (2022)

W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho

Progress of Underground Nuclear Astrophysics Experiment JUNA in China

NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.

doi: 10.1007/s00601-022-01735-3
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2017WU11      Eur.Phys.J. A 53, 183 (2017)

F.Wu, C.L.Bai, J.M.Yao, H.Q.Zhang, X.Z.Zhang

Existence problem of proton semi-bubble structure in the 21+ state of 34Si

NUCLEAR STRUCTURE 34Si, 36S; calculated first proton orbitals, proton sp levels, J, B(E2), proton density distribution vs radius using HF (Hartree-Fock) plus RPA (Random Phase Approximation) based on Skyrme-type interaction; deduced possibility of lower proton density ("bubble") in the center of nucleus.

doi: 10.1140/epja/i2017-12375-5
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2016MA06      Phys.Rev. C 93, 014317 (2016)

H.-L.Ma, B.-G.Dong, Y.-L.Yan, H.-Q.Zhang, D.-Q.Yuan, S.-Y.Zhu, X.-Z.Zhang

Pygmy and giant dipole resonances in the nitrogen isotopes

NUCLEAR STRUCTURE 17,18,19,20N; calculated S(p), S(n), mass radii, B(E1), transition densities and transition matrix elements, and energy-weighted sum rule (EWSR) for pygmy dipole resonances (PDR), GDR energies and splitting of isospin doublets, photoabsorption cross sections. Configuration-interaction shell model with the WBP10 effective interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.014317
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2014BA55      Phys.Rev. C 90, 054335 (2014)

C.L.Bai, H.Sagawa, G.Colo, Y.Fujita, H.Q.Zhang, X.Z.Zhang, F.R.Xu

Low-energy collective Gamow-Teller states and isoscalar pairing interaction

NUCLEAR STRUCTURE 42Ca, 46Ti, 50Cr, 54Fe, 58Ni; calculate neutron pairing gaps, Gamow-Teller (GT) strength distributions and sum rule values for IAR states, energy differences between the lowest GT and IAR states in N=Z+2 nuclei. HFB+QRPA calculations with the Skyrme forces SGII, SGII+Te3, and SAMi. Comparison with experimental values.

doi: 10.1103/PhysRevC.90.054335
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2013MA64      Phys.Rev. C 88, 034322 (2013)

H.L.Ma, S.-H.Yao, B.-G.Dong, X.-G.Wu, H.-Q.Zhang, X.-Z.Zhang

Risk of misinterpreting nearly degenerate doublet bands as chiral partners in odd-even 103, 105, 107Ag and odd-odd 106Ag

NUCLEAR STRUCTURE 103,105,106,107Ag; calculated single particle Routhians as function of rotational frequencies, energies of nearly degenerate negative-parity doublet bands, deformation trajectories, B(E2); comparison with experimental data suggests consistency with planar cranking model interpretation. Existence of chiral structure of such degenerate bands questioned. Configuration-dependent cranked Nilsson-Strutinsky (CNS) calculations.

doi: 10.1103/PhysRevC.88.034322
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2012MA12      Phys.Rev. C 85, 044307 (2012)

H.-L.Ma, B.-G.Dong, Y.-L.Yan, H.-Q.Zhang, X.-Z.Zhang

Proton pygmy dipole resonances in 17, 18Ne: Collective versus noncollective excitations

NUCLEAR STRUCTURE 17,18Ne; calculated nucleon and matter density distributions, mass and charge radii, E1 response functions from excited states, EWSR, E1 transition densities, contribution to total matrix elements for deexcitation from proton pygmy dipole resonances (PDRs). Interacting shell model with self-consistent Skyrme-Hartree-Fock wave functions. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.044307
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2012MA44      Eur.Phys.J. A 48, 125 (2012)

H.-L.Ma, B.-G.Dong, Y.-L.Yan, X.-Z.Zhang

Shell model study on the astrophysical neutron capture of 8Li

NUCLEAR STRUCTURE 6,7,8,9Li; calculated magnetic moment, 9Li levels, J, π using combined shell and potential models with three different interactions.

NUCLEAR REACTIONS 8Li(n, γ), E=0-1 MeV; calculated resonant capture γ transition B(M1) from first unbound to the ground state, spectroscopic factor, resonance widths, direct capture σ, reaction rate using combined shell and potential models with three different interactions.

doi: 10.1140/epja/i2012-12125-3
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2012YU08      J.Phys.(London) G39, 105105 (2012)

N.Yu, H.Q.Zhang, X.Z.Zhang

Vorticity of threshold strength in neutron drip-line nuclei

doi: 10.1088/0954-3899/39/10/105105
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2011BA18      Phys.Rev. C 83, 054316 (2011)

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

Spin-isospin excitations as quantitative constraints for the tensor force

NUCLEAR STRUCTURE 90Zr, 208Pb; calculated Gamow-Teller (GT) and charge-exchange spin-dipole (SD) excitation energies, centroid energies. HF+RPA model with Skyrme interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.054316
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2011BA38      Phys.Rev. C 84, 044329 (2011)

C.L.Bai, H.Sagawa, G.Colo, H.Q.Zhang, X.Z.Zhang

Spin-dipole excitations in 16O and tensor correlations

NUCLEAR STRUCTURE 16F, 208Bi; calculated charge-exchange spin-dipole (SD) strength distributions and energies using different interactions. Hartree-Fock (HF) plus self-consistent random-phase approximation (RPA) using Skyrme-type interactions. 16O; investigated effect of tensor force on the charge-exchange SD transition. Role of triplet-even and triplet-odd tensor interactions.

doi: 10.1103/PhysRevC.84.044329
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2011DO12      Phys.Rev. C 84, 014303 (2011)

J.M.Dong, W.Zuo, J.Z.Gu, Y.Z.Wang, L.G.Cao, X.Z.Zhang

Effects of tensor interaction on pseudospin energy splitting and shell correction

NUCLEAR STRUCTURE 106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn; calculated proton and neutron pseudospin orbit splittings. 132Sn, 298Fl; calculated neutron and proton shell correction energies, single particle spectra. Skyrme-Hartree-Fock approach with the SLy5+TF and T31+TF parameter sets combined with the BCS method.

doi: 10.1103/PhysRevC.84.014303
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2011WA10      Phys.Rev. C 83, 054305 (2011)

Y.Z.Wang, J.Z.Gu, J.M.Dong, X.Z.Zhang

Systematic study of tensor effects in shell evolution

NUCLEAR STRUCTURE Z=8, 20, 28, N=8-50 (even N); N=8, 20, 28, Z=6-32 (even Z); calculated evolution of magic gaps with and without tensor forces, proton spin-orbit potentials and radial wave function square, energy differences between the 1d5/2 and 1d3/2 single proton states in Ca isotopes. Hartree-Fock-Bogliubov approach with several Skyrme interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.054305
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2011WA28      Chin.Phys.Lett. 28, 102101 (2011)

Y.-Z.Wang, J.-Z.Gu, X.-Z.Zhang, J.-M.Dong

Tensor Effect on Bubble Nuclei

NUCLEAR STRUCTURE 34Si, 46Ar; calculated proton density distributions, single-particle spectra and proton spin-orbit potential. Hartree-Fock-Bogoliubov (HFB) approach.

doi: 10.1088/0256-307X/28/10/102101
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2011WA29      Phys.Rev. C 84, 044333 (2011)

Y.Z.Wang, J.Z.Gu, X.Z.Zhang, J.M.Dong

Tensor effects on the proton sd states in neutron-rich Ca isotopes and bubble structure of exotic nuclei

NUCLEAR STRUCTURE 40,42,44,46,48,50,52,54,56,58,60,62,64,66,68Ca; calculated energy differences of the proton single-particle states with and without tensor force. 48,64Ca; calculated proton spin-orbit potentials and squared radial wave functions, proton single-particle energies. 46Ar, 206Hg; calculated proton single-particle spectrum, proton density distributions. Hartree-Fock-Bogoliubov (HFB) approach with Skyrme interactions SLy5+T, SLy5+Tw and several sets of the TIJ parameterizations. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.044333
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2010BA22      Phys.Rev.Lett. 105, 072501 (2010)

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

Effect of the Tensor Force on the Charge Exchange Spin-Dipole Excitations of 208Pb

NUCLEAR STRUCTURE 208Pb; calculated charge exchange spin-dipole excitations; deduced tensor correlations, tensor strength parameters, strength distributions. Self-consistent Skyrme hartree-Fock formalism.

doi: 10.1103/PhysRevLett.105.072501
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2010BA26      Nucl.Phys. A834, 65c (2010)

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

Tensor Effects on Spin-Dependent Charge-Exchange transitions

NUCLEAR STRUCTURE 208Pb; calculated GT (Gamow-Teller) and SD (Spin-Dipole) transition strength functions.

doi: 10.1016/j.nuclphysa.2010.01.019
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2010BA34      Chin.Phys.Lett. 27, 102101 (2010)

C.-L.Bai, H.-Q.Zhang, X.-Z.Zhang, F.-R.Xu, H.Sagawa, G.Colo

Effect of the Tensor Force on Charge-Exchange Spin-Dependent Multipole Excitations

NUCLEAR STRUCTURE 90Zr; calculated charge-exchange spin-dipole and spin-quadrupole strength functions; deduced RPA tensor correlation shift.

doi: 10.1088/0256-307X/27/10/102101
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2010YU03      Chin.Phys.B 19, 062701 (2010)

D.-Q.Yuan, Y.-N.Zheng, Y.Zuo, P.Fan, D.-M.Zhou, X.-G.Wu, L.-H.Zhu, G.-S.Li, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

The g-factors and magnetic rotation in 82Rb

NUCLEAR REACTIONS 60Ni(27Al, n4p)82Rb, E=130 MeV; measured Eγ, Iγ, γ-γ-coin.; deduced g factors. Comparison with semiclassical model calculations.

doi: 10.1088/1674-1056/19/6/062701
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2010ZH03      Chin.Phys.Lett. 27, 022102 (2010)

Y.-N.Zheng, D.-M.Zhou, D.-Q.Yuan, Y.zuo, P.fan, M.Mihara, K.Matsuta, M.Fukuda, T.Minamisono, T.Suzuki, Y.-J.Xu, J.-Z.Zhu, Z.-Q.Wang, H.-L.Luo, X.-Z.Zhang, S.-Y.Zhu

Nuclear Structure and Magnetic Moment of the Unstable 12B-12N Mirror Pair

NUCLEAR MOMENTS 12B, 12N; measured β-NMR spectra; deduced magnetic moments, magic numbers. Comparison with shell model calculations.

doi: 10.1088/0256-307X/27/2/022102
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2009BA17      Phys.Lett. B 675, 28 (2009)

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

Effect of tensor correlations on Gamow-Teller states in 90Zr and 208Pb

NUCLEAR STRUCTURE 90Zr, 208Pb; calculated Gamow-Teller strength distributions including tensor correlation in HF and RPA model. Comparison with data.

doi: 10.1016/j.physletb.2009.03.077
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2009BA19      Phys.Rev. C 79, 041301 (2009)

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

Quenching of Gamow-Teller strength due to tensor correlations in 90Zr and 208Pb

NUCLEAR STRUCTURE 90Zr, 208Pb; calculated Gamow-Teller (GT) and spin-quadrupole (SQ) strength distributions. Random-phase approximation (RPA) and Hartree-Fock (HF) calculations.

doi: 10.1103/PhysRevC.79.041301
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2009FA14      Chin.Phys.C 33, Supplement 1, 206 (2009)

P.Fan, D.-Q.Yuan, Y.Zuo, Y.-N.Zheng, D.-M.Zhou, X.-G.Wu, G.-S.Li, L-H.Zhu, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

Proton alignment in 82Sr investigated by g-factor measurements

NUCLEAR REACTIONS 58Ni(28Si, 4p)82Sr, E=110 MeV; measured Eγ, Iγ; deduced rotational bands, g factors, proton alignment.

doi: 10.1088/1674-1137/33/S1/066
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2009MA37      Phys.Rev. C 80, 014316 (2009)

H.-li.Ma, B.-g.Dong, Y.-li.Yan, Xi.-z.Zhang

Polarization charges and electric quadrupole transitions of yrast terminating bands in 44, 46, 48Ti

NUCLEAR STRUCTURE 44,46,48Ti; calculated levels, J, π, electric quadrupole moments, magnetic moments, B(E2), yrast bands and polarization effects using microscopic particle-vibration model calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.014316
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2009MA73      Chin.Phys.C 33, Supplement 1, 67 (2009)

H.-L.Ma, Y.-L.Yan, X.-Z.Zhang, D.-M.Zhou, B.-G.Dong

Spectroscopy and reduced transition probabilities of negative parity bands up to band termination in 45Ti

NUCLEAR STRUCTURE 45Ti; calculated negative parity high-spin states, J, π, B(E2), electric quadrupole moment and magnetic moment. Configuration-dependent cranked Nilsson-Strutinsky (CNS) approach.

doi: 10.1088/1674-1137/33/S1/022
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2009YU10      Chin.Phys.C 33, Supplement 1, 188 (2009)

D.-Q.Yuan, Y.-N.Zheng, Y.Zuo, P.Fan, D.-M.Zhou, M.Liu, X.-G.Wu, L.-H.Zhu, G.-S.Li, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

Study of magnetic-rotation in 82Rb by g-factor measurements

NUCLEAR REACTIONS 60Ni(27Al, n4p)82Rb, E=130 MeV; measured Eγ, Iγ, γ-γ-coin.; deduced magnetic rotational bands, g factors.

doi: 10.1088/1674-1137/33/S1/060
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2009ZH52      Chin.Phys.C 33, Supplement 1, 215 (2009)

Y.-N.Zheng, D.-M.Zhou, K.Matsuta, M.Mihara, M.Fukuda, D.Nishimura, J.Komurasaki, D.Ishikawa, R.Matsumiya, T.Nagatomo, T.Izumikawa, S.Takahashi, H.Hirano, T.Ohtsubo, S.Momota, Y.Nojiri, A.Kitagawa, M.Kanazawa, M.Torikoshi, S.Sato, T.Minamisono, J.R.Alonso, G.F.Krebs, T.J.M.Symons, D.-Q.Yuan, Y.Zuo, P.Fan, T.Suzuki, X.-Z.Zhang, S.-Y.Zhu

Nuclear structure of proton-rich unstable nucleus 28P studied by g-factor measurement

RADIOACTIVITY 28P(β+) [from Be(28Si, X)28P, E=100 MeV/nucleon]; measured decay products, β-NMR spectra; deduced g factors, magnetic moment.

doi: 10.1088/1674-1137/33/S1/069
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2009ZH53      Chin.Phys.C 33, Supplement 1, 218 (2009)

D.-M.Zhou, Y.-N.Zheng, X.-Z.Zhang, D.-Q.Yuan, Y.Zuo, P.Fan, Z.-Q.Wang, H.-L.Luo, G.-J.Xu, S.-Y.Zhu

Structure of β-emitting nuclei 29P

RADIOACTIVITY 29P(β+) [from 28Si(d, n)29P, E=3 MeV]; measured decay products, β-NMR spectra; deduced magnetic moment, density distribution of protons, neutrons and matter.

doi: 10.1088/1674-1137/33/S1/070
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2008YU04      Chin.Phys.Lett. 25, 3617 (2008)

D.-Q.Yuan, P.Fan, Y.-N.Zheng, Y.Zuo, D.-M.Zhou, X.-G.Wu, G.-S.Li, L.-H.Zhu, G.-J.Xu, Q.-W.Fan, X.-Z.Zhang, S.-Y.Zhu

Measurements of g-Factor of Rotational Band States in 82Sr

NUCLEAR REACTIONS 58Ni(28Si, 4p), E=110 MeV; measured Eγ, Iγ, γγ-coin. 82Sr; deduced g-factors for positive parity rotational states. Transient magnetic field ion implantation perturbed angular distribution method.

doi: 10.1088/0256-307X/25/10/026
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2007LI65      Phys.Rev. C 76, 044321 (2007)

C.J.Lin, X.Z.Zhang, R.Zhang, Z.H.Liu, H.Q.Zhang

Low-lying E1 strength in light drip-line nuclei

NUCLEAR STRUCTURE 11Be; calculated E1 strengths as function of excitation energy, DWA approximation, comparisons with experimental data, deduced spectroscopic factors.

doi: 10.1103/PhysRevC.76.044321
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2007SA46      Phys.Rev. C 76, 034327 (2007); Erratum Phys.Rev. C 77, 049902 (2008)

H.Sagawa, S.Yoshida, G.-M.Zeng, J.-Z.Gu, X.-Z.Zhang

Isospin dependence of incompressibility in relativistic and nonrelativistic mean field calculations

NUCLEAR STRUCTURE 112,114,116,118,120,122,124Sn, 208Pb; calculated isoscalar giant monopole resonance strength distributions using Skyrme-HF and relativistic mean field models.

doi: 10.1103/PhysRevC.76.034327
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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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2006ZH44      Int.J.Mod.Phys. E15, 1779 (2006)

X.-R.Zhou, H.Sagawa, X.-Z.Zhang

Evolution of deformations in sd and pf shell nuclei

NUCLEAR STRUCTURE 18O, 20,22Ne, 24Mg, 28,30Si, 32,34S, 36Ar, 42Ca, 46Ti, 50Cr, 54Fe, 58Ni; calculated energy surfaces, deformation, quadrupole moments.

doi: 10.1142/S0218301306005368
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2005SA59      Phys.Rev. C 72, 054311 (2005)

H.Sagawa, X.R.Zhou, X.Z.Zhang

Evolution of deformations in medium-mass nuclei

NUCLEAR STRUCTURE 16O, 18,20Ne, 22,24Mg, 26,28Si, 30,32S, 34,36Ar, 38,40Ca, 42,44Ti, 46,48Cr, 50,52Fe, 54,56Ni; calculated deformation parameters, quadrupole moments. Deformed Skyrme-Hartree-Fock model with pairing correlations.

doi: 10.1103/PhysRevC.72.054311
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2005SA63      Eur.Phys.J. A 25, Supplement 1, 535 (2005)

H.Sagawa, X.R.Zhou, X.Z.Zhang, T.Suzuki

Deformations and electromagnetic moments of light exotic nuclei

NUCLEAR STRUCTURE 12,14,16,18,20,22C, 18,20,22,24,26,28,30,32Ne; calculated deformation energy, transitions B(E2). 9,11,13,15,17,19C; calculated quadrupole moments, μ. Deformed Skyrme-Hartree-Fock and shell model calculations.

doi: 10.1140/epjad/i2005-06-065-5
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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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2004LI16      Chin.Phys.Lett. 21, 273 (2004)

Z.-H.Liu, X.-Z.Zhang, H.-Q.Zhang

Direct Radiative Capture of Neutron in Drip-Line Nuclei

doi: 10.1088/0256-307X/21/2/016
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2004SA58      Phys.Rev. C 70, 054316 (2004)

H.Sagawa, X.R.Zhou, X.Z.Zhang, T.Suzuki

Deformations and electromagnetic moments in carbon and neon isotopes

NUCLEAR STRUCTURE 9,10,11,12,13,14,15,16,17,18,19,20,21,22C, 18,19,20,21,22,23,24,25,26,28Ne; calculated level energies, deformation, quadrupole moments, μ, B(E2). Deformed Skyrme Hartree-Fock model, isospin-dependent core polarization charges.

doi: 10.1103/PhysRevC.70.054316
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2003LI24      Chin.Phys.Lett. 20, 1017 (2003)

Z.-H.Liu, X.-Z.Zhang, H.-Q.Zhang

Scaling Laws and Occurrence Conditions of Nuclear Halo

NUCLEAR STRUCTURE 8,12B, 11Be, 13,14,15,19C, 17F, 21Na; analyzed radii, asymptotic normalization coefficients; deduced halo occurance condition, scaling law.

doi: 10.1088/0256-307X/20/7/313
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2003LI31      Phys.Rev. C 68, 024305 (2003)

Z.H.Liu, X.Z.Zhang, H.Q.Zhang

Nuclear halo and its scaling laws

NUCLEAR STRUCTURE 11Be, 12B, 13,14,15,19C; analyzed asymptotic normalization coefficients; deduced halo features.

doi: 10.1103/PhysRevC.68.024305
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2003ZH22      Nucl.Phys. A723, 375 (2003)

X.R.Zhou, E.G.Zhao, B.G.Dong, X.Z.Zhang, G.L.Long

Collective properties of low-lying octupole excitations in 20882Pb126, 6020Ca40 and 288O20

NUCLEAR STRUCTURE 28O, 60Ca, 208Pb; calculated isoscalar and isovector octupole strength distributions, transition densities, giant resonance features. Self-consistent Hartree-Fock approach, RPA, particle-vibration coupling.

doi: 10.1016/S0375-9474(03)01366-6
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2001HA10      Nucl.Phys. A683, 255 (2001)

I.Hamamoto, S.V.Lukyanov, X.Z.Zhang

Kinetic Energy and Spin-Orbit Splitting in Nuclei Near Neutron Drip Line

doi: 10.1016/S0375-9474(00)00443-7
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2001HA45      Phys.Rev. C64, 024313 (2001)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Shape, Shell Structure, and Low-Lying Strong Octupole Strength in 2060Ca40

NUCLEAR STRUCTURE 60Ca, 68Ni, 80Zr; calculated levels, J, π, octupole strength distributions. Self-consistent Hartree-Fock, RPA, Skyrme interactions.

doi: 10.1103/PhysRevC.64.024313
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2001UR04      Phys.Rev. C64, 054304 (2001)

P.Urkedal, X.Z.Zhang, I.Hamamoto

Low-Lying Appreciable Gamow-Teller Strength in Deformed Neutron-Rich Nuclei

NUCLEAR STRUCTURE 100,102,104,106,108,110Sr, 102,104,106,108,110,112Zr, 104,106,108,110,112Mo, 106,108,110,112,114Ru, 110,112,114,116Pd, 158,160,162,164,166Gd, 160,162,164,166,168Dy, 162,164,166,168,170,172,174Er, 164,166,168,170,172,174,176,178Yb, 170,172,174,176,178,180,182Hf, 176,178,180,182,184W; calculated pair-correlation parameters, quadrupole moments, deformation. 108Mo, 160Gd, 162,164Dy, 170Er, 176Yb, 178Hf; calculated Gamow-Teller strength distributions. 160Gd, 164Dy, 170Er, 176Yb; deduced appreciable low-lying Gamow-Teller strength. Skyrme-Hartree-Fock calculations, Tamm-Dancoff approximation, RPA.

doi: 10.1103/PhysRevC.64.054304
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2001ZH44      Hyperfine Interactions 136/137, 205 (2001)

S.Y.Zhu, Q.Luo, Y.G.Wang, Z.G.Fan, Y.J.Xu, R.Wang, J.Z.Zhu, G.S.Li, X.A.Liu, X.G.Wu, S.X.Wen, G.J.Xu, Z.C.Gao, X.Z.Zhang, Y.S.Chen, K.Matsuta, M.Fukuda, M.Mihara, T.Minamisono

g-Factor Measurements of Rotational States in 84, 86Zr

NUCLEAR REACTIONS 58Ni(28Si, 2p), E=98 MeV; 58Ni(32S, 4p), E=110 MeV; measured Eγ, Iγ(θ, H, t). 84,86Zr deduced g factors for rotational band states. Transient-field technique.

doi: 10.1023/A:1020532332334
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1999HA09      Nucl.Phys. A648, 203 (1999)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Displacement Fields of Excited States in Stable and Neutron Drip-Line Nuclei

NUCLEAR STRUCTURE 11Be, 60Ca, 208Pb; calculated multipole excitation modes transition densities, displacement fields. Self-consistent Hartree-Fock plus RPA.

doi: 10.1016/S0375-9474(99)00024-X
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1999SA22      Nucl.Phys. A649, 319c (1999)

H.Sagawa, I.Hamamoto, X.Z.Zhang

A Microscopic Study of Giant Resonances in Nuclei Near Drip Lines

NUCLEAR STRUCTURE 208Pb, 34,40,48,60Ca; calculated giant monopole resonance strength distributions. 100Sn; calculated core polarization charges, B(E2). 90Zr, 100Sn; calculated neutron, proton effective charges. Self-consistent Hartree-Fock plus RPA model.

doi: 10.1016/S0375-9474(99)00094-9
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1998HA09      Phys.Rev. C57, R1064 (1998)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Isoscalar and Isovector Dipole Mode in Drip Line Nuclei in Comparison with β-Stable Nuclei

NUCLEAR STRUCTURE 22C, 28O, 34,40,60Ca, 208Pb; calculated isoscalar, isovector dipole strength vs excitation energy; deduced giant resonance features. Hartree-Fock plus RPA calculations, Skyrme interactions.

doi: 10.1103/PhysRevC.57.R1064
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1998HA39      J.Phys.(London) G24, 1417 (1998)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Collective Modes of Nuclei Far from β-Stability Line

NUCLEAR STRUCTURE 28O, 34Ca, 100Sn, 208Pb; calculated isoscalar, isovector dipole strength distributions.

doi: 10.1088/0954-3899/24/8/016
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1998HA60      Phys.Rev. C58, 3388 (1998)

I.Hamamoto, X.Z.Zhang

Coupling of Particles Near Threshold to Shape Oscillations

doi: 10.1103/PhysRevC.58.3388
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1998SA26      Phys.Rev. C58, 1101 (1998)

B.-H.Sa, Y.-M.Zheng, H.Wang, X.-Z.Zhang

Disassembly of Projectile Remnants in a Simple Dynamics and Statistics Model

NUCLEAR REACTIONS 197Au(197Au, X), E=600 MeV/nucleon; analyzed data; deduced parameters, caloric curve.

doi: 10.1103/PhysRevC.58.1101
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1998SA28      J.Phys.(London) G24, 1445 (1998)

H.Sagawa, I.Hamamoto, X.Z.Zhang

Giant Monopole States in Nuclei Near Drip Lines

NUCLEAR STRUCTURE 34,40,48,60Ca, 208Pb; calculated isocalar, isovector monopole strength distributions. Hartree-Fock plus RPA model.

doi: 10.1088/0954-3899/24/8/019
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1997HA20      Phys.Rev. C55, 2361 (1997)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Structure of Giant Quadrupole Resonances in Neutron Drip Line Nuclei

NUCLEAR STRUCTURE 28O; 48Ca; calculated isoscalar GQR associated radial transition density, strength function. Self-consistent Hartree-Fock plus RPA, Skyrme interaction.

doi: 10.1103/PhysRevC.55.2361
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1997HA55      Nucl.Phys. A626, 669 (1997)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Quadrupole Strength Function and Core Polarization in Drip Line Nuclei

NUCLEAR STRUCTURE 28O, 34,40,60Ca, 48Ni, 48Ca; calculated isoscalar, isovector quadrupole RPA strength functions, polarizations. Self-consistent Hartree-Fock calculations, Skyrme interactions.

doi: 10.1016/S0375-9474(97)00478-8
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1997HA57      Phys.Rev. C56, 3121 (1997)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Giant Monopole Resonances in Nuclei Near Stable and Drip Lines

NUCLEAR STRUCTURE 34,40,48,60Ca, 90Zr, 208Pb; calculated giant monopole strength distributions, related features. Hartree-Fock, RPA calculations, Skyrme interactions.

doi: 10.1103/PhysRevC.56.3121
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1996HA02      Phys.Rev. C53, 765 (1996)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Single-Particle and Collective Properties of Drip-Line Nuclei

NUCLEAR STRUCTURE 110Ni, 100,120Sn, 120Sr; calculated Hartree-Fock density, Hartree-Fock potential vs r. 110Ni, 100Sn; calculated isoscalar, isovector monopole, isovector dipole, isoscalar quadrupole modes strength functions. Hartree-Fock with Skyrme interactions, RPA.

doi: 10.1103/PhysRevC.53.765
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1996WA14      Phys.Rev. C54, 254 (1996)

F.Wang, B.-H.Sa, Y.-M.Zheng, X.-Z.Zhang

Competition Among the Decay Modes of Projectile Remnants in (600 MeV/nucleon) Au + Cu Reactions

NUCLEAR REACTIONS Cu(197Au, X), E=600 MeV/nucleon; analyzed projectile remnant decay modes relative yield. Incomplete fusion-fragmentation model.

doi: 10.1103/PhysRevC.54.254
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1996ZH08      Phys.Rev. C53, 1868 (1996)

Y.-M.Zheng, F.Wang, B.-H.Sa, X.-Z.Zhang

Incomplete-Fusion-Fragmentation Model: Multifragmentation data from 600A MeV heavy-ion collisions

NUCLEAR REACTIONS Cu(197Au, X), E=600 MeV/nucleon; analyzed multi-fragmentation data. Incomplete-fusion-fragmentation model.

doi: 10.1103/PhysRevC.53.1868
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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.


1995FR19      Phys.Rev. C52, 2468 (1995)

F.Frisk, I.Hamamoto, X.Z.Zhang

Gamow-Teller β+ Decay of Deformed Nuclei Near the Proton Drip Line

NUCLEAR STRUCTURE Z=28-66; calculated β+-decay associated Gamow-Teller transition strength. Deformed Hartree-Fock based quasiparticle TDA, Skyrme interactions.

doi: 10.1103/PhysRevC.52.2468
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1995HA30      Phys.Rev. C52, R2326 (1995)

I.Hamamoto, X.Z.Zhang

Neutron Skin of Nuclei Near the Neutron Drip Line

NUCLEAR STRUCTURE 152Dy; analyzed Hartree-Fock minima density distribution at superdeformed shape. A=152; A=178; A=208; calculated one-neutron levels vs N=78-110, 94-126, 118-142 respectively; deduced neutron skin related features. Skyrme type deformed Hartree-Fock calculations.

doi: 10.1103/PhysRevC.52.R2326
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1995HA39      Z.Phys. A353, 145 (1995)

I.Hamamoto, X.Z.Zhang

Dependence of Gamow-Teller β+-Decay of 80Zr, 76Sr and 72Kr on Nuclear Shape

NUCLEAR STRUCTURE 80Zr, 76Sr, 72Kr; calculated Gamow-Teller β+-decay probability. Skyrme-type deformed Hartree-Fock calculation based quasiparticle TDA.

doi: 10.1007/BF01295892
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1995SA19      J.Phys.(London) G21, 241 (1995)

B.-H.Sa, H.-M.Liu, Y.-M.Zheng, Z.-D.Lu, X.-Z.Zhang

Correlations between Conditional Moments Might not Necessarily Imply Evidence of a Phase Transition in a Diassembly of Hot Nuclei

NUCLEAR STRUCTURE 197Au; calculated disassembly fragment charge distribution; deduced conditional moments correlations related features. Monte Carlo, partition method approaches.

doi: 10.1088/0954-3899/21/2/011
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1994SA38      Phys.Rev. C50, 2614 (1994)

B.-H.Sa, R.-H.Wang, X.-Z.Zhang, Y.-M.Zheng, Z.-D.Lu

Thermal Equilibrium of the Nuclear System in the 40Ca(35 MeV/nucleon) + 40Ca Reaction

NUCLEAR REACTIONS 40Ca(40Ca, X), E=35 MeV/nucleon; analyzed fragment charge dispersion; deduced nearly central collisions thermal equilibrium features.

doi: 10.1103/PhysRevC.50.2614
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1994ZH45      Chin.J.Nucl.Phys. 16, No 4, 337 (1994)

X.-Z.Zhang, B.-G.Dong

Symmetry of Y5 Deformation and Two-Level Model


1990CH38      Phys.Rev. C42, 2187 (1990)

T.-H.Chih, B.-H.Sa, X.-Z.Zhang, Y.-M.Zheng

Dependence of Physical Observables on the Incident Energy in Intermediate Energy Nucleus-Nucleus Collision

NUCLEAR REACTIONS 63Cu(12C, X), E=15-45 MeV/nucleon; calculated fragment yield distribution with mass; deduced physical variables incident energy dependence.

doi: 10.1103/PhysRevC.42.2187
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1990SA09      Nucl.Phys. A509, 499 (1990)

B.-H.Sa, Y.-M.Zheng, X.-Z.Zhang

Dependence of the Phase Transition on the Mass Number of Hot Nuclei before Break-Up

NUCLEAR STRUCTURE 48Ti, 56Ni, 63Cu, 84Kr, 131Xe, 197Au, 238U; calculated excitation energy vs thermodynamic temperature, fissility, Coulomb energy; deduced phase transition mass number dependence.

doi: 10.1016/0375-9474(90)90088-4
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1989GR10      Nucl.Phys. A495, 231c (1989)

D.H.E.Gross, X.-Z.Zhang

Thermodynamics of Nuclei and Nuclear Fragmentation

NUCLEAR STRUCTURE 131Xe, 197Au; calculated excitation energy vs temperature. Equipartition model.

doi: 10.1016/0375-9474(89)90322-9
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1989HA21      Phys.Lett. 226B, 17 (1989)

I.Hamamoto, J.Holler, X.Z.Zhang

Electric-Dipole Transitions in Deformed Rare-Earth Nuclei

NUCLEAR STRUCTURE 169Lu; calculated B(E1). 177Hf; calculated E1 transition amplitudes; deduced octupole vibration coupling role.

doi: 10.1016/0370-2693(89)90280-3
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1989SA43      Phys.Rev. C40, 2680 (1989)

B.-H.Sa, Y.-M.Zheng, X.-Z.Zhang

Modified Statistical Model for the Disassembly of Hot Nuclei Formed in Intermediate-Energy Heavy-Ion Collisions

NUCLEAR REACTIONS 63Cu(12C, X), E=35 MeV/nucleon; calculated fragment yield vs mass. Modified statistical model.

doi: 10.1103/PhysRevC.40.2680
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1989ZH08      Nucl.Phys. A499, 487 (1989)

D.Zhang, B.-H.Sa, X.-Z.Zhang, X.N.Jin

A Simplified Method of the Monte Carlo Simulation for the Disassembly of Hot Nuclei

NUCLEAR STRUCTURE 238U; calculated disassociation σ vs fragment mass yield distributions.

doi: 10.1016/0375-9474(89)90541-1
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1987PO17      Nucl.Phys. A474, 557 (1987); Erratum Nucl.Phys. A550, 563 (1992)

H.Popping, P.U.Sauer, Zhang Xi-Zheng

The Two-Nucleon System above Pion Threshold: A force model with Δ-isobar and pion degrees of freedom

NUCLEAR REACTIONS 1H(p, X), (p, p), (p, π+), E=200-1000 MeV; calculated σ(E). Force model, isobar, pion degrees of freedom.

doi: 10.1016/0375-9474(87)90595-1
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1987ZH02      Nucl.Phys. A461, 641 (1987)

X.-Z.Zhang, D.H.E.Gross, S.-Y.Xu, Y.-M.Zheng

On the Decay of Very Hot Nuclei. (I). Canonical Metropolis Sampling of Multifragmentation

NUCLEAR REACTIONS 238U(p, X), E=1-400 GeV; calculated σ vs fragment mass, yields vs fragment energy. Canonical Metropolis sampling method.

doi: 10.1016/0375-9474(87)90414-3
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1987ZH03      Nucl.Phys. A461, 668 (1987)

X.-Z.Zhang, D.H.E.Gross, S.-Y.Xu, Y.-M.Zheng

On the Decay of Very Hot Nuclei. (II). Microcanonical Metropolis Sampling of Multifragmentation

NUCLEAR REACTIONS 238U(p, X), E=1-400 GeV; calculated σ vs fragment mass, yield vs temperature, charge fragment multiplicities. Microcanonical Metropolis sampling method.

doi: 10.1016/0375-9474(87)90415-5
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1986GR03      Phys.Rev.Lett. 56, 1544 (1986)

D.H.E.Gross, Zhang Xiao-Ze, Xu Shu-yan

Decay of very Hot Nuclei

NUCLEAR STRUCTURE 235U; calculated average charged fragment, prompt, evaporated neutron numbers, heavy fragment multiplicity, temperature.

doi: 10.1103/PhysRevLett.56.1544
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1979LI18      Chin.J.Nucl.Phys. 1, 73 (1979)

Li Zhu-Xia, Zhang Xi-Zhen, Sa Ben-Hao, Shi Yi-Jin

The Effects of Core Polarization on the Single Particle State in 208Pb

NUCLEAR STRUCTURE 208Pb; calculated levels, B(λ), strength distribution. Core polarization, higher order diagram partial summation.


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