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NSR database version of April 27, 2024.

Search: Author = X.Xia

Found 17 matches.

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2023LI53      Phys.Rev. C 108, 044902 (2023)

H.Li, X.-L.Xia, X.-G.Huang, H.Z.Huang

Dynamic calculations of magnetic field and implications on spin polarization and spin alignment in heavy ion collisions

doi: 10.1103/PhysRevC.108.044902
Citations: PlumX Metrics

2023NI11      Nucl.Instrum.Methods Phys.Res. A1057, 168703 (2023)

M.Niu, Z.Long, R.Fan, W.Jiang, J.Liu, Q.Xiu, R.Xu, H.Wang, Zh.Zhou, K.Sun, Zh.Zhang, H.Zhang, H.Yi, Y.Chen, D.Wang, X.Xia, H.Liang

Research on the performance of a diamond detector for the cross-section measurements at CSNS Back-n

NUCLEAR REACTIONS ¹²C, ⁶Li(n, α), ¹²C(n, n'), E=0.00001-100 MeV; measured reaction products, En, In, TOF; deduced the bi-parametric contour plot facilitated the identification of event bands in a bi-parameter experiment (neutron time of flight and deposited energy). Comparison with MATLAB simulations. The Back-n white neutron facility located within the China Spallation Neutron Source (CSNS).

doi: 10.1016/j.nima.2023.168703
Citations: PlumX Metrics

2023ZH37      Phys.Rev. C 108, 024310 (2023)

X.Y.Zhang, Z.M.Niu, W.Sun, X.W.Xia

Nuclear charge radii and shape evolution of Kr and Sr isotopes with the deformed relativistic Hartree-Bogoliubov theory in continuum

NUCLEAR STRUCTURE ^{70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Kr, ^{78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144}Sr; calculated binding energy, two-neutron separation energy S(2n), charge radii, quadrupole deformation parameters, potential energy curves. ¹⁰⁰Sn; calculated wave function, charge radii as a function of quadrupole deformation parameter. Deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) calculations and DRHBc extended to go beyond mean-field framework by performing a two-dimensional collective Hamiltonian (2DCH). Comparison to experimental data.

doi: 10.1103/PhysRevC.108.024310
Citations: PlumX Metrics

2020WA19      Phys.Rev. C 102, 014321 (2020)

F.Wang, Z.Shi, X.W.Xia

Description of the superdeformed rotational band in ⁴⁰Ca with a shell-model-like approach

NUCLEAR STRUCTURE ⁴⁰Ca; calculated potential energy surface (PES) in (β, γ) plane, neutron single particle levels, potential energy curves for spherical, normal deformed, and superdeformed configurations, neutron single particle Routhians for superdeformed band, level energy spectra and pairing energy, kinematic and dynamic moments of inertia plots, transition quadrupole moments, B(E2) for superdeformed band in ⁴⁰Ca. Shell-model-like approach based on cranking covariant density functional theory. Comparison with experimental data for the superdeformed band.

doi: 10.1103/PhysRevC.102.014321
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2019XI05      Phys.Rev. C 100, 014913 (2019)

X.-L.Xia, H.Li, X.-G.Huang, H.Z.Huang

Feed-down effect on Λ spin polarization

doi: 10.1103/PhysRevC.100.014913
Citations: PlumX Metrics

2018XI02      At.Data Nucl.Data Tables 121-122, 1 (2018)

X.W.Xia, Y.Lim, P.W.Zhao, H.Z.Liang, X.Y.Qu, Y.Chen, H.Liu, L.F.Zhang, S.Q.Zhang, Y.Kim, J.Meng

The limits of the nuclear landscape explored by the relativistic continuum Hartree-Bogoliubov theory

NUCLEAR STRUCTURE Z=8-120; calculated ground-state properties using the spherical relativistic continuum Hartree-Bogoliubov (RCHB) theory with the relativistic density functional PC-PK1.

doi: 10.1016/j.adt.2017.09.001
Citations: PlumX Metrics

2018XI06      Phys.Rev. C 98, 024905 (2018)

Xi.-L.Xia, H.Li, Z.Tang, Q.Wang

Probing vorticity structure in heavy-ion collisions by local Λ polarization

doi: 10.1103/PhysRevC.98.024905
Citations: PlumX Metrics

2017LI31      Nucl.Phys. A967, 772 (2017)

H.Li, H.Petersen, L.-G.Pang, Q.Wang, X.-L.Xia, X.-N.Wang

Local and global Λ polarization in a vortical fluid

doi: 10.1016/j.nuclphysa.2017.04.008
Citations: PlumX Metrics

2017LI40      Phys.Rev. C 96, 054908 (2017)

H.Li, L.-G.Pang, Q.Wang, X.-L.Xia

Global Λ polarization in heavy-ion collisions from a transport model

doi: 10.1103/PhysRevC.96.054908
Citations: PlumX Metrics

2016LI04      Phys.Rev. C 93, 014314 (2016)

Y.Lim, X.Xia, Y.Kim

Proton radioactivity in relativistic continuum Hartree-Bogoliubov theory

RADIOACTIVITY ¹⁰⁹I, ^112,113Cs, ^{144,145,146,146m,147,147m}Tm, ^{150,150m,151,151m}Lu, ^{155,156,156m,157}Ta, ^{159m,160,161,161m}Re, ^{164m,165m,166,166m,167,167m}Ir, ^{170,170m,171,171m}Au, ^176,177,177mTl, ¹⁸⁵Bi(p); calculated half-lives, nonoccupation probabilities u² of corresponding orbitals in the daughter nuclei. Wentzel-Kramers-Brillouin (WKB) method for half-lives, with continuum effect treated by using relativistic continuum Hartree-Bogoliubov theory with energy density functional PC-PK1. Comparison with experimental half-lives.

doi: 10.1103/PhysRevC.93.014314
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2016XI08      Chin.Phys.C 40, 074101 (2016)

X.-W.Xia

Evolution of N = 28 shell closure in relativistic continuum Hartree-Bogoliubov theory

NUCLEAR STRUCTURE ⁴⁴S, ⁴⁶Ar, ⁴⁸Ca, ⁵⁰Ti; calculated neutron single particle states, effective potential, change of single particle energy. Relativistic continuum Hatree-Bogoliubov (RCHB) theory.

doi: 10.1088/1674-1137/40/7/074101
Citations: PlumX Metrics

2016ZH18      Chin.Phys.C 40, 054102 (2016)

L.-F.Zhang, X.-W.Xia

Global α-decay study based on the mass table of the relativistic continuum Hartree-Bogoliubov theory

NUCLEAR STRUCTURE Z=10-120; calculated α-decay Q-values using the relativistic continuum Hartree-Bogoliubov (RCHB) theory with the covariant density functional PC-PK1. Comparison with experimental data.

doi: 10.1088/1674-1137/40/5/054102
Citations: PlumX Metrics

2009DI02      Nucl.Instrum.Methods Phys.Res. B267, 2341 (2009)

W.Ding, L.Q.Shi, X.G.Long, S.Z.Luo, S.M.Peng, B.Zhang, X.J.Xia

Cross-section for D(p, p)D elastic scattering from 1.8 to 3.2 MeV at the laboratory angles of 155 degrees and 165 degrees

NUCLEAR REACTIONS ²H(p, p), E=1.8-3.2 MeV; measured Eπ, Iπ, s(θ).

doi: 10.1016/j.nimb.2009.03.108
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0572.

2008XI03      Nucl.Instrum.Methods Phys.Res. B266, 705 (2008)

X.J.Xia, W.Ding, B.Zhang, X.G.Long, S.Z.Luo, S.M.Peng, R.Hutton, L.Q.Shi

Cross-section for proton-tritium scattering from 1.4 to 3.4 MeV at the laboratory angle of 165 degrees

NUCLEAR REACTIONS ³H(p, p), E=1.4-3.4 MeV; measured proton energies, yields, σ at backward angle.

doi: 10.1016/j.nimb.2008.01.005
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0459.

1996AN24      Phys.Rev. A54, 3067 (1996)

Z.An, T.H.Li, L.M.Wang, X.Y.Xia, Z.M.Luo

Correction of Substrate Effect in the Measurement of 8-25-keV Electron-Impact K-Shell Ionization Cross Sections of Cu and Co Elements

ATOMIC PHYSICS Cu, ⁵⁹Co(e, X), E=8-25 keV; measured K-shell ionization σ. Thin targets substrate influence corrected.

NUCLEAR REACTIONS Cu, ⁵⁹Co(e, X), E=8-25 keV; measured K-shell ionization σ. Thin targets substrate influence corrected.

doi: 10.1103/PhysRevA.54.3067
Citations: PlumX Metrics

1993WA27      Chin.Phys.Lett. 10, 397 (1993)

S.Wang, J.Zhang, C.Xiao, W.Xiong, J.Kou, X.Xia, Y.Zhong

Split-Bin Correlation Functions for Multi-Particle Processes in PP Collisions at 400 GeV/c

NUCLEAR REACTIONS ¹H(p, X), E at 400 GeV/c; measured charged particle pseudorapidity, azimuthal angluar distribution; deduced correlations production by resonance-like processes. Split-bin correlation function calculations.

doi: 10.1088/0256-307X/10/7/004
Citations: PlumX Metrics

1993XI03      Chin.J.Nucl.Phys. 15, No 3, 248 (1993)

Z.Xia, H.Ma, X.Xia, Y.Zhong, H.Liu, X.Lu

Polarization of L₁ X-Ray Emitted from He⁺²-Au Impact Ionization

NUCLEAR REACTIONS ¹⁹⁷Au(α, X), E=1.2-4.5 MeV; measured L X-ray polarization vs projectile velocity.

ATOMIC PHYSICS ¹⁹⁷Au(α, X), E=1.2-4.5 MeV; measured L X-ray polarization vs projectile velocity.

Note: The following list of authors and aliases matches the search parameter X.Xia: , X.J.XIA, X.L.XIA, X.W.XIA, X.Y.XIA