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The \(\Lambda_c(2860),\; \Lambda_c(2880),\; \Xi_{c}(3055)\; \text{and}\; \Xi_{c}(3080)\) as D-wave baryon states in QCD

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Publication:1695949
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DOI10.1016/j.nuclphysb.2017.11.014zbMath1380.81449arXiv1705.07745OpenAlexW2619757149MaRDI QIDQ1695949

Zhi-Gang Wang

Publication date: 14 February 2018

Published in: Nuclear Physics. B (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/1705.07745



Mathematics Subject Classification ID

Nuclear physics (81V35) Strong interaction, including quantum chromodynamics (81V05)


Related Items (1)

Spectrum of nonstrange singly charmed baryons in the constituent quark model



Cites Work

  • Analysis of the Zc(4200) as axial-vector molecule-like state
  • HEAVY BARYONS IN A QUARK MODEL
  • Analysis of the Triply Heavy Baryon States with QCD Sum Rules
  • Analysis of the Light-Flavor Scalar and Axial-Vector Diquark States with QCD Sum Rules
  • Temperature Dependence of Decuplet Baryon Masses from Thermal QCD Sum Rules


This page was built for publication: The \(\Lambda_c(2860),\; \Lambda_c(2880),\; \Xi_{c}(3055)\; \text{and}\; \Xi_{c}(3080)\) as D-wave baryon states in QCD

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