{
  "abstract": "Motivated by the rapidly accumulating experimental data, we systematically calculate the $Ξ_c$ and $Ξ_c'$ mass spectra for the $1S$-, $1P$-, and $1D$-wave states and investigate the strong decay properties of the $1P$- and $1D$-wave states, thereby interpreting the internal structure of the currently controversial excited states and providing useful guidance for future experimental searches. The main conclusions are summarized as follows. $Ξ_c(2790)$ and $Ξ_c(2815)$ can be well explained as $Ξ_c1P\\big|J^P=1/2^-,1\\big\\rangle_λ$ and $Ξ_c1P\\big|J^P=3/2^-,1\\big\\rangle_λ$, respectively. $Ξ_c(2882)$ may correspond to $Ξ_c1P\\big|J^P=1/2^-,0\\big\\rangle_ρ$ or $Ξ_c1P\\big|J^P=1/2^-,1\\big\\rangle_ρ$; under this interpretation, $Ξ_cπ$ and $Ξ_c'π$ would be promising channels for its detection. $Ξ_c(2923)$ might be assigned to $Ξ_c'1P\\big|J^P=3/2^-,1\\big\\rangle_λ$, but further confirmation is required. $Ξ_c(2939)$ is very likely to be $Ξ_c'1P\\big|J^P=3/2^-,2\\big\\rangle_λ$ and has a good potential to be observed in the final states $Ξ_cπ$ and $Ξ_c'^{*}π$. $Ξ_c(2965)$ can be explained as $Ξ_c'1P\\big|J^P=5/2^-,2\\big\\rangle_λ$ and $Ξ_cπ$ decay channel is a promising additional mode for future experimental searches. $Ξ_c(3055)$ and $Ξ_c(3080)$ can be assigned as the quark configurations $Ξ_c1D\\big|J^P=3/2^+,2\\big\\rangle_{λλ}$ and $Ξ_c1D\\big|J^P=5/2^+,2\\big\\rangle_{λλ}$, respectively. $Ξ_c(3123)$ is possibly state $Ξ_c'1D\\big|J^P=1/2^+,1\\big\\rangle_{λλ}$ or $Ξ_c'1D\\big|J^P=5/2^+,3\\big\\rangle_{λλ}$, with the latter being more favorable. Decay channels $Λ/ΣD$ are very likely to serve as a criterion for distinguishing between these two possible candidates.",
  "abstract_shown": true,
  "affiliations": [],
  "article_type": null,
  "arxiv": "2611.00666",
  "author_total": 4,
  "authors": [
    {
      "name": "Yi-Heng Wang"
    },
    {
      "name": "Xin-Yu Chang"
    },
    {
      "name": "Hui-Hua Zhong"
    },
    {
      "name": "Li-Ye Xiao"
    }
  ],
  "bibtex": "https://research.draconitic.com/paper/5t90p0a2pensj.bib",
  "cited_by": 0,
  "doi": "10.48550/arxiv.2611.00666",
  "fulltext_url": null,
  "id": "5t90p0a2pensj",
  "issns": [],
  "landing_url": "https://arxiv.org/abs/2611.00666",
  "language": null,
  "licence": "LicenseRef-arXiv-nonexclusive-1.0",
  "licence_label": "arXiv licence",
  "licence_source": "article",
  "licence_url": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
  "metadata_licence": "CC0-1.0",
  "native_subjects": [
    [
      "arxiv",
      "hep-ph"
    ]
  ],
  "openalex": null,
  "pdf_url": "https://arxiv.org/pdf/2611.00666",
  "pmcid": null,
  "pmid": null,
  "published": "2026-11-01",
  "publisher": null,
  "ris": "https://research.draconitic.com/paper/5t90p0a2pensj.ris",
  "sources": [
    {
      "first_seen": "2026-11-03T12:20:59Z",
      "native_id": "2611.00666",
      "source": "arxiv",
      "url": "https://arxiv.org/abs/2611.00666"
    }
  ],
  "subjects": [
    {
      "field": "physics",
      "origin": "arxiv:hep-ph",
      "subfield": "high-energy"
    }
  ],
  "title": "Exploring the properties of low-lying excited $Ξ_c$ and $Ξ_c'$ baryons",
  "title_text": "Exploring the properties of low-lying excited Ξ_c and Ξ_c' baryons",
  "type": "preprint",
  "updated_at": "2026-11-05T15:20:18Z",
  "url": "https://research.draconitic.com/paper/5t90p0a2pensj",
  "venue": "arXiv",
  "versions": []
}