{"paper":{"title":"Doubly Heavy Baryon Production at A High Luminosity $e^+ e^-$ Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jun Jiang, Qi-Li Liao, Xing-Gang Wu, Xu-Chang Zheng, Zhen-Yun Fang","submitted_at":"2012-08-15T07:56:39Z","abstract_excerpt":"Within the framework of nonrelativistic QCD, we make a detailed discussion on the doubly heavy baryon production through the $e^+ e^-$ annihilation channel, $e^{+}e^{-}\\rightarrow\\gamma/Z^0 \\rightarrow \\Xi_{QQ^{\\prime}} +\\bar{Q} +\\bar{Q^{\\prime}}$, at a high luminosity $e^{+}e^{-}$ collider. Here $Q^{(\\prime)}$ stands for the heavy $b$ or $c$ quark. In addition to the channel through the usually considered diquark state $(QQ^{\\prime})[^3S_1]_{\\bf\\bar{3}}$, contributions from the channels through other same important diquark states such as $(QQ^{\\prime})[^1S_0]_{\\bf 6}$ have also been discussed"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.3051","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}