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Its electromagnetic (EM) decay is also calculated by the Bethe-Salpeter method within Mandelstam formalism. The strong decay widths are {$\\Gamma[X(3842)\\rightarrow D^{0}\\bar{D}^{0}]=1.28$ MeV}, $\\Gamma[X(3823)\\rightarrow D^{+}D^{-}]=1.08$ MeV, and the ratio ${\\cal B}[X(3842)\\rightarrow D^{+}D^{-}]/{\\cal B}[X(3823)\\rightarrow D^{0}\\bar{D}^{0}]=0.84$. The EM decay"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2308.02280","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-08-04T12:22:16Z","cross_cats_sorted":[],"title_canon_sha256":"2af2b627a3255a545cbf8e1d953dd3284bc9a286c37020bdd3c73adb4f7e256d","abstract_canon_sha256":"6bc04e15a05c12d116edf33efd56b1ed5be10432b3fa342d9e02332ba9a636a2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:32:43.715044Z","signature_b64":"hRmxqy1nAqxs40vX8OJKopt+ujw9kUx2HGNhvBTK5KFqrdxTZLrhwWYsLwrtk5WR/Cjp9r2WJAMGnqbyJXFRAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"050463e8a0fe3bda52a23fb06b5ab16cd127cbf48456366f448d4ce5f6a39e03","last_reissued_at":"2026-07-05T07:32:43.714520Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:32:43.714520Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The decay property of the $X(3842)$ as the $\\psi_{_3}(1^3D_{_3})$ state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guo-Li Wang, Su-Yan Pei, Tai-Fu Feng, Tianhong Wang, Wei Li","submitted_at":"2023-08-04T12:22:16Z","abstract_excerpt":"In this paper, the new particle $X(3842)$ discovered by the LHCb Collaboration is identified to be the $\\psi_{_3}(1^3D_{_3})$ state. We study its strong decays with the combination of the Bethe-Salpeter method and the $^3P_{_0}$ model. Its electromagnetic (EM) decay is also calculated by the Bethe-Salpeter method within Mandelstam formalism. The strong decay widths are {$\\Gamma[X(3842)\\rightarrow D^{0}\\bar{D}^{0}]=1.28$ MeV}, $\\Gamma[X(3823)\\rightarrow D^{+}D^{-}]=1.08$ MeV, and the ratio ${\\cal B}[X(3842)\\rightarrow D^{+}D^{-}]/{\\cal B}[X(3823)\\rightarrow D^{0}\\bar{D}^{0}]=0.84$. 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