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By considering only the S-wave $MM'$-pair contributions without resonance effects, the decays of ${\\bf B_c}\\to {\\bf B_n}MM'$ can be decomposed into irreducible forms with 11 parameters under $SU(3)_f$, which are fitted by the 14 existing data, resulting in a reasonable value of $\\chi^2/d.o.f=2.8$ for the fit."},"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":"1810.01079","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-10-02T05:44:50Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"7445985def4a48874a6c21380b1c6b64cb5bd0aa1326e0057bf30262c9113781","abstract_canon_sha256":"151bbd2af7480b808dcada91b6c875134cabe9fdadf67585b2bdd50c4e5137ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:48:31.943699Z","signature_b64":"XDvM5pfTbloDw91PdFwnWGLnSpXoGExJZmJxi2d63WmLI+HT77/kILc5NwU4M3ERT2+kwgkuxGLBvOQeKSdSBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e69fe8398b7ab42398465bc926f6e08bee00cbcccac7b97e70aa56bcf9f0cbd2","last_reissued_at":"2026-05-17T23:48:31.943169Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:48:31.943169Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three-body charmed baryon Decays with SU(3) flavor symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Chia-Wei Liu, C.Q. 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