{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:SCSSSQVHMJLRLBJKTISHFZUIWB","short_pith_number":"pith:SCSSSQVH","schema_version":"1.0","canonical_sha256":"90a52942a7625715852a9a2472e688b05ce371d993f4470433e1f2b3443f1458","source":{"kind":"arxiv","id":"1705.00449","version":4},"attestation_state":"computed","paper":{"title":"$X(4260)$ Revisited: A Coupled Channel Perspective","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bing-Song Zou, Muhammad Naeem Anwar, Yu Lu","submitted_at":"2017-05-01T09:01:24Z","abstract_excerpt":"We calculate the probabilities of various charmed meson molecules for $X(4260)$ under the framework of ${}^3P_0$ model. The results indicate that even though heavy quark spin symmetry forbids $S$ wave coupling of $D_1\\bar{D}$ to the ${}^3S_1$ charmonia ($\\psi(nS)$), the $D$ wave coupling is allowed and not negligible. Under this symmetry, the $D_1\\bar{D}$ can couple to ${}^3D_1$ charmonia ($\\psi(nD)$) via both $S$ and $D$ wave, and the overall coupling is around three times larger than that of $\\psi(nS)$. The $X(4260)$ cannot be a pure molecule but a mixture of a charmonium and various charmed"},"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":"1705.00449","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-01T09:01:24Z","cross_cats_sorted":[],"title_canon_sha256":"497630b09880060039d11c9e679d19051182b6beca863c55973b26ef1c1b11d7","abstract_canon_sha256":"552601598b777d2072c8564d02f47bf5a9ef2d21f6620b4658cb8b2e931179c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:13.566669Z","signature_b64":"KDwEsjnhN0q5aOulS3miDWAcu9Ky8ZXIpQVupXH5XJ8/bn8zajFVzgyGnt+NEH9GcyfTDX9BQ3c8mzZZN3n5DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"90a52942a7625715852a9a2472e688b05ce371d993f4470433e1f2b3443f1458","last_reissued_at":"2026-05-18T00:27:13.566200Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:13.566200Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$X(4260)$ Revisited: A Coupled Channel Perspective","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bing-Song Zou, Muhammad Naeem Anwar, Yu Lu","submitted_at":"2017-05-01T09:01:24Z","abstract_excerpt":"We calculate the probabilities of various charmed meson molecules for $X(4260)$ under the framework of ${}^3P_0$ model. The results indicate that even though heavy quark spin symmetry forbids $S$ wave coupling of $D_1\\bar{D}$ to the ${}^3S_1$ charmonia ($\\psi(nS)$), the $D$ wave coupling is allowed and not negligible. Under this symmetry, the $D_1\\bar{D}$ can couple to ${}^3D_1$ charmonia ($\\psi(nD)$) via both $S$ and $D$ wave, and the overall coupling is around three times larger than that of $\\psi(nS)$. The $X(4260)$ cannot be a pure molecule but a mixture of a charmonium and various charmed"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.00449","kind":"arxiv","version":4},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1705.00449","created_at":"2026-05-18T00:27:13.566275+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.00449v4","created_at":"2026-05-18T00:27:13.566275+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.00449","created_at":"2026-05-18T00:27:13.566275+00:00"},{"alias_kind":"pith_short_12","alias_value":"SCSSSQVHMJLR","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_16","alias_value":"SCSSSQVHMJLRLBJK","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_8","alias_value":"SCSSSQVH","created_at":"2026-05-18T12:31:43.269735+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2503.00552","citing_title":"Study of $1^{--}$ P wave charmoniumlike and bottomoniumlike tetraquark spectroscopy","ref_index":11,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB","json":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB.json","graph_json":"https://pith.science/api/pith-number/SCSSSQVHMJLRLBJKTISHFZUIWB/graph.json","events_json":"https://pith.science/api/pith-number/SCSSSQVHMJLRLBJKTISHFZUIWB/events.json","paper":"https://pith.science/paper/SCSSSQVH"},"agent_actions":{"view_html":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB","download_json":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB.json","view_paper":"https://pith.science/paper/SCSSSQVH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.00449&json=true","fetch_graph":"https://pith.science/api/pith-number/SCSSSQVHMJLRLBJKTISHFZUIWB/graph.json","fetch_events":"https://pith.science/api/pith-number/SCSSSQVHMJLRLBJKTISHFZUIWB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB/action/storage_attestation","attest_author":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB/action/author_attestation","sign_citation":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB/action/citation_signature","submit_replication":"https://pith.science/pith/SCSSSQVHMJLRLBJKTISHFZUIWB/action/replication_record"}},"created_at":"2026-05-18T00:27:13.566275+00:00","updated_at":"2026-05-18T00:27:13.566275+00:00"}