{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:4J6WGU6OSNRTNCCHB5T6LX72X7","short_pith_number":"pith:4J6WGU6O","schema_version":"1.0","canonical_sha256":"e27d6353ce93633688470f67e5dffabfea7eabd08a8e902d552e34f10194e9d4","source":{"kind":"arxiv","id":"2212.13683","version":3},"attestation_state":"computed","paper":{"title":"Exploring the molecular scenario of X(4160)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dazhuang He, Hao Sun, Ruitian Li, Xuan Luo","submitted_at":"2022-12-28T03:40:26Z","abstract_excerpt":"In this work, we investigate the decays of meson $X(4160)$ in the molecular frame. By using an effective lagrangian approach, we calculate the widths of $X(4160)\\to J/\\psi\\phi$, $D^*\\bar{D}^*$, $D^*\\bar{D}$ and $D\\bar{D}$ through the triangle loop mechanism in the molecular scenario. Based on the compositeness condition, the coupling between $X(4160)$ and the $D_s^*\\bar{D}_s^*$ molecular state is determined. The other coupling constants used are determined phenomenologically. The calculation of the decay widths shows that the $D^*\\bar{D}^*$ decay mode has a larger branching ratio. These predic"},"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":"2212.13683","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-12-28T03:40:26Z","cross_cats_sorted":[],"title_canon_sha256":"70d5782c038348f01fac162faab2ac5077adb7264f283aa96b1790f07c5accdd","abstract_canon_sha256":"91c1ccff9efc6436fd24a3b103a5272a4ebc1571a9cb9996fd79eabd337ed6c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:03:46.567069Z","signature_b64":"WYVCIKTe+RsOv2MiQ09ZYg1VZPf6Hah9ESvVefQv1/Lynq+oAreDsWxVfWlT15q6cVOWB3dCqeOQ9IdrYm3MBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e27d6353ce93633688470f67e5dffabfea7eabd08a8e902d552e34f10194e9d4","last_reissued_at":"2026-07-05T09:03:46.566538Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:03:46.566538Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploring the molecular scenario of X(4160)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dazhuang He, Hao Sun, Ruitian Li, Xuan Luo","submitted_at":"2022-12-28T03:40:26Z","abstract_excerpt":"In this work, we investigate the decays of meson $X(4160)$ in the molecular frame. By using an effective lagrangian approach, we calculate the widths of $X(4160)\\to J/\\psi\\phi$, $D^*\\bar{D}^*$, $D^*\\bar{D}$ and $D\\bar{D}$ through the triangle loop mechanism in the molecular scenario. Based on the compositeness condition, the coupling between $X(4160)$ and the $D_s^*\\bar{D}_s^*$ molecular state is determined. The other coupling constants used are determined phenomenologically. The calculation of the decay widths shows that the $D^*\\bar{D}^*$ decay mode has a larger branching ratio. These predic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.13683","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2212.13683/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2212.13683","created_at":"2026-07-05T09:03:46.566612+00:00"},{"alias_kind":"arxiv_version","alias_value":"2212.13683v3","created_at":"2026-07-05T09:03:46.566612+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.13683","created_at":"2026-07-05T09:03:46.566612+00:00"},{"alias_kind":"pith_short_12","alias_value":"4J6WGU6OSNRT","created_at":"2026-07-05T09:03:46.566612+00:00"},{"alias_kind":"pith_short_16","alias_value":"4J6WGU6OSNRTNCCH","created_at":"2026-07-05T09:03:46.566612+00:00"},{"alias_kind":"pith_short_8","alias_value":"4J6WGU6O","created_at":"2026-07-05T09:03:46.566612+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7","json":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7.json","graph_json":"https://pith.science/api/pith-number/4J6WGU6OSNRTNCCHB5T6LX72X7/graph.json","events_json":"https://pith.science/api/pith-number/4J6WGU6OSNRTNCCHB5T6LX72X7/events.json","paper":"https://pith.science/paper/4J6WGU6O"},"agent_actions":{"view_html":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7","download_json":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7.json","view_paper":"https://pith.science/paper/4J6WGU6O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2212.13683&json=true","fetch_graph":"https://pith.science/api/pith-number/4J6WGU6OSNRTNCCHB5T6LX72X7/graph.json","fetch_events":"https://pith.science/api/pith-number/4J6WGU6OSNRTNCCHB5T6LX72X7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7/action/storage_attestation","attest_author":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7/action/author_attestation","sign_citation":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7/action/citation_signature","submit_replication":"https://pith.science/pith/4J6WGU6OSNRTNCCHB5T6LX72X7/action/replication_record"}},"created_at":"2026-07-05T09:03:46.566612+00:00","updated_at":"2026-07-05T09:03:46.566612+00:00"}