{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:SLC5YVGXCPGSCZLXVYMGTBRLU4","short_pith_number":"pith:SLC5YVGX","schema_version":"1.0","canonical_sha256":"92c5dc54d713cd216577ae1869862ba72932c1d1ce8dea982673a921bfa3b96d","source":{"kind":"arxiv","id":"1704.06763","version":3},"attestation_state":"computed","paper":{"title":"The analysis of the charmonium-like states $X^{*}(3860)$,$X(3872)$, $X(3915)$, $X(3930)$ and $X(3940)$ according to its strong decay behaviors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guo Liang Yu, Zhen Yu Li, Zhi Gang Wang","submitted_at":"2017-04-22T08:11:21Z","abstract_excerpt":"Inspired by the newly observed state $X^{*}(3860)$, we analyze the strong decay behaviors of some charmonium-like states $X^{*}(3860)$,$X(3872)$, $X(3915)$, $X(3930)$ and $X(3940)$ by the $^{3}P_{0}$ model. We carry out our work based on the hypothesis that these states are all being the charmonium systems. Our analysis indicates that $0^{++}$ charmonium state can be a good candidate for $X^{*}(3860)$ and $1^{++}$ state is the possible assignment for $X(3872)$. Considering as the $3^{1}S_{0}$ state, the decay behavior of $X(3940)$ is inconsistent with the experimental data. So, we can not assi"},"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":"1704.06763","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-22T08:11:21Z","cross_cats_sorted":[],"title_canon_sha256":"34d751884f4a5d61272f5653cb0cd8e1b62abb7295c4258559905f67de4c9055","abstract_canon_sha256":"f025e77c7fe2ddce64de927d207ffa8db430fde1e5e1ce01e5116196e357173f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:00:27.662547Z","signature_b64":"OxJ5d+vYUHkBnyz1yT2uWBhoOE6rQKPDKTNxILOWkQfCFG3A7YYv2VZ1Br8DOo/JK/1/Fdz4Kq/yzz4klLP6Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"92c5dc54d713cd216577ae1869862ba72932c1d1ce8dea982673a921bfa3b96d","last_reissued_at":"2026-07-05T06:00:27.662014Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:00:27.662014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The analysis of the charmonium-like states $X^{*}(3860)$,$X(3872)$, $X(3915)$, $X(3930)$ and $X(3940)$ according to its strong decay behaviors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guo Liang Yu, Zhen Yu Li, Zhi Gang Wang","submitted_at":"2017-04-22T08:11:21Z","abstract_excerpt":"Inspired by the newly observed state $X^{*}(3860)$, we analyze the strong decay behaviors of some charmonium-like states $X^{*}(3860)$,$X(3872)$, $X(3915)$, $X(3930)$ and $X(3940)$ by the $^{3}P_{0}$ model. We carry out our work based on the hypothesis that these states are all being the charmonium systems. Our analysis indicates that $0^{++}$ charmonium state can be a good candidate for $X^{*}(3860)$ and $1^{++}$ state is the possible assignment for $X(3872)$. Considering as the $3^{1}S_{0}$ state, the decay behavior of $X(3940)$ is inconsistent with the experimental data. So, we can not assi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.06763","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/1704.06763/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":"1704.06763","created_at":"2026-07-05T06:00:27.662076+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.06763v3","created_at":"2026-07-05T06:00:27.662076+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.06763","created_at":"2026-07-05T06:00:27.662076+00:00"},{"alias_kind":"pith_short_12","alias_value":"SLC5YVGXCPGS","created_at":"2026-07-05T06:00:27.662076+00:00"},{"alias_kind":"pith_short_16","alias_value":"SLC5YVGXCPGSCZLX","created_at":"2026-07-05T06:00:27.662076+00:00"},{"alias_kind":"pith_short_8","alias_value":"SLC5YVGX","created_at":"2026-07-05T06:00:27.662076+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.12149","citing_title":"Study on charmonium(-like) mesons within a diabatic approach","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4","json":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4.json","graph_json":"https://pith.science/api/pith-number/SLC5YVGXCPGSCZLXVYMGTBRLU4/graph.json","events_json":"https://pith.science/api/pith-number/SLC5YVGXCPGSCZLXVYMGTBRLU4/events.json","paper":"https://pith.science/paper/SLC5YVGX"},"agent_actions":{"view_html":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4","download_json":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4.json","view_paper":"https://pith.science/paper/SLC5YVGX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.06763&json=true","fetch_graph":"https://pith.science/api/pith-number/SLC5YVGXCPGSCZLXVYMGTBRLU4/graph.json","fetch_events":"https://pith.science/api/pith-number/SLC5YVGXCPGSCZLXVYMGTBRLU4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4/action/storage_attestation","attest_author":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4/action/author_attestation","sign_citation":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4/action/citation_signature","submit_replication":"https://pith.science/pith/SLC5YVGXCPGSCZLXVYMGTBRLU4/action/replication_record"}},"created_at":"2026-07-05T06:00:27.662076+00:00","updated_at":"2026-07-05T06:00:27.662076+00:00"}