{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:HL3XPLGLHSVYSACSCTVTFIC6HS","short_pith_number":"pith:HL3XPLGL","schema_version":"1.0","canonical_sha256":"3af777accb3cab89005214eb32a05e3c88b7d9ae6a4f5d00c26c14d05505d583","source":{"kind":"arxiv","id":"2107.14438","version":2},"attestation_state":"computed","paper":{"title":"Where are $3P$ and higher $P-$wave states in the charmonium family?","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ming-Xiao Duan, Xiang Liu","submitted_at":"2021-07-30T05:57:22Z","abstract_excerpt":"How to hunt for higher $P$-wave states of charmonium is still an open topic when $2P$ charmonia were identified. {In this work, we present an unquenched quark model calculation to illustrate the spectroscopy behavior of these $3P$, $4P$ and $5P$ states in charmonium family.} For the $3P$ charmonia, the predicted masses are around 4.2 GeV and their two-body open-charm decay behaviors were given, by which we propose that searching for these $3P$ states via their open-charm decay channels from $\\gamma\\gamma$ fusion and $B$ decay can be accessible at future experiment like LHCb and Belle II. We co"},"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":"2107.14438","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"hep-ph","submitted_at":"2021-07-30T05:57:22Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"b0c5074119768d507351e08d104f5b7c3b40c980ad71d9375109fa67fc25561a","abstract_canon_sha256":"8167ae1f500011e1c83eb40e45aaca7157d99e13c5265546f35de9d81ca619fd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:22:36.306812Z","signature_b64":"JVoSypGPpGQZrQG9bnvKz2yD9QnyJqIu9c7ZCkEIP+ZKF/IMJFVonvtX0hbab7WGDMFRFO/QIuFiwai02yjQAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3af777accb3cab89005214eb32a05e3c88b7d9ae6a4f5d00c26c14d05505d583","last_reissued_at":"2026-07-05T03:22:36.306303Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:22:36.306303Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Where are $3P$ and higher $P-$wave states in the charmonium family?","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ming-Xiao Duan, Xiang Liu","submitted_at":"2021-07-30T05:57:22Z","abstract_excerpt":"How to hunt for higher $P$-wave states of charmonium is still an open topic when $2P$ charmonia were identified. {In this work, we present an unquenched quark model calculation to illustrate the spectroscopy behavior of these $3P$, $4P$ and $5P$ states in charmonium family.} For the $3P$ charmonia, the predicted masses are around 4.2 GeV and their two-body open-charm decay behaviors were given, by which we propose that searching for these $3P$ states via their open-charm decay channels from $\\gamma\\gamma$ fusion and $B$ decay can be accessible at future experiment like LHCb and Belle II. We co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.14438","kind":"arxiv","version":2},"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/2107.14438/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":"2107.14438","created_at":"2026-07-05T03:22:36.306382+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.14438v2","created_at":"2026-07-05T03:22:36.306382+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.14438","created_at":"2026-07-05T03:22:36.306382+00:00"},{"alias_kind":"pith_short_12","alias_value":"HL3XPLGLHSVY","created_at":"2026-07-05T03:22:36.306382+00:00"},{"alias_kind":"pith_short_16","alias_value":"HL3XPLGLHSVYSACS","created_at":"2026-07-05T03:22:36.306382+00:00"},{"alias_kind":"pith_short_8","alias_value":"HL3XPLGL","created_at":"2026-07-05T03:22:36.306382+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.17832","citing_title":"Higher excited charmed and charmed-strange mesons in an unquenched quark model","ref_index":86,"is_internal_anchor":false},{"citing_arxiv_id":"2604.17193","citing_title":"Proposed mixing between $2P$ and $1F$ wave charmonia","ref_index":40,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS","json":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS.json","graph_json":"https://pith.science/api/pith-number/HL3XPLGLHSVYSACSCTVTFIC6HS/graph.json","events_json":"https://pith.science/api/pith-number/HL3XPLGLHSVYSACSCTVTFIC6HS/events.json","paper":"https://pith.science/paper/HL3XPLGL"},"agent_actions":{"view_html":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS","download_json":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS.json","view_paper":"https://pith.science/paper/HL3XPLGL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.14438&json=true","fetch_graph":"https://pith.science/api/pith-number/HL3XPLGLHSVYSACSCTVTFIC6HS/graph.json","fetch_events":"https://pith.science/api/pith-number/HL3XPLGLHSVYSACSCTVTFIC6HS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS/action/storage_attestation","attest_author":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS/action/author_attestation","sign_citation":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS/action/citation_signature","submit_replication":"https://pith.science/pith/HL3XPLGLHSVYSACSCTVTFIC6HS/action/replication_record"}},"created_at":"2026-07-05T03:22:36.306382+00:00","updated_at":"2026-07-05T03:22:36.306382+00:00"}