{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:ME2M73CH74337XWXVONPQTGJCC","short_pith_number":"pith:ME2M73CH","schema_version":"1.0","canonical_sha256":"6134cfec47ff37bfded7ab9af84cc910bb7f24049f586671b756c02fa9c4c35c","source":{"kind":"arxiv","id":"hep-ph/0211457","version":2},"attestation_state":"computed","paper":{"title":"Covariant tensor formalism for partial wave analyses of psi decay to mesons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Beijing), B.S.Zou (IHEP, D.V.Bugg (QMC, London)","submitted_at":"2002-11-29T12:10:53Z","abstract_excerpt":"J/psi and psi' decay to mesons are a good place to look for glueballs, hybrids and for extracting strange and nonstrange components in mesons. Abundant J/psi and psi' events have been collected at the Beijing Electron Positron Collider (BEPC). More data will be collected at upgraded BEPC and CLEO-C. Here we provide explicit PWA formulae for many interesting channels in the covariant tensor formalism."},"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":"hep-ph/0211457","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-11-29T12:10:53Z","cross_cats_sorted":[],"title_canon_sha256":"f3e433258bdbafa66f5c8c8aa584f2658cabcdd879ceebde952c5fb4b2191e91","abstract_canon_sha256":"2921053c5db0e4b16a8ba00b3e83c61c836c15b5949ec5ec2b806b5e8354a9df"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:28:30.911703Z","signature_b64":"Vfu3fy+LQBTSG4niVvWpZKqIZ/dmWNEFClvIq12z18wsHQ4WCXNna/riziZ8+56dByNUMslH4b7LGYx4usx7Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6134cfec47ff37bfded7ab9af84cc910bb7f24049f586671b756c02fa9c4c35c","last_reissued_at":"2026-07-04T14:28:30.911276Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:28:30.911276Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Covariant tensor formalism for partial wave analyses of psi decay to mesons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Beijing), B.S.Zou (IHEP, D.V.Bugg (QMC, London)","submitted_at":"2002-11-29T12:10:53Z","abstract_excerpt":"J/psi and psi' decay to mesons are a good place to look for glueballs, hybrids and for extracting strange and nonstrange components in mesons. Abundant J/psi and psi' events have been collected at the Beijing Electron Positron Collider (BEPC). More data will be collected at upgraded BEPC and CLEO-C. Here we provide explicit PWA formulae for many interesting channels in the covariant tensor formalism."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0211457","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/hep-ph/0211457/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":"hep-ph/0211457","created_at":"2026-07-04T14:28:30.911341+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0211457v2","created_at":"2026-07-04T14:28:30.911341+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0211457","created_at":"2026-07-04T14:28:30.911341+00:00"},{"alias_kind":"pith_short_12","alias_value":"ME2M73CH7433","created_at":"2026-07-04T14:28:30.911341+00:00"},{"alias_kind":"pith_short_16","alias_value":"ME2M73CH74337XWX","created_at":"2026-07-04T14:28:30.911341+00:00"},{"alias_kind":"pith_short_8","alias_value":"ME2M73CH","created_at":"2026-07-04T14:28:30.911341+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.07225","citing_title":"Simultaneous Dalitz-plot decomposition of the $e^+ e^- \\to J/\\psi \\, \\pi \\, \\pi \\, (K \\bar{K})$ processes in the 4.13-4.36 GeV region using dispersive final-state interactions","ref_index":40,"is_internal_anchor":true},{"citing_arxiv_id":"2502.13540","citing_title":"Amplitude analysis of $\\psi(3686)\\to \\gamma K_S^0 K_S^0 $","ref_index":41,"is_internal_anchor":true},{"citing_arxiv_id":"2604.27028","citing_title":"Observation of a Doubly-strange Hyperon $\\Xi(1720)$ in $J/\\psi\\rightarrow{}K^{-}\\Sigma^0\\bar{\\Xi}^{+}+c.c.$","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC","json":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC.json","graph_json":"https://pith.science/api/pith-number/ME2M73CH74337XWXVONPQTGJCC/graph.json","events_json":"https://pith.science/api/pith-number/ME2M73CH74337XWXVONPQTGJCC/events.json","paper":"https://pith.science/paper/ME2M73CH"},"agent_actions":{"view_html":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC","download_json":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC.json","view_paper":"https://pith.science/paper/ME2M73CH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0211457&json=true","fetch_graph":"https://pith.science/api/pith-number/ME2M73CH74337XWXVONPQTGJCC/graph.json","fetch_events":"https://pith.science/api/pith-number/ME2M73CH74337XWXVONPQTGJCC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC/action/storage_attestation","attest_author":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC/action/author_attestation","sign_citation":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC/action/citation_signature","submit_replication":"https://pith.science/pith/ME2M73CH74337XWXVONPQTGJCC/action/replication_record"}},"created_at":"2026-07-04T14:28:30.911341+00:00","updated_at":"2026-07-04T14:28:30.911341+00:00"}