{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:GAAACSX23ZSZMMJYMZIEM23P2S","short_pith_number":"pith:GAAACSX2","schema_version":"1.0","canonical_sha256":"3000014afade659631386650466b6fd489d591aa33d77d3317c02cac23ab37b8","source":{"kind":"arxiv","id":"hep-ph/9811518","version":2},"attestation_state":"computed","paper":{"title":"Identification of the glueballs and the scalar meson nonet of lowest mass","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Peter Minkowski, Wolfgang Ochs","submitted_at":"1998-11-30T16:12:39Z","abstract_excerpt":"We discuss the theoretical expectations and phenomenological evidence for the lightest glueballs and the members of the meson nonet with quantum numbers J^PC=0^{++}. We reconsider the recent evidence for candidate states with masses below ~1700 MeV, but include also the results from earlier phase-shift analyses. Arguments are presented to classify the scalars f_0(980) and f_0(1500) as members of the 0^{++} nonet, with a mixing rather similar to that of the pseudoscalars eta' and eta. The S-wave states called f_0(400-1200) and f_0(1370) are considered as different signals from a single broad re"},"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/9811518","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-11-30T16:12:39Z","cross_cats_sorted":[],"title_canon_sha256":"13075c18141e29fb46767bac0b65df1a9d766768e82a007ea4e8b1f13ded51dd","abstract_canon_sha256":"60e9f036ed14ef287c3eaaa2f3efb07fcdb88e40a9f8cb8eccee9b7f29b5fa12"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:18:25.263588Z","signature_b64":"/gxp8mNp5+n0xRjgNHd7ADstbcZYjz/tO4nyYorE7PyAeCGmgtC89ZBWWDLDfin+qHQjsogXSu3ZkCaoACNPDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3000014afade659631386650466b6fd489d591aa33d77d3317c02cac23ab37b8","last_reissued_at":"2026-07-04T15:18:25.263230Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:18:25.263230Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Identification of the glueballs and the scalar meson nonet of lowest mass","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Peter Minkowski, Wolfgang Ochs","submitted_at":"1998-11-30T16:12:39Z","abstract_excerpt":"We discuss the theoretical expectations and phenomenological evidence for the lightest glueballs and the members of the meson nonet with quantum numbers J^PC=0^{++}. We reconsider the recent evidence for candidate states with masses below ~1700 MeV, but include also the results from earlier phase-shift analyses. Arguments are presented to classify the scalars f_0(980) and f_0(1500) as members of the 0^{++} nonet, with a mixing rather similar to that of the pseudoscalars eta' and eta. The S-wave states called f_0(400-1200) and f_0(1370) are considered as different signals from a single broad re"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9811518","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/9811518/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/9811518","created_at":"2026-07-04T15:18:25.263291+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9811518v2","created_at":"2026-07-04T15:18:25.263291+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9811518","created_at":"2026-07-04T15:18:25.263291+00:00"},{"alias_kind":"pith_short_12","alias_value":"GAAACSX23ZSZ","created_at":"2026-07-04T15:18:25.263291+00:00"},{"alias_kind":"pith_short_16","alias_value":"GAAACSX23ZSZMMJY","created_at":"2026-07-04T15:18:25.263291+00:00"},{"alias_kind":"pith_short_8","alias_value":"GAAACSX2","created_at":"2026-07-04T15:18:25.263291+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.11646","citing_title":"All-charm tetraquarks at hadron colliders: A high-precision fragmentation perspective","ref_index":30,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S","json":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S.json","graph_json":"https://pith.science/api/pith-number/GAAACSX23ZSZMMJYMZIEM23P2S/graph.json","events_json":"https://pith.science/api/pith-number/GAAACSX23ZSZMMJYMZIEM23P2S/events.json","paper":"https://pith.science/paper/GAAACSX2"},"agent_actions":{"view_html":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S","download_json":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S.json","view_paper":"https://pith.science/paper/GAAACSX2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9811518&json=true","fetch_graph":"https://pith.science/api/pith-number/GAAACSX23ZSZMMJYMZIEM23P2S/graph.json","fetch_events":"https://pith.science/api/pith-number/GAAACSX23ZSZMMJYMZIEM23P2S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S/action/storage_attestation","attest_author":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S/action/author_attestation","sign_citation":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S/action/citation_signature","submit_replication":"https://pith.science/pith/GAAACSX23ZSZMMJYMZIEM23P2S/action/replication_record"}},"created_at":"2026-07-04T15:18:25.263291+00:00","updated_at":"2026-07-04T15:18:25.263291+00:00"}