{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:A6DIY6UKQ4LIEXSLYAJSTTLX47","short_pith_number":"pith:A6DIY6UK","schema_version":"1.0","canonical_sha256":"07868c7a8a8716825e4bc01329cd77e7fb95698c745297974f310313c4c70654","source":{"kind":"arxiv","id":"hep-ph/0701208","version":3},"attestation_state":"computed","paper":{"title":"Quarkonia and their transitions","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Estia Eichten, Hanna Mahlke, Jonathan L. Rosner, Stephen Godfrey","submitted_at":"2007-01-24T19:35:24Z","abstract_excerpt":"Valuable data on quarkonia (the bound states of a heavy quark Q=c,b and the corresponding antiquark) have recently been provided by a variety of sources, mainly e+ e- collisions, but also hadronic interactions. This permits a thorough updating of the experimental and theoretical status of electromagnetic and strong transitions in quarkonia. We discuss QQbar transitions to other QQbar states, with some reference to processes involving QQbar annihilation."},"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/0701208","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-01-24T19:35:24Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"419a04b631dbe4f6489aa5b493646ccf27f09b7819daeaeead01ebe8073052f8","abstract_canon_sha256":"6849bdfe41af1999c69a214b233ce4f8cbeea2c1ec085c950185aea2ba139fa5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:34:27.849480Z","signature_b64":"Jca+0v6SD+c54oLLSe13k2gagGmHFrBrxfd1Q25JzrRRsaJqNy1jPzR7ZqNG6Okzr3ItEDyJuvsHfVH0UuTcBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07868c7a8a8716825e4bc01329cd77e7fb95698c745297974f310313c4c70654","last_reissued_at":"2026-07-04T15:34:27.849094Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:34:27.849094Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quarkonia and their transitions","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Estia Eichten, Hanna Mahlke, Jonathan L. Rosner, Stephen Godfrey","submitted_at":"2007-01-24T19:35:24Z","abstract_excerpt":"Valuable data on quarkonia (the bound states of a heavy quark Q=c,b and the corresponding antiquark) have recently been provided by a variety of sources, mainly e+ e- collisions, but also hadronic interactions. This permits a thorough updating of the experimental and theoretical status of electromagnetic and strong transitions in quarkonia. We discuss QQbar transitions to other QQbar states, with some reference to processes involving QQbar annihilation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0701208","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/hep-ph/0701208/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/0701208","created_at":"2026-07-04T15:34:27.849157+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0701208v3","created_at":"2026-07-04T15:34:27.849157+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0701208","created_at":"2026-07-04T15:34:27.849157+00:00"},{"alias_kind":"pith_short_12","alias_value":"A6DIY6UKQ4LI","created_at":"2026-07-04T15:34:27.849157+00:00"},{"alias_kind":"pith_short_16","alias_value":"A6DIY6UKQ4LIEXSL","created_at":"2026-07-04T15:34:27.849157+00:00"},{"alias_kind":"pith_short_8","alias_value":"A6DIY6UK","created_at":"2026-07-04T15:34:27.849157+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.08489","citing_title":"Principles and Possibilities for Bound States in Gauge Theory","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2606.08489","citing_title":"Principles and Possibilities for Bound States in Gauge Theory","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47","json":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47.json","graph_json":"https://pith.science/api/pith-number/A6DIY6UKQ4LIEXSLYAJSTTLX47/graph.json","events_json":"https://pith.science/api/pith-number/A6DIY6UKQ4LIEXSLYAJSTTLX47/events.json","paper":"https://pith.science/paper/A6DIY6UK"},"agent_actions":{"view_html":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47","download_json":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47.json","view_paper":"https://pith.science/paper/A6DIY6UK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0701208&json=true","fetch_graph":"https://pith.science/api/pith-number/A6DIY6UKQ4LIEXSLYAJSTTLX47/graph.json","fetch_events":"https://pith.science/api/pith-number/A6DIY6UKQ4LIEXSLYAJSTTLX47/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47/action/storage_attestation","attest_author":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47/action/author_attestation","sign_citation":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47/action/citation_signature","submit_replication":"https://pith.science/pith/A6DIY6UKQ4LIEXSLYAJSTTLX47/action/replication_record"}},"created_at":"2026-07-04T15:34:27.849157+00:00","updated_at":"2026-07-04T15:34:27.849157+00:00"}