{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:5ZIAF2WEHENCCXAIZMOFQI4VSY","short_pith_number":"pith:5ZIAF2WE","schema_version":"1.0","canonical_sha256":"ee5002eac4391a215c08cb1c582395961d32f39c41a882a0776c734ed00e78ab","source":{"kind":"arxiv","id":"1210.2624","version":1},"attestation_state":"computed","paper":{"title":"Renormalized Quarkonium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"D. R. Entem, E. Ruiz Arriola, F. Fern\\'andez, J. Segovia","submitted_at":"2012-10-09T14:58:10Z","abstract_excerpt":"We extend our previous study of the vector charmonium states within a renormalization approach with boundary conditions to the full spectrum of charmonium and bottomonium. On the light of the predicted spectrum we comply to assignments suggested in the literature. A comparison with the regularized quark model is also included."},"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":"1210.2624","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-10-09T14:58:10Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"2be8cf2fd1fe20999f1a9c26c5d4bb783eff7b99feda803d37a4ea20e9bb31a5","abstract_canon_sha256":"9e3ea68e478f3491f071172efe7f220b458074f12fc605f57ea6c2e1fd152874"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:54:04.046995Z","signature_b64":"xXeP2ms00JiVTdrJ3PCXitHhbWhj/PNt81EIzBtYlZ2egYkKVveBhFr1GKOPR+dfXTs9kohwt33B1FRUwrbeCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee5002eac4391a215c08cb1c582395961d32f39c41a882a0776c734ed00e78ab","last_reissued_at":"2026-05-18T01:54:04.046338Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:54:04.046338Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Renormalized Quarkonium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"D. R. Entem, E. Ruiz Arriola, F. Fern\\'andez, J. Segovia","submitted_at":"2012-10-09T14:58:10Z","abstract_excerpt":"We extend our previous study of the vector charmonium states within a renormalization approach with boundary conditions to the full spectrum of charmonium and bottomonium. On the light of the predicted spectrum we comply to assignments suggested in the literature. A comparison with the regularized quark model is also included."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.2624","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1210.2624","created_at":"2026-05-18T01:54:04.046435+00:00"},{"alias_kind":"arxiv_version","alias_value":"1210.2624v1","created_at":"2026-05-18T01:54:04.046435+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.2624","created_at":"2026-05-18T01:54:04.046435+00:00"},{"alias_kind":"pith_short_12","alias_value":"5ZIAF2WEHENC","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"5ZIAF2WEHENCCXAI","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"5ZIAF2WE","created_at":"2026-05-18T12:26:56.085431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY","json":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY.json","graph_json":"https://pith.science/api/pith-number/5ZIAF2WEHENCCXAIZMOFQI4VSY/graph.json","events_json":"https://pith.science/api/pith-number/5ZIAF2WEHENCCXAIZMOFQI4VSY/events.json","paper":"https://pith.science/paper/5ZIAF2WE"},"agent_actions":{"view_html":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY","download_json":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY.json","view_paper":"https://pith.science/paper/5ZIAF2WE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1210.2624&json=true","fetch_graph":"https://pith.science/api/pith-number/5ZIAF2WEHENCCXAIZMOFQI4VSY/graph.json","fetch_events":"https://pith.science/api/pith-number/5ZIAF2WEHENCCXAIZMOFQI4VSY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY/action/storage_attestation","attest_author":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY/action/author_attestation","sign_citation":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY/action/citation_signature","submit_replication":"https://pith.science/pith/5ZIAF2WEHENCCXAIZMOFQI4VSY/action/replication_record"}},"created_at":"2026-05-18T01:54:04.046435+00:00","updated_at":"2026-05-18T01:54:04.046435+00:00"}