{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:UKOLMMCRH3JLQ3WIU6AAZQBVG7","short_pith_number":"pith:UKOLMMCR","schema_version":"1.0","canonical_sha256":"a29cb630513ed2b86ec8a7800cc03537f3b83902d8fd584fa568c32e92188385","source":{"kind":"arxiv","id":"2005.08219","version":1},"attestation_state":"computed","paper":{"title":"Microscopic Model of Charmonium Strong Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D.R. Entem, F. Fern\\'andez, J. Segovia","submitted_at":"2020-05-17T11:01:17Z","abstract_excerpt":"Although the spectra of heavy quarkonium systems has been successfully explained by certain QCD motivated potential models, their strong decays are difficult to deal with. We perform a microscopic calculation of charmonium strong decays using the same constituent quark model which successfully describes the $c\\bar{c}$ meson spectrum. We compare the numerical results with the $^{3}P_{0}$ and the experimental data. Comparison with other predictions from similar models are 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":"2005.08219","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-05-17T11:01:17Z","cross_cats_sorted":[],"title_canon_sha256":"39e426b1117dc8fd44fc2551627f6ba34b55f7332552bd50982c0dbd1a7beee2","abstract_canon_sha256":"938cc31875d745647194e603a0f1136e0518e935d07f100791adad439bb966b8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:03:29.375343Z","signature_b64":"hbL0da9ixLPd/nKm3Sc6Dd/E3BYHxKh6NlNmNzQ/qhle/3OHM0uUuNu2kJursZM9NWXHYh5hm/5KJbkItIy2CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a29cb630513ed2b86ec8a7800cc03537f3b83902d8fd584fa568c32e92188385","last_reissued_at":"2026-07-05T01:03:29.374880Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:03:29.374880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microscopic Model of Charmonium Strong Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D.R. Entem, F. Fern\\'andez, J. Segovia","submitted_at":"2020-05-17T11:01:17Z","abstract_excerpt":"Although the spectra of heavy quarkonium systems has been successfully explained by certain QCD motivated potential models, their strong decays are difficult to deal with. We perform a microscopic calculation of charmonium strong decays using the same constituent quark model which successfully describes the $c\\bar{c}$ meson spectrum. We compare the numerical results with the $^{3}P_{0}$ and the experimental data. Comparison with other predictions from similar models are included."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.08219","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2005.08219/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":"2005.08219","created_at":"2026-07-05T01:03:29.374935+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.08219v1","created_at":"2026-07-05T01:03:29.374935+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.08219","created_at":"2026-07-05T01:03:29.374935+00:00"},{"alias_kind":"pith_short_12","alias_value":"UKOLMMCRH3JL","created_at":"2026-07-05T01:03:29.374935+00:00"},{"alias_kind":"pith_short_16","alias_value":"UKOLMMCRH3JLQ3WI","created_at":"2026-07-05T01:03:29.374935+00:00"},{"alias_kind":"pith_short_8","alias_value":"UKOLMMCR","created_at":"2026-07-05T01:03:29.374935+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/UKOLMMCRH3JLQ3WIU6AAZQBVG7","json":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7.json","graph_json":"https://pith.science/api/pith-number/UKOLMMCRH3JLQ3WIU6AAZQBVG7/graph.json","events_json":"https://pith.science/api/pith-number/UKOLMMCRH3JLQ3WIU6AAZQBVG7/events.json","paper":"https://pith.science/paper/UKOLMMCR"},"agent_actions":{"view_html":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7","download_json":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7.json","view_paper":"https://pith.science/paper/UKOLMMCR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.08219&json=true","fetch_graph":"https://pith.science/api/pith-number/UKOLMMCRH3JLQ3WIU6AAZQBVG7/graph.json","fetch_events":"https://pith.science/api/pith-number/UKOLMMCRH3JLQ3WIU6AAZQBVG7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7/action/storage_attestation","attest_author":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7/action/author_attestation","sign_citation":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7/action/citation_signature","submit_replication":"https://pith.science/pith/UKOLMMCRH3JLQ3WIU6AAZQBVG7/action/replication_record"}},"created_at":"2026-07-05T01:03:29.374935+00:00","updated_at":"2026-07-05T01:03:29.374935+00:00"}