{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:HDXT4QC2TDZ7A74QVNO3UFDWLX","short_pith_number":"pith:HDXT4QC2","schema_version":"1.0","canonical_sha256":"38ef3e405a98f3f07f90ab5dba14765dd025eb988e7419d1ea5284d9e85949e1","source":{"kind":"arxiv","id":"1810.11031","version":2},"attestation_state":"computed","paper":{"title":"S-wave heavy quarkonium spectrum with next-to-next-to-next-to-leading logarithmic accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Pineda, C. Anzai, D. Moreno","submitted_at":"2018-10-25T18:00:15Z","abstract_excerpt":"We obtain the Potential NRQCD Lagrangian relevant for S-wave states with next-next-to-next-to-leading logarithmic (NNNLL) accuracy. We compute the heavy quarkonium mass of spin-averaged $l= 0$ (angular momentum) states, with otherwise arbitrary quantum numbers, with NNNLL accuracy. These results are complete up to a missing contribution of the two-loop soft running."},"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":"1810.11031","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-10-25T18:00:15Z","cross_cats_sorted":[],"title_canon_sha256":"595cb0ad00c7b86703d428439f91e5202025a54795a051e2624132155763662a","abstract_canon_sha256":"c4c2b7f84b7ea343b0a4b5706b13c27552c4f1ac8b352cfaefc53e4bf8e2ed05"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:57:08.295938Z","signature_b64":"o302jx3INamPAqkTMkIFriV2wUuRf7uFnmxafN2a8zbxTNsg/xRtErz6BKqR/ynlcaC7gvcdixkkBFcxxvVZDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38ef3e405a98f3f07f90ab5dba14765dd025eb988e7419d1ea5284d9e85949e1","last_reissued_at":"2026-05-17T23:57:08.295422Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:57:08.295422Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"S-wave heavy quarkonium spectrum with next-to-next-to-next-to-leading logarithmic accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Pineda, C. Anzai, D. Moreno","submitted_at":"2018-10-25T18:00:15Z","abstract_excerpt":"We obtain the Potential NRQCD Lagrangian relevant for S-wave states with next-next-to-next-to-leading logarithmic (NNNLL) accuracy. We compute the heavy quarkonium mass of spin-averaged $l= 0$ (angular momentum) states, with otherwise arbitrary quantum numbers, with NNNLL accuracy. These results are complete up to a missing contribution of the two-loop soft running."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.11031","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":""},"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":"1810.11031","created_at":"2026-05-17T23:57:08.295496+00:00"},{"alias_kind":"arxiv_version","alias_value":"1810.11031v2","created_at":"2026-05-17T23:57:08.295496+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.11031","created_at":"2026-05-17T23:57:08.295496+00:00"},{"alias_kind":"pith_short_12","alias_value":"HDXT4QC2TDZ7","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_16","alias_value":"HDXT4QC2TDZ7A74Q","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_8","alias_value":"HDXT4QC2","created_at":"2026-05-18T12:32:28.185984+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/HDXT4QC2TDZ7A74QVNO3UFDWLX","json":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX.json","graph_json":"https://pith.science/api/pith-number/HDXT4QC2TDZ7A74QVNO3UFDWLX/graph.json","events_json":"https://pith.science/api/pith-number/HDXT4QC2TDZ7A74QVNO3UFDWLX/events.json","paper":"https://pith.science/paper/HDXT4QC2"},"agent_actions":{"view_html":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX","download_json":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX.json","view_paper":"https://pith.science/paper/HDXT4QC2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1810.11031&json=true","fetch_graph":"https://pith.science/api/pith-number/HDXT4QC2TDZ7A74QVNO3UFDWLX/graph.json","fetch_events":"https://pith.science/api/pith-number/HDXT4QC2TDZ7A74QVNO3UFDWLX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX/action/storage_attestation","attest_author":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX/action/author_attestation","sign_citation":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX/action/citation_signature","submit_replication":"https://pith.science/pith/HDXT4QC2TDZ7A74QVNO3UFDWLX/action/replication_record"}},"created_at":"2026-05-17T23:57:08.295496+00:00","updated_at":"2026-05-17T23:57:08.295496+00:00"}