{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:WCI26XMTO3PEVOMATNCCMOI4TI","short_pith_number":"pith:WCI26XMT","schema_version":"1.0","canonical_sha256":"b091af5d9376de4ab9809b4426391c9a3f08377440828ad9ac6ce1b13083540b","source":{"kind":"arxiv","id":"1412.5395","version":1},"attestation_state":"computed","paper":{"title":"Regge behaviour within the Bethe-Salpeter approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christian S Fischer, Richard Williams, Stanislav Kubrak","submitted_at":"2014-12-17T14:01:13Z","abstract_excerpt":"We present a calculation of the spectrum of light and heavy quark bound states in the rainbow-ladder truncation of Dyson-Schwinger/Bethe-Salpeter equations. By extending the formalism include the case of total angular momentum J=3, we are able to explore Regge trajectories and make prediction of tensor bound states for light and heavy quarkonia."},"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":"1412.5395","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-17T14:01:13Z","cross_cats_sorted":[],"title_canon_sha256":"1e3b0a45f68ccdd8e11ddbcda1edff6228949fba847499a22b2618abc05a60fc","abstract_canon_sha256":"5479186cc7ec4546b9d3994ddf75dbb0c3a988a084f507f0ae696b2eccf3241b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:18.501608Z","signature_b64":"lMOdJRxylNHbhNWOQ0X7/YmrPFWSUmzURbE5OxL5gm8tnLBan+qOvsuWN0Ub16ebmaDUK/5ux4flRBo19JMDDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b091af5d9376de4ab9809b4426391c9a3f08377440828ad9ac6ce1b13083540b","last_reissued_at":"2026-05-18T01:41:18.501050Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:18.501050Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Regge behaviour within the Bethe-Salpeter approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christian S Fischer, Richard Williams, Stanislav Kubrak","submitted_at":"2014-12-17T14:01:13Z","abstract_excerpt":"We present a calculation of the spectrum of light and heavy quark bound states in the rainbow-ladder truncation of Dyson-Schwinger/Bethe-Salpeter equations. By extending the formalism include the case of total angular momentum J=3, we are able to explore Regge trajectories and make prediction of tensor bound states for light and heavy quarkonia."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5395","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":"1412.5395","created_at":"2026-05-18T01:41:18.501122+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.5395v1","created_at":"2026-05-18T01:41:18.501122+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5395","created_at":"2026-05-18T01:41:18.501122+00:00"},{"alias_kind":"pith_short_12","alias_value":"WCI26XMTO3PE","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"WCI26XMTO3PEVOMA","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"WCI26XMT","created_at":"2026-05-18T12:28:54.890064+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/WCI26XMTO3PEVOMATNCCMOI4TI","json":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI.json","graph_json":"https://pith.science/api/pith-number/WCI26XMTO3PEVOMATNCCMOI4TI/graph.json","events_json":"https://pith.science/api/pith-number/WCI26XMTO3PEVOMATNCCMOI4TI/events.json","paper":"https://pith.science/paper/WCI26XMT"},"agent_actions":{"view_html":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI","download_json":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI.json","view_paper":"https://pith.science/paper/WCI26XMT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.5395&json=true","fetch_graph":"https://pith.science/api/pith-number/WCI26XMTO3PEVOMATNCCMOI4TI/graph.json","fetch_events":"https://pith.science/api/pith-number/WCI26XMTO3PEVOMATNCCMOI4TI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI/action/storage_attestation","attest_author":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI/action/author_attestation","sign_citation":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI/action/citation_signature","submit_replication":"https://pith.science/pith/WCI26XMTO3PEVOMATNCCMOI4TI/action/replication_record"}},"created_at":"2026-05-18T01:41:18.501122+00:00","updated_at":"2026-05-18T01:41:18.501122+00:00"}