{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:RMED5J4EHOVY5V7GP56TCPCDYA","short_pith_number":"pith:RMED5J4E","schema_version":"1.0","canonical_sha256":"8b083ea7843bab8ed7e67f7d313c43c01cf19da5f1aa8c927bbea67bd28fe384","source":{"kind":"arxiv","id":"0910.4548","version":2},"attestation_state":"computed","paper":{"title":"Equal-time two-point correlation functions in Coulomb gauge Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Weber, D. Campagnari, F. Astorga, H. Reinhardt, W. Schleifenbaum","submitted_at":"2009-10-23T16:44:49Z","abstract_excerpt":"We apply a functional perturbative approach to the calculation of the equal-time two-point correlation functions and the potential between static color charges to one-loop order in Coulomb gauge Yang-Mills theory. The functional approach proceeds through a solution of the Schroedinger equation for the vacuum wave functional to order g^2 and derives the equal-time correlation functions from a functional integral representation via new diagrammatic rules. We show that the results coincide with those obtained from the usual Lagrangian functional integral approach, extract the beta function, and d"},"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":"0910.4548","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-10-23T16:44:49Z","cross_cats_sorted":[],"title_canon_sha256":"4701510b25be129d4d3b0bed25396b31ae856edacc951965698d7e94b51e911d","abstract_canon_sha256":"3949866d0e9c3b8a559cf414735adf5fc19e222156198eba443b36d7ce9a3e36"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:54:26.458031Z","signature_b64":"dzvNTCQRZdvLOJB2CBLXAqpIjCA6xgWaHdc8F3L6CEBHW28JhE6k34ZjFjTbNHgRfeibreSohvrxZHYmPwnTCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b083ea7843bab8ed7e67f7d313c43c01cf19da5f1aa8c927bbea67bd28fe384","last_reissued_at":"2026-05-18T03:54:26.457395Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:54:26.457395Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Equal-time two-point correlation functions in Coulomb gauge Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Weber, D. Campagnari, F. Astorga, H. Reinhardt, W. Schleifenbaum","submitted_at":"2009-10-23T16:44:49Z","abstract_excerpt":"We apply a functional perturbative approach to the calculation of the equal-time two-point correlation functions and the potential between static color charges to one-loop order in Coulomb gauge Yang-Mills theory. The functional approach proceeds through a solution of the Schroedinger equation for the vacuum wave functional to order g^2 and derives the equal-time correlation functions from a functional integral representation via new diagrammatic rules. We show that the results coincide with those obtained from the usual Lagrangian functional integral approach, extract the beta function, and d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0910.4548","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":"0910.4548","created_at":"2026-05-18T03:54:26.457489+00:00"},{"alias_kind":"arxiv_version","alias_value":"0910.4548v2","created_at":"2026-05-18T03:54:26.457489+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0910.4548","created_at":"2026-05-18T03:54:26.457489+00:00"},{"alias_kind":"pith_short_12","alias_value":"RMED5J4EHOVY","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"RMED5J4EHOVY5V7G","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"RMED5J4E","created_at":"2026-05-18T12:26:01.383474+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/RMED5J4EHOVY5V7GP56TCPCDYA","json":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA.json","graph_json":"https://pith.science/api/pith-number/RMED5J4EHOVY5V7GP56TCPCDYA/graph.json","events_json":"https://pith.science/api/pith-number/RMED5J4EHOVY5V7GP56TCPCDYA/events.json","paper":"https://pith.science/paper/RMED5J4E"},"agent_actions":{"view_html":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA","download_json":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA.json","view_paper":"https://pith.science/paper/RMED5J4E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0910.4548&json=true","fetch_graph":"https://pith.science/api/pith-number/RMED5J4EHOVY5V7GP56TCPCDYA/graph.json","fetch_events":"https://pith.science/api/pith-number/RMED5J4EHOVY5V7GP56TCPCDYA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA/action/storage_attestation","attest_author":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA/action/author_attestation","sign_citation":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA/action/citation_signature","submit_replication":"https://pith.science/pith/RMED5J4EHOVY5V7GP56TCPCDYA/action/replication_record"}},"created_at":"2026-05-18T03:54:26.457489+00:00","updated_at":"2026-05-18T03:54:26.457489+00:00"}