{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:HV6HMQNCM6KBPPKVH34UN2EEBY","short_pith_number":"pith:HV6HMQNC","schema_version":"1.0","canonical_sha256":"3d7c7641a2679417bd553ef946e8840e27fbc29af7d9c4c5a2a06e739b3b8e15","source":{"kind":"arxiv","id":"1103.4786","version":1},"attestation_state":"computed","paper":{"title":"Higher order heavy quark Green's functions in Coulomb gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"C. Popovici, H. Reinhardt, P. Watson","submitted_at":"2011-03-24T15:28:18Z","abstract_excerpt":"The Dyson-Schwinger equation for the 4-point quark Green's functions is studied. In the limit of the heavy quark mass and with the truncation to include only the dressed two point functions for the Yang-Mills sector, we provide an exact solution for the 4-point quark Green's functions, in both quark-antiquark and diquark channels, and show that the corresponding poles relate to the bound state energy of the heavy quark systems. Moreover, a natural separation between physical and unphysical poles in the Green's functions emerges."},"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":"1103.4786","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-03-24T15:28:18Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"66eb88ef77220a6fd8a155ce5fd3f40016cf18e6535802a7f1a2994c5396474c","abstract_canon_sha256":"d41f53459b9df6bd8262a7ccb94501e785ec8a649dd0b015d7b7cd35f56ba395"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:19:02.039040Z","signature_b64":"wgs9/1VdJk7qH/479WFhOyg095+zsjass+rrPVk0rhairQPXgFdDrJevI8wPjo3llTxGC+kWioIKb2/5usQmBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3d7c7641a2679417bd553ef946e8840e27fbc29af7d9c4c5a2a06e739b3b8e15","last_reissued_at":"2026-05-18T04:19:02.038381Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:19:02.038381Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher order heavy quark Green's functions in Coulomb gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"C. Popovici, H. Reinhardt, P. Watson","submitted_at":"2011-03-24T15:28:18Z","abstract_excerpt":"The Dyson-Schwinger equation for the 4-point quark Green's functions is studied. In the limit of the heavy quark mass and with the truncation to include only the dressed two point functions for the Yang-Mills sector, we provide an exact solution for the 4-point quark Green's functions, in both quark-antiquark and diquark channels, and show that the corresponding poles relate to the bound state energy of the heavy quark systems. Moreover, a natural separation between physical and unphysical poles in the Green's functions emerges."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.4786","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":"1103.4786","created_at":"2026-05-18T04:19:02.038470+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.4786v1","created_at":"2026-05-18T04:19:02.038470+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.4786","created_at":"2026-05-18T04:19:02.038470+00:00"},{"alias_kind":"pith_short_12","alias_value":"HV6HMQNCM6KB","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_16","alias_value":"HV6HMQNCM6KBPPKV","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_8","alias_value":"HV6HMQNC","created_at":"2026-05-18T12:26:30.835961+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/HV6HMQNCM6KBPPKVH34UN2EEBY","json":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY.json","graph_json":"https://pith.science/api/pith-number/HV6HMQNCM6KBPPKVH34UN2EEBY/graph.json","events_json":"https://pith.science/api/pith-number/HV6HMQNCM6KBPPKVH34UN2EEBY/events.json","paper":"https://pith.science/paper/HV6HMQNC"},"agent_actions":{"view_html":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY","download_json":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY.json","view_paper":"https://pith.science/paper/HV6HMQNC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.4786&json=true","fetch_graph":"https://pith.science/api/pith-number/HV6HMQNCM6KBPPKVH34UN2EEBY/graph.json","fetch_events":"https://pith.science/api/pith-number/HV6HMQNCM6KBPPKVH34UN2EEBY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY/action/storage_attestation","attest_author":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY/action/author_attestation","sign_citation":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY/action/citation_signature","submit_replication":"https://pith.science/pith/HV6HMQNCM6KBPPKVH34UN2EEBY/action/replication_record"}},"created_at":"2026-05-18T04:19:02.038470+00:00","updated_at":"2026-05-18T04:19:02.038470+00:00"}