{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:MEXNF5ZJLRLVQIPQBRGVUBTPDS","short_pith_number":"pith:MEXNF5ZJ","schema_version":"1.0","canonical_sha256":"612ed2f7295c575821f00c4d5a066f1cad1b3bda979c52fa986caa37ac2f6331","source":{"kind":"arxiv","id":"1103.4179","version":2},"attestation_state":"computed","paper":{"title":"A Non-Perturbative Gauge-Invariant QCD: Ideal vs. Realistic QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"H. M. Fried (Brown), T. Grandou (INLN), Y.-M. Sheu (INLN)","submitted_at":"2011-03-22T00:34:04Z","abstract_excerpt":"A basic distinction, long overlooked, between the conventional, \"idealistic\" formulation of QCD, and a more \"realistic\" formulation is brought into focus by a rigorous, non-perturbative, gauge-invariant evaluation of the Schwinger solution for the QCD generating functional in terms of exact Fradkin representations for the Green's functional $\\mathbf{G}_{c}(x,y|A)$ and the vacuum functional $\\mathbf{L}[A]$. The quanta of all (Abelian) quantized fields may be expected to obey standard quantum-mechanical measurement properties, perfect position dependence at the cost of unknown momenta, and vice-"},"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":"1103.4179","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-03-22T00:34:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"e95b05ecf67deb7753a1576eea600cd972f21537210dbc8f42c8b4efae77437f","abstract_canon_sha256":"0637935087ab30a4a49beb67260e1d385866482f47896e3abd47eb27b94cf737"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:20:37.758623Z","signature_b64":"gr+bMVwkzsgtjywQdHKPJ1UGFXv3xlCtUhaGUJ6dO+XDBriFSQlhUL5opRho/GmZ+j05yaXMA/07C+JXh+nIDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"612ed2f7295c575821f00c4d5a066f1cad1b3bda979c52fa986caa37ac2f6331","last_reissued_at":"2026-05-18T04:20:37.757914Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:20:37.757914Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Non-Perturbative Gauge-Invariant QCD: Ideal vs. Realistic QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"H. M. Fried (Brown), T. Grandou (INLN), Y.-M. Sheu (INLN)","submitted_at":"2011-03-22T00:34:04Z","abstract_excerpt":"A basic distinction, long overlooked, between the conventional, \"idealistic\" formulation of QCD, and a more \"realistic\" formulation is brought into focus by a rigorous, non-perturbative, gauge-invariant evaluation of the Schwinger solution for the QCD generating functional in terms of exact Fradkin representations for the Green's functional $\\mathbf{G}_{c}(x,y|A)$ and the vacuum functional $\\mathbf{L}[A]$. The quanta of all (Abelian) quantized fields may be expected to obey standard quantum-mechanical measurement properties, perfect position dependence at the cost of unknown momenta, and vice-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.4179","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":"1103.4179","created_at":"2026-05-18T04:20:37.758024+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.4179v2","created_at":"2026-05-18T04:20:37.758024+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.4179","created_at":"2026-05-18T04:20:37.758024+00:00"},{"alias_kind":"pith_short_12","alias_value":"MEXNF5ZJLRLV","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_16","alias_value":"MEXNF5ZJLRLVQIPQ","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_8","alias_value":"MEXNF5ZJ","created_at":"2026-05-18T12:26:34.985390+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.10738","citing_title":"Accessing gluon GTMD $F^g_{1,4}$ via the $\\langle\\sin(2\\phi)\\rangle$ azimuthal asymmetry of exclusive $\\pi^0$ production in $ep$ collisions","ref_index":100,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS","json":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS.json","graph_json":"https://pith.science/api/pith-number/MEXNF5ZJLRLVQIPQBRGVUBTPDS/graph.json","events_json":"https://pith.science/api/pith-number/MEXNF5ZJLRLVQIPQBRGVUBTPDS/events.json","paper":"https://pith.science/paper/MEXNF5ZJ"},"agent_actions":{"view_html":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS","download_json":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS.json","view_paper":"https://pith.science/paper/MEXNF5ZJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.4179&json=true","fetch_graph":"https://pith.science/api/pith-number/MEXNF5ZJLRLVQIPQBRGVUBTPDS/graph.json","fetch_events":"https://pith.science/api/pith-number/MEXNF5ZJLRLVQIPQBRGVUBTPDS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS/action/storage_attestation","attest_author":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS/action/author_attestation","sign_citation":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS/action/citation_signature","submit_replication":"https://pith.science/pith/MEXNF5ZJLRLVQIPQBRGVUBTPDS/action/replication_record"}},"created_at":"2026-05-18T04:20:37.758024+00:00","updated_at":"2026-05-18T04:20:37.758024+00:00"}