{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:GLU4D6EMJOZ4MXYRFL7ZPN655L","short_pith_number":"pith:GLU4D6EM","schema_version":"1.0","canonical_sha256":"32e9c1f88c4bb3c65f112aff97b7ddeaefbd65c0104d5d784b93fd5a0307bb05","source":{"kind":"arxiv","id":"1803.06597","version":3},"attestation_state":"computed","paper":{"title":"Schwinger-Dyson Equations in Coulomb Gauge Consistent with Numerical Simulation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Zwanziger, Patrick Cooper","submitted_at":"2018-03-18T03:21:44Z","abstract_excerpt":"In the present work we undertake a study of the Schwinger-Dyson equation (SDE) in the Euclidean formulation of local quantum gauge field theory, with Coulomb gauge condition $\\partial_i A_i = 0$. We continue a previous study which kept only instantaneous terms in the SDE that are proportional to $\\delta(t)$ in order to calculate the instantaneous part of the time component of the gluon propagator $D_{A_0 A_0}(t, R)$. We compare the results of that study with a numerical simulation of lattice gauge theory and find that the infrared critical exponents and related quantities agree to within 1\\% t"},"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":"1803.06597","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-18T03:21:44Z","cross_cats_sorted":[],"title_canon_sha256":"94c5ec4363f41628f47c7b92998ee4cecd113672b19a43ee9826f725bc8aab5e","abstract_canon_sha256":"c4a10e6d8119d41c33a42c656b0a58f08ec8677c29776ec1da8779750e597bf8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:58:05.102375Z","signature_b64":"TPu1Bhwmm1b1IJL5Q6v/+cDOj6fAkUlwXV1JFB9h5DP22ol1a1bmyWpX7atNJI3RjjJy1PFNAqL4LlZd0Dm/DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"32e9c1f88c4bb3c65f112aff97b7ddeaefbd65c0104d5d784b93fd5a0307bb05","last_reissued_at":"2026-05-17T23:58:05.101978Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:58:05.101978Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Schwinger-Dyson Equations in Coulomb Gauge Consistent with Numerical Simulation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Zwanziger, Patrick Cooper","submitted_at":"2018-03-18T03:21:44Z","abstract_excerpt":"In the present work we undertake a study of the Schwinger-Dyson equation (SDE) in the Euclidean formulation of local quantum gauge field theory, with Coulomb gauge condition $\\partial_i A_i = 0$. We continue a previous study which kept only instantaneous terms in the SDE that are proportional to $\\delta(t)$ in order to calculate the instantaneous part of the time component of the gluon propagator $D_{A_0 A_0}(t, R)$. We compare the results of that study with a numerical simulation of lattice gauge theory and find that the infrared critical exponents and related quantities agree to within 1\\% t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.06597","kind":"arxiv","version":3},"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":"1803.06597","created_at":"2026-05-17T23:58:05.102032+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.06597v3","created_at":"2026-05-17T23:58:05.102032+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.06597","created_at":"2026-05-17T23:58:05.102032+00:00"},{"alias_kind":"pith_short_12","alias_value":"GLU4D6EMJOZ4","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_16","alias_value":"GLU4D6EMJOZ4MXYR","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_8","alias_value":"GLU4D6EM","created_at":"2026-05-18T12:32:25.280505+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/GLU4D6EMJOZ4MXYRFL7ZPN655L","json":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L.json","graph_json":"https://pith.science/api/pith-number/GLU4D6EMJOZ4MXYRFL7ZPN655L/graph.json","events_json":"https://pith.science/api/pith-number/GLU4D6EMJOZ4MXYRFL7ZPN655L/events.json","paper":"https://pith.science/paper/GLU4D6EM"},"agent_actions":{"view_html":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L","download_json":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L.json","view_paper":"https://pith.science/paper/GLU4D6EM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.06597&json=true","fetch_graph":"https://pith.science/api/pith-number/GLU4D6EMJOZ4MXYRFL7ZPN655L/graph.json","fetch_events":"https://pith.science/api/pith-number/GLU4D6EMJOZ4MXYRFL7ZPN655L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L/action/storage_attestation","attest_author":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L/action/author_attestation","sign_citation":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L/action/citation_signature","submit_replication":"https://pith.science/pith/GLU4D6EMJOZ4MXYRFL7ZPN655L/action/replication_record"}},"created_at":"2026-05-17T23:58:05.102032+00:00","updated_at":"2026-05-17T23:58:05.102032+00:00"}