{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:2G266PRFZAOHP7DBDOB2UH6LUY","short_pith_number":"pith:2G266PRF","schema_version":"1.0","canonical_sha256":"d1b5ef3e25c81c77fc611b83aa1fcba62deee81e49f1f43c4b08e4c8c668eb60","source":{"kind":"arxiv","id":"cond-mat/0204309","version":2},"attestation_state":"computed","paper":{"title":"Green's function of the half-filled Landau level Chern-Simons theory in the temporal gauge","license":"","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"J. Dietel","submitted_at":"2002-04-15T09:10:13Z","abstract_excerpt":"We study the Green's function of the $ \\nu=1/2 $ Chern-Simons system in the temporal (Weyl) gauge. We derive the Chern-Simons path integral in the temporal gauge. In order to do this, we gauge transform the path integral in the Coulomb gauge which represents the partition function of the correct normal ordered Chern-Simons Hamiltonian. We calculate the self energy of this path integral in the random-phase approximation (RPA) for temperature $T=0 $. This self energy does not have the divergence with the logarithm of the area, which is known to imply the vanishing of the exact Green's function i"},"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":"cond-mat/0204309","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2002-04-15T09:10:13Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"23594a2f541ba9fe73a8ac9b1ae05600fcb574025aaa5ffe3e603327f0c83c35","abstract_canon_sha256":"5748f04020d09294b514b56a48710807fe5f68ca31a629a0d443651863849dfc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:11:40.982114Z","signature_b64":"bHq7HP/yGGUul1N0NhyVVnJVCaZOLHXAtfed3mEAQSo/iMHEXVEZ+ygQaCj2VJFd/VGHqC1dr+b8bC1OTByJCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1b5ef3e25c81c77fc611b83aa1fcba62deee81e49f1f43c4b08e4c8c668eb60","last_reissued_at":"2026-05-18T04:11:40.981583Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:11:40.981583Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Green's function of the half-filled Landau level Chern-Simons theory in the temporal gauge","license":"","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"J. Dietel","submitted_at":"2002-04-15T09:10:13Z","abstract_excerpt":"We study the Green's function of the $ \\nu=1/2 $ Chern-Simons system in the temporal (Weyl) gauge. We derive the Chern-Simons path integral in the temporal gauge. In order to do this, we gauge transform the path integral in the Coulomb gauge which represents the partition function of the correct normal ordered Chern-Simons Hamiltonian. We calculate the self energy of this path integral in the random-phase approximation (RPA) for temperature $T=0 $. This self energy does not have the divergence with the logarithm of the area, which is known to imply the vanishing of the exact Green's function i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0204309","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":"cond-mat/0204309","created_at":"2026-05-18T04:11:40.981664+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0204309v2","created_at":"2026-05-18T04:11:40.981664+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0204309","created_at":"2026-05-18T04:11:40.981664+00:00"},{"alias_kind":"pith_short_12","alias_value":"2G266PRFZAOH","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_16","alias_value":"2G266PRFZAOHP7DB","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_8","alias_value":"2G266PRF","created_at":"2026-05-18T12:25:50.845339+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/2G266PRFZAOHP7DBDOB2UH6LUY","json":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY.json","graph_json":"https://pith.science/api/pith-number/2G266PRFZAOHP7DBDOB2UH6LUY/graph.json","events_json":"https://pith.science/api/pith-number/2G266PRFZAOHP7DBDOB2UH6LUY/events.json","paper":"https://pith.science/paper/2G266PRF"},"agent_actions":{"view_html":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY","download_json":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY.json","view_paper":"https://pith.science/paper/2G266PRF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0204309&json=true","fetch_graph":"https://pith.science/api/pith-number/2G266PRFZAOHP7DBDOB2UH6LUY/graph.json","fetch_events":"https://pith.science/api/pith-number/2G266PRFZAOHP7DBDOB2UH6LUY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY/action/storage_attestation","attest_author":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY/action/author_attestation","sign_citation":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY/action/citation_signature","submit_replication":"https://pith.science/pith/2G266PRFZAOHP7DBDOB2UH6LUY/action/replication_record"}},"created_at":"2026-05-18T04:11:40.981664+00:00","updated_at":"2026-05-18T04:11:40.981664+00:00"}