{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:477B44HHKWNPNWXZUWFO3T5Q7E","short_pith_number":"pith:477B44HH","schema_version":"1.0","canonical_sha256":"e7fe1e70e7559af6daf9a58aedcfb0f938ca1323f2b622544e961a70fb039524","source":{"kind":"arxiv","id":"hep-th/0407146","version":2},"attestation_state":"computed","paper":{"title":"Physical Variables of $d=3$ Maxwell-Chern-Simons Theory by Symplectic Projector Method","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"I. V. Vancea, J. A. Helayel-Neto, M. A. Santos","submitted_at":"2004-07-16T17:53:32Z","abstract_excerpt":"The Symplectic Projector Method is applied to derive the local physical degrees of freedom and the physical Hamiltonian of the Maxwell-Chern-Simons theory in $d=1+2$. The results agree with the ones obtained in the literature through different approaches."},"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":"hep-th/0407146","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-07-16T17:53:32Z","cross_cats_sorted":[],"title_canon_sha256":"dda348e18b0ea9f36d268b5faca281671bedc26e5c9e743c6a51931acb06a4fc","abstract_canon_sha256":"ac0c6bc0096b0a11bf6e8c3e9f1d90bd9c276153c56ca299a21057cab2179df0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:46.181674Z","signature_b64":"wlEfSkOFU8RoHuIBmhoU2i/xbrNjQC9vKxoSScsScAht9Q9Hm4BihMqDvMy+/pt8hmF19dUWWRwzmkfx65POCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7fe1e70e7559af6daf9a58aedcfb0f938ca1323f2b622544e961a70fb039524","last_reissued_at":"2026-05-18T01:38:46.181275Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:46.181275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Physical Variables of $d=3$ Maxwell-Chern-Simons Theory by Symplectic Projector Method","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"I. V. Vancea, J. A. Helayel-Neto, M. A. Santos","submitted_at":"2004-07-16T17:53:32Z","abstract_excerpt":"The Symplectic Projector Method is applied to derive the local physical degrees of freedom and the physical Hamiltonian of the Maxwell-Chern-Simons theory in $d=1+2$. The results agree with the ones obtained in the literature through different approaches."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0407146","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":"hep-th/0407146","created_at":"2026-05-18T01:38:46.181350+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0407146v2","created_at":"2026-05-18T01:38:46.181350+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0407146","created_at":"2026-05-18T01:38:46.181350+00:00"},{"alias_kind":"pith_short_12","alias_value":"477B44HHKWNP","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"477B44HHKWNPNWXZ","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"477B44HH","created_at":"2026-05-18T12:25:52.051335+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/477B44HHKWNPNWXZUWFO3T5Q7E","json":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E.json","graph_json":"https://pith.science/api/pith-number/477B44HHKWNPNWXZUWFO3T5Q7E/graph.json","events_json":"https://pith.science/api/pith-number/477B44HHKWNPNWXZUWFO3T5Q7E/events.json","paper":"https://pith.science/paper/477B44HH"},"agent_actions":{"view_html":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E","download_json":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E.json","view_paper":"https://pith.science/paper/477B44HH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0407146&json=true","fetch_graph":"https://pith.science/api/pith-number/477B44HHKWNPNWXZUWFO3T5Q7E/graph.json","fetch_events":"https://pith.science/api/pith-number/477B44HHKWNPNWXZUWFO3T5Q7E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E/action/storage_attestation","attest_author":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E/action/author_attestation","sign_citation":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E/action/citation_signature","submit_replication":"https://pith.science/pith/477B44HHKWNPNWXZUWFO3T5Q7E/action/replication_record"}},"created_at":"2026-05-18T01:38:46.181350+00:00","updated_at":"2026-05-18T01:38:46.181350+00:00"}