{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:NNVEPUVXNFH2EY6ZH3CMOPC4UE","short_pith_number":"pith:NNVEPUVX","schema_version":"1.0","canonical_sha256":"6b6a47d2b7694fa263d93ec4c73c5ca132cb0f96cb032f112e64ae533ecac411","source":{"kind":"arxiv","id":"1001.2003","version":2},"attestation_state":"computed","paper":{"title":"Chern-Simons Theory in the Temporal Gauge and Knot Invariants through the Universal Quantum R-Matrix","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alexei Morozov, Andrey Smirnov","submitted_at":"2010-01-12T20:58:39Z","abstract_excerpt":"In temporal gauge A_{0}=0 the 3d Chern-Simons theory acquires quadratic action and an ultralocal propagator. This directly implies a 2d R-matrix representation for the correlators of Wilson lines (knot invariants), where only the crossing points of the contours projection on the xy plane contribute. Though the theory is quadratic, P-exponents remain non-trivial operators and R-factors are easier to guess then derive. We show that the topological invariants arise if additional flag structure (xy plane and an y line in it) is introduced, R is the universal quantum R-matrix and turning points con"},"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":"1001.2003","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-01-12T20:58:39Z","cross_cats_sorted":[],"title_canon_sha256":"469cb5ec36318605893fea5cdbb89ffe1b2cdff627d2b88115b80cabc5b59db5","abstract_canon_sha256":"a9c72da704115b7a8a70d92746904b75642ba20b98f39b62d648d96866c74062"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:09:55.340010Z","signature_b64":"KvZA+X77GyjD6zXnKEJdQWq8F8BgZnacB2z2TkJlqqEMbRxJNbIPFWvOitxvpINjXiKXWxExAmol2CSSZ2zsDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6b6a47d2b7694fa263d93ec4c73c5ca132cb0f96cb032f112e64ae533ecac411","last_reissued_at":"2026-05-18T02:09:55.339313Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:09:55.339313Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chern-Simons Theory in the Temporal Gauge and Knot Invariants through the Universal Quantum R-Matrix","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alexei Morozov, Andrey Smirnov","submitted_at":"2010-01-12T20:58:39Z","abstract_excerpt":"In temporal gauge A_{0}=0 the 3d Chern-Simons theory acquires quadratic action and an ultralocal propagator. This directly implies a 2d R-matrix representation for the correlators of Wilson lines (knot invariants), where only the crossing points of the contours projection on the xy plane contribute. Though the theory is quadratic, P-exponents remain non-trivial operators and R-factors are easier to guess then derive. We show that the topological invariants arise if additional flag structure (xy plane and an y line in it) is introduced, R is the universal quantum R-matrix and turning points con"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.2003","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":"1001.2003","created_at":"2026-05-18T02:09:55.339435+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.2003v2","created_at":"2026-05-18T02:09:55.339435+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.2003","created_at":"2026-05-18T02:09:55.339435+00:00"},{"alias_kind":"pith_short_12","alias_value":"NNVEPUVXNFH2","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_16","alias_value":"NNVEPUVXNFH2EY6Z","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_8","alias_value":"NNVEPUVX","created_at":"2026-05-18T12:26:10.704358+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.07255","citing_title":"Non-commutative creation operators for symmetric polynomials","ref_index":55,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE","json":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE.json","graph_json":"https://pith.science/api/pith-number/NNVEPUVXNFH2EY6ZH3CMOPC4UE/graph.json","events_json":"https://pith.science/api/pith-number/NNVEPUVXNFH2EY6ZH3CMOPC4UE/events.json","paper":"https://pith.science/paper/NNVEPUVX"},"agent_actions":{"view_html":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE","download_json":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE.json","view_paper":"https://pith.science/paper/NNVEPUVX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.2003&json=true","fetch_graph":"https://pith.science/api/pith-number/NNVEPUVXNFH2EY6ZH3CMOPC4UE/graph.json","fetch_events":"https://pith.science/api/pith-number/NNVEPUVXNFH2EY6ZH3CMOPC4UE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE/action/storage_attestation","attest_author":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE/action/author_attestation","sign_citation":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE/action/citation_signature","submit_replication":"https://pith.science/pith/NNVEPUVXNFH2EY6ZH3CMOPC4UE/action/replication_record"}},"created_at":"2026-05-18T02:09:55.339435+00:00","updated_at":"2026-05-18T02:09:55.339435+00:00"}