{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:LHZ3BWVWFTY6HRJUUIRLDSWKUB","short_pith_number":"pith:LHZ3BWVW","schema_version":"1.0","canonical_sha256":"59f3b0dab62cf1e3c534a222b1cacaa041f045a4f3658b5803ae77c9bdffc0dd","source":{"kind":"arxiv","id":"hep-th/9403066","version":2},"attestation_state":"computed","paper":{"title":"Combinatorial quantization of the Hamiltonian Chern-Simons theory I","license":"","headline":"","cross_cats":["math.QA"],"primary_cat":"hep-th","authors_text":"A. Yu. Alekseev, H. Grosse, V. Schomerus","submitted_at":"1994-03-10T20:45:34Z","abstract_excerpt":"Motivated by a recent paper of Fock and Rosly \\cite{FoRo} we describe a mathematically precise quantization of the Hamiltonian Chern-Simons theory. We introduce the Chern-Simons theory on the lattice which is expected to reproduce the results of the continuous theory exactly. The lattice model enjoys the symmetry with respect to a quantum gauge group. Using this fact we construct the algebra of observables of the Hamiltonian Chern-Simons theory equipped with a *-operation and a positive inner product."},"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/9403066","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-03-10T20:45:34Z","cross_cats_sorted":["math.QA"],"title_canon_sha256":"b3bf7a7e1f0f2b1ce0e3d04d9dc29058d46cab81e31f5101bc6dbf73a74ae64c","abstract_canon_sha256":"665a1765f8232fa42ac4a062a741b8f64305b1d7afa793801e832c969ebb15b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:57:42.368034Z","signature_b64":"ArlZQu51Jke2LqvkYEk8K5UEg+hD+7S4xZssJw/XS68dL+bviSFhDbAD7CQJMoTBtJJB+pqaAu+f3KGIWv5BCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"59f3b0dab62cf1e3c534a222b1cacaa041f045a4f3658b5803ae77c9bdffc0dd","last_reissued_at":"2026-07-04T15:57:42.367621Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:57:42.367621Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Combinatorial quantization of the Hamiltonian Chern-Simons theory I","license":"","headline":"","cross_cats":["math.QA"],"primary_cat":"hep-th","authors_text":"A. Yu. Alekseev, H. Grosse, V. Schomerus","submitted_at":"1994-03-10T20:45:34Z","abstract_excerpt":"Motivated by a recent paper of Fock and Rosly \\cite{FoRo} we describe a mathematically precise quantization of the Hamiltonian Chern-Simons theory. We introduce the Chern-Simons theory on the lattice which is expected to reproduce the results of the continuous theory exactly. The lattice model enjoys the symmetry with respect to a quantum gauge group. Using this fact we construct the algebra of observables of the Hamiltonian Chern-Simons theory equipped with a *-operation and a positive inner product."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9403066","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9403066/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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/9403066","created_at":"2026-07-04T15:57:42.367686+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9403066v2","created_at":"2026-07-04T15:57:42.367686+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9403066","created_at":"2026-07-04T15:57:42.367686+00:00"},{"alias_kind":"pith_short_12","alias_value":"LHZ3BWVWFTY6","created_at":"2026-07-04T15:57:42.367686+00:00"},{"alias_kind":"pith_short_16","alias_value":"LHZ3BWVWFTY6HRJU","created_at":"2026-07-04T15:57:42.367686+00:00"},{"alias_kind":"pith_short_8","alias_value":"LHZ3BWVW","created_at":"2026-07-04T15:57:42.367686+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.00501","citing_title":"Minimal Factorization of Chern-Simons Theory -- Gravitational Anyonic Edge Modes","ref_index":47,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB","json":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB.json","graph_json":"https://pith.science/api/pith-number/LHZ3BWVWFTY6HRJUUIRLDSWKUB/graph.json","events_json":"https://pith.science/api/pith-number/LHZ3BWVWFTY6HRJUUIRLDSWKUB/events.json","paper":"https://pith.science/paper/LHZ3BWVW"},"agent_actions":{"view_html":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB","download_json":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB.json","view_paper":"https://pith.science/paper/LHZ3BWVW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9403066&json=true","fetch_graph":"https://pith.science/api/pith-number/LHZ3BWVWFTY6HRJUUIRLDSWKUB/graph.json","fetch_events":"https://pith.science/api/pith-number/LHZ3BWVWFTY6HRJUUIRLDSWKUB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB/action/storage_attestation","attest_author":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB/action/author_attestation","sign_citation":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB/action/citation_signature","submit_replication":"https://pith.science/pith/LHZ3BWVWFTY6HRJUUIRLDSWKUB/action/replication_record"}},"created_at":"2026-07-04T15:57:42.367686+00:00","updated_at":"2026-07-04T15:57:42.367686+00:00"}