{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:3HWMSLYQQB4NKF2BFM6EKBTTT4","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"c1987508bf723ebe40edeb93a782532430fffd2ed9111ced33ce7d4f650e4402","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-31T17:04:57Z","title_canon_sha256":"561d2227e8f07a6026a5e3ded6487d94c3b4477753f3fdeaf3955c68f4e7bca7"},"schema_version":"1.0","source":{"id":"2410.24142","kind":"arxiv","version":5}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.24142","created_at":"2026-07-05T11:57:32Z"},{"alias_kind":"arxiv_version","alias_value":"2410.24142v5","created_at":"2026-07-05T11:57:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.24142","created_at":"2026-07-05T11:57:32Z"},{"alias_kind":"pith_short_12","alias_value":"3HWMSLYQQB4N","created_at":"2026-07-05T11:57:32Z"},{"alias_kind":"pith_short_16","alias_value":"3HWMSLYQQB4NKF2B","created_at":"2026-07-05T11:57:32Z"},{"alias_kind":"pith_short_8","alias_value":"3HWMSLYQ","created_at":"2026-07-05T11:57:32Z"}],"graph_snapshots":[{"event_id":"sha256:faed777a7077327db343d5e74392e16c839fb735354afa22ce95b792317b24f0","target":"graph","created_at":"2026-07-05T11:57:32Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2410.24142/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study quantum field theories which have quantum groups as global internal symmetries. We show that in such theories operators are generically non-local, and should be thought as living at the ends of topological lines. We describe the general constraints of the quantum group symmetry, given by Ward identities, that correlation functions of the theory should satisfy. We also show that generators of the symmetry can be represented by topological lines with some novel properties. We then discuss a particular example of $U_q(sl_2)$ symmetric CFT, which we solve using the bootstrap techniques an","authors_text":"Aleksandr Zhabin, Barak Gabai, Bernardo Zan, Jiaxin Qiao, Victor Gorbenko","cross_cats":["cond-mat.stat-mech","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-31T17:04:57Z","title":"Quantum Groups as Global Symmetries"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.24142","kind":"arxiv","version":5},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a26ca8dc7a32d69234662f64799d6283472205f2a922ab6c3c39af6be8db9e7a","target":"record","created_at":"2026-07-05T11:57:32Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"c1987508bf723ebe40edeb93a782532430fffd2ed9111ced33ce7d4f650e4402","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-31T17:04:57Z","title_canon_sha256":"561d2227e8f07a6026a5e3ded6487d94c3b4477753f3fdeaf3955c68f4e7bca7"},"schema_version":"1.0","source":{"id":"2410.24142","kind":"arxiv","version":5}},"canonical_sha256":"d9ecc92f108078d517412b3c4506739f2d4a7aab44c1a13bf030a1e29c5d2b83","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d9ecc92f108078d517412b3c4506739f2d4a7aab44c1a13bf030a1e29c5d2b83","first_computed_at":"2026-07-05T11:57:32.726489Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:57:32.726489Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ijYnDUCCSy1Kvjr0fxd1Lc8gJFAYRJV8GqaeVzB6hyI6VWVys6Bf3FTpuvI76xXcOLpzWyfdp6EYo2EEgDo7Dg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:57:32.726947Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.24142","source_kind":"arxiv","source_version":5}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a26ca8dc7a32d69234662f64799d6283472205f2a922ab6c3c39af6be8db9e7a","sha256:faed777a7077327db343d5e74392e16c839fb735354afa22ce95b792317b24f0"],"state_sha256":"6df2543b053d6162c2ab23a1ddc9ea3d3a96f6195b8796d4fa85603b616385ff"}