{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:4UVR7KSCIKXR7RFEEKF4BX7ILA","short_pith_number":"pith:4UVR7KSC","schema_version":"1.0","canonical_sha256":"e52b1faa4242af1fc4a4228bc0dfe85837ff2ba5d265d833b9bbc04d3a2761ea","source":{"kind":"arxiv","id":"1609.02560","version":1},"attestation_state":"computed","paper":{"title":"A series of (2+1)d Stable Self-Dual Interacting Conformal Field Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Cenke Xu, Meng Cheng","submitted_at":"2016-09-08T20:00:03Z","abstract_excerpt":"Using the duality between seemingly different (2+1)d conformal field theories (CFT) proposed recently, we study a series of (2+1)d stable self-dual interacting CFTs. These CFTs can be realized (for instance) on the boundary of the (3+1)d bosonic topological insulator protected by U(1) and time-reversal symmetry, and they remain stable as long as these symmetries are preserved. When realized as a boundary system, these CFTs can be driven into anomalous fractional quantum Hall states once time-reversal is broken. We demonstrate that the newly proposed dualities allow us to study these CFTs quant"},"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":"1609.02560","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-09-08T20:00:03Z","cross_cats_sorted":[],"title_canon_sha256":"982d14ba2cb0e0896bd796cc2ebcc3b4383e349e36bf30656a647dd791d5733f","abstract_canon_sha256":"1b7771f8a1e0148054ad89f9fbdb648714d027e3da5ca121ac180d1b0d68eea5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:19.576821Z","signature_b64":"CFCb925qmjcKxFD+vK12VnBfJqM4Oe2Z8kakVbqBH/kzZMqJmsz2IYLwCX8KB/SokmZ2iWEGFS4KgcJKolI7Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e52b1faa4242af1fc4a4228bc0dfe85837ff2ba5d265d833b9bbc04d3a2761ea","last_reissued_at":"2026-05-18T00:54:19.576413Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:19.576413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A series of (2+1)d Stable Self-Dual Interacting Conformal Field Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Cenke Xu, Meng Cheng","submitted_at":"2016-09-08T20:00:03Z","abstract_excerpt":"Using the duality between seemingly different (2+1)d conformal field theories (CFT) proposed recently, we study a series of (2+1)d stable self-dual interacting CFTs. These CFTs can be realized (for instance) on the boundary of the (3+1)d bosonic topological insulator protected by U(1) and time-reversal symmetry, and they remain stable as long as these symmetries are preserved. When realized as a boundary system, these CFTs can be driven into anomalous fractional quantum Hall states once time-reversal is broken. We demonstrate that the newly proposed dualities allow us to study these CFTs quant"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.02560","kind":"arxiv","version":1},"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":"1609.02560","created_at":"2026-05-18T00:54:19.576481+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.02560v1","created_at":"2026-05-18T00:54:19.576481+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.02560","created_at":"2026-05-18T00:54:19.576481+00:00"},{"alias_kind":"pith_short_12","alias_value":"4UVR7KSCIKXR","created_at":"2026-05-18T12:29:58.707656+00:00"},{"alias_kind":"pith_short_16","alias_value":"4UVR7KSCIKXR7RFE","created_at":"2026-05-18T12:29:58.707656+00:00"},{"alias_kind":"pith_short_8","alias_value":"4UVR7KSC","created_at":"2026-05-18T12:29:58.707656+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/4UVR7KSCIKXR7RFEEKF4BX7ILA","json":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA.json","graph_json":"https://pith.science/api/pith-number/4UVR7KSCIKXR7RFEEKF4BX7ILA/graph.json","events_json":"https://pith.science/api/pith-number/4UVR7KSCIKXR7RFEEKF4BX7ILA/events.json","paper":"https://pith.science/paper/4UVR7KSC"},"agent_actions":{"view_html":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA","download_json":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA.json","view_paper":"https://pith.science/paper/4UVR7KSC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.02560&json=true","fetch_graph":"https://pith.science/api/pith-number/4UVR7KSCIKXR7RFEEKF4BX7ILA/graph.json","fetch_events":"https://pith.science/api/pith-number/4UVR7KSCIKXR7RFEEKF4BX7ILA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA/action/storage_attestation","attest_author":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA/action/author_attestation","sign_citation":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA/action/citation_signature","submit_replication":"https://pith.science/pith/4UVR7KSCIKXR7RFEEKF4BX7ILA/action/replication_record"}},"created_at":"2026-05-18T00:54:19.576481+00:00","updated_at":"2026-05-18T00:54:19.576481+00:00"}