{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:7BN5LRMOYOT7NW7OMXYHWLMGT5","short_pith_number":"pith:7BN5LRMO","schema_version":"1.0","canonical_sha256":"f85bd5c58ec3a7f6dbee65f07b2d869f76bc700799a02f15cb90c5b2bfb3c191","source":{"kind":"arxiv","id":"1411.3676","version":2},"attestation_state":"computed","paper":{"title":"Integrability and the Conformal Field Theory of the Higgs branch","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alessandro Sfondrini, Bogdan Stefanski jr, Olof Ohlsson Sax","submitted_at":"2014-11-13T19:37:17Z","abstract_excerpt":"In the context of the AdS$_3$/CFT$_2$ correspondence, we investigate the Higgs branch CFT$_2$. Witten showed that states localised near the small instanton singularity can be described in terms of vector multiplet variables. This theory has a planar, weak-coupling limit, in which anomalous dimensions of single-trace composite operators can be calculated. At one loop, the calculation reduces to finding the spectrum of a spin-chain with nearest-neighbour interactions. This CFT$_2$ spin-chain matches precisely the one that was previously found as the weak-coupling limit of the integrable system d"},"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":"1411.3676","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-11-13T19:37:17Z","cross_cats_sorted":[],"title_canon_sha256":"8651aaee807e7a9aae4277016541e5b0fd2f642cd93e6ba869583de7c51b937c","abstract_canon_sha256":"23a1f59f545bc229d641b5d9f32b5a1dab970f5204f64e7a8fe9f2053e1de933"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:16:41.097771Z","signature_b64":"KJnu4oqSt/VXky+wfHZmBn3j499DMUpSAI7DWajo0Owi6banDljCIAoTm4uznp5kOAgVRTvTv2krz/tXmuUKBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f85bd5c58ec3a7f6dbee65f07b2d869f76bc700799a02f15cb90c5b2bfb3c191","last_reissued_at":"2026-05-18T02:16:41.097216Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:16:41.097216Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Integrability and the Conformal Field Theory of the Higgs branch","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alessandro Sfondrini, Bogdan Stefanski jr, Olof Ohlsson Sax","submitted_at":"2014-11-13T19:37:17Z","abstract_excerpt":"In the context of the AdS$_3$/CFT$_2$ correspondence, we investigate the Higgs branch CFT$_2$. Witten showed that states localised near the small instanton singularity can be described in terms of vector multiplet variables. This theory has a planar, weak-coupling limit, in which anomalous dimensions of single-trace composite operators can be calculated. At one loop, the calculation reduces to finding the spectrum of a spin-chain with nearest-neighbour interactions. This CFT$_2$ spin-chain matches precisely the one that was previously found as the weak-coupling limit of the integrable system d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.3676","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":"1411.3676","created_at":"2026-05-18T02:16:41.097289+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.3676v2","created_at":"2026-05-18T02:16:41.097289+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.3676","created_at":"2026-05-18T02:16:41.097289+00:00"},{"alias_kind":"pith_short_12","alias_value":"7BN5LRMOYOT7","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_16","alias_value":"7BN5LRMOYOT7NW7O","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_8","alias_value":"7BN5LRMO","created_at":"2026-05-18T12:28:16.859392+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2603.25590","citing_title":"Wilson loop in AdS$_3 \\times S^3 \\times T^4$ from quantum M2 brane","ref_index":12,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5","json":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5.json","graph_json":"https://pith.science/api/pith-number/7BN5LRMOYOT7NW7OMXYHWLMGT5/graph.json","events_json":"https://pith.science/api/pith-number/7BN5LRMOYOT7NW7OMXYHWLMGT5/events.json","paper":"https://pith.science/paper/7BN5LRMO"},"agent_actions":{"view_html":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5","download_json":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5.json","view_paper":"https://pith.science/paper/7BN5LRMO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.3676&json=true","fetch_graph":"https://pith.science/api/pith-number/7BN5LRMOYOT7NW7OMXYHWLMGT5/graph.json","fetch_events":"https://pith.science/api/pith-number/7BN5LRMOYOT7NW7OMXYHWLMGT5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5/action/storage_attestation","attest_author":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5/action/author_attestation","sign_citation":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5/action/citation_signature","submit_replication":"https://pith.science/pith/7BN5LRMOYOT7NW7OMXYHWLMGT5/action/replication_record"}},"created_at":"2026-05-18T02:16:41.097289+00:00","updated_at":"2026-05-18T02:16:41.097289+00:00"}