{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:6LYTOLO4PE5O6LK2M3Q6U2ROAL","short_pith_number":"pith:6LYTOLO4","schema_version":"1.0","canonical_sha256":"f2f1372ddc793aef2d5a66e1ea6a2e02d8f6259fafb3357eddf8404a4a766b8a","source":{"kind":"arxiv","id":"1901.07591","version":1},"attestation_state":"computed","paper":{"title":"Rationalizing CFTs and Anyonic Imprints on Higgs Branches","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","math.QA","math.RT"],"primary_cat":"hep-th","authors_text":"Matthew Buican, Zoltan Laczko","submitted_at":"2019-01-22T19:40:35Z","abstract_excerpt":"We continue our program of mapping data of 4D $\\mathcal{N}=2$ superconformal field theories (SCFTs) onto observables of 2D chiral rational conformal field theories (RCFTs) by revisiting an infinite set of strongly coupled Argyres-Douglas (AD) SCFTs and their associated logarithmic 2D chiral algebras. First, we turn on discrete flavor fugacities (for continuous flavor symmetries) in a known correspondence between certain unrefined characters of these logarithmic theories and unrefined characters of a set of unitary 2D chiral RCFTs. Motivated by this discussion, we then study 4D Higgs branch ren"},"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":"1901.07591","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-01-22T19:40:35Z","cross_cats_sorted":["cond-mat.str-el","math.QA","math.RT"],"title_canon_sha256":"8cdcb5d21e73b05be02abba874aebb0d96a6ac0efd9e4316f0a7576e525ec65c","abstract_canon_sha256":"e46e6acd96ab211c6538a4b3930d68d0954b02f9fc7554e269cce7ae86a1a1e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:21.744066Z","signature_b64":"UkaxrXQLVb9cjfhAa2WJoIeoVVPzGLG+c2+P22XId5vgdOwVh5rffmKsQWdOjmA09d0Q81KUVSBB7U0ReBroBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2f1372ddc793aef2d5a66e1ea6a2e02d8f6259fafb3357eddf8404a4a766b8a","last_reissued_at":"2026-05-17T23:50:21.743460Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:21.743460Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rationalizing CFTs and Anyonic Imprints on Higgs Branches","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","math.QA","math.RT"],"primary_cat":"hep-th","authors_text":"Matthew Buican, Zoltan Laczko","submitted_at":"2019-01-22T19:40:35Z","abstract_excerpt":"We continue our program of mapping data of 4D $\\mathcal{N}=2$ superconformal field theories (SCFTs) onto observables of 2D chiral rational conformal field theories (RCFTs) by revisiting an infinite set of strongly coupled Argyres-Douglas (AD) SCFTs and their associated logarithmic 2D chiral algebras. First, we turn on discrete flavor fugacities (for continuous flavor symmetries) in a known correspondence between certain unrefined characters of these logarithmic theories and unrefined characters of a set of unitary 2D chiral RCFTs. Motivated by this discussion, we then study 4D Higgs branch ren"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.07591","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":"1901.07591","created_at":"2026-05-17T23:50:21.743559+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.07591v1","created_at":"2026-05-17T23:50:21.743559+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.07591","created_at":"2026-05-17T23:50:21.743559+00:00"},{"alias_kind":"pith_short_12","alias_value":"6LYTOLO4PE5O","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_16","alias_value":"6LYTOLO4PE5O6LK2","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_8","alias_value":"6LYTOLO4","created_at":"2026-05-18T12:33:10.108867+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2409.18130","citing_title":"Bridging 4D QFTs and 2D VOAs via 3D high-temperature EFTs","ref_index":100,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL","json":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL.json","graph_json":"https://pith.science/api/pith-number/6LYTOLO4PE5O6LK2M3Q6U2ROAL/graph.json","events_json":"https://pith.science/api/pith-number/6LYTOLO4PE5O6LK2M3Q6U2ROAL/events.json","paper":"https://pith.science/paper/6LYTOLO4"},"agent_actions":{"view_html":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL","download_json":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL.json","view_paper":"https://pith.science/paper/6LYTOLO4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.07591&json=true","fetch_graph":"https://pith.science/api/pith-number/6LYTOLO4PE5O6LK2M3Q6U2ROAL/graph.json","fetch_events":"https://pith.science/api/pith-number/6LYTOLO4PE5O6LK2M3Q6U2ROAL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL/action/storage_attestation","attest_author":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL/action/author_attestation","sign_citation":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL/action/citation_signature","submit_replication":"https://pith.science/pith/6LYTOLO4PE5O6LK2M3Q6U2ROAL/action/replication_record"}},"created_at":"2026-05-17T23:50:21.743559+00:00","updated_at":"2026-05-17T23:50:21.743559+00:00"}