{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:HEV7JF46N6YE5EAWQYIPS4VOG7","short_pith_number":"pith:HEV7JF46","schema_version":"1.0","canonical_sha256":"392bf4979e6fb04e90168610f972ae37d1477b5dd3f2684e4094f3839739ca2e","source":{"kind":"arxiv","id":"2111.12092","version":3},"attestation_state":"computed","paper":{"title":"Infinitely many 4d N=1 SCFTs with a=c","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Craig Lawrie, Jaewon Song, Ki-Hong Lee, Monica Jinwoo Kang","submitted_at":"2021-11-23T19:00:00Z","abstract_excerpt":"We study a rich set of four-dimensional $\\mathcal{N}=1$ superconformal field theories (SCFTs) with both central charges identical: $a = c$. We construct them via the diagonal $\\mathcal{N}=1$ gauging of the flavor symmetry $G$ of a collection of $\\mathcal{N}=2$ Argyres--Douglas theories of type $\\mathcal{D}_p(G)$, with or without additional adjoint chiral multiplets. In this way, we construct infinitely-many theories that flow to interacting SCFTs with $a = c$ in the infrared. Finally, we briefly highlight the features of the SCFTs without $a = c$ that arise from generalizing this construction."},"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":"2111.12092","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-11-23T19:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"bfb2d2bb3da2730efea73c341ce777a2974c6e134c50125e59e3020293d93c39","abstract_canon_sha256":"b2ac7279c76431f2a393a80fe873eb054c863c9adbcca0239919a1c414728291"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:54:26.772164Z","signature_b64":"LJcsbYotzr2heYnlZHHJg8/WqCaPfsy99ydNaxTV5j4f18au1n1lynEDhpTePIj4QuGGloWjnPuRQYgWNQLACg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"392bf4979e6fb04e90168610f972ae37d1477b5dd3f2684e4094f3839739ca2e","last_reissued_at":"2026-07-05T05:54:26.771697Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:54:26.771697Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Infinitely many 4d N=1 SCFTs with a=c","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Craig Lawrie, Jaewon Song, Ki-Hong Lee, Monica Jinwoo Kang","submitted_at":"2021-11-23T19:00:00Z","abstract_excerpt":"We study a rich set of four-dimensional $\\mathcal{N}=1$ superconformal field theories (SCFTs) with both central charges identical: $a = c$. We construct them via the diagonal $\\mathcal{N}=1$ gauging of the flavor symmetry $G$ of a collection of $\\mathcal{N}=2$ Argyres--Douglas theories of type $\\mathcal{D}_p(G)$, with or without additional adjoint chiral multiplets. In this way, we construct infinitely-many theories that flow to interacting SCFTs with $a = c$ in the infrared. Finally, we briefly highlight the features of the SCFTs without $a = c$ that arise from generalizing this construction."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.12092","kind":"arxiv","version":3},"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/2111.12092/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":"2111.12092","created_at":"2026-07-05T05:54:26.771757+00:00"},{"alias_kind":"arxiv_version","alias_value":"2111.12092v3","created_at":"2026-07-05T05:54:26.771757+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.12092","created_at":"2026-07-05T05:54:26.771757+00:00"},{"alias_kind":"pith_short_12","alias_value":"HEV7JF46N6YE","created_at":"2026-07-05T05:54:26.771757+00:00"},{"alias_kind":"pith_short_16","alias_value":"HEV7JF46N6YE5EAW","created_at":"2026-07-05T05:54:26.771757+00:00"},{"alias_kind":"pith_short_8","alias_value":"HEV7JF46","created_at":"2026-07-05T05:54:26.771757+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.17895","citing_title":"A landscape of 4d N=1 SCFTs with a=c","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7","json":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7.json","graph_json":"https://pith.science/api/pith-number/HEV7JF46N6YE5EAWQYIPS4VOG7/graph.json","events_json":"https://pith.science/api/pith-number/HEV7JF46N6YE5EAWQYIPS4VOG7/events.json","paper":"https://pith.science/paper/HEV7JF46"},"agent_actions":{"view_html":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7","download_json":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7.json","view_paper":"https://pith.science/paper/HEV7JF46","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2111.12092&json=true","fetch_graph":"https://pith.science/api/pith-number/HEV7JF46N6YE5EAWQYIPS4VOG7/graph.json","fetch_events":"https://pith.science/api/pith-number/HEV7JF46N6YE5EAWQYIPS4VOG7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7/action/storage_attestation","attest_author":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7/action/author_attestation","sign_citation":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7/action/citation_signature","submit_replication":"https://pith.science/pith/HEV7JF46N6YE5EAWQYIPS4VOG7/action/replication_record"}},"created_at":"2026-07-05T05:54:26.771757+00:00","updated_at":"2026-07-05T05:54:26.771757+00:00"}