{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:X4CNTRLRA77F5R3IWNHIUKRMBN","short_pith_number":"pith:X4CNTRLR","schema_version":"1.0","canonical_sha256":"bf04d9c57107fe5ec768b34e8a2a2c0b54c1191ddd1317020287d464fb71d4ad","source":{"kind":"arxiv","id":"1806.08353","version":3},"attestation_state":"computed","paper":{"title":"Landscape of Simple Superconformal Field Theories in 4d","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emily Nardoni, Jaewon Song, Kazunobu Maruyoshi","submitted_at":"2018-06-21T17:58:39Z","abstract_excerpt":"We explore the space of renormalization group flows that originate from $\\mathcal{N}=1$ supersymmetric $SU(2)$ gauge theory with one adjoint and a pair of fundamental chiral multiplets. By considering all possible relevant deformations - including coupling to gauge-singlet chiral multiplets - we find 34 fixed points in this simple setup. We observe that theories in this class exhibit many novel phenomena: emergent symmetry, decoupling of operators, and narrow distribution of central charges $a/c$. This set of theories includes two of the $\\mathcal{N}=2$ minimal Argyres-Douglas theories and the"},"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":"1806.08353","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-06-21T17:58:39Z","cross_cats_sorted":[],"title_canon_sha256":"ae7a8659a994a884b8d05a7ca7c62ad9b16d81de1b9ed893e39b47079a922211","abstract_canon_sha256":"1a3858b3ced60e4f9214f3e0ae9817e7b8d50732ddef8236652d0c9eb77997e1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:49:43.560113Z","signature_b64":"pKqXCB36ok/uHhD96RZ8BCddUDxare42Hbg/cSWoHlPOzhjdbmfeI4xYezKkLSsv6Lgs6Jt4YqFwM0Al3kqwAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf04d9c57107fe5ec768b34e8a2a2c0b54c1191ddd1317020287d464fb71d4ad","last_reissued_at":"2026-05-17T23:49:43.559537Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:49:43.559537Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Landscape of Simple Superconformal Field Theories in 4d","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emily Nardoni, Jaewon Song, Kazunobu Maruyoshi","submitted_at":"2018-06-21T17:58:39Z","abstract_excerpt":"We explore the space of renormalization group flows that originate from $\\mathcal{N}=1$ supersymmetric $SU(2)$ gauge theory with one adjoint and a pair of fundamental chiral multiplets. By considering all possible relevant deformations - including coupling to gauge-singlet chiral multiplets - we find 34 fixed points in this simple setup. We observe that theories in this class exhibit many novel phenomena: emergent symmetry, decoupling of operators, and narrow distribution of central charges $a/c$. This set of theories includes two of the $\\mathcal{N}=2$ minimal Argyres-Douglas theories and the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.08353","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":""},"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":"1806.08353","created_at":"2026-05-17T23:49:43.559631+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.08353v3","created_at":"2026-05-17T23:49:43.559631+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.08353","created_at":"2026-05-17T23:49:43.559631+00:00"},{"alias_kind":"pith_short_12","alias_value":"X4CNTRLRA77F","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_16","alias_value":"X4CNTRLRA77F5R3I","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_8","alias_value":"X4CNTRLR","created_at":"2026-05-18T12:33:01.666342+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":60,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN","json":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN.json","graph_json":"https://pith.science/api/pith-number/X4CNTRLRA77F5R3IWNHIUKRMBN/graph.json","events_json":"https://pith.science/api/pith-number/X4CNTRLRA77F5R3IWNHIUKRMBN/events.json","paper":"https://pith.science/paper/X4CNTRLR"},"agent_actions":{"view_html":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN","download_json":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN.json","view_paper":"https://pith.science/paper/X4CNTRLR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.08353&json=true","fetch_graph":"https://pith.science/api/pith-number/X4CNTRLRA77F5R3IWNHIUKRMBN/graph.json","fetch_events":"https://pith.science/api/pith-number/X4CNTRLRA77F5R3IWNHIUKRMBN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN/action/storage_attestation","attest_author":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN/action/author_attestation","sign_citation":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN/action/citation_signature","submit_replication":"https://pith.science/pith/X4CNTRLRA77F5R3IWNHIUKRMBN/action/replication_record"}},"created_at":"2026-05-17T23:49:43.559631+00:00","updated_at":"2026-05-17T23:49:43.559631+00:00"}