{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:IVMYSOQY6WGWRAKFRANXRLV6ER","short_pith_number":"pith:IVMYSOQY","schema_version":"1.0","canonical_sha256":"4559893a18f58d688145881b78aebe247aae7da9a4e3ea13f5650b31ec46646d","source":{"kind":"arxiv","id":"1704.00799","version":1},"attestation_state":"computed","paper":{"title":"Three dimensional canonical singularity and five dimensional N=1 SCFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dan Xie, Shing-Tung Yau","submitted_at":"2017-04-03T20:35:59Z","abstract_excerpt":"We conjecture that every three dimensional canonical singularity defines a five dimensional N=1 SCFT. Flavor symmetry can be found from singularity structure: non-abelian flavor symmetry is read from the singularity type over one dimensional singular locus. The dimension of Coulomb branch is given by the number of compact crepant divisors from a crepant resolution of singularity. The detailed structure of Coulomb branch is described as follows: a): A chamber of Coulomb branch is described by a crepant resolution, and this chamber is given by its Nef cone and the prepotential is computed from t"},"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":"1704.00799","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-04-03T20:35:59Z","cross_cats_sorted":[],"title_canon_sha256":"57c88c792ba98042d69c1d42b8eeb214826e2dc8298309f6663fb6f6f0a75f96","abstract_canon_sha256":"2949d3f59a42a489185acce062a40d6dbf8dd361791dc44562f168e53b7bdd12"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:55.911891Z","signature_b64":"AFTNqMrECJaO2/FD1BXg8ZskXqe/C9djAJW57RKTu4KK6EEjwlAmCP5s2cKj1WefzBfaxpL1llYFJp4sg3G+AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4559893a18f58d688145881b78aebe247aae7da9a4e3ea13f5650b31ec46646d","last_reissued_at":"2026-05-18T00:38:55.911439Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:55.911439Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three dimensional canonical singularity and five dimensional N=1 SCFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dan Xie, Shing-Tung Yau","submitted_at":"2017-04-03T20:35:59Z","abstract_excerpt":"We conjecture that every three dimensional canonical singularity defines a five dimensional N=1 SCFT. Flavor symmetry can be found from singularity structure: non-abelian flavor symmetry is read from the singularity type over one dimensional singular locus. The dimension of Coulomb branch is given by the number of compact crepant divisors from a crepant resolution of singularity. The detailed structure of Coulomb branch is described as follows: a): A chamber of Coulomb branch is described by a crepant resolution, and this chamber is given by its Nef cone and the prepotential is computed from t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.00799","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":"1704.00799","created_at":"2026-05-18T00:38:55.911498+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.00799v1","created_at":"2026-05-18T00:38:55.911498+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.00799","created_at":"2026-05-18T00:38:55.911498+00:00"},{"alias_kind":"pith_short_12","alias_value":"IVMYSOQY6WGW","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_16","alias_value":"IVMYSOQY6WGWRAKF","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_8","alias_value":"IVMYSOQY","created_at":"2026-05-18T12:31:21.493067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2112.02092","citing_title":"Symmetry TFTs from String Theory","ref_index":53,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16497","citing_title":"5d Trinions and Tetraons","ref_index":43,"is_internal_anchor":true},{"citing_arxiv_id":"2605.03119","citing_title":"From Quivers to Geometry: 5d Conformal Matter","ref_index":73,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER","json":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER.json","graph_json":"https://pith.science/api/pith-number/IVMYSOQY6WGWRAKFRANXRLV6ER/graph.json","events_json":"https://pith.science/api/pith-number/IVMYSOQY6WGWRAKFRANXRLV6ER/events.json","paper":"https://pith.science/paper/IVMYSOQY"},"agent_actions":{"view_html":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER","download_json":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER.json","view_paper":"https://pith.science/paper/IVMYSOQY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.00799&json=true","fetch_graph":"https://pith.science/api/pith-number/IVMYSOQY6WGWRAKFRANXRLV6ER/graph.json","fetch_events":"https://pith.science/api/pith-number/IVMYSOQY6WGWRAKFRANXRLV6ER/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER/action/storage_attestation","attest_author":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER/action/author_attestation","sign_citation":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER/action/citation_signature","submit_replication":"https://pith.science/pith/IVMYSOQY6WGWRAKFRANXRLV6ER/action/replication_record"}},"created_at":"2026-05-18T00:38:55.911498+00:00","updated_at":"2026-05-18T00:38:55.911498+00:00"}