{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:SNNEKC2PHTTDYR2WLY7XAQ2JT5","short_pith_number":"pith:SNNEKC2P","schema_version":"1.0","canonical_sha256":"935a450b4f3ce63c47565e3f7043499f5032b9656e8db23759af9ec65c584069","source":{"kind":"arxiv","id":"2111.13564","version":2},"attestation_state":"computed","paper":{"title":"Coulomb and Higgs Branches from Canonical Singularities, Part 1: Hypersurfaces with Smooth Calabi-Yau Resolutions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Cyril Closset, Sakura Schafer-Nameki, Yi-Nan Wang","submitted_at":"2021-11-26T16:00:34Z","abstract_excerpt":"Compactification of M-theory and of IIB string theory on threefold canonical singularities gives rise to superconformal field theories (SCFTs) in 5d and 4d, respectively. The resolutions and deformations of the singularities encode salient features of the SCFTs and of their moduli spaces. In this paper, we build on Part 0 of this series (arXiv:2007.15600) and further explore the physics of SCFTs arising from isolated hypersurface singularities. We study in detail these canonical isolated hypersurface singularities that admit a smooth Calabi-Yau (crepant) resolution. Their 5d and 4d physics is "},"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":"2111.13564","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-11-26T16:00:34Z","cross_cats_sorted":[],"title_canon_sha256":"5264feda722e836b43c5e88ecc9be2bd023c20f07e7f367df6c2769b1c72d1fe","abstract_canon_sha256":"627d0ec1e98f2ec8dd14e2e21c2f554ce2f6089f5a7956c701f7fb4bd6085ea7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:52:50.999000Z","signature_b64":"TY3YeXpTpW1OAH+53UmvimynPb0AR0a05F3bMUISAuXHZZ+9ipx/t7HwrHsPhNy5tltPgF/uGHuQTaD/923KCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"935a450b4f3ce63c47565e3f7043499f5032b9656e8db23759af9ec65c584069","last_reissued_at":"2026-07-05T05:52:50.998537Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:52:50.998537Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coulomb and Higgs Branches from Canonical Singularities, Part 1: Hypersurfaces with Smooth Calabi-Yau Resolutions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Cyril Closset, Sakura Schafer-Nameki, Yi-Nan Wang","submitted_at":"2021-11-26T16:00:34Z","abstract_excerpt":"Compactification of M-theory and of IIB string theory on threefold canonical singularities gives rise to superconformal field theories (SCFTs) in 5d and 4d, respectively. The resolutions and deformations of the singularities encode salient features of the SCFTs and of their moduli spaces. In this paper, we build on Part 0 of this series (arXiv:2007.15600) and further explore the physics of SCFTs arising from isolated hypersurface singularities. We study in detail these canonical isolated hypersurface singularities that admit a smooth Calabi-Yau (crepant) resolution. Their 5d and 4d physics is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.13564","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2111.13564/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":"2111.13564","created_at":"2026-07-05T05:52:50.998593+00:00"},{"alias_kind":"arxiv_version","alias_value":"2111.13564v2","created_at":"2026-07-05T05:52:50.998593+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.13564","created_at":"2026-07-05T05:52:50.998593+00:00"},{"alias_kind":"pith_short_12","alias_value":"SNNEKC2PHTTD","created_at":"2026-07-05T05:52:50.998593+00:00"},{"alias_kind":"pith_short_16","alias_value":"SNNEKC2PHTTDYR2W","created_at":"2026-07-05T05:52:50.998593+00:00"},{"alias_kind":"pith_short_8","alias_value":"SNNEKC2P","created_at":"2026-07-05T05:52:50.998593+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2112.02092","citing_title":"Symmetry TFTs from String Theory","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16497","citing_title":"5d Trinions and Tetraons","ref_index":46,"is_internal_anchor":false},{"citing_arxiv_id":"2307.07547","citing_title":"Lectures on Generalized Symmetries","ref_index":70,"is_internal_anchor":false},{"citing_arxiv_id":"2305.18296","citing_title":"ICTP Lectures on (Non-)Invertible Generalized Symmetries","ref_index":141,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03119","citing_title":"From Quivers to Geometry: 5d Conformal Matter","ref_index":42,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5","json":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5.json","graph_json":"https://pith.science/api/pith-number/SNNEKC2PHTTDYR2WLY7XAQ2JT5/graph.json","events_json":"https://pith.science/api/pith-number/SNNEKC2PHTTDYR2WLY7XAQ2JT5/events.json","paper":"https://pith.science/paper/SNNEKC2P"},"agent_actions":{"view_html":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5","download_json":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5.json","view_paper":"https://pith.science/paper/SNNEKC2P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2111.13564&json=true","fetch_graph":"https://pith.science/api/pith-number/SNNEKC2PHTTDYR2WLY7XAQ2JT5/graph.json","fetch_events":"https://pith.science/api/pith-number/SNNEKC2PHTTDYR2WLY7XAQ2JT5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5/action/storage_attestation","attest_author":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5/action/author_attestation","sign_citation":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5/action/citation_signature","submit_replication":"https://pith.science/pith/SNNEKC2PHTTDYR2WLY7XAQ2JT5/action/replication_record"}},"created_at":"2026-07-05T05:52:50.998593+00:00","updated_at":"2026-07-05T05:52:50.998593+00:00"}