{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:SQWRMGEUPZ4QIB6MD22U67LVUG","short_pith_number":"pith:SQWRMGEU","schema_version":"1.0","canonical_sha256":"942d1618947e790407cc1eb54f7d75a19043167241c257d08f726544563b5716","source":{"kind":"arxiv","id":"1807.01754","version":2},"attestation_state":"computed","paper":{"title":"Moduli space singularities for $3d$ $\\mathcal{N} = 4$ circular quiver gauge theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jamie Rogers, Radu Tatar","submitted_at":"2018-07-04T19:31:21Z","abstract_excerpt":"The singularity structure of the Coulomb and Higgs branches of good $3d$ $\\mathcal{N}=4$ circular quiver gauge theories (CQGTs) with unitary gauge groups is studied. The central method employed is the Kraft--Procesi transition. CQGTs are described as a generalisation of a class of linear quivers. This class degenerates into the familiar class $T_{\\rho}^{\\sigma}(SU(N))$ in the linear case, however the circular case does not have the degeneracy and so the class of CQGTs contains many more theories and much more structure. We describe a collection of good, unitary, CQGTs from which the entire cla"},"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":"1807.01754","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-07-04T19:31:21Z","cross_cats_sorted":[],"title_canon_sha256":"94fd3c68a7c33e2520a9b88aa7132ba907752dc7c87a5078fce3eb7346f71345","abstract_canon_sha256":"86babbfbb7ee6c3651ce851fd6307f8cc025b0ffa56a0e1c773bf6c948216a52"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:01:19.399546Z","signature_b64":"fbPvEk3OCRXggYY+MN2PhBQcfDHgya4l2whp4FhWztUrODdAWPhB9BOJWbJt/m2A+5wIiyVmO/f038ZTj7QWDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"942d1618947e790407cc1eb54f7d75a19043167241c257d08f726544563b5716","last_reissued_at":"2026-05-18T00:01:19.398983Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:01:19.398983Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Moduli space singularities for $3d$ $\\mathcal{N} = 4$ circular quiver gauge theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jamie Rogers, Radu Tatar","submitted_at":"2018-07-04T19:31:21Z","abstract_excerpt":"The singularity structure of the Coulomb and Higgs branches of good $3d$ $\\mathcal{N}=4$ circular quiver gauge theories (CQGTs) with unitary gauge groups is studied. The central method employed is the Kraft--Procesi transition. CQGTs are described as a generalisation of a class of linear quivers. This class degenerates into the familiar class $T_{\\rho}^{\\sigma}(SU(N))$ in the linear case, however the circular case does not have the degeneracy and so the class of CQGTs contains many more theories and much more structure. We describe a collection of good, unitary, CQGTs from which the entire cla"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.01754","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":""},"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":"1807.01754","created_at":"2026-05-18T00:01:19.399057+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.01754v2","created_at":"2026-05-18T00:01:19.399057+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.01754","created_at":"2026-05-18T00:01:19.399057+00:00"},{"alias_kind":"pith_short_12","alias_value":"SQWRMGEUPZ4Q","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_16","alias_value":"SQWRMGEUPZ4QIB6M","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_8","alias_value":"SQWRMGEU","created_at":"2026-05-18T12:32:53.628368+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG","json":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG.json","graph_json":"https://pith.science/api/pith-number/SQWRMGEUPZ4QIB6MD22U67LVUG/graph.json","events_json":"https://pith.science/api/pith-number/SQWRMGEUPZ4QIB6MD22U67LVUG/events.json","paper":"https://pith.science/paper/SQWRMGEU"},"agent_actions":{"view_html":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG","download_json":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG.json","view_paper":"https://pith.science/paper/SQWRMGEU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.01754&json=true","fetch_graph":"https://pith.science/api/pith-number/SQWRMGEUPZ4QIB6MD22U67LVUG/graph.json","fetch_events":"https://pith.science/api/pith-number/SQWRMGEUPZ4QIB6MD22U67LVUG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG/action/storage_attestation","attest_author":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG/action/author_attestation","sign_citation":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG/action/citation_signature","submit_replication":"https://pith.science/pith/SQWRMGEUPZ4QIB6MD22U67LVUG/action/replication_record"}},"created_at":"2026-05-18T00:01:19.399057+00:00","updated_at":"2026-05-18T00:01:19.399057+00:00"}