{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:42CXVKLAFAAU4UEULU2FSZVWIR","short_pith_number":"pith:42CXVKLA","schema_version":"1.0","canonical_sha256":"e6857aa96028014e50945d345966b644595d31bc189a2ed1414f09beb3a7d506","source":{"kind":"arxiv","id":"2004.09738","version":3},"attestation_state":"computed","paper":{"title":"Three Dimensional Mirror Symmetry beyond $ADE$ quivers and Argyres-Douglas theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Anindya Dey","submitted_at":"2020-04-21T03:34:03Z","abstract_excerpt":"Mirror symmetry, a three dimensional $\\mathcal{N}=4$ IR duality, has been studied in detail for quiver gauge theories of the $ADE$-type (as well as their affine versions) with unitary gauge groups. The $A$-type quivers (also known as linear quivers) and the associated mirror dualities have a particularly simple realization in terms of a Type IIB system of D3-D5-NS5-branes. In this paper, we present a systematic field theory prescription for constructing 3d mirror pairs beyond the $ADE$ quiver gauge theories, starting from a dual pair of $A$-type quivers with unitary gauge groups. The construct"},"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":"2004.09738","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-04-21T03:34:03Z","cross_cats_sorted":[],"title_canon_sha256":"f04a6a55991d4971e4ea9bca2cf5da9e76b5b8a3ef50677b67786436758bfebf","abstract_canon_sha256":"e80167faf43083fc2d17f846744af0eb22c977f0e3b97a8ad89613bcbac635e7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:43:34.248878Z","signature_b64":"q7UYOFyutnT5Q6n7scguUms0UjHQvuBe/A0r62fmx9FLLYNglOLfMVJk+PiZcZpqilUwqU+OT9btDY3D9IaxCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6857aa96028014e50945d345966b644595d31bc189a2ed1414f09beb3a7d506","last_reissued_at":"2026-07-05T05:43:34.248389Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:43:34.248389Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three Dimensional Mirror Symmetry beyond $ADE$ quivers and Argyres-Douglas theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Anindya Dey","submitted_at":"2020-04-21T03:34:03Z","abstract_excerpt":"Mirror symmetry, a three dimensional $\\mathcal{N}=4$ IR duality, has been studied in detail for quiver gauge theories of the $ADE$-type (as well as their affine versions) with unitary gauge groups. The $A$-type quivers (also known as linear quivers) and the associated mirror dualities have a particularly simple realization in terms of a Type IIB system of D3-D5-NS5-branes. In this paper, we present a systematic field theory prescription for constructing 3d mirror pairs beyond the $ADE$ quiver gauge theories, starting from a dual pair of $A$-type quivers with unitary gauge groups. The construct"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2004.09738","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/2004.09738/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":"2004.09738","created_at":"2026-07-05T05:43:34.248450+00:00"},{"alias_kind":"arxiv_version","alias_value":"2004.09738v3","created_at":"2026-07-05T05:43:34.248450+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2004.09738","created_at":"2026-07-05T05:43:34.248450+00:00"},{"alias_kind":"pith_short_12","alias_value":"42CXVKLAFAAU","created_at":"2026-07-05T05:43:34.248450+00:00"},{"alias_kind":"pith_short_16","alias_value":"42CXVKLAFAAU4UEU","created_at":"2026-07-05T05:43:34.248450+00:00"},{"alias_kind":"pith_short_8","alias_value":"42CXVKLA","created_at":"2026-07-05T05:43:34.248450+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.14531","citing_title":"A Bound on 3d Mirror Pairs","ref_index":62,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR","json":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR.json","graph_json":"https://pith.science/api/pith-number/42CXVKLAFAAU4UEULU2FSZVWIR/graph.json","events_json":"https://pith.science/api/pith-number/42CXVKLAFAAU4UEULU2FSZVWIR/events.json","paper":"https://pith.science/paper/42CXVKLA"},"agent_actions":{"view_html":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR","download_json":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR.json","view_paper":"https://pith.science/paper/42CXVKLA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2004.09738&json=true","fetch_graph":"https://pith.science/api/pith-number/42CXVKLAFAAU4UEULU2FSZVWIR/graph.json","fetch_events":"https://pith.science/api/pith-number/42CXVKLAFAAU4UEULU2FSZVWIR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR/action/storage_attestation","attest_author":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR/action/author_attestation","sign_citation":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR/action/citation_signature","submit_replication":"https://pith.science/pith/42CXVKLAFAAU4UEULU2FSZVWIR/action/replication_record"}},"created_at":"2026-07-05T05:43:34.248450+00:00","updated_at":"2026-07-05T05:43:34.248450+00:00"}