{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:GRTWBXCPIOR7LT3AXQA5FCOR4Y","short_pith_number":"pith:GRTWBXCP","schema_version":"1.0","canonical_sha256":"346760dc4f43a3f5cf60bc01d289d1e62376a8c3fd1e85c3c07d60e379a10558","source":{"kind":"arxiv","id":"2401.00628","version":1},"attestation_state":"computed","paper":{"title":"On the 2D Yang-Mills/Hurwitz Correspondence","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"math.CO","authors_text":"Jonathan Novak","submitted_at":"2024-01-01T01:26:53Z","abstract_excerpt":"In this paper, we show that in the large $N$ limit two-dimensional Yang-Mills theory with $U(N)$ gauge group becomes mixed Hurwitz theory, in the sense that the $1/N$ expansion of the chiral partition function receives contributions from both classical and monotone Hurwitz theory for all but finitely many compact orientable spacetimes."},"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":"2401.00628","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"math.CO","submitted_at":"2024-01-01T01:26:53Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"c24b3ff1b2cda655ab8c7dff39484b614943a336be7c4a583be25d1e4a2587a7","abstract_canon_sha256":"dca7cf1214e2f5c8a7f81200b230ec02ecad5a912abb145324e39f0ce0324c76"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:29:21.006272Z","signature_b64":"o1QGnI6mwCenPD8ZxbIJCetXiQV0mXWhAQgRor9FWpTP5EcNJnZrAaPyr0nvGD2mBaVcNE1wje5uek05Kkf0CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"346760dc4f43a3f5cf60bc01d289d1e62376a8c3fd1e85c3c07d60e379a10558","last_reissued_at":"2026-07-05T07:29:21.005825Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:29:21.005825Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the 2D Yang-Mills/Hurwitz Correspondence","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"math.CO","authors_text":"Jonathan Novak","submitted_at":"2024-01-01T01:26:53Z","abstract_excerpt":"In this paper, we show that in the large $N$ limit two-dimensional Yang-Mills theory with $U(N)$ gauge group becomes mixed Hurwitz theory, in the sense that the $1/N$ expansion of the chiral partition function receives contributions from both classical and monotone Hurwitz theory for all but finitely many compact orientable spacetimes."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.00628","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2401.00628/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":"2401.00628","created_at":"2026-07-05T07:29:21.005881+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.00628v1","created_at":"2026-07-05T07:29:21.005881+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.00628","created_at":"2026-07-05T07:29:21.005881+00:00"},{"alias_kind":"pith_short_12","alias_value":"GRTWBXCPIOR7","created_at":"2026-07-05T07:29:21.005881+00:00"},{"alias_kind":"pith_short_16","alias_value":"GRTWBXCPIOR7LT3A","created_at":"2026-07-05T07:29:21.005881+00:00"},{"alias_kind":"pith_short_8","alias_value":"GRTWBXCP","created_at":"2026-07-05T07:29:21.005881+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.28945","citing_title":"The heat-kernel master field on $\\mathbb{Z}^d$ at strong coupling","ref_index":73,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y","json":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y.json","graph_json":"https://pith.science/api/pith-number/GRTWBXCPIOR7LT3AXQA5FCOR4Y/graph.json","events_json":"https://pith.science/api/pith-number/GRTWBXCPIOR7LT3AXQA5FCOR4Y/events.json","paper":"https://pith.science/paper/GRTWBXCP"},"agent_actions":{"view_html":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y","download_json":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y.json","view_paper":"https://pith.science/paper/GRTWBXCP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.00628&json=true","fetch_graph":"https://pith.science/api/pith-number/GRTWBXCPIOR7LT3AXQA5FCOR4Y/graph.json","fetch_events":"https://pith.science/api/pith-number/GRTWBXCPIOR7LT3AXQA5FCOR4Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y/action/storage_attestation","attest_author":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y/action/author_attestation","sign_citation":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y/action/citation_signature","submit_replication":"https://pith.science/pith/GRTWBXCPIOR7LT3AXQA5FCOR4Y/action/replication_record"}},"created_at":"2026-07-05T07:29:21.005881+00:00","updated_at":"2026-07-05T07:29:21.005881+00:00"}