{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:FL5NPGJCXTMXL5TIRM5RFLBCBN","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"364f787ce7395ace4b8211cbd568e4d73dbbbc5d5912cbc0e6b6b017b47586bb","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-12-11T19:04:07Z","title_canon_sha256":"c2dcbb841417071f576853e196a5ff115fac987e217e950144389dfc1a8cb0b9"},"schema_version":"1.0","source":{"id":"2412.08732","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2412.08732","created_at":"2026-07-05T11:33:48Z"},{"alias_kind":"arxiv_version","alias_value":"2412.08732v2","created_at":"2026-07-05T11:33:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.08732","created_at":"2026-07-05T11:33:48Z"},{"alias_kind":"pith_short_12","alias_value":"FL5NPGJCXTMX","created_at":"2026-07-05T11:33:48Z"},{"alias_kind":"pith_short_16","alias_value":"FL5NPGJCXTMXL5TI","created_at":"2026-07-05T11:33:48Z"},{"alias_kind":"pith_short_8","alias_value":"FL5NPGJC","created_at":"2026-07-05T11:33:48Z"}],"graph_snapshots":[{"event_id":"sha256:aa1fd643e2a2815e861428fad99b90d5c03dbeaa32af8874ab7810ece51456ac","target":"graph","created_at":"2026-07-05T11:33:48Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2412.08732/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A broad class of observables in four-dimensional $\\mathcal{N}=2$ and $\\mathcal{N}=4$ superconformal Yang-Mills theories can be exactly computed for arbitrary 't Hooft coupling as Fredholm determinants of integrable Bessel operators. These observables admit a unifying description through a one-parameter generating function, which possesses a determinant representation involving a matrix generalization of the Bessel operator. We analyze this generating function over a wide range of parameter values and finite 't Hooft coupling. We demonstrate that it has a well-behaved weak-coupling expansion wi","authors_text":"Bercel Boldis, Gregory P. Korchemsky, Zoltan Bajnok","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-12-11T19:04:07Z","title":"Exploring superconformal Yang-Mills theories through matrix Bessel kernels"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.08732","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:06823119371d9e08b2cbb666175b124d3df89cf7527a840ccb2fb0146c1cb938","target":"record","created_at":"2026-07-05T11:33:48Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"364f787ce7395ace4b8211cbd568e4d73dbbbc5d5912cbc0e6b6b017b47586bb","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-12-11T19:04:07Z","title_canon_sha256":"c2dcbb841417071f576853e196a5ff115fac987e217e950144389dfc1a8cb0b9"},"schema_version":"1.0","source":{"id":"2412.08732","kind":"arxiv","version":2}},"canonical_sha256":"2afad79922bcd975f6688b3b12ac220b57710e2e5305f87904ac82aa8e161783","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2afad79922bcd975f6688b3b12ac220b57710e2e5305f87904ac82aa8e161783","first_computed_at":"2026-07-05T11:33:48.369564Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:33:48.369564Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"513gTTkhhiUr/hCmaXD97QjqLa0jrBvrqyHp+ih9ginbtgw6DJlHCDh+tJRvQFNk9Sd8TJbtTxvArGUOOabeAg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:33:48.370000Z","signed_message":"canonical_sha256_bytes"},"source_id":"2412.08732","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:06823119371d9e08b2cbb666175b124d3df89cf7527a840ccb2fb0146c1cb938","sha256:aa1fd643e2a2815e861428fad99b90d5c03dbeaa32af8874ab7810ece51456ac"],"state_sha256":"c885ae2a8883b7848e4482dfd635ebd13732311dc7812719d94224dc8af74cd4"}