{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:6UOH67KHE42OYS24PV253LREDQ","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":"c2af8e02e8a113241cc4e73b11d7516047fbbdf288311e4bbf5e0ab0d121eb63","cross_cats_sorted":["gr-qc","math-ph","math.CA","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-06-10T18:00:03Z","title_canon_sha256":"2e61b596f5e2fed9d6a8e7e52c39da0ef75fc3a1143092881b16b8839feac929"},"schema_version":"1.0","source":{"id":"2606.12529","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.12529","created_at":"2026-06-12T00:07:53Z"},{"alias_kind":"arxiv_version","alias_value":"2606.12529v1","created_at":"2026-06-12T00:07:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.12529","created_at":"2026-06-12T00:07:53Z"},{"alias_kind":"pith_short_12","alias_value":"6UOH67KHE42O","created_at":"2026-06-12T00:07:53Z"},{"alias_kind":"pith_short_16","alias_value":"6UOH67KHE42OYS24","created_at":"2026-06-12T00:07:53Z"},{"alias_kind":"pith_short_8","alias_value":"6UOH67KH","created_at":"2026-06-12T00:07:53Z"}],"graph_snapshots":[{"event_id":"sha256:4bbfaeed8c08e5db8d8833f41ace2e566c83b65a47a6a3def04fb83c1a3dc22d","target":"graph","created_at":"2026-06-12T00:07:53Z","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/2606.12529/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study perturbations of Yang-Mills plasma, represented by scalar quasinormal modes of AdS black branes, as functions of the wave number $q$ in the entire range from zero to infinity. At finite $q$, these modes can be computed by classical spectral methods based on truncating the boundary value problem. We show that this truncation admits a natural analytic interpretation in terms of quantum Seiberg--Witten periods in the Nekrasov--Shatashvili limit, with the spectral condition organised as an instanton expansion around small values of the counting parameter. The physical black-brane problem ","authors_text":"Alex Ratcliffe, In\\^es Aniceto, Micha{\\l} Spali\\'nski, Paolo Arnaudo","cross_cats":["gr-qc","math-ph","math.CA","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-06-10T18:00:03Z","title":"Analytic approaches to perturbations of strongly coupled Yang-Mills plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.12529","kind":"arxiv","version":1},"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":"sha256:548100127226832f7dcff89218463d8259263365e90c483bd411b7badd67eab9","target":"record","created_at":"2026-06-12T00:07:53Z","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":"c2af8e02e8a113241cc4e73b11d7516047fbbdf288311e4bbf5e0ab0d121eb63","cross_cats_sorted":["gr-qc","math-ph","math.CA","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-06-10T18:00:03Z","title_canon_sha256":"2e61b596f5e2fed9d6a8e7e52c39da0ef75fc3a1143092881b16b8839feac929"},"schema_version":"1.0","source":{"id":"2606.12529","kind":"arxiv","version":1}},"canonical_sha256":"f51c7f7d472734ec4b5c7d75ddae241c0f035ba2086396004a95da86f3fef862","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f51c7f7d472734ec4b5c7d75ddae241c0f035ba2086396004a95da86f3fef862","first_computed_at":"2026-06-12T00:07:53.657668Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-12T00:07:53.657668Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tr82co66ulLXJbimoi2iFjIBJHec8K+ghT8vhKsFM12GsNu9VYPaCq4STf+cwd/2vt7jSoPdjM0HlDxCfwn/Dw==","signature_status":"signed_v1","signed_at":"2026-06-12T00:07:53.658105Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.12529","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:548100127226832f7dcff89218463d8259263365e90c483bd411b7badd67eab9","sha256:4bbfaeed8c08e5db8d8833f41ace2e566c83b65a47a6a3def04fb83c1a3dc22d"],"state_sha256":"51132da6da71dbb71857a484096a3830619b7f58d265371e77cac86742a8e4a2"}