{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:ILD6NMAJDH6PC35X67H7RCYVAK","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":"aaec437112b373c2d4ec6dc20742660755f19d333780952f3c02eb6e127c2be7","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2023-11-11T19:22:57Z","title_canon_sha256":"7350777203e883ceedb89686c1510e59138ad68ae1e8dd7a3c09f26b897a2721"},"schema_version":"1.0","source":{"id":"2311.06646","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.06646","created_at":"2026-07-05T07:29:29Z"},{"alias_kind":"arxiv_version","alias_value":"2311.06646v2","created_at":"2026-07-05T07:29:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.06646","created_at":"2026-07-05T07:29:29Z"},{"alias_kind":"pith_short_12","alias_value":"ILD6NMAJDH6P","created_at":"2026-07-05T07:29:29Z"},{"alias_kind":"pith_short_16","alias_value":"ILD6NMAJDH6PC35X","created_at":"2026-07-05T07:29:29Z"},{"alias_kind":"pith_short_8","alias_value":"ILD6NMAJ","created_at":"2026-07-05T07:29:29Z"}],"graph_snapshots":[{"event_id":"sha256:b1ccb1b048f6ab1a5a8ae8346724ee1600051a4782a8db12c744054cc07f24f3","target":"graph","created_at":"2026-07-05T07:29:29Z","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/2311.06646/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We determine the pure-gauge $\\mathrm{SU}(3)$ topological susceptibility slope $\\chi^\\prime$, related to the next-to-leading-order term of the momentum expansion of the topological charge density 2-point correlator, from numerical lattice Monte Carlo simulations. Our strategy consists in performing a double-limit extrapolation: first we take the continuum limit at fixed smoothing radius, then we take the zero-smoothing-radius limit. Our final result is $\\chi^\\prime = [17.1(2.1)~\\mathrm{MeV}]^2$. We also discuss a theoretical argument to predict its value in the large-$N$ limit, which turns out ","authors_text":"Claudio Bonanno","cross_cats":["hep-ph","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2023-11-11T19:22:57Z","title":"The topological susceptibility slope $\\chi^\\prime$ of the pure-gauge SU(3) Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.06646","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":"sha256:226c83dcd11703435ecd2fa79442be1894159dd778848fdd7311f388358e4cde","target":"record","created_at":"2026-07-05T07:29:29Z","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":"aaec437112b373c2d4ec6dc20742660755f19d333780952f3c02eb6e127c2be7","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2023-11-11T19:22:57Z","title_canon_sha256":"7350777203e883ceedb89686c1510e59138ad68ae1e8dd7a3c09f26b897a2721"},"schema_version":"1.0","source":{"id":"2311.06646","kind":"arxiv","version":2}},"canonical_sha256":"42c7e6b00919fcf16fb7f7cff88b1502bec771f6fe419e4aa13bf20696711969","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"42c7e6b00919fcf16fb7f7cff88b1502bec771f6fe419e4aa13bf20696711969","first_computed_at":"2026-07-05T07:29:29.459450Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:29:29.459450Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Oe/jstH7RvV3El14torGqQLWimFV34LsCrtEcjX51wVs8Pyk/Fwwzkcs0nHplJ6jIDJvOT35wuXjN3Z6jwXZBA==","signature_status":"signed_v1","signed_at":"2026-07-05T07:29:29.460643Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.06646","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:226c83dcd11703435ecd2fa79442be1894159dd778848fdd7311f388358e4cde","sha256:b1ccb1b048f6ab1a5a8ae8346724ee1600051a4782a8db12c744054cc07f24f3"],"state_sha256":"cb56fcb42288904869775ee40cb72a06a03613bd853ca296fd9b788194e4cbb7"}