{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:KHQ6I3FTXOEC2TRV264P6QH2QQ","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":"4ce4ba9a1b5d05e5289584643b2150b7f8f96ed06d51fcf6397d373a029b7a00","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2021-07-21T11:12:27Z","title_canon_sha256":"872bbe6b4cf211ff2e87f0f73909345fc18b27cd79fd12e671e2d31437a90619"},"schema_version":"1.0","source":{"id":"2107.10011","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2107.10011","created_at":"2026-07-05T03:29:17Z"},{"alias_kind":"arxiv_version","alias_value":"2107.10011v2","created_at":"2026-07-05T03:29:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.10011","created_at":"2026-07-05T03:29:17Z"},{"alias_kind":"pith_short_12","alias_value":"KHQ6I3FTXOEC","created_at":"2026-07-05T03:29:17Z"},{"alias_kind":"pith_short_16","alias_value":"KHQ6I3FTXOEC2TRV","created_at":"2026-07-05T03:29:17Z"},{"alias_kind":"pith_short_8","alias_value":"KHQ6I3FT","created_at":"2026-07-05T03:29:17Z"}],"graph_snapshots":[{"event_id":"sha256:211a155364b46c4bd6bb2385ca41bcbc2a7d064b91f2cf03206a0e677725f47c","target":"graph","created_at":"2026-07-05T03:29:17Z","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/2107.10011/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We update lattice QCD results for second order cumulants of conserved charge fluctuations and correlations at non-zero temperature and vanishing values of the conserved charge chemical potentials. We compare these results to hadron resonance gas calculations with and without excluded volume terms as well as S-matrix results in the hadronic phase of QCD, and comment on their current limitations. We, furthermore, use these results to characterize thermal conditions in the vicinity of the pseudo-critical line of the chiral transition in QCD. We argue that the ratio of strange to baryon chemical p","authors_text":"C. Schmidt, D. Bollweg, F. Karsch, J. Goswami, O. Kaczmarek, P. Petreczky, P. Scior, Swagato Mukherjee","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2021-07-21T11:12:27Z","title":"Second order cumulants of conserved charge fluctuations revisited I. Vanishing chemical potentials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.10011","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":"sha256:3a6312a0347b8a6b3dc7de31cb66ce843edcff92a64dea03f6c05c0eb984dc95","target":"record","created_at":"2026-07-05T03:29:17Z","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":"4ce4ba9a1b5d05e5289584643b2150b7f8f96ed06d51fcf6397d373a029b7a00","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2021-07-21T11:12:27Z","title_canon_sha256":"872bbe6b4cf211ff2e87f0f73909345fc18b27cd79fd12e671e2d31437a90619"},"schema_version":"1.0","source":{"id":"2107.10011","kind":"arxiv","version":2}},"canonical_sha256":"51e1e46cb3bb882d4e35d7b8ff40fa8429b3a67f98a4a8c8866eba09d2d1e2cd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"51e1e46cb3bb882d4e35d7b8ff40fa8429b3a67f98a4a8c8866eba09d2d1e2cd","first_computed_at":"2026-07-05T03:29:17.938785Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:29:17.938785Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/xkbK0uVHdrg1oMdVJ9ejdWFttJhzqic1O6KrqoBysQGUw7xssIZjzv6/L1sDuSLZaJZc1+GgrML8oFA3I54Aw==","signature_status":"signed_v1","signed_at":"2026-07-05T03:29:17.939228Z","signed_message":"canonical_sha256_bytes"},"source_id":"2107.10011","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3a6312a0347b8a6b3dc7de31cb66ce843edcff92a64dea03f6c05c0eb984dc95","sha256:211a155364b46c4bd6bb2385ca41bcbc2a7d064b91f2cf03206a0e677725f47c"],"state_sha256":"d3cba81854dfedb1a010b3e162f1deac2f760181f7ef66d0f6b15f2ff1ccca6c"}