{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:Z3QK3HZYX73NDTYYJKSZ5QFZZU","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":"af467188dcc4996ba970b3a575b2968352ee6e845aa58eaab9cace2d96abdbb8","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-02-11T12:13:38Z","title_canon_sha256":"a1e73437f5423b77dda7e05a15ac5653164559f1debb0bda419507e7cdb20997"},"schema_version":"1.0","source":{"id":"2202.05574","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.05574","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"arxiv_version","alias_value":"2202.05574v2","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.05574","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_12","alias_value":"Z3QK3HZYX73N","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_16","alias_value":"Z3QK3HZYX73NDTYY","created_at":"2026-07-05T04:35:43Z"},{"alias_kind":"pith_short_8","alias_value":"Z3QK3HZY","created_at":"2026-07-05T04:35:43Z"}],"graph_snapshots":[{"event_id":"sha256:cacc8da88b7f56f58eb28455905a657d1ea33ba13ae9448e2797a2b285f25972","target":"graph","created_at":"2026-07-05T04:35:43Z","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/2202.05574/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate a resummed equation of state with lattice QCD simulations at imaginary chemical potentials. This work presents a generalization of the scheme introduced in 2102.06660 to the case of non-zero $\\mu_S$, focusing on the line of strangeness neutrality. We present results up to $\\mu_B/T \\leq 3.5$ on the strangeness neutral line $\\left\\langle S \\right\\rangle = 0$ in the temperature range $130 \\rm{MeV} \\leq T \\leq 280 \\rm{MeV}$. We also extrapolate the finite baryon density equation of state to small non-zero values of the strangeness-to-baryon ratio $R=\\left\\langle S \\right\\rangle / \\lef","authors_text":"Attila Pasztor, Claudia Ratti, Jana N. Guenther, Kalman K. Szabo, Paolo Parotto, Ruben Kara, Szabolcs Borsanyi, Zoltan Fodor","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-02-11T12:13:38Z","title":"Resummed lattice QCD equation of state at finite baryon density: strangeness neutrality and beyond"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.05574","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:eec407c7d5a5077c97e2790bd19ac850f032b7862a9769d911bf10f8d52f3e99","target":"record","created_at":"2026-07-05T04:35:43Z","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":"af467188dcc4996ba970b3a575b2968352ee6e845aa58eaab9cace2d96abdbb8","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-02-11T12:13:38Z","title_canon_sha256":"a1e73437f5423b77dda7e05a15ac5653164559f1debb0bda419507e7cdb20997"},"schema_version":"1.0","source":{"id":"2202.05574","kind":"arxiv","version":2}},"canonical_sha256":"cee0ad9f38bff6d1cf184aa59ec0b9cd1e4881f48934fa1e45d4202a03774749","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cee0ad9f38bff6d1cf184aa59ec0b9cd1e4881f48934fa1e45d4202a03774749","first_computed_at":"2026-07-05T04:35:43.715666Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:35:43.715666Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kulfg0Ckg1n9G/6thV10nSRHgqxWyToxW/UGzL6FXGE+FJ8gU/Oawtm2VUTRYEoIShrygNsc5v9rf8MBRUwPAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:35:43.716154Z","signed_message":"canonical_sha256_bytes"},"source_id":"2202.05574","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:eec407c7d5a5077c97e2790bd19ac850f032b7862a9769d911bf10f8d52f3e99","sha256:cacc8da88b7f56f58eb28455905a657d1ea33ba13ae9448e2797a2b285f25972"],"state_sha256":"52c2fae765dad7678c3a4cda4eaf645849b994ba30996f1c09ed847ba919163f"}