{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:ETNSYVTBB5N3KUDLBT3ULG5GFR","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":"7da48a395c67c347c194828c44099862edf0a5b21739c826f508a35279947aa8","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"1996-05-24T01:57:55Z","title_canon_sha256":"0dab33354be81105abd99993764c0b55d3d27a516403cc48b3602c570a6b269a"},"schema_version":"1.0","source":{"id":"hep-lat/9605030","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9605030","created_at":"2026-07-04T16:01:21Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9605030v1","created_at":"2026-07-04T16:01:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9605030","created_at":"2026-07-04T16:01:21Z"},{"alias_kind":"pith_short_12","alias_value":"ETNSYVTBB5N3","created_at":"2026-07-04T16:01:21Z"},{"alias_kind":"pith_short_16","alias_value":"ETNSYVTBB5N3KUDL","created_at":"2026-07-04T16:01:21Z"},{"alias_kind":"pith_short_8","alias_value":"ETNSYVTB","created_at":"2026-07-04T16:01:21Z"}],"graph_snapshots":[{"event_id":"sha256:c64faa8a565d82461540a69245b196621cffa12a75ee4ff50dc2bd179c176ef6","target":"graph","created_at":"2026-07-04T16:01:21Z","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/hep-lat/9605030/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The nature of finite temperature transitions in lattice QCD with Wilson quarks is studied near the chiral limit for the cases of 2, 3, and 6 flavors of degenerate quarks ($N_F=2$, 3, and 6) and also for the case of massless up and down quarks and a light strange quark ($N_F=2+1$). Our simulations mainly performed on lattices with the temporal direction extension $N_t=4$ indicate that the finite temperature transition in the chiral limit (chiral transition) is continuous for $N_F=2$, while it is of first order for $N_F=3$ and 6. We find that the transition is of first order for the case of mass","authors_text":"K. Kanaya, S. Kaya, S. Sakai, T. Yoshi\\'e, Y. Iwasaki","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"1996-05-24T01:57:55Z","title":"Finite Temperature Transitions in Lattice QCD with Wilson Quarks --- Chiral Transitions and the Influence of the Strange Quark ---"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9605030","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":"sha256:92f0fcff4f8e4ac2b31df36301b50c1c865a3e3b1964801f08294d09b48db748","target":"record","created_at":"2026-07-04T16:01:21Z","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":"7da48a395c67c347c194828c44099862edf0a5b21739c826f508a35279947aa8","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"1996-05-24T01:57:55Z","title_canon_sha256":"0dab33354be81105abd99993764c0b55d3d27a516403cc48b3602c570a6b269a"},"schema_version":"1.0","source":{"id":"hep-lat/9605030","kind":"arxiv","version":1}},"canonical_sha256":"24db2c56610f5bb5506b0cf7459ba62c79e098959a1bd6bec2add45dfdbe73bc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"24db2c56610f5bb5506b0cf7459ba62c79e098959a1bd6bec2add45dfdbe73bc","first_computed_at":"2026-07-04T16:01:21.916458Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:01:21.916458Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m5XNR5FITtibZSvUgrjrcGby4AfxGWcrAfVnQfwPod9DXyPcMFYyWyJa0zl0xLCCz51z14MHXz6dl0yChhAyDw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:01:21.916824Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/9605030","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:92f0fcff4f8e4ac2b31df36301b50c1c865a3e3b1964801f08294d09b48db748","sha256:c64faa8a565d82461540a69245b196621cffa12a75ee4ff50dc2bd179c176ef6"],"state_sha256":"6cde57559a49ee878344f0b28f777c9d9f56b329a5ecd3b1a2c9abce67ca4284"}