{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:6S2DG3TWQURCERVSPQU5XEEDEE","short_pith_number":"pith:6S2DG3TW","canonical_record":{"source":{"id":"1301.3943","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-01-16T22:57:08Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"424c295b3afc8ed946013fa1fbdb953d1019bda7051830d4b4da8cd115e60446","abstract_canon_sha256":"6da294a61cfd84e3793cf2b328d9bd94c258666446e5c03ea67ef1482927759a"},"schema_version":"1.0"},"canonical_sha256":"f4b4336e7685222246b27c29db9083211c35fa125be0d0eb97a6b7cd744f3c36","source":{"kind":"arxiv","id":"1301.3943","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.3943","created_at":"2026-05-18T03:25:15Z"},{"alias_kind":"arxiv_version","alias_value":"1301.3943v3","created_at":"2026-05-18T03:25:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.3943","created_at":"2026-05-18T03:25:15Z"},{"alias_kind":"pith_short_12","alias_value":"6S2DG3TWQURC","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"6S2DG3TWQURCERVS","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"6S2DG3TW","created_at":"2026-05-18T12:27:36Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:6S2DG3TWQURCERVSPQU5XEEDEE","target":"record","payload":{"canonical_record":{"source":{"id":"1301.3943","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-01-16T22:57:08Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"424c295b3afc8ed946013fa1fbdb953d1019bda7051830d4b4da8cd115e60446","abstract_canon_sha256":"6da294a61cfd84e3793cf2b328d9bd94c258666446e5c03ea67ef1482927759a"},"schema_version":"1.0"},"canonical_sha256":"f4b4336e7685222246b27c29db9083211c35fa125be0d0eb97a6b7cd744f3c36","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:25:15.957424Z","signature_b64":"ShrRafiA5Yyqp5dk1kZ3BMcGc+3DbjvHBmJtO2Oz94lzaTAkzCe/HrJ9i43aclu5NcRNfn7Xu9M1VazOotZcAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f4b4336e7685222246b27c29db9083211c35fa125be0d0eb97a6b7cd744f3c36","last_reissued_at":"2026-05-18T03:25:15.956948Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:25:15.956948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1301.3943","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:25:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fpMAQmBPJxFoe+Cm7HTreXlMkkDXHdWv+pASBzGNLX13o7ui2g6P1b+gvat20dWjLvqNV3ngDAWpiXFTJOw2Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T14:13:03.706014Z"},"content_sha256":"8134697b5e157b686d60b93d9ceac2ce41e89946394aa152be8780ddd407d171","schema_version":"1.0","event_id":"sha256:8134697b5e157b686d60b93d9ceac2ce41e89946394aa152be8780ddd407d171"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:6S2DG3TWQURCERVSPQU5XEEDEE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Polyakov loop in 2+1 flavor QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, P. Petreczky","submitted_at":"2013-01-16T22:57:08Z","abstract_excerpt":"We study the temperature dependence of the renormalized Polyakov loop in 2+1 flavor QCD for temperatures T<210 MeV. We extend previous calculations by the HotQCD collaboration using the highly improved staggered quark action and perform a continuum extrapolation of the renormalized Polyakov loop. We compare the lattice results with the prediction of non-interacting static-light hadron resonance gas, which describes the temperature dependence of the renormalized Polyakov loop up to T<140 MeV but fails above that temperature. Furthermore, we discuss the temperature dependence of the light and st"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.3943","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:25:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SgLiiHj78Z86nXYLh8nvOBlHpLk4Tg8NoWLBUyGbpZQ9tUTMMSvcYlKnyGGDWR565h7gwQqjZtff7ynRT3mGDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T14:13:03.706995Z"},"content_sha256":"6eef6653226fae9d3dfa1b14998119e82197d26a8a235763fc5df51379a81566","schema_version":"1.0","event_id":"sha256:6eef6653226fae9d3dfa1b14998119e82197d26a8a235763fc5df51379a81566"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6S2DG3TWQURCERVSPQU5XEEDEE/bundle.json","state_url":"https://pith.science/pith/6S2DG3TWQURCERVSPQU5XEEDEE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6S2DG3TWQURCERVSPQU5XEEDEE/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-06T14:13:03Z","links":{"resolver":"https://pith.science/pith/6S2DG3TWQURCERVSPQU5XEEDEE","bundle":"https://pith.science/pith/6S2DG3TWQURCERVSPQU5XEEDEE/bundle.json","state":"https://pith.science/pith/6S2DG3TWQURCERVSPQU5XEEDEE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6S2DG3TWQURCERVSPQU5XEEDEE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:6S2DG3TWQURCERVSPQU5XEEDEE","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":"6da294a61cfd84e3793cf2b328d9bd94c258666446e5c03ea67ef1482927759a","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-01-16T22:57:08Z","title_canon_sha256":"424c295b3afc8ed946013fa1fbdb953d1019bda7051830d4b4da8cd115e60446"},"schema_version":"1.0","source":{"id":"1301.3943","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.3943","created_at":"2026-05-18T03:25:15Z"},{"alias_kind":"arxiv_version","alias_value":"1301.3943v3","created_at":"2026-05-18T03:25:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.3943","created_at":"2026-05-18T03:25:15Z"},{"alias_kind":"pith_short_12","alias_value":"6S2DG3TWQURC","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"6S2DG3TWQURCERVS","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"6S2DG3TW","created_at":"2026-05-18T12:27:36Z"}],"graph_snapshots":[{"event_id":"sha256:6eef6653226fae9d3dfa1b14998119e82197d26a8a235763fc5df51379a81566","target":"graph","created_at":"2026-05-18T03:25:15Z","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"},"paper":{"abstract_excerpt":"We study the temperature dependence of the renormalized Polyakov loop in 2+1 flavor QCD for temperatures T<210 MeV. We extend previous calculations by the HotQCD collaboration using the highly improved staggered quark action and perform a continuum extrapolation of the renormalized Polyakov loop. We compare the lattice results with the prediction of non-interacting static-light hadron resonance gas, which describes the temperature dependence of the renormalized Polyakov loop up to T<140 MeV but fails above that temperature. Furthermore, we discuss the temperature dependence of the light and st","authors_text":"A. Bazavov, P. Petreczky","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-01-16T22:57:08Z","title":"Polyakov loop in 2+1 flavor QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.3943","kind":"arxiv","version":3},"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":"sha256:8134697b5e157b686d60b93d9ceac2ce41e89946394aa152be8780ddd407d171","target":"record","created_at":"2026-05-18T03:25:15Z","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":"6da294a61cfd84e3793cf2b328d9bd94c258666446e5c03ea67ef1482927759a","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-01-16T22:57:08Z","title_canon_sha256":"424c295b3afc8ed946013fa1fbdb953d1019bda7051830d4b4da8cd115e60446"},"schema_version":"1.0","source":{"id":"1301.3943","kind":"arxiv","version":3}},"canonical_sha256":"f4b4336e7685222246b27c29db9083211c35fa125be0d0eb97a6b7cd744f3c36","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f4b4336e7685222246b27c29db9083211c35fa125be0d0eb97a6b7cd744f3c36","first_computed_at":"2026-05-18T03:25:15.956948Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:25:15.956948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ShrRafiA5Yyqp5dk1kZ3BMcGc+3DbjvHBmJtO2Oz94lzaTAkzCe/HrJ9i43aclu5NcRNfn7Xu9M1VazOotZcAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:25:15.957424Z","signed_message":"canonical_sha256_bytes"},"source_id":"1301.3943","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8134697b5e157b686d60b93d9ceac2ce41e89946394aa152be8780ddd407d171","sha256:6eef6653226fae9d3dfa1b14998119e82197d26a8a235763fc5df51379a81566"],"state_sha256":"f1710707a6158fe778e7ed3de531b04ebfbfd7cf4e42407fb0c308fe819d0e2b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V/KfxpvANOJsok7aH6mqLbAc6rS/JCjwCa/o5bVc0cQmh3z9oDu/CgJlP5rDdRoyVgr6Jxw68NgISdwf0pZBDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T14:13:03.710214Z","bundle_sha256":"fb305752432c54eb9eccda6607ece123b6e629a2b8d77318dced02c771b84d22"}}