{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:NX6GQ2WODOMZUQTVT5EDOGXSEE","short_pith_number":"pith:NX6GQ2WO","canonical_record":{"source":{"id":"1011.4230","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-11-18T17:05:18Z","cross_cats_sorted":[],"title_canon_sha256":"4111a5a32a99428b9dfe62cec1e6d58962cf7e2d40f790f64ad1c2c93d9e2c80","abstract_canon_sha256":"f51e0c0c6abcd25865196bd55bc1d2b81718cf68a248057ffdac8430f90ec555"},"schema_version":"1.0"},"canonical_sha256":"6dfc686ace1b999a42759f48371af22113e14d434ff9c0f556118cb79bd8b175","source":{"kind":"arxiv","id":"1011.4230","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.4230","created_at":"2026-05-18T04:35:36Z"},{"alias_kind":"arxiv_version","alias_value":"1011.4230v1","created_at":"2026-05-18T04:35:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.4230","created_at":"2026-05-18T04:35:36Z"},{"alias_kind":"pith_short_12","alias_value":"NX6GQ2WODOMZ","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_16","alias_value":"NX6GQ2WODOMZUQTV","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_8","alias_value":"NX6GQ2WO","created_at":"2026-05-18T12:26:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:NX6GQ2WODOMZUQTVT5EDOGXSEE","target":"record","payload":{"canonical_record":{"source":{"id":"1011.4230","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-11-18T17:05:18Z","cross_cats_sorted":[],"title_canon_sha256":"4111a5a32a99428b9dfe62cec1e6d58962cf7e2d40f790f64ad1c2c93d9e2c80","abstract_canon_sha256":"f51e0c0c6abcd25865196bd55bc1d2b81718cf68a248057ffdac8430f90ec555"},"schema_version":"1.0"},"canonical_sha256":"6dfc686ace1b999a42759f48371af22113e14d434ff9c0f556118cb79bd8b175","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:35:36.249264Z","signature_b64":"JgDLlyolW2AjgGtR/wNsTRQFB4q6CpEkoABmKaJjXkxRnNUfPOf2Uyw3QFdgbVIaUYTZn+EYaYwaP/+EL6IxCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6dfc686ace1b999a42759f48371af22113e14d434ff9c0f556118cb79bd8b175","last_reissued_at":"2026-05-18T04:35:36.248647Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:35:36.248647Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1011.4230","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:35:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XCyvndyPYr2nWNiuf/bIkBLvLBhcbuH76HgmNAFHMaq4bs6gdXS7WPi9UY55KnVTYKlnejQahDGTXky8IQnRCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T03:50:45.400915Z"},"content_sha256":"177509d6c7ac0067e64154008abda5832c12c7fde8ecffe2fff8e444d91ccd85","schema_version":"1.0","event_id":"sha256:177509d6c7ac0067e64154008abda5832c12c7fde8ecffe2fff8e444d91ccd85"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:NX6GQ2WODOMZUQTVT5EDOGXSEE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"QCD transition temperature: full staggered result","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Christian Hoelbling, Claudia Ratti, Kalman K.Szabo, Sandor D. Katz, Stefan Krieg, Szabolcs Borsanyi, Zoltan Fodor","submitted_at":"2010-11-18T17:05:18Z","abstract_excerpt":"We conclude our investigations on the QCD cross-over transition temperatures with 2+1 staggered flavours and one-link stout improvement. We extend our previous two studies [Phys. Lett. B643 (2006) 46, JHEP 0906:088 (2009)] by choosing even finer lattices (N_t=16) and we work again with physical quark masses. These new results [for details see JHEP 1009:073,2010] support our earlier findings. We compare them with the published results of the hotQCD collaboration. All these results are confronted with the predictions of the Hadron Resonance Gas model and Chiral Perturbation Theory for temperatur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.4230","kind":"arxiv","version":1},"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":"2026-05-18T04:35:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DTyd+LEbq3jpdfPeWqBpq7CBL6ZmYGuzdEsSnuI+JXO98+NPI7IuNOOqEFwh2laRgXw+bXxCLs6/s42DzAtoBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T03:50:45.401257Z"},"content_sha256":"427e2b2352a8bf4c7236c8bc5f9e69712c3bc52bc7ecc6c0b94bf8ed1acb84b9","schema_version":"1.0","event_id":"sha256:427e2b2352a8bf4c7236c8bc5f9e69712c3bc52bc7ecc6c0b94bf8ed1acb84b9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NX6GQ2WODOMZUQTVT5EDOGXSEE/bundle.json","state_url":"https://pith.science/pith/NX6GQ2WODOMZUQTVT5EDOGXSEE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NX6GQ2WODOMZUQTVT5EDOGXSEE/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":"2026-06-01T03:50:45Z","links":{"resolver":"https://pith.science/pith/NX6GQ2WODOMZUQTVT5EDOGXSEE","bundle":"https://pith.science/pith/NX6GQ2WODOMZUQTVT5EDOGXSEE/bundle.json","state":"https://pith.science/pith/NX6GQ2WODOMZUQTVT5EDOGXSEE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NX6GQ2WODOMZUQTVT5EDOGXSEE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:NX6GQ2WODOMZUQTVT5EDOGXSEE","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":"f51e0c0c6abcd25865196bd55bc1d2b81718cf68a248057ffdac8430f90ec555","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-11-18T17:05:18Z","title_canon_sha256":"4111a5a32a99428b9dfe62cec1e6d58962cf7e2d40f790f64ad1c2c93d9e2c80"},"schema_version":"1.0","source":{"id":"1011.4230","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.4230","created_at":"2026-05-18T04:35:36Z"},{"alias_kind":"arxiv_version","alias_value":"1011.4230v1","created_at":"2026-05-18T04:35:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.4230","created_at":"2026-05-18T04:35:36Z"},{"alias_kind":"pith_short_12","alias_value":"NX6GQ2WODOMZ","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_16","alias_value":"NX6GQ2WODOMZUQTV","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_8","alias_value":"NX6GQ2WO","created_at":"2026-05-18T12:26:10Z"}],"graph_snapshots":[{"event_id":"sha256:427e2b2352a8bf4c7236c8bc5f9e69712c3bc52bc7ecc6c0b94bf8ed1acb84b9","target":"graph","created_at":"2026-05-18T04:35:36Z","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 conclude our investigations on the QCD cross-over transition temperatures with 2+1 staggered flavours and one-link stout improvement. We extend our previous two studies [Phys. Lett. B643 (2006) 46, JHEP 0906:088 (2009)] by choosing even finer lattices (N_t=16) and we work again with physical quark masses. These new results [for details see JHEP 1009:073,2010] support our earlier findings. We compare them with the published results of the hotQCD collaboration. All these results are confronted with the predictions of the Hadron Resonance Gas model and Chiral Perturbation Theory for temperatur","authors_text":"Christian Hoelbling, Claudia Ratti, Kalman K.Szabo, Sandor D. Katz, Stefan Krieg, Szabolcs Borsanyi, Zoltan Fodor","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-11-18T17:05:18Z","title":"QCD transition temperature: full staggered result"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.4230","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":"sha256:177509d6c7ac0067e64154008abda5832c12c7fde8ecffe2fff8e444d91ccd85","target":"record","created_at":"2026-05-18T04:35:36Z","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":"f51e0c0c6abcd25865196bd55bc1d2b81718cf68a248057ffdac8430f90ec555","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-11-18T17:05:18Z","title_canon_sha256":"4111a5a32a99428b9dfe62cec1e6d58962cf7e2d40f790f64ad1c2c93d9e2c80"},"schema_version":"1.0","source":{"id":"1011.4230","kind":"arxiv","version":1}},"canonical_sha256":"6dfc686ace1b999a42759f48371af22113e14d434ff9c0f556118cb79bd8b175","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6dfc686ace1b999a42759f48371af22113e14d434ff9c0f556118cb79bd8b175","first_computed_at":"2026-05-18T04:35:36.248647Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:35:36.248647Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"JgDLlyolW2AjgGtR/wNsTRQFB4q6CpEkoABmKaJjXkxRnNUfPOf2Uyw3QFdgbVIaUYTZn+EYaYwaP/+EL6IxCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:35:36.249264Z","signed_message":"canonical_sha256_bytes"},"source_id":"1011.4230","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:177509d6c7ac0067e64154008abda5832c12c7fde8ecffe2fff8e444d91ccd85","sha256:427e2b2352a8bf4c7236c8bc5f9e69712c3bc52bc7ecc6c0b94bf8ed1acb84b9"],"state_sha256":"f243e4b584d10a681446cd49fb17309b8c09ebe3dc8e58aa3000a3423d146d51"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EtogG4md9yB/Wdiu2HNKVfgFgMp8fHTGa9z+k96UYF6geJNR3UHNALv+GRz6YKkxIVjThG83eDX5DaZTQORlBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T03:50:45.403173Z","bundle_sha256":"9299ab8bcd709a90f0c2c122d51a420c86e6160c90da3e32bdd567964028130b"}}