{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:KTKXXGSZ4UAMXF3LD4V2ZONEMP","short_pith_number":"pith:KTKXXGSZ","canonical_record":{"source":{"id":"hep-lat/0106019","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2001-06-26T09:48:02Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"18b9448655682d935a992a76b82835f269ec498a606bd2fbddb0e970e32b4bc2","abstract_canon_sha256":"cf725996be530eb8ec7bfe82b43a97e6547d9d4dc446f4d72c6962159116be7c"},"schema_version":"1.0"},"canonical_sha256":"54d57b9a59e500cb976b1f2bacb9a463c50d4163b4ead227d7232a8165ee4176","source":{"kind":"arxiv","id":"hep-lat/0106019","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0106019","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0106019v2","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0106019","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"pith_short_12","alias_value":"KTKXXGSZ4UAM","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"pith_short_16","alias_value":"KTKXXGSZ4UAMXF3L","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"pith_short_8","alias_value":"KTKXXGSZ","created_at":"2026-07-04T14:27:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:KTKXXGSZ4UAMXF3LD4V2ZONEMP","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0106019","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2001-06-26T09:48:02Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"18b9448655682d935a992a76b82835f269ec498a606bd2fbddb0e970e32b4bc2","abstract_canon_sha256":"cf725996be530eb8ec7bfe82b43a97e6547d9d4dc446f4d72c6962159116be7c"},"schema_version":"1.0"},"canonical_sha256":"54d57b9a59e500cb976b1f2bacb9a463c50d4163b4ead227d7232a8165ee4176","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:27:07.800136Z","signature_b64":"/YmRpI/6Ox1lmKjcpLAxsAEPTjJxMiBqeWDs1PN1X9v8+46bRzPtenYs/4BK2fBfp+LXBxkacQ0zBM3m2n4xDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"54d57b9a59e500cb976b1f2bacb9a463c50d4163b4ead227d7232a8165ee4176","last_reissued_at":"2026-07-04T14:27:07.799733Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:27:07.799733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0106019","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T14:27:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GHddIyPjhdrlRF1poHZ8RtTZbpxkTFqni1aiuFpe0Lk4qRjAWWbcJnsuUha79mssJyioOln62B24P+ktTAHjDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-02T18:03:35.724650Z"},"content_sha256":"d982bf06b688906f59d96ce66890028ab7e6942a90853955487229c0386bab94","schema_version":"1.0","event_id":"sha256:d982bf06b688906f59d96ce66890028ab7e6942a90853955487229c0386bab94"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:KTKXXGSZ4UAMXF3LD4V2ZONEMP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lattice QCD at High Temperature and Density","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Frithjof Karsch","submitted_at":"2001-06-26T09:48:02Z","abstract_excerpt":"After a brief introduction into basic aspects of the formulation of lattice regularized QCD at finite temperature and density we discuss our current understanding of the QCD phase diagram at finite temperature. We present results from lattice calculations that emphasize the deconfining as well as chiral symmetry restoring features of the QCD transition, and discuss the thermodynamics of the high temperature phase."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0106019","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/0106019/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T14:27:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sT/8o+zmNjW0IZGQRt9T3Jr1Oz/dqnorqQMkp6UGG+iL7QrBPErzYApQoB0j0MWqyAU3TTwj8FqgtCUB6iT6Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-02T18:03:35.725138Z"},"content_sha256":"eda28fef40657206f155f0027ddf489a6b24d73651c9b499877a38ba954056df","schema_version":"1.0","event_id":"sha256:eda28fef40657206f155f0027ddf489a6b24d73651c9b499877a38ba954056df"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KTKXXGSZ4UAMXF3LD4V2ZONEMP/bundle.json","state_url":"https://pith.science/pith/KTKXXGSZ4UAMXF3LD4V2ZONEMP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KTKXXGSZ4UAMXF3LD4V2ZONEMP/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":"2026-08-02T18:03:35Z","links":{"resolver":"https://pith.science/pith/KTKXXGSZ4UAMXF3LD4V2ZONEMP","bundle":"https://pith.science/pith/KTKXXGSZ4UAMXF3LD4V2ZONEMP/bundle.json","state":"https://pith.science/pith/KTKXXGSZ4UAMXF3LD4V2ZONEMP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KTKXXGSZ4UAMXF3LD4V2ZONEMP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:KTKXXGSZ4UAMXF3LD4V2ZONEMP","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":"cf725996be530eb8ec7bfe82b43a97e6547d9d4dc446f4d72c6962159116be7c","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2001-06-26T09:48:02Z","title_canon_sha256":"18b9448655682d935a992a76b82835f269ec498a606bd2fbddb0e970e32b4bc2"},"schema_version":"1.0","source":{"id":"hep-lat/0106019","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0106019","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0106019v2","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0106019","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"pith_short_12","alias_value":"KTKXXGSZ4UAM","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"pith_short_16","alias_value":"KTKXXGSZ4UAMXF3L","created_at":"2026-07-04T14:27:07Z"},{"alias_kind":"pith_short_8","alias_value":"KTKXXGSZ","created_at":"2026-07-04T14:27:07Z"}],"graph_snapshots":[{"event_id":"sha256:eda28fef40657206f155f0027ddf489a6b24d73651c9b499877a38ba954056df","target":"graph","created_at":"2026-07-04T14:27:07Z","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/0106019/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"After a brief introduction into basic aspects of the formulation of lattice regularized QCD at finite temperature and density we discuss our current understanding of the QCD phase diagram at finite temperature. We present results from lattice calculations that emphasize the deconfining as well as chiral symmetry restoring features of the QCD transition, and discuss the thermodynamics of the high temperature phase.","authors_text":"Frithjof Karsch","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2001-06-26T09:48:02Z","title":"Lattice QCD at High Temperature and Density"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0106019","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:d982bf06b688906f59d96ce66890028ab7e6942a90853955487229c0386bab94","target":"record","created_at":"2026-07-04T14:27:07Z","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":"cf725996be530eb8ec7bfe82b43a97e6547d9d4dc446f4d72c6962159116be7c","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2001-06-26T09:48:02Z","title_canon_sha256":"18b9448655682d935a992a76b82835f269ec498a606bd2fbddb0e970e32b4bc2"},"schema_version":"1.0","source":{"id":"hep-lat/0106019","kind":"arxiv","version":2}},"canonical_sha256":"54d57b9a59e500cb976b1f2bacb9a463c50d4163b4ead227d7232a8165ee4176","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"54d57b9a59e500cb976b1f2bacb9a463c50d4163b4ead227d7232a8165ee4176","first_computed_at":"2026-07-04T14:27:07.799733Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:27:07.799733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/YmRpI/6Ox1lmKjcpLAxsAEPTjJxMiBqeWDs1PN1X9v8+46bRzPtenYs/4BK2fBfp+LXBxkacQ0zBM3m2n4xDw==","signature_status":"signed_v1","signed_at":"2026-07-04T14:27:07.800136Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0106019","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d982bf06b688906f59d96ce66890028ab7e6942a90853955487229c0386bab94","sha256:eda28fef40657206f155f0027ddf489a6b24d73651c9b499877a38ba954056df"],"state_sha256":"4c8a9b0e8987b800bbae5a57b659547367888c5dcd1076594c9a6ea55c6fe535"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"M6Z09A+HucZuQw/p+QU9mUHiabAS/HBJ3vfYgdwG461oBAxyLQeBZgF1gvvzElPIhcyA6Su6PwZ8KwIh0MM4Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-02T18:03:35.729230Z","bundle_sha256":"699e5b202124e4634349c4f50a7534afd5454a89cc3c74ceac476d8afefd8feb"}}