{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:2YKNDXMBU5MFMLKIDMKYPKM3OT","short_pith_number":"pith:2YKNDXMB","canonical_record":{"source":{"id":"hep-lat/0207002","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2002-07-04T16:01:38Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"fe258d9d2a2d0937b7b3dc7a219b30422bd5965f07704e2abccbd7ff1f52d5f0","abstract_canon_sha256":"cd1f6a79f1bfd72f3fbac0cc2b4bea1f97db552802a6841540e1ab9d9639b77f"},"schema_version":"1.0"},"canonical_sha256":"d614d1dd81a758562d481b1587a99b74ff65bc76be71fcd72ac1c38aea1b05f8","source":{"kind":"arxiv","id":"hep-lat/0207002","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0207002","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0207002v2","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0207002","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"pith_short_12","alias_value":"2YKNDXMBU5MF","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"pith_short_16","alias_value":"2YKNDXMBU5MFMLKI","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"pith_short_8","alias_value":"2YKNDXMB","created_at":"2026-07-04T15:18:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:2YKNDXMBU5MFMLKIDMKYPKM3OT","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0207002","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2002-07-04T16:01:38Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"fe258d9d2a2d0937b7b3dc7a219b30422bd5965f07704e2abccbd7ff1f52d5f0","abstract_canon_sha256":"cd1f6a79f1bfd72f3fbac0cc2b4bea1f97db552802a6841540e1ab9d9639b77f"},"schema_version":"1.0"},"canonical_sha256":"d614d1dd81a758562d481b1587a99b74ff65bc76be71fcd72ac1c38aea1b05f8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:18:15.585406Z","signature_b64":"AfL46X8tgCKtHYOYZrMgGeXiMzw0midWB85sNTtLYfr5XAJAH/uRqhDJ1oTt4pm0hljGbnrEo2yUoxJbs49fCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d614d1dd81a758562d481b1587a99b74ff65bc76be71fcd72ac1c38aea1b05f8","last_reissued_at":"2026-07-04T15:18:15.584987Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:18:15.584987Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0207002","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":"2026-07-04T15:18:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KuLwypbbXwNRUMjgxS5ShTvurbenwZbXIwccbSD/H0gL/Wqhq3Nn2qNO2/Sh6wVth5WcxK/cnGMs6SIaU+yKBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T20:31:18.431245Z"},"content_sha256":"8265eb3972f5adc08a2d712f26ac6b856433cd29efb08f6adf80116964c8927f","schema_version":"1.0","event_id":"sha256:8265eb3972f5adc08a2d712f26ac6b856433cd29efb08f6adf80116964c8927f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:2YKNDXMBU5MFMLKIDMKYPKM3OT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Heavy Quark Anti-Quark Free Energy and the Renormalized Polyakov Loop","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"F. Karsch, F. Zantow, O. Kaczmarek, P. Petreczky","submitted_at":"2002-07-04T16:01:38Z","abstract_excerpt":"We calculate the colour averaged and colour singlet free energies of static quark anti-quark sources placed in a thermal gluonic heat bath. We discuss the renormalization of these free energies using the short distance properties of the zero temperature heavy quark potential. This leads to the definition of the renormalized Polyakov loop as an order parameter for the deconfinement phase transition of the SU(3) gauge theory which is well behaved in the continuum limit."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0207002","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/0207002/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":"2026-07-04T15:18:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VLnRh8p35AhiC8omaDCVpk5OoxOzxRP6+CoYcjvgVnZj/k4lm+EclvS03Mu8ywbMmILk+iZhgkq8DnspQV5KAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T20:31:18.433986Z"},"content_sha256":"5ecfaf89e876b3552a350c6f758e4a73ea38cf83a9be10fd292e6922f3b1381e","schema_version":"1.0","event_id":"sha256:5ecfaf89e876b3552a350c6f758e4a73ea38cf83a9be10fd292e6922f3b1381e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2YKNDXMBU5MFMLKIDMKYPKM3OT/bundle.json","state_url":"https://pith.science/pith/2YKNDXMBU5MFMLKIDMKYPKM3OT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2YKNDXMBU5MFMLKIDMKYPKM3OT/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":"2026-08-16T20:31:18Z","links":{"resolver":"https://pith.science/pith/2YKNDXMBU5MFMLKIDMKYPKM3OT","bundle":"https://pith.science/pith/2YKNDXMBU5MFMLKIDMKYPKM3OT/bundle.json","state":"https://pith.science/pith/2YKNDXMBU5MFMLKIDMKYPKM3OT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2YKNDXMBU5MFMLKIDMKYPKM3OT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:2YKNDXMBU5MFMLKIDMKYPKM3OT","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":"cd1f6a79f1bfd72f3fbac0cc2b4bea1f97db552802a6841540e1ab9d9639b77f","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"2002-07-04T16:01:38Z","title_canon_sha256":"fe258d9d2a2d0937b7b3dc7a219b30422bd5965f07704e2abccbd7ff1f52d5f0"},"schema_version":"1.0","source":{"id":"hep-lat/0207002","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0207002","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0207002v2","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0207002","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"pith_short_12","alias_value":"2YKNDXMBU5MF","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"pith_short_16","alias_value":"2YKNDXMBU5MFMLKI","created_at":"2026-07-04T15:18:15Z"},{"alias_kind":"pith_short_8","alias_value":"2YKNDXMB","created_at":"2026-07-04T15:18:15Z"}],"graph_snapshots":[{"event_id":"sha256:5ecfaf89e876b3552a350c6f758e4a73ea38cf83a9be10fd292e6922f3b1381e","target":"graph","created_at":"2026-07-04T15:18:15Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-lat/0207002/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate the colour averaged and colour singlet free energies of static quark anti-quark sources placed in a thermal gluonic heat bath. We discuss the renormalization of these free energies using the short distance properties of the zero temperature heavy quark potential. This leads to the definition of the renormalized Polyakov loop as an order parameter for the deconfinement phase transition of the SU(3) gauge theory which is well behaved in the continuum limit.","authors_text":"F. Karsch, F. Zantow, O. Kaczmarek, P. Petreczky","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2002-07-04T16:01:38Z","title":"Heavy Quark Anti-Quark Free Energy and the Renormalized Polyakov Loop"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0207002","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":"sha256:8265eb3972f5adc08a2d712f26ac6b856433cd29efb08f6adf80116964c8927f","target":"record","created_at":"2026-07-04T15:18:15Z","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":"cd1f6a79f1bfd72f3fbac0cc2b4bea1f97db552802a6841540e1ab9d9639b77f","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"2002-07-04T16:01:38Z","title_canon_sha256":"fe258d9d2a2d0937b7b3dc7a219b30422bd5965f07704e2abccbd7ff1f52d5f0"},"schema_version":"1.0","source":{"id":"hep-lat/0207002","kind":"arxiv","version":2}},"canonical_sha256":"d614d1dd81a758562d481b1587a99b74ff65bc76be71fcd72ac1c38aea1b05f8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d614d1dd81a758562d481b1587a99b74ff65bc76be71fcd72ac1c38aea1b05f8","first_computed_at":"2026-07-04T15:18:15.584987Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:18:15.584987Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AfL46X8tgCKtHYOYZrMgGeXiMzw0midWB85sNTtLYfr5XAJAH/uRqhDJ1oTt4pm0hljGbnrEo2yUoxJbs49fCQ==","signature_status":"signed_v1","signed_at":"2026-07-04T15:18:15.585406Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0207002","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8265eb3972f5adc08a2d712f26ac6b856433cd29efb08f6adf80116964c8927f","sha256:5ecfaf89e876b3552a350c6f758e4a73ea38cf83a9be10fd292e6922f3b1381e"],"state_sha256":"bdfcb25e381a5132116a7138a4523d56a0a2f532b50c8242545f58eb7ce9f2e8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ntrv0HuT4ZRaXjREkCbFSfygCqaDkMiYo0/Escby0M3SbPNGNg94u3d+1w4SQCxfzd5IYt1igSktw5ME7J+qDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T20:31:18.458278Z","bundle_sha256":"ec3e8f57f755399b1f7673778a92e4859bbcd14c253fd5b90f029a240d941569"}}