{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:EYHGLJRLZSGV4PMCPXI2JMNS7S","short_pith_number":"pith:EYHGLJRL","canonical_record":{"source":{"id":"hep-ph/9409245","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-07T13:39:57Z","cross_cats_sorted":[],"title_canon_sha256":"0ca69b4e5572d8f40fd999b2ad9a0f0798385914b4262cc230f77b8a0d50094f","abstract_canon_sha256":"69375d24208d953cb2d87ea2aee9b23cb5abb014d04307133b41c920d704d3a8"},"schema_version":"1.0"},"canonical_sha256":"260e65a62bcc8d5e3d827dd1a4b1b2fc9238813d776d62d11c6ee96e89b9b2a2","source":{"kind":"arxiv","id":"hep-ph/9409245","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9409245","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9409245v1","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9409245","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"pith_short_12","alias_value":"EYHGLJRLZSGV","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"pith_short_16","alias_value":"EYHGLJRLZSGV4PMC","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"pith_short_8","alias_value":"EYHGLJRL","created_at":"2026-07-04T15:57:35Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:EYHGLJRLZSGV4PMCPXI2JMNS7S","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9409245","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-07T13:39:57Z","cross_cats_sorted":[],"title_canon_sha256":"0ca69b4e5572d8f40fd999b2ad9a0f0798385914b4262cc230f77b8a0d50094f","abstract_canon_sha256":"69375d24208d953cb2d87ea2aee9b23cb5abb014d04307133b41c920d704d3a8"},"schema_version":"1.0"},"canonical_sha256":"260e65a62bcc8d5e3d827dd1a4b1b2fc9238813d776d62d11c6ee96e89b9b2a2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:57:35.098904Z","signature_b64":"JRHl0eHr5ZRIYhOXOyRKdApC4Z0iV8PzmNClNcyJld/lNzJhyHBjdWpoMcX0XOskwCYlOyGRf0L6EKO1eozqAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"260e65a62bcc8d5e3d827dd1a4b1b2fc9238813d776d62d11c6ee96e89b9b2a2","last_reissued_at":"2026-07-04T15:57:35.098539Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:57:35.098539Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9409245","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":"2026-07-04T15:57:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J6ch5vGYS6Z1g8wx05yCNv8aM/qwhTy+5iDJjsTA/lf59RXeApNIgH7pyE/aiah36mFln0Aic3qt+2LuPv75AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T01:14:08.400714Z"},"content_sha256":"6e71cc0b8a14dc08474dc61e742ead19b98e292dc9352110d621073f2e8f80e0","schema_version":"1.0","event_id":"sha256:6e71cc0b8a14dc08474dc61e742ead19b98e292dc9352110d621073f2e8f80e0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:EYHGLJRLZSGV4PMCPXI2JMNS7S","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Operator product expansion and duality at finite temperature","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C.A.Dominguez","submitted_at":"1994-09-07T13:39:57Z","abstract_excerpt":"The operator product expansion of current correlators at short distances, and the notion of QCD-hadron duality are the cornerstone of QCD sum rules. The extension of this programme to $T \\neq 0$ is discussed, together with applications to hot hadronic propagators. Indications are that the hadronic spectrum suffers a substantial rearrangement with increasing temperature, and hint on the existence of a quark deconfining phase transition. Phenomenological order parameters to characterize this phase transition are discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9409245","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9409245/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":"2026-07-04T15:57:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QudEoAw2a6fXvvIQUKvo+8epU64+/LZBDKukbz33A+PSL5Ip17iJQ7lJP8KVXMRL5YKQdHb62KmqqC+KJyVmDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T01:14:08.401559Z"},"content_sha256":"50166bb8451c9da1361f4ae7f58b2bd21e3ed91092f677ad4aaea08f12448143","schema_version":"1.0","event_id":"sha256:50166bb8451c9da1361f4ae7f58b2bd21e3ed91092f677ad4aaea08f12448143"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EYHGLJRLZSGV4PMCPXI2JMNS7S/bundle.json","state_url":"https://pith.science/pith/EYHGLJRLZSGV4PMCPXI2JMNS7S/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EYHGLJRLZSGV4PMCPXI2JMNS7S/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":"2026-08-05T01:14:08Z","links":{"resolver":"https://pith.science/pith/EYHGLJRLZSGV4PMCPXI2JMNS7S","bundle":"https://pith.science/pith/EYHGLJRLZSGV4PMCPXI2JMNS7S/bundle.json","state":"https://pith.science/pith/EYHGLJRLZSGV4PMCPXI2JMNS7S/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EYHGLJRLZSGV4PMCPXI2JMNS7S/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:EYHGLJRLZSGV4PMCPXI2JMNS7S","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":"69375d24208d953cb2d87ea2aee9b23cb5abb014d04307133b41c920d704d3a8","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-07T13:39:57Z","title_canon_sha256":"0ca69b4e5572d8f40fd999b2ad9a0f0798385914b4262cc230f77b8a0d50094f"},"schema_version":"1.0","source":{"id":"hep-ph/9409245","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9409245","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9409245v1","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9409245","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"pith_short_12","alias_value":"EYHGLJRLZSGV","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"pith_short_16","alias_value":"EYHGLJRLZSGV4PMC","created_at":"2026-07-04T15:57:35Z"},{"alias_kind":"pith_short_8","alias_value":"EYHGLJRL","created_at":"2026-07-04T15:57:35Z"}],"graph_snapshots":[{"event_id":"sha256:50166bb8451c9da1361f4ae7f58b2bd21e3ed91092f677ad4aaea08f12448143","target":"graph","created_at":"2026-07-04T15:57:35Z","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-ph/9409245/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The operator product expansion of current correlators at short distances, and the notion of QCD-hadron duality are the cornerstone of QCD sum rules. The extension of this programme to $T \\neq 0$ is discussed, together with applications to hot hadronic propagators. Indications are that the hadronic spectrum suffers a substantial rearrangement with increasing temperature, and hint on the existence of a quark deconfining phase transition. Phenomenological order parameters to characterize this phase transition are discussed.","authors_text":"C.A.Dominguez","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1994-09-07T13:39:57Z","title":"Operator product expansion and duality at finite temperature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9409245","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":"sha256:6e71cc0b8a14dc08474dc61e742ead19b98e292dc9352110d621073f2e8f80e0","target":"record","created_at":"2026-07-04T15:57:35Z","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":"69375d24208d953cb2d87ea2aee9b23cb5abb014d04307133b41c920d704d3a8","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-07T13:39:57Z","title_canon_sha256":"0ca69b4e5572d8f40fd999b2ad9a0f0798385914b4262cc230f77b8a0d50094f"},"schema_version":"1.0","source":{"id":"hep-ph/9409245","kind":"arxiv","version":1}},"canonical_sha256":"260e65a62bcc8d5e3d827dd1a4b1b2fc9238813d776d62d11c6ee96e89b9b2a2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"260e65a62bcc8d5e3d827dd1a4b1b2fc9238813d776d62d11c6ee96e89b9b2a2","first_computed_at":"2026-07-04T15:57:35.098539Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:57:35.098539Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"JRHl0eHr5ZRIYhOXOyRKdApC4Z0iV8PzmNClNcyJld/lNzJhyHBjdWpoMcX0XOskwCYlOyGRf0L6EKO1eozqAA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:57:35.098904Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9409245","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6e71cc0b8a14dc08474dc61e742ead19b98e292dc9352110d621073f2e8f80e0","sha256:50166bb8451c9da1361f4ae7f58b2bd21e3ed91092f677ad4aaea08f12448143"],"state_sha256":"a349225c80941403ffb3518f51b433734b1a4b30f1ff78a8be0514a95839fd2d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k/+nMz4Z231hgTNrpUL8VcdwQaBSjMtxvg+vi8NTQQo+eWslGmUe/S6KNJLQw2fsgOotzLfWgjijHo/V1439Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T01:14:08.414397Z","bundle_sha256":"3a1b92002c2611778e05cde03334ab4312170e828f0364bd93c83d96595f89da"}}