{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2005:MBV6G6Y7MCLV7SLILXPGHEZ5GP","short_pith_number":"pith:MBV6G6Y7","canonical_record":{"source":{"id":"hep-ph/0512125","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-09T15:52:13Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"32ae126a70a9134857dd1f8ed9a1a301cfcf7ceacc12d6d1b933851bc7ec93c2","abstract_canon_sha256":"bcbd0cfe753fdfdd76f3d9ee96334eafc4d532cdf64f2b3554832e5d4f207520"},"schema_version":"1.0"},"canonical_sha256":"606be37b1f60975fc9685dde63933d33f80d6f5295b3bf855d41b072536dcc54","source":{"kind":"arxiv","id":"hep-ph/0512125","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0512125","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0512125v2","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0512125","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_12","alias_value":"MBV6G6Y7MCLV","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_16","alias_value":"MBV6G6Y7MCLV7SLI","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_8","alias_value":"MBV6G6Y7","created_at":"2026-07-04T15:19:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2005:MBV6G6Y7MCLV7SLILXPGHEZ5GP","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0512125","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-09T15:52:13Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"32ae126a70a9134857dd1f8ed9a1a301cfcf7ceacc12d6d1b933851bc7ec93c2","abstract_canon_sha256":"bcbd0cfe753fdfdd76f3d9ee96334eafc4d532cdf64f2b3554832e5d4f207520"},"schema_version":"1.0"},"canonical_sha256":"606be37b1f60975fc9685dde63933d33f80d6f5295b3bf855d41b072536dcc54","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:19:47.469793Z","signature_b64":"/PwV0mQfFTH+zTdVPE4yd6/MoYPbWhtkXf6BNEyFnSMxFZ+ufowGlbSPk8/41XabOqxomdkn33yQbA98ZODeBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"606be37b1f60975fc9685dde63933d33f80d6f5295b3bf855d41b072536dcc54","last_reissued_at":"2026-07-04T15:19:47.469405Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:19:47.469405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0512125","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":"2026-07-04T15:19:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Abg6epbq2YtUH5LBl6cVCL9uo9ep4lkTv8YcqjiKMdW8s8ruUZxpcUGXbQs7VJSrMljDRswma2LeTsufDozUBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T15:47:36.568367Z"},"content_sha256":"bdfcdb9cbe8c1814c18945b4557e568447286f1d8abcb6be70698837f6652133","schema_version":"1.0","event_id":"sha256:bdfcdb9cbe8c1814c18945b4557e568447286f1d8abcb6be70698837f6652133"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2005:MBV6G6Y7MCLV7SLILXPGHEZ5GP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamics of quark-gluon plasma from Field correlators","license":"","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Di Giacomo, A.I. Veselov, E. Meggiolaro, Yu.A. Simonov","submitted_at":"2005-12-09T15:52:13Z","abstract_excerpt":"It is argued that strong dynamics in the quark-gluon plasma and bound states of quarks and gluons is mostly due to nonperturbative effects described by field correlators. The emphasis in the paper is made on two explicit calculations of these effects from the first principles: one analytic using gluelump Green's functions and another using independent lattice data on correlators. The resulting hadron spectra are investigated in the range T_c < T < 2T_c. The spectra of charmonia, bottomonia, light s-sbar mesons, glueballs and quark-gluon states calculated numerically are in general agreement wi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0512125","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-ph/0512125/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":"2026-07-04T15:19:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"x0aujYXmG3tSg59ACrf0YxGM0Ud6HFYus+6LJFQ7pi+3PC0i2xCx61SVuOS+NmKO4/DJqNMmyM+qvt9F4TuCAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T15:47:36.568752Z"},"content_sha256":"29941f1ae1753402b23e970535a7782dd0242274f1da2535cf4667eee5afe716","schema_version":"1.0","event_id":"sha256:29941f1ae1753402b23e970535a7782dd0242274f1da2535cf4667eee5afe716"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MBV6G6Y7MCLV7SLILXPGHEZ5GP/bundle.json","state_url":"https://pith.science/pith/MBV6G6Y7MCLV7SLILXPGHEZ5GP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MBV6G6Y7MCLV7SLILXPGHEZ5GP/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":"2026-07-06T15:47:36Z","links":{"resolver":"https://pith.science/pith/MBV6G6Y7MCLV7SLILXPGHEZ5GP","bundle":"https://pith.science/pith/MBV6G6Y7MCLV7SLILXPGHEZ5GP/bundle.json","state":"https://pith.science/pith/MBV6G6Y7MCLV7SLILXPGHEZ5GP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MBV6G6Y7MCLV7SLILXPGHEZ5GP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2005:MBV6G6Y7MCLV7SLILXPGHEZ5GP","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":"bcbd0cfe753fdfdd76f3d9ee96334eafc4d532cdf64f2b3554832e5d4f207520","cross_cats_sorted":["hep-lat","nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-09T15:52:13Z","title_canon_sha256":"32ae126a70a9134857dd1f8ed9a1a301cfcf7ceacc12d6d1b933851bc7ec93c2"},"schema_version":"1.0","source":{"id":"hep-ph/0512125","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0512125","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0512125v2","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0512125","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_12","alias_value":"MBV6G6Y7MCLV","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_16","alias_value":"MBV6G6Y7MCLV7SLI","created_at":"2026-07-04T15:19:47Z"},{"alias_kind":"pith_short_8","alias_value":"MBV6G6Y7","created_at":"2026-07-04T15:19:47Z"}],"graph_snapshots":[{"event_id":"sha256:29941f1ae1753402b23e970535a7782dd0242274f1da2535cf4667eee5afe716","target":"graph","created_at":"2026-07-04T15:19:47Z","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/0512125/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"It is argued that strong dynamics in the quark-gluon plasma and bound states of quarks and gluons is mostly due to nonperturbative effects described by field correlators. The emphasis in the paper is made on two explicit calculations of these effects from the first principles: one analytic using gluelump Green's functions and another using independent lattice data on correlators. The resulting hadron spectra are investigated in the range T_c < T < 2T_c. The spectra of charmonia, bottomonia, light s-sbar mesons, glueballs and quark-gluon states calculated numerically are in general agreement wi","authors_text":"A. Di Giacomo, A.I. Veselov, E. Meggiolaro, Yu.A. Simonov","cross_cats":["hep-lat","nucl-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2005-12-09T15:52:13Z","title":"Dynamics of quark-gluon plasma from Field correlators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0512125","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:bdfcdb9cbe8c1814c18945b4557e568447286f1d8abcb6be70698837f6652133","target":"record","created_at":"2026-07-04T15:19:47Z","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":"bcbd0cfe753fdfdd76f3d9ee96334eafc4d532cdf64f2b3554832e5d4f207520","cross_cats_sorted":["hep-lat","nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-09T15:52:13Z","title_canon_sha256":"32ae126a70a9134857dd1f8ed9a1a301cfcf7ceacc12d6d1b933851bc7ec93c2"},"schema_version":"1.0","source":{"id":"hep-ph/0512125","kind":"arxiv","version":2}},"canonical_sha256":"606be37b1f60975fc9685dde63933d33f80d6f5295b3bf855d41b072536dcc54","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"606be37b1f60975fc9685dde63933d33f80d6f5295b3bf855d41b072536dcc54","first_computed_at":"2026-07-04T15:19:47.469405Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:19:47.469405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/PwV0mQfFTH+zTdVPE4yd6/MoYPbWhtkXf6BNEyFnSMxFZ+ufowGlbSPk8/41XabOqxomdkn33yQbA98ZODeBQ==","signature_status":"signed_v1","signed_at":"2026-07-04T15:19:47.469793Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0512125","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bdfcdb9cbe8c1814c18945b4557e568447286f1d8abcb6be70698837f6652133","sha256:29941f1ae1753402b23e970535a7782dd0242274f1da2535cf4667eee5afe716"],"state_sha256":"d9dc664b1268dc46ba28f35960f2e14114981b89727b27ee419f945e7988b3dd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V2+nxWME9F+8AwDuu5VxvsG5chOptxZBFRA1ySMsqGae6oAfTBAX8ZgkXfYnx3HgoS+vtlyyNCNW1lvei1IgAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-06T15:47:36.570824Z","bundle_sha256":"e1c0de3f6cf14db7b24b90cea10361a1344244052942ae8342c5b52accd4075a"}}