{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:LFEWDSPQNVUE7VH3ZLGCLGWFSR","short_pith_number":"pith:LFEWDSPQ","canonical_record":{"source":{"id":"1403.2241","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T13:46:54Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"7d1245a4ef50376d9fe50db07d73df456d366ee39c4a483469d16868ec0d3453","abstract_canon_sha256":"9092b83e13a2a6dd08121cbbfc883fdf72a6972e6f386f1d55ddec241d223817"},"schema_version":"1.0"},"canonical_sha256":"594961c9f06d684fd4fbcacc259ac59467137aedfdef0894d7196344c069d3b2","source":{"kind":"arxiv","id":"1403.2241","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2241","created_at":"2026-05-18T01:44:09Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2241v1","created_at":"2026-05-18T01:44:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2241","created_at":"2026-05-18T01:44:09Z"},{"alias_kind":"pith_short_12","alias_value":"LFEWDSPQNVUE","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LFEWDSPQNVUE7VH3","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LFEWDSPQ","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:LFEWDSPQNVUE7VH3ZLGCLGWFSR","target":"record","payload":{"canonical_record":{"source":{"id":"1403.2241","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T13:46:54Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"7d1245a4ef50376d9fe50db07d73df456d366ee39c4a483469d16868ec0d3453","abstract_canon_sha256":"9092b83e13a2a6dd08121cbbfc883fdf72a6972e6f386f1d55ddec241d223817"},"schema_version":"1.0"},"canonical_sha256":"594961c9f06d684fd4fbcacc259ac59467137aedfdef0894d7196344c069d3b2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:44:09.557247Z","signature_b64":"EzyNEkX88U8aeTl5Ljm04aCjCiZwv7JIA4wn1uu6FrwfP6yTUCfqu3bcpFmCy/x06+FxrS5cBMZBim/MHgzIDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"594961c9f06d684fd4fbcacc259ac59467137aedfdef0894d7196344c069d3b2","last_reissued_at":"2026-05-18T01:44:09.556505Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:44:09.556505Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.2241","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":"2026-05-18T01:44:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zV5iAOV8wJiaYFcKyaKovNuufrOPa7mdokwRE9k1eU100/aEUghufizl+27Yta8FolRqYIp9Z75lelH05nypBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T05:06:12.716852Z"},"content_sha256":"cd3bcde63b8a0b25a56b82efcdffdfa15c43f8ed64140a50211478f4bc4c0219","schema_version":"1.0","event_id":"sha256:cd3bcde63b8a0b25a56b82efcdffdfa15c43f8ed64140a50211478f4bc4c0219"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:LFEWDSPQNVUE7VH3ZLGCLGWFSR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quadratic thermal terms in the deconfined phase from holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Fen Zuo, Yi-hong Gao","submitted_at":"2014-03-10T13:46:54Z","abstract_excerpt":"Recent lattice simulation has uncovered many interesting properties of SU(N) gauge theory at finite temperature. Especially, above the deconfinement phase transition all the thermodynamics quantities acquire significant quadratic contributions in inverse temperature. Such a term is also found to dominate the logarithmic of the renormalized Polyakov loop. Using the Hawking-Page transition in Anti-de Sitter space as an example, we show how such contributions can be naturally generated in the holographic approach."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2241","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":"2026-05-18T01:44:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rcx0B1zKgUISoTKTOomfk1w/f3eqAFmQ2QnTuNu+MIAOjVEroQ2lSF1s9W3B91U1RzhU+gPWRFWWnRG/I+eTBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T05:06:12.717334Z"},"content_sha256":"eb5cc250ad5f1d9163a0db9ffd1ef48f6f90c2397d5b03ef8374e45c7771c13d","schema_version":"1.0","event_id":"sha256:eb5cc250ad5f1d9163a0db9ffd1ef48f6f90c2397d5b03ef8374e45c7771c13d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LFEWDSPQNVUE7VH3ZLGCLGWFSR/bundle.json","state_url":"https://pith.science/pith/LFEWDSPQNVUE7VH3ZLGCLGWFSR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LFEWDSPQNVUE7VH3ZLGCLGWFSR/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":"2026-05-30T05:06:12Z","links":{"resolver":"https://pith.science/pith/LFEWDSPQNVUE7VH3ZLGCLGWFSR","bundle":"https://pith.science/pith/LFEWDSPQNVUE7VH3ZLGCLGWFSR/bundle.json","state":"https://pith.science/pith/LFEWDSPQNVUE7VH3ZLGCLGWFSR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LFEWDSPQNVUE7VH3ZLGCLGWFSR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:LFEWDSPQNVUE7VH3ZLGCLGWFSR","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":"9092b83e13a2a6dd08121cbbfc883fdf72a6972e6f386f1d55ddec241d223817","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T13:46:54Z","title_canon_sha256":"7d1245a4ef50376d9fe50db07d73df456d366ee39c4a483469d16868ec0d3453"},"schema_version":"1.0","source":{"id":"1403.2241","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2241","created_at":"2026-05-18T01:44:09Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2241v1","created_at":"2026-05-18T01:44:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2241","created_at":"2026-05-18T01:44:09Z"},{"alias_kind":"pith_short_12","alias_value":"LFEWDSPQNVUE","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LFEWDSPQNVUE7VH3","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LFEWDSPQ","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:eb5cc250ad5f1d9163a0db9ffd1ef48f6f90c2397d5b03ef8374e45c7771c13d","target":"graph","created_at":"2026-05-18T01:44:09Z","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":"Recent lattice simulation has uncovered many interesting properties of SU(N) gauge theory at finite temperature. Especially, above the deconfinement phase transition all the thermodynamics quantities acquire significant quadratic contributions in inverse temperature. Such a term is also found to dominate the logarithmic of the renormalized Polyakov loop. Using the Hawking-Page transition in Anti-de Sitter space as an example, we show how such contributions can be naturally generated in the holographic approach.","authors_text":"Fen Zuo, Yi-hong Gao","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T13:46:54Z","title":"Quadratic thermal terms in the deconfined phase from holography"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2241","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:cd3bcde63b8a0b25a56b82efcdffdfa15c43f8ed64140a50211478f4bc4c0219","target":"record","created_at":"2026-05-18T01:44:09Z","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":"9092b83e13a2a6dd08121cbbfc883fdf72a6972e6f386f1d55ddec241d223817","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T13:46:54Z","title_canon_sha256":"7d1245a4ef50376d9fe50db07d73df456d366ee39c4a483469d16868ec0d3453"},"schema_version":"1.0","source":{"id":"1403.2241","kind":"arxiv","version":1}},"canonical_sha256":"594961c9f06d684fd4fbcacc259ac59467137aedfdef0894d7196344c069d3b2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"594961c9f06d684fd4fbcacc259ac59467137aedfdef0894d7196344c069d3b2","first_computed_at":"2026-05-18T01:44:09.556505Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:44:09.556505Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EzyNEkX88U8aeTl5Ljm04aCjCiZwv7JIA4wn1uu6FrwfP6yTUCfqu3bcpFmCy/x06+FxrS5cBMZBim/MHgzIDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:44:09.557247Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.2241","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cd3bcde63b8a0b25a56b82efcdffdfa15c43f8ed64140a50211478f4bc4c0219","sha256:eb5cc250ad5f1d9163a0db9ffd1ef48f6f90c2397d5b03ef8374e45c7771c13d"],"state_sha256":"f11bbef8d2f23b6686ee7532eabb6258af0ca7c0170bbbd58e8038b9b5a51693"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gQyxiYTVgyNoUqYRsSdKa2C+HZiJIRLk+lZyVbfGIwHSxB2bFkog+QrYy8dIhmgomyTAQ36DfKKKN+7+Hu/GCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T05:06:12.720584Z","bundle_sha256":"a188123c08a7d34e2a9417aa0d339aa1c04d4cf57e669d65435010839516fe3c"}}