{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:UCYZKUZ3MIY5EZDOLAC2ILC3QF","short_pith_number":"pith:UCYZKUZ3","canonical_record":{"source":{"id":"1405.4829","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-05-19T18:31:16Z","cross_cats_sorted":["cond-mat.stat-mech","gr-qc"],"title_canon_sha256":"608e919fb00ea6b0941298a158db00f257ec56187dfc9aac128bb2dcba359de3","abstract_canon_sha256":"8805db02aed3cafabb20d75b94985c83d18a4ecfabb665115af056390f67356b"},"schema_version":"1.0"},"canonical_sha256":"a0b195533b6231d2646e5805a42c5b8158c0837320cd480cc8bfb634fa2eca9d","source":{"kind":"arxiv","id":"1405.4829","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.4829","created_at":"2026-05-18T02:29:23Z"},{"alias_kind":"arxiv_version","alias_value":"1405.4829v3","created_at":"2026-05-18T02:29:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.4829","created_at":"2026-05-18T02:29:23Z"},{"alias_kind":"pith_short_12","alias_value":"UCYZKUZ3MIY5","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_16","alias_value":"UCYZKUZ3MIY5EZDO","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_8","alias_value":"UCYZKUZ3","created_at":"2026-05-18T12:28:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:UCYZKUZ3MIY5EZDOLAC2ILC3QF","target":"record","payload":{"canonical_record":{"source":{"id":"1405.4829","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-05-19T18:31:16Z","cross_cats_sorted":["cond-mat.stat-mech","gr-qc"],"title_canon_sha256":"608e919fb00ea6b0941298a158db00f257ec56187dfc9aac128bb2dcba359de3","abstract_canon_sha256":"8805db02aed3cafabb20d75b94985c83d18a4ecfabb665115af056390f67356b"},"schema_version":"1.0"},"canonical_sha256":"a0b195533b6231d2646e5805a42c5b8158c0837320cd480cc8bfb634fa2eca9d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:29:23.452253Z","signature_b64":"R1mCpRWo9MPnN1l0fBhEhCQ4URDpP6YCEUuPW9qjsUs9F53wnWjPUGX/Wi8jHMbg1FOyfQzLqMjRuyctxQQ0CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0b195533b6231d2646e5805a42c5b8158c0837320cd480cc8bfb634fa2eca9d","last_reissued_at":"2026-05-18T02:29:23.451796Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:29:23.451796Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1405.4829","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:29:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uUsMrmFLdp8HdX9Ku0XEDAJqe5Mvm4b1w5RXnEivZn4/ZVTOYeyZsOGQc6QNMt9Bc6go2leGCfzlHe0wRFOvDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:41:13.776985Z"},"content_sha256":"e3a7978ca6a9a3d59fd68af03221aa39c503cadbecb86a2012eb318272ac964b","schema_version":"1.0","event_id":"sha256:e3a7978ca6a9a3d59fd68af03221aa39c503cadbecb86a2012eb318272ac964b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:UCYZKUZ3MIY5EZDOLAC2ILC3QF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Classical and quantum temperature fluctuations via holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","gr-qc"],"primary_cat":"hep-th","authors_text":"Alexander Balatsky, Alexander Krikun, Konstantin Zarembo, Larus Thorlacius, Sven Bjarke Gudnason, Yaron Kedem","submitted_at":"2014-05-19T18:31:16Z","abstract_excerpt":"We study local temperature fluctuations in a 2+1 dimensional CFT on the sphere, dual to a black hole in asymptotically AdS spacetime. The fluctuation spectrum is governed by the lowest-lying hydrodynamic modes of the system whose frequency and damping rate determine whether temperature fluctuations are thermal or quantum. We calculate numerically the corresponding quasinormal frequencies and match the result with the hydrodynamics of the dual CFT at large temperature. As a by-product of our analysis we determine the appropriate boundary conditions for calculating low-lying quasinormal modes fo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.4829","kind":"arxiv","version":3},"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":"2026-05-18T02:29:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ebXOgnKR6Mm+varZzXtehfw41k78NHZsdyb8MHE8HIb4sQ+bewGPUNcWjVatz8yDVmnFVnxEVsiR0I4IDkesAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:41:13.777619Z"},"content_sha256":"c0f409c1807e0a4415d5081f69d2008a21bff0ef00c77aa392542ea95f8fd18f","schema_version":"1.0","event_id":"sha256:c0f409c1807e0a4415d5081f69d2008a21bff0ef00c77aa392542ea95f8fd18f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UCYZKUZ3MIY5EZDOLAC2ILC3QF/bundle.json","state_url":"https://pith.science/pith/UCYZKUZ3MIY5EZDOLAC2ILC3QF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UCYZKUZ3MIY5EZDOLAC2ILC3QF/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":"2026-05-25T19:41:13Z","links":{"resolver":"https://pith.science/pith/UCYZKUZ3MIY5EZDOLAC2ILC3QF","bundle":"https://pith.science/pith/UCYZKUZ3MIY5EZDOLAC2ILC3QF/bundle.json","state":"https://pith.science/pith/UCYZKUZ3MIY5EZDOLAC2ILC3QF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UCYZKUZ3MIY5EZDOLAC2ILC3QF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:UCYZKUZ3MIY5EZDOLAC2ILC3QF","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":"8805db02aed3cafabb20d75b94985c83d18a4ecfabb665115af056390f67356b","cross_cats_sorted":["cond-mat.stat-mech","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-05-19T18:31:16Z","title_canon_sha256":"608e919fb00ea6b0941298a158db00f257ec56187dfc9aac128bb2dcba359de3"},"schema_version":"1.0","source":{"id":"1405.4829","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.4829","created_at":"2026-05-18T02:29:23Z"},{"alias_kind":"arxiv_version","alias_value":"1405.4829v3","created_at":"2026-05-18T02:29:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.4829","created_at":"2026-05-18T02:29:23Z"},{"alias_kind":"pith_short_12","alias_value":"UCYZKUZ3MIY5","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_16","alias_value":"UCYZKUZ3MIY5EZDO","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_8","alias_value":"UCYZKUZ3","created_at":"2026-05-18T12:28:52Z"}],"graph_snapshots":[{"event_id":"sha256:c0f409c1807e0a4415d5081f69d2008a21bff0ef00c77aa392542ea95f8fd18f","target":"graph","created_at":"2026-05-18T02:29:23Z","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":"We study local temperature fluctuations in a 2+1 dimensional CFT on the sphere, dual to a black hole in asymptotically AdS spacetime. The fluctuation spectrum is governed by the lowest-lying hydrodynamic modes of the system whose frequency and damping rate determine whether temperature fluctuations are thermal or quantum. We calculate numerically the corresponding quasinormal frequencies and match the result with the hydrodynamics of the dual CFT at large temperature. As a by-product of our analysis we determine the appropriate boundary conditions for calculating low-lying quasinormal modes fo","authors_text":"Alexander Balatsky, Alexander Krikun, Konstantin Zarembo, Larus Thorlacius, Sven Bjarke Gudnason, Yaron Kedem","cross_cats":["cond-mat.stat-mech","gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-05-19T18:31:16Z","title":"Classical and quantum temperature fluctuations via holography"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.4829","kind":"arxiv","version":3},"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:e3a7978ca6a9a3d59fd68af03221aa39c503cadbecb86a2012eb318272ac964b","target":"record","created_at":"2026-05-18T02:29:23Z","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":"8805db02aed3cafabb20d75b94985c83d18a4ecfabb665115af056390f67356b","cross_cats_sorted":["cond-mat.stat-mech","gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-05-19T18:31:16Z","title_canon_sha256":"608e919fb00ea6b0941298a158db00f257ec56187dfc9aac128bb2dcba359de3"},"schema_version":"1.0","source":{"id":"1405.4829","kind":"arxiv","version":3}},"canonical_sha256":"a0b195533b6231d2646e5805a42c5b8158c0837320cd480cc8bfb634fa2eca9d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a0b195533b6231d2646e5805a42c5b8158c0837320cd480cc8bfb634fa2eca9d","first_computed_at":"2026-05-18T02:29:23.451796Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:29:23.451796Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"R1mCpRWo9MPnN1l0fBhEhCQ4URDpP6YCEUuPW9qjsUs9F53wnWjPUGX/Wi8jHMbg1FOyfQzLqMjRuyctxQQ0CA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:29:23.452253Z","signed_message":"canonical_sha256_bytes"},"source_id":"1405.4829","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e3a7978ca6a9a3d59fd68af03221aa39c503cadbecb86a2012eb318272ac964b","sha256:c0f409c1807e0a4415d5081f69d2008a21bff0ef00c77aa392542ea95f8fd18f"],"state_sha256":"1e0e54de641f7fdef2bb34234be18577cafff4177222e2092b0461ced6021ac1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/a0FgQ+es4osClAZPguR4ML90wNprU2rVfO+2T3TBILU0kjvStSnn/ewC9sAZ3vMvf3wEz/ImY9UBReFAuSUDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T19:41:13.780984Z","bundle_sha256":"e751ddf35ea4e843838df25aa996ea0354ff1fb944addab01dfb703b0f50fd46"}}