{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:226TAW66MKSN6O4DTO2QMA3R4E","short_pith_number":"pith:226TAW66","schema_version":"1.0","canonical_sha256":"d6bd305bde62a4df3b839bb5060371e124bf4e2b609d2f8d6a40b25236e3559c","source":{"kind":"arxiv","id":"0901.1487","version":2},"attestation_state":"computed","paper":{"title":"Universal hydrodynamics of non-conformal branes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ingmar Kanitscheider, Kostas Skenderis","submitted_at":"2009-01-12T17:29:15Z","abstract_excerpt":"We examine the hydrodynamic limit of non-conformal branes using the recently developed precise holographic dictionary. We first streamline the discussion of holography for backgrounds that asymptote locally to non-conformal brane solutions by showing that all such solutions can be obtained from higher dimensional asymptotically locally AdS solutions by suitable dimensional reduction and continuation in the dimension. As a consequence, many holographic results for such backgrounds follow from the corresponding results of the Asymptotically AdS case. In particular, the hydrodynamics of non-confo"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"0901.1487","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-01-12T17:29:15Z","cross_cats_sorted":[],"title_canon_sha256":"9a0df19fd26c3e22a99dbdea6af168e1408bf8fbf87a0a65c7bca060340ebe7e","abstract_canon_sha256":"bd0a8687cd6a091ab5f99625ecded64f54f52bd04a6386e67e8be0314e53c758"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:41:34.436941Z","signature_b64":"xiifig+KyJMs2WoFYyNTG4DGPdp5xp7OVirdpnAcrT6BJd1kFLSv2McVBI353/SNhrDxUm12FbTHJzhwrbMuAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d6bd305bde62a4df3b839bb5060371e124bf4e2b609d2f8d6a40b25236e3559c","last_reissued_at":"2026-07-04T15:41:34.436586Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:41:34.436586Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal hydrodynamics of non-conformal branes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ingmar Kanitscheider, Kostas Skenderis","submitted_at":"2009-01-12T17:29:15Z","abstract_excerpt":"We examine the hydrodynamic limit of non-conformal branes using the recently developed precise holographic dictionary. We first streamline the discussion of holography for backgrounds that asymptote locally to non-conformal brane solutions by showing that all such solutions can be obtained from higher dimensional asymptotically locally AdS solutions by suitable dimensional reduction and continuation in the dimension. As a consequence, many holographic results for such backgrounds follow from the corresponding results of the Asymptotically AdS case. In particular, the hydrodynamics of non-confo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0901.1487","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/0901.1487/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0901.1487","created_at":"2026-07-04T15:41:34.436644+00:00"},{"alias_kind":"arxiv_version","alias_value":"0901.1487v2","created_at":"2026-07-04T15:41:34.436644+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0901.1487","created_at":"2026-07-04T15:41:34.436644+00:00"},{"alias_kind":"pith_short_12","alias_value":"226TAW66MKSN","created_at":"2026-07-04T15:41:34.436644+00:00"},{"alias_kind":"pith_short_16","alias_value":"226TAW66MKSN6O4D","created_at":"2026-07-04T15:41:34.436644+00:00"},{"alias_kind":"pith_short_8","alias_value":"226TAW66","created_at":"2026-07-04T15:41:34.436644+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.31901","citing_title":"Exact Planar Black Hole in AdS-Einstein-Scalar Gravity with IR Emergent Nearly Conformal Fluid","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"1907.02974","citing_title":"Ricci cosmology","ref_index":34,"is_internal_anchor":true},{"citing_arxiv_id":"2605.18942","citing_title":"Covariant unification of holographic c-functions","ref_index":91,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E","json":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E.json","graph_json":"https://pith.science/api/pith-number/226TAW66MKSN6O4DTO2QMA3R4E/graph.json","events_json":"https://pith.science/api/pith-number/226TAW66MKSN6O4DTO2QMA3R4E/events.json","paper":"https://pith.science/paper/226TAW66"},"agent_actions":{"view_html":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E","download_json":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E.json","view_paper":"https://pith.science/paper/226TAW66","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0901.1487&json=true","fetch_graph":"https://pith.science/api/pith-number/226TAW66MKSN6O4DTO2QMA3R4E/graph.json","fetch_events":"https://pith.science/api/pith-number/226TAW66MKSN6O4DTO2QMA3R4E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E/action/storage_attestation","attest_author":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E/action/author_attestation","sign_citation":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E/action/citation_signature","submit_replication":"https://pith.science/pith/226TAW66MKSN6O4DTO2QMA3R4E/action/replication_record"}},"created_at":"2026-07-04T15:41:34.436644+00:00","updated_at":"2026-07-04T15:41:34.436644+00:00"}