{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:BL3ZKA74Y2S6IWUESCTCYAALPW","short_pith_number":"pith:BL3ZKA74","schema_version":"1.0","canonical_sha256":"0af79503fcc6a5e45a8490a62c000b7dac0ae3aeddb0f8bff87fc2150f3ca6da","source":{"kind":"arxiv","id":"1211.5972","version":3},"attestation_state":"computed","paper":{"title":"Transport in non-conformal holographic fluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bum-Hoon Lee, Chanyong Park, Jae-Hyuk Oh, Raju Roychowdhury, Shailesh Kulkarni","submitted_at":"2012-11-26T14:42:39Z","abstract_excerpt":"We have considered non-conformal fluid dynamics whose gravity dual is a certain Einstein dilaton system with Liouville type dilaton potential, characterized by an intrinsic parameter $\\eta$. We have discussed the Hawking-Page transition in this framework using hard-wall model and it turns out that the critical temperature of the Hawking-Page transition encapsulates a non-trivial dependence on $\\eta$. We also obtained transport coefficients such as AC conductivity, shear viscosity and diffusion constant in the hydrodynamic limit, which show non-trivial $\\eta$ dependent deviations from those in "},"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":"1211.5972","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-11-26T14:42:39Z","cross_cats_sorted":[],"title_canon_sha256":"4754a8766a0a77862c27b695392414df37ff1cd38eba08f343814e4d0e1ac5fc","abstract_canon_sha256":"d47c111e877177d57d2fac88716408319c8820c335d6472f2a50af73a9ed296e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:52:55.034655Z","signature_b64":"U8yj/ZMysUV7d0+rsig3kpomvSZ04/Pl95GqNcKeTO0/bbdKqlBcDSXMKIiCLOU2ywo+ZENhWGuOzeywQIisCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0af79503fcc6a5e45a8490a62c000b7dac0ae3aeddb0f8bff87fc2150f3ca6da","last_reissued_at":"2026-05-18T01:52:55.033963Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:52:55.033963Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transport in non-conformal holographic fluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bum-Hoon Lee, Chanyong Park, Jae-Hyuk Oh, Raju Roychowdhury, Shailesh Kulkarni","submitted_at":"2012-11-26T14:42:39Z","abstract_excerpt":"We have considered non-conformal fluid dynamics whose gravity dual is a certain Einstein dilaton system with Liouville type dilaton potential, characterized by an intrinsic parameter $\\eta$. We have discussed the Hawking-Page transition in this framework using hard-wall model and it turns out that the critical temperature of the Hawking-Page transition encapsulates a non-trivial dependence on $\\eta$. We also obtained transport coefficients such as AC conductivity, shear viscosity and diffusion constant in the hydrodynamic limit, which show non-trivial $\\eta$ dependent deviations from those in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.5972","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1211.5972","created_at":"2026-05-18T01:52:55.034078+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.5972v3","created_at":"2026-05-18T01:52:55.034078+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.5972","created_at":"2026-05-18T01:52:55.034078+00:00"},{"alias_kind":"pith_short_12","alias_value":"BL3ZKA74Y2S6","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_16","alias_value":"BL3ZKA74Y2S6IWUE","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_8","alias_value":"BL3ZKA74","created_at":"2026-05-18T12:27:01.376967+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.09431","citing_title":"Effect of non-conformal deformation on the gapped quasi-normal modes and the holographic implications","ref_index":75,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW","json":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW.json","graph_json":"https://pith.science/api/pith-number/BL3ZKA74Y2S6IWUESCTCYAALPW/graph.json","events_json":"https://pith.science/api/pith-number/BL3ZKA74Y2S6IWUESCTCYAALPW/events.json","paper":"https://pith.science/paper/BL3ZKA74"},"agent_actions":{"view_html":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW","download_json":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW.json","view_paper":"https://pith.science/paper/BL3ZKA74","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.5972&json=true","fetch_graph":"https://pith.science/api/pith-number/BL3ZKA74Y2S6IWUESCTCYAALPW/graph.json","fetch_events":"https://pith.science/api/pith-number/BL3ZKA74Y2S6IWUESCTCYAALPW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW/action/storage_attestation","attest_author":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW/action/author_attestation","sign_citation":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW/action/citation_signature","submit_replication":"https://pith.science/pith/BL3ZKA74Y2S6IWUESCTCYAALPW/action/replication_record"}},"created_at":"2026-05-18T01:52:55.034078+00:00","updated_at":"2026-05-18T01:52:55.034078+00:00"}