{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:UZWHQROOISMKC5WMVZOF5LYACS","short_pith_number":"pith:UZWHQROO","schema_version":"1.0","canonical_sha256":"a66c7845ce4498a176ccae5c5eaf00149024aecda32d94ae2af92f17abf4144d","source":{"kind":"arxiv","id":"1304.0898","version":1},"attestation_state":"computed","paper":{"title":"Higher Spin Contributions to Holographic Fluid Dynamics in $AdS_5/CFT_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dimitri Polyakov, Seungjin Lee","submitted_at":"2013-04-03T10:10:21Z","abstract_excerpt":"We calculate the graviton's $\\beta$-function in $AdS$ string-theoretic sigma-model, perturbed by vertex operators for Vasiliev's higher spin gauge fields in $AdS_5$. The result is given by $\\beta_{mn}=R_{mn}+4T_{mn}(g,u)$ (with the AdS radius set to 1 and the graviton polarized along the $AdS_5$ boundary), with the matter stress-energy tensor given by that of conformal holographic fluid in $d=4$, evaluated at the temperature given by $T={1\\over{\\pi}}$. The stress-energy tensor is given by $T_{mn}={g_{mn}}+4u_mu_n+\\sum_{N}T^{(N)}_{mn}$ where $u$ is the vector excitation satisfying $u^2=-1$ and "},"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":"1304.0898","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-04-03T10:10:21Z","cross_cats_sorted":[],"title_canon_sha256":"ba6785609e3bf376e9ca475cd0becbe38ad657ab981b438648364ca82fdba178","abstract_canon_sha256":"1ecd14eb098dc924de7c01d6004889cb80cd369af8a4c45964987090f22c441f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:50:49.656782Z","signature_b64":"xuQxJuYTPe3N5aAcIUchb6w/zOFdwl7pI03l4i1xR1jZo/JtJEmDr/65YGHBkVUNaSlWRS9pM3zHTMe/ZD8/Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a66c7845ce4498a176ccae5c5eaf00149024aecda32d94ae2af92f17abf4144d","last_reissued_at":"2026-05-18T01:50:49.656153Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:50:49.656153Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher Spin Contributions to Holographic Fluid Dynamics in $AdS_5/CFT_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dimitri Polyakov, Seungjin Lee","submitted_at":"2013-04-03T10:10:21Z","abstract_excerpt":"We calculate the graviton's $\\beta$-function in $AdS$ string-theoretic sigma-model, perturbed by vertex operators for Vasiliev's higher spin gauge fields in $AdS_5$. The result is given by $\\beta_{mn}=R_{mn}+4T_{mn}(g,u)$ (with the AdS radius set to 1 and the graviton polarized along the $AdS_5$ boundary), with the matter stress-energy tensor given by that of conformal holographic fluid in $d=4$, evaluated at the temperature given by $T={1\\over{\\pi}}$. The stress-energy tensor is given by $T_{mn}={g_{mn}}+4u_mu_n+\\sum_{N}T^{(N)}_{mn}$ where $u$ is the vector excitation satisfying $u^2=-1$ and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.0898","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1304.0898","created_at":"2026-05-18T01:50:49.656232+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.0898v1","created_at":"2026-05-18T01:50:49.656232+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.0898","created_at":"2026-05-18T01:50:49.656232+00:00"},{"alias_kind":"pith_short_12","alias_value":"UZWHQROOISMK","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_16","alias_value":"UZWHQROOISMKC5WM","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_8","alias_value":"UZWHQROO","created_at":"2026-05-18T12:28:02.375192+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS","json":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS.json","graph_json":"https://pith.science/api/pith-number/UZWHQROOISMKC5WMVZOF5LYACS/graph.json","events_json":"https://pith.science/api/pith-number/UZWHQROOISMKC5WMVZOF5LYACS/events.json","paper":"https://pith.science/paper/UZWHQROO"},"agent_actions":{"view_html":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS","download_json":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS.json","view_paper":"https://pith.science/paper/UZWHQROO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.0898&json=true","fetch_graph":"https://pith.science/api/pith-number/UZWHQROOISMKC5WMVZOF5LYACS/graph.json","fetch_events":"https://pith.science/api/pith-number/UZWHQROOISMKC5WMVZOF5LYACS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS/action/storage_attestation","attest_author":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS/action/author_attestation","sign_citation":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS/action/citation_signature","submit_replication":"https://pith.science/pith/UZWHQROOISMKC5WMVZOF5LYACS/action/replication_record"}},"created_at":"2026-05-18T01:50:49.656232+00:00","updated_at":"2026-05-18T01:50:49.656232+00:00"}