{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:HMK3BZPJSPDSHQKNOUDGLMSI7T","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":"35b6e872d063570d459f7e092e3a50da62b586d3e126cbb3488be7b49d893912","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-05-15T09:54:08Z","title_canon_sha256":"e5140ca703ce444fdc551e10d97a810d86421adeb1bd48038ab027d9416617b9"},"schema_version":"1.0","source":{"id":"2605.15797","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15797","created_at":"2026-05-20T00:01:18Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15797v1","created_at":"2026-05-20T00:01:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15797","created_at":"2026-05-20T00:01:18Z"},{"alias_kind":"pith_short_12","alias_value":"HMK3BZPJSPDS","created_at":"2026-05-20T00:01:18Z"},{"alias_kind":"pith_short_16","alias_value":"HMK3BZPJSPDSHQKN","created_at":"2026-05-20T00:01:18Z"},{"alias_kind":"pith_short_8","alias_value":"HMK3BZPJ","created_at":"2026-05-20T00:01:18Z"}],"graph_snapshots":[{"event_id":"sha256:4e5927a02c9278dc8aeed557db8cbcba66ef2b570b51b9fbcccfe891c6e36ea5","target":"graph","created_at":"2026-05-20T00:01:18Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T17:33:48.740631Z","status":"skipped","version":"1.0.0"},{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T17:21:55.905425Z","status":"completed","version":"1.0.0"}],"endpoint":"/pith/2605.15797/integrity.json","findings":[],"snapshot_sha256":"4bfa10d06b6a8ba3adebad1884d4321e3738baebc3fc480fa14a2394d28e39f6","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"According to the formulation of the charged large $D$ membrane paradigm, an arbitrary dynamic black hole solution to a theory of gravity with a $U(1)$ gauge field is dual to the dynamics of a membrane in a non-gravitational background. This membrane is endowed with a stress-energy tensor and a charge current, whose conservation equations govern its dynamics. In this work, we demonstrate that the dynamics of these membrane configurations (at the leading nontrivial order in $1/D$) can be mapped to a relativistic charged fluid. Establishing a correspondence for asymptotically flat black holes wit","authors_text":"Mangesh Mandlik, Manu Kurian, Supratim Halder","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-05-15T09:54:08Z","title":"A fluid dual to charged large D membrane paradigm"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.15797","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:fba8957fd5c2305d990cc10b51efbd722bbae8e2f460039c7aa27a227b1c2aca","target":"record","created_at":"2026-05-20T00:01:18Z","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":"35b6e872d063570d459f7e092e3a50da62b586d3e126cbb3488be7b49d893912","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-05-15T09:54:08Z","title_canon_sha256":"e5140ca703ce444fdc551e10d97a810d86421adeb1bd48038ab027d9416617b9"},"schema_version":"1.0","source":{"id":"2605.15797","kind":"arxiv","version":1}},"canonical_sha256":"3b15b0e5e993c723c14d750665b248fcc1a92761663a71dd1e3f644e6941a2fd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3b15b0e5e993c723c14d750665b248fcc1a92761663a71dd1e3f644e6941a2fd","first_computed_at":"2026-05-20T00:01:18.839668Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:01:18.839668Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"57oy62E9HX6FFUcFMiHR2WRzfxdS7eIf0uLHelae7a/dnTrrTUhwPqbHRioj3HSNqmGYiBgqiM3US2MrUYDSAw==","signature_status":"signed_v1","signed_at":"2026-05-20T00:01:18.840380Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.15797","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fba8957fd5c2305d990cc10b51efbd722bbae8e2f460039c7aa27a227b1c2aca","sha256:4e5927a02c9278dc8aeed557db8cbcba66ef2b570b51b9fbcccfe891c6e36ea5"],"state_sha256":"8b974bdad582b7a1985945bcad25c2fd381fb58ccd1137e52675a5d0a02447b0"}