{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:ZMPGJPCESXCY3PVJQ4ZWQLBXN4","short_pith_number":"pith:ZMPGJPCE","canonical_record":{"source":{"id":"1104.3281","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-17T06:56:26Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"073d55092e7810117f74641caee1ff543ab30ba6816ebd2eb1c281d1e3ad5b6d","abstract_canon_sha256":"d8df50dbeb2801f2498d577a821188968a309b45e15859bc414f751b074d8cde"},"schema_version":"1.0"},"canonical_sha256":"cb1e64bc4495c58dbea98733682c376f1d02d702b970ec6eef8119c85fb69d6a","source":{"kind":"arxiv","id":"1104.3281","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.3281","created_at":"2026-05-18T04:17:14Z"},{"alias_kind":"arxiv_version","alias_value":"1104.3281v2","created_at":"2026-05-18T04:17:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.3281","created_at":"2026-05-18T04:17:14Z"},{"alias_kind":"pith_short_12","alias_value":"ZMPGJPCESXCY","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"ZMPGJPCESXCY3PVJ","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"ZMPGJPCE","created_at":"2026-05-18T12:26:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:ZMPGJPCESXCY3PVJQ4ZWQLBXN4","target":"record","payload":{"canonical_record":{"source":{"id":"1104.3281","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-17T06:56:26Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"073d55092e7810117f74641caee1ff543ab30ba6816ebd2eb1c281d1e3ad5b6d","abstract_canon_sha256":"d8df50dbeb2801f2498d577a821188968a309b45e15859bc414f751b074d8cde"},"schema_version":"1.0"},"canonical_sha256":"cb1e64bc4495c58dbea98733682c376f1d02d702b970ec6eef8119c85fb69d6a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:14.826295Z","signature_b64":"6D6K9eS08Kt5LNmZieRe3z0Y1KIKDwwFv6caAw3E3vNPJB0ZYTCgChSi64ow6zyKVqau4eNdTN+LSRkOfGmAAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb1e64bc4495c58dbea98733682c376f1d02d702b970ec6eef8119c85fb69d6a","last_reissued_at":"2026-05-18T04:17:14.825659Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:14.825659Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1104.3281","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:17:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"d1rlCY5y1rH0KNZ9Hs0b0FmzLq/1DpMX2lFwk5Ls33zNdDoax616SqAJ/5R18w7Xn5gwj592gTHfkmbMr67OBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T16:04:06.824101Z"},"content_sha256":"919cd9e8a998d18d3ba671ea4ac1354769284e5a182ae6ea1f9308cbe0587098","schema_version":"1.0","event_id":"sha256:919cd9e8a998d18d3ba671ea4ac1354769284e5a182ae6ea1f9308cbe0587098"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:ZMPGJPCESXCY3PVJQ4ZWQLBXN4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-Relativistic Fluid Dual to Asymptotically AdS Gravity at Finite Cutoff Surface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Li Li, Rong-Gen Cai, Yun-Long Zhang","submitted_at":"2011-04-17T06:56:26Z","abstract_excerpt":"Using the non-relativistic hydrodynamic expansion, we solve equations of motion for Einstein gravity and Gauss-Bonnet gravity with a negative cosmological constant within the region between a finite cutoff surface and a black brane horizon, up to the second order of the expansion parameter. Through the Brown-York tensor, we calculate the stress energy tensor of dual fluids living on the cutoff surface. With the black brane solutions, we show that for both Einstein gravity and Gauss-Bonnet gravity, the ratio of shear viscosity to entropy ensity of dual fluid does not run with the cutoff surface"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.3281","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":""},"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":"2026-05-18T04:17:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J8KftcLtEPABq2BdRs3+Km0asCMCVd+A0DeGu3K9ZokuxR5nUa4i5HTUnPRKuv/Z7f8KxgpNc9jHqg5oeRxdAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T16:04:06.824469Z"},"content_sha256":"bd2b441f78f54fc1009d90dec0cd7f393956c10e24bec78b1fa9ea404e5027be","schema_version":"1.0","event_id":"sha256:bd2b441f78f54fc1009d90dec0cd7f393956c10e24bec78b1fa9ea404e5027be"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZMPGJPCESXCY3PVJQ4ZWQLBXN4/bundle.json","state_url":"https://pith.science/pith/ZMPGJPCESXCY3PVJQ4ZWQLBXN4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZMPGJPCESXCY3PVJQ4ZWQLBXN4/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":"2026-05-28T16:04:06Z","links":{"resolver":"https://pith.science/pith/ZMPGJPCESXCY3PVJQ4ZWQLBXN4","bundle":"https://pith.science/pith/ZMPGJPCESXCY3PVJQ4ZWQLBXN4/bundle.json","state":"https://pith.science/pith/ZMPGJPCESXCY3PVJQ4ZWQLBXN4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZMPGJPCESXCY3PVJQ4ZWQLBXN4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:ZMPGJPCESXCY3PVJQ4ZWQLBXN4","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":"d8df50dbeb2801f2498d577a821188968a309b45e15859bc414f751b074d8cde","cross_cats_sorted":["gr-qc","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-17T06:56:26Z","title_canon_sha256":"073d55092e7810117f74641caee1ff543ab30ba6816ebd2eb1c281d1e3ad5b6d"},"schema_version":"1.0","source":{"id":"1104.3281","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.3281","created_at":"2026-05-18T04:17:14Z"},{"alias_kind":"arxiv_version","alias_value":"1104.3281v2","created_at":"2026-05-18T04:17:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.3281","created_at":"2026-05-18T04:17:14Z"},{"alias_kind":"pith_short_12","alias_value":"ZMPGJPCESXCY","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"ZMPGJPCESXCY3PVJ","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"ZMPGJPCE","created_at":"2026-05-18T12:26:47Z"}],"graph_snapshots":[{"event_id":"sha256:bd2b441f78f54fc1009d90dec0cd7f393956c10e24bec78b1fa9ea404e5027be","target":"graph","created_at":"2026-05-18T04:17:14Z","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":"Using the non-relativistic hydrodynamic expansion, we solve equations of motion for Einstein gravity and Gauss-Bonnet gravity with a negative cosmological constant within the region between a finite cutoff surface and a black brane horizon, up to the second order of the expansion parameter. Through the Brown-York tensor, we calculate the stress energy tensor of dual fluids living on the cutoff surface. With the black brane solutions, we show that for both Einstein gravity and Gauss-Bonnet gravity, the ratio of shear viscosity to entropy ensity of dual fluid does not run with the cutoff surface","authors_text":"Li Li, Rong-Gen Cai, Yun-Long Zhang","cross_cats":["gr-qc","hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-17T06:56:26Z","title":"Non-Relativistic Fluid Dual to Asymptotically AdS Gravity at Finite Cutoff Surface"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.3281","kind":"arxiv","version":2},"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":"sha256:919cd9e8a998d18d3ba671ea4ac1354769284e5a182ae6ea1f9308cbe0587098","target":"record","created_at":"2026-05-18T04:17:14Z","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":"d8df50dbeb2801f2498d577a821188968a309b45e15859bc414f751b074d8cde","cross_cats_sorted":["gr-qc","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-17T06:56:26Z","title_canon_sha256":"073d55092e7810117f74641caee1ff543ab30ba6816ebd2eb1c281d1e3ad5b6d"},"schema_version":"1.0","source":{"id":"1104.3281","kind":"arxiv","version":2}},"canonical_sha256":"cb1e64bc4495c58dbea98733682c376f1d02d702b970ec6eef8119c85fb69d6a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cb1e64bc4495c58dbea98733682c376f1d02d702b970ec6eef8119c85fb69d6a","first_computed_at":"2026-05-18T04:17:14.825659Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:17:14.825659Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6D6K9eS08Kt5LNmZieRe3z0Y1KIKDwwFv6caAw3E3vNPJB0ZYTCgChSi64ow6zyKVqau4eNdTN+LSRkOfGmAAg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:17:14.826295Z","signed_message":"canonical_sha256_bytes"},"source_id":"1104.3281","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:919cd9e8a998d18d3ba671ea4ac1354769284e5a182ae6ea1f9308cbe0587098","sha256:bd2b441f78f54fc1009d90dec0cd7f393956c10e24bec78b1fa9ea404e5027be"],"state_sha256":"1150c6529eb7d2cabab75d311ccb6283bede9deefcbd385c5ba59c771bffb248"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bUCGsatOhqjWuuKBi4+8Jc0TzRLFSpuUjuR5Fmo8PvRsWCdGVAkhuYc+woIOuBzhtnlwwViNmlC0Zh+r8lKqBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T16:04:06.826513Z","bundle_sha256":"8b50fa80eb3c20a9683a83f65c68a03177a21116452c4039804f6ecc80513752"}}