{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:QR2SEZXO5BD2LZKFWBL7MDLFE2","short_pith_number":"pith:QR2SEZXO","schema_version":"1.0","canonical_sha256":"84752266eee847a5e545b057f60d6526b089e8325612f2d0c676d88acfaad139","source":{"kind":"arxiv","id":"1411.5579","version":6},"attestation_state":"computed","paper":{"title":"Holographic Entanglement Entropy for the Most General Higher Derivative Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Rong-Xin Miao, Wu-zhong Guo","submitted_at":"2014-11-20T15:47:19Z","abstract_excerpt":"The holographic entanglement entropy for the most general higher derivative gravity is investigated. We find a new type of Wald entropy, which appears on entangling surface without the rotational symmetry and reduces to usual Wald entropy on Killing horizon. Furthermore, we obtain a formal formula of HEE for the most general higher derivative gravity and work it out exactly for some squashed cones. As an important application, we derive HEE for gravitational action with one derivative of the curvature when the extrinsic curvature vanishes. We also study some toy models with non-zero extrinsic "},"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":"1411.5579","kind":"arxiv","version":6},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-11-20T15:47:19Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"9a7510b61d1e5c4a303d60c1ec79ff10655a0cd0846ec445c0eb242b45393c1d","abstract_canon_sha256":"b1ef04014d5b2e102ec20b4e517911fbc3d18650bdd5d9f78f65d79f01fde8e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:35:38.308972Z","signature_b64":"aPG3qQgk7BgMJPoTYAw57KpbKphUG4Ox/ciDLgn1CP8rNgfDyTGXkcBFdZhJJjl1uQlOII1qfRuoPrGeLecADg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"84752266eee847a5e545b057f60d6526b089e8325612f2d0c676d88acfaad139","last_reissued_at":"2026-05-18T01:35:38.308289Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:35:38.308289Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic Entanglement Entropy for the Most General Higher Derivative Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Rong-Xin Miao, Wu-zhong Guo","submitted_at":"2014-11-20T15:47:19Z","abstract_excerpt":"The holographic entanglement entropy for the most general higher derivative gravity is investigated. We find a new type of Wald entropy, which appears on entangling surface without the rotational symmetry and reduces to usual Wald entropy on Killing horizon. Furthermore, we obtain a formal formula of HEE for the most general higher derivative gravity and work it out exactly for some squashed cones. As an important application, we derive HEE for gravitational action with one derivative of the curvature when the extrinsic curvature vanishes. We also study some toy models with non-zero extrinsic "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.5579","kind":"arxiv","version":6},"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":"1411.5579","created_at":"2026-05-18T01:35:38.308413+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.5579v6","created_at":"2026-05-18T01:35:38.308413+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.5579","created_at":"2026-05-18T01:35:38.308413+00:00"},{"alias_kind":"pith_short_12","alias_value":"QR2SEZXO5BD2","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"QR2SEZXO5BD2LZKF","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"QR2SEZXO","created_at":"2026-05-18T12:28:46.137349+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1905.08762","citing_title":"The entropy of bulk quantum fields and the entanglement wedge of an evaporating black hole","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2","json":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2.json","graph_json":"https://pith.science/api/pith-number/QR2SEZXO5BD2LZKFWBL7MDLFE2/graph.json","events_json":"https://pith.science/api/pith-number/QR2SEZXO5BD2LZKFWBL7MDLFE2/events.json","paper":"https://pith.science/paper/QR2SEZXO"},"agent_actions":{"view_html":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2","download_json":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2.json","view_paper":"https://pith.science/paper/QR2SEZXO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.5579&json=true","fetch_graph":"https://pith.science/api/pith-number/QR2SEZXO5BD2LZKFWBL7MDLFE2/graph.json","fetch_events":"https://pith.science/api/pith-number/QR2SEZXO5BD2LZKFWBL7MDLFE2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2/action/storage_attestation","attest_author":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2/action/author_attestation","sign_citation":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2/action/citation_signature","submit_replication":"https://pith.science/pith/QR2SEZXO5BD2LZKFWBL7MDLFE2/action/replication_record"}},"created_at":"2026-05-18T01:35:38.308413+00:00","updated_at":"2026-05-18T01:35:38.308413+00:00"}