{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:UEME73QIGLF6T2NYLG5F2ASYXG","short_pith_number":"pith:UEME73QI","canonical_record":{"source":{"id":"1810.08037","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-09-28T11:20:25Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"edc304beeed07eca98f0305d2bace16bf2a354e377458dd264415c81f5729c89","abstract_canon_sha256":"99cd90f79d8079d05c9d930276964d1fbe27e377c2984b6334496cab588e7fe3"},"schema_version":"1.0"},"canonical_sha256":"a1184fee0832cbe9e9b859ba5d0258b9ac961e32a2e7702d74e3a3bee7d537a7","source":{"kind":"arxiv","id":"1810.08037","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.08037","created_at":"2026-05-17T23:59:32Z"},{"alias_kind":"arxiv_version","alias_value":"1810.08037v1","created_at":"2026-05-17T23:59:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.08037","created_at":"2026-05-17T23:59:32Z"},{"alias_kind":"pith_short_12","alias_value":"UEME73QIGLF6","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"UEME73QIGLF6T2NY","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"UEME73QI","created_at":"2026-05-18T12:32:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:UEME73QIGLF6T2NYLG5F2ASYXG","target":"record","payload":{"canonical_record":{"source":{"id":"1810.08037","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-09-28T11:20:25Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"edc304beeed07eca98f0305d2bace16bf2a354e377458dd264415c81f5729c89","abstract_canon_sha256":"99cd90f79d8079d05c9d930276964d1fbe27e377c2984b6334496cab588e7fe3"},"schema_version":"1.0"},"canonical_sha256":"a1184fee0832cbe9e9b859ba5d0258b9ac961e32a2e7702d74e3a3bee7d537a7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:32.120773Z","signature_b64":"jYVuSL5bAbxUsaig3x1rV7dCPKaMNkDfDPfRWtbmwnZn69j5Yf6ASXWhSEnhCnDfR5U7xakGTEgV4octkeCACA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a1184fee0832cbe9e9b859ba5d0258b9ac961e32a2e7702d74e3a3bee7d537a7","last_reissued_at":"2026-05-17T23:59:32.120091Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:32.120091Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1810.08037","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:59:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rvr75WOjjBIzlc7V2GMNbHDwT9amLIAyRBKdz/hgTJkKfb59IF+RUG9rPU8CFl5Ihtlzagv7h/SEAN06SBoUDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T00:28:09.237783Z"},"content_sha256":"494ecfc46f65fb4ace4cd45892836f3382d196b42b0dc0cd7a2c86a6951fe39f","schema_version":"1.0","event_id":"sha256:494ecfc46f65fb4ace4cd45892836f3382d196b42b0dc0cd7a2c86a6951fe39f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:UEME73QIGLF6T2NYLG5F2ASYXG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Holographic entanglement thermodynamics for higher dimensional charged black hole","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Debabrata Ghorai, Sourav Karar, Sunandan Gangopadhyay","submitted_at":"2018-09-28T11:20:25Z","abstract_excerpt":"In this paper, we have investigated the entanglement thermodynamics for $d$-dimensional charged $AdS$ black hole by studying the holographic entanglement entropy in different cases. We have first computed the holographic entanglement entropy in extremal and non-extremal cases in two different regimes, namely, the low temperature and high temperature limits. We then obtain the first law of entanglement thermodynamics for boundary field theory in the low temperature regime in $d$-dimensions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.08037","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:59:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IOnSd2BQp2zETq1//hsxeEUzDdrFWkLwEwyQkwNdx4ANJyHFJWDiiFjjr8cnP9q5yP3+6fNHI8A/sjXHMcPeDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T00:28:09.238447Z"},"content_sha256":"7c51bff1088fc0d02f8181174d162fe6dbc745df6a508b4bde5bb0a1875ee14b","schema_version":"1.0","event_id":"sha256:7c51bff1088fc0d02f8181174d162fe6dbc745df6a508b4bde5bb0a1875ee14b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UEME73QIGLF6T2NYLG5F2ASYXG/bundle.json","state_url":"https://pith.science/pith/UEME73QIGLF6T2NYLG5F2ASYXG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UEME73QIGLF6T2NYLG5F2ASYXG/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":"2026-05-30T00:28:09Z","links":{"resolver":"https://pith.science/pith/UEME73QIGLF6T2NYLG5F2ASYXG","bundle":"https://pith.science/pith/UEME73QIGLF6T2NYLG5F2ASYXG/bundle.json","state":"https://pith.science/pith/UEME73QIGLF6T2NYLG5F2ASYXG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UEME73QIGLF6T2NYLG5F2ASYXG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:UEME73QIGLF6T2NYLG5F2ASYXG","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":"99cd90f79d8079d05c9d930276964d1fbe27e377c2984b6334496cab588e7fe3","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-09-28T11:20:25Z","title_canon_sha256":"edc304beeed07eca98f0305d2bace16bf2a354e377458dd264415c81f5729c89"},"schema_version":"1.0","source":{"id":"1810.08037","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.08037","created_at":"2026-05-17T23:59:32Z"},{"alias_kind":"arxiv_version","alias_value":"1810.08037v1","created_at":"2026-05-17T23:59:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.08037","created_at":"2026-05-17T23:59:32Z"},{"alias_kind":"pith_short_12","alias_value":"UEME73QIGLF6","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"UEME73QIGLF6T2NY","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"UEME73QI","created_at":"2026-05-18T12:32:56Z"}],"graph_snapshots":[{"event_id":"sha256:7c51bff1088fc0d02f8181174d162fe6dbc745df6a508b4bde5bb0a1875ee14b","target":"graph","created_at":"2026-05-17T23:59:32Z","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":"In this paper, we have investigated the entanglement thermodynamics for $d$-dimensional charged $AdS$ black hole by studying the holographic entanglement entropy in different cases. We have first computed the holographic entanglement entropy in extremal and non-extremal cases in two different regimes, namely, the low temperature and high temperature limits. We then obtain the first law of entanglement thermodynamics for boundary field theory in the low temperature regime in $d$-dimensions.","authors_text":"Debabrata Ghorai, Sourav Karar, Sunandan Gangopadhyay","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-09-28T11:20:25Z","title":"Holographic entanglement thermodynamics for higher dimensional charged black hole"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.08037","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":"sha256:494ecfc46f65fb4ace4cd45892836f3382d196b42b0dc0cd7a2c86a6951fe39f","target":"record","created_at":"2026-05-17T23:59:32Z","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":"99cd90f79d8079d05c9d930276964d1fbe27e377c2984b6334496cab588e7fe3","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-09-28T11:20:25Z","title_canon_sha256":"edc304beeed07eca98f0305d2bace16bf2a354e377458dd264415c81f5729c89"},"schema_version":"1.0","source":{"id":"1810.08037","kind":"arxiv","version":1}},"canonical_sha256":"a1184fee0832cbe9e9b859ba5d0258b9ac961e32a2e7702d74e3a3bee7d537a7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a1184fee0832cbe9e9b859ba5d0258b9ac961e32a2e7702d74e3a3bee7d537a7","first_computed_at":"2026-05-17T23:59:32.120091Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:32.120091Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jYVuSL5bAbxUsaig3x1rV7dCPKaMNkDfDPfRWtbmwnZn69j5Yf6ASXWhSEnhCnDfR5U7xakGTEgV4octkeCACA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:32.120773Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.08037","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:494ecfc46f65fb4ace4cd45892836f3382d196b42b0dc0cd7a2c86a6951fe39f","sha256:7c51bff1088fc0d02f8181174d162fe6dbc745df6a508b4bde5bb0a1875ee14b"],"state_sha256":"d8a9887f6994155e082565b0bf9549d4c721e931119f59d4bcc0811a0a3aa7ad"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AnFqeQ/Qi/cHtcGNoHMFI0iPMrcwgxJQI+KrqGx8OqdvyOuIgPKIqchfhtcl/Z81dUuXGxCW6t4F/xS0S1uYCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T00:28:09.241838Z","bundle_sha256":"d5d7a9dae99022b22acadf4b6a2d2f01df6e975ebb33d977a3bec5eba3d1c2c5"}}