{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2020:GOZ2QKV37C7Q5TWL5UBV2WSIEK","short_pith_number":"pith:GOZ2QKV3","canonical_record":{"source":{"id":"2002.05029","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2020-02-12T14:37:55Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"24dc105983eb408929fa78ad92e202499169e2a9772f6bee4feabb051eef670b","abstract_canon_sha256":"2b0d06355f54ab456aadff48c1c30e4c53bf439595c8de28c7b96edaa62663fa"},"schema_version":"1.0"},"canonical_sha256":"33b3a82abbf8bf0ececbed035d5a4822a47d9507e67fd97ca077302d5b88f331","source":{"kind":"arxiv","id":"2002.05029","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2002.05029","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"arxiv_version","alias_value":"2002.05029v1","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.05029","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"pith_short_12","alias_value":"GOZ2QKV37C7Q","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"pith_short_16","alias_value":"GOZ2QKV37C7Q5TWL","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"pith_short_8","alias_value":"GOZ2QKV3","created_at":"2026-07-05T00:55:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2020:GOZ2QKV37C7Q5TWL5UBV2WSIEK","target":"record","payload":{"canonical_record":{"source":{"id":"2002.05029","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2020-02-12T14:37:55Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"24dc105983eb408929fa78ad92e202499169e2a9772f6bee4feabb051eef670b","abstract_canon_sha256":"2b0d06355f54ab456aadff48c1c30e4c53bf439595c8de28c7b96edaa62663fa"},"schema_version":"1.0"},"canonical_sha256":"33b3a82abbf8bf0ececbed035d5a4822a47d9507e67fd97ca077302d5b88f331","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:55:10.040757Z","signature_b64":"sBtudaSSu06jB4q01nZMpRjvKijmZ8HW+nrBgv36oaXkL4u7UaMpv7CFTC7ChVzfs3jH4AP+RGEQBW/TzGjyBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"33b3a82abbf8bf0ececbed035d5a4822a47d9507e67fd97ca077302d5b88f331","last_reissued_at":"2026-07-05T00:55:10.040348Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:55:10.040348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2002.05029","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":"2026-07-05T00:55:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CWTIx8j+wM8E/fi3+YVLzQVO/E+hDtgpO0D0DSkb64r7y1GubMcTo03ilqb1102ZnmwiZRqVIVoqle3phh9IAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:48:16.973359Z"},"content_sha256":"9627ba69171ee6b1bfe63941c4098e88797e4da86b9f54e77ddb8318528b0638","schema_version":"1.0","event_id":"sha256:9627ba69171ee6b1bfe63941c4098e88797e4da86b9f54e77ddb8318528b0638"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2020:GOZ2QKV37C7Q5TWL5UBV2WSIEK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Entropy in general relativity: Kerr-AdS black hole","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Branislav Cvetkovi\\'c, Milutin Blagojevi\\'c","submitted_at":"2020-02-12T14:37:55Z","abstract_excerpt":"A general Hamiltonian approach to black hole thermodynamics is used to study entropy and conserved charges for Kerr-AdS solutions in general relativity. These thermodynamic variables are first consistently defined by choosing suitable boundary conditions, and then, they are shown to satisfy the first law of black hole dynamics"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.05029","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2002.05029/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T00:55:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oLLBeH/sWO8UrSNQMPLb4CcTnhMcdPEMNwY/Xi9klZBTtHoobkN7vPkFliQnUC5nFeiXGm64vYTqJOmpd53PCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:48:16.974317Z"},"content_sha256":"c0f81396ebf2de2cd1c1c7e71f141a236edd2316b15fba6c8b6f6a760dcc47fe","schema_version":"1.0","event_id":"sha256:c0f81396ebf2de2cd1c1c7e71f141a236edd2316b15fba6c8b6f6a760dcc47fe"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GOZ2QKV37C7Q5TWL5UBV2WSIEK/bundle.json","state_url":"https://pith.science/pith/GOZ2QKV37C7Q5TWL5UBV2WSIEK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GOZ2QKV37C7Q5TWL5UBV2WSIEK/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":"2026-08-11T10:48:16Z","links":{"resolver":"https://pith.science/pith/GOZ2QKV37C7Q5TWL5UBV2WSIEK","bundle":"https://pith.science/pith/GOZ2QKV37C7Q5TWL5UBV2WSIEK/bundle.json","state":"https://pith.science/pith/GOZ2QKV37C7Q5TWL5UBV2WSIEK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GOZ2QKV37C7Q5TWL5UBV2WSIEK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:GOZ2QKV37C7Q5TWL5UBV2WSIEK","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":"2b0d06355f54ab456aadff48c1c30e4c53bf439595c8de28c7b96edaa62663fa","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2020-02-12T14:37:55Z","title_canon_sha256":"24dc105983eb408929fa78ad92e202499169e2a9772f6bee4feabb051eef670b"},"schema_version":"1.0","source":{"id":"2002.05029","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2002.05029","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"arxiv_version","alias_value":"2002.05029v1","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.05029","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"pith_short_12","alias_value":"GOZ2QKV37C7Q","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"pith_short_16","alias_value":"GOZ2QKV37C7Q5TWL","created_at":"2026-07-05T00:55:10Z"},{"alias_kind":"pith_short_8","alias_value":"GOZ2QKV3","created_at":"2026-07-05T00:55:10Z"}],"graph_snapshots":[{"event_id":"sha256:c0f81396ebf2de2cd1c1c7e71f141a236edd2316b15fba6c8b6f6a760dcc47fe","target":"graph","created_at":"2026-07-05T00:55:10Z","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":[],"endpoint":"/pith/2002.05029/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A general Hamiltonian approach to black hole thermodynamics is used to study entropy and conserved charges for Kerr-AdS solutions in general relativity. These thermodynamic variables are first consistently defined by choosing suitable boundary conditions, and then, they are shown to satisfy the first law of black hole dynamics","authors_text":"Branislav Cvetkovi\\'c, Milutin Blagojevi\\'c","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2020-02-12T14:37:55Z","title":"Entropy in general relativity: Kerr-AdS black hole"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.05029","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":"sha256:9627ba69171ee6b1bfe63941c4098e88797e4da86b9f54e77ddb8318528b0638","target":"record","created_at":"2026-07-05T00:55:10Z","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":"2b0d06355f54ab456aadff48c1c30e4c53bf439595c8de28c7b96edaa62663fa","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2020-02-12T14:37:55Z","title_canon_sha256":"24dc105983eb408929fa78ad92e202499169e2a9772f6bee4feabb051eef670b"},"schema_version":"1.0","source":{"id":"2002.05029","kind":"arxiv","version":1}},"canonical_sha256":"33b3a82abbf8bf0ececbed035d5a4822a47d9507e67fd97ca077302d5b88f331","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"33b3a82abbf8bf0ececbed035d5a4822a47d9507e67fd97ca077302d5b88f331","first_computed_at":"2026-07-05T00:55:10.040348Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:55:10.040348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sBtudaSSu06jB4q01nZMpRjvKijmZ8HW+nrBgv36oaXkL4u7UaMpv7CFTC7ChVzfs3jH4AP+RGEQBW/TzGjyBA==","signature_status":"signed_v1","signed_at":"2026-07-05T00:55:10.040757Z","signed_message":"canonical_sha256_bytes"},"source_id":"2002.05029","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9627ba69171ee6b1bfe63941c4098e88797e4da86b9f54e77ddb8318528b0638","sha256:c0f81396ebf2de2cd1c1c7e71f141a236edd2316b15fba6c8b6f6a760dcc47fe"],"state_sha256":"f473e9ecf8b0580065f005a7fbf18835b3ce728b4f147eeba135fbbd7c8d5712"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WtNW4xYKOuzqs3CWgPT4JdI3bZpsVycrwiA+ED2Y4CkFdptLaS0kaFNC6JU7okFTUtyFLm7KtrmXpmJkRI5DCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T10:48:16.989597Z","bundle_sha256":"a5172729b1719314f56b6d5f61b6e74643ff5aff8f8e5c76b66ae17cba460e4e"}}