{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:3EZMFHUPKDLRP4LTEEZG5H2GMU","short_pith_number":"pith:3EZMFHUP","schema_version":"1.0","canonical_sha256":"d932c29e8f50d717f17321326e9f46650223eb4a11a1c2304fe1640437557905","source":{"kind":"arxiv","id":"0912.3386","version":2},"attestation_state":"computed","paper":{"title":"On the Bekenstein-Hawking area law for black objects with conical singularities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Burkhard Kleihaus, Carlos Herdeiro, Eugen Radu, Jutta Kunz","submitted_at":"2009-12-17T12:33:30Z","abstract_excerpt":"We argue that, when working with the appropriate set of thermodynamical variables, the Bekenstein-Hawking law still holds for asymptotically flat black objects with conical singularities. The mass-energy which enters the first law of thermodynamics does not, however, coincide with the ADM mass; it differs from the latter by the energy associated with the conical singularity, as seen by an asymptotic, static observer. These statements are supported by a number of examples: the Bach-Weyl (double-Schwarzschild) solution, its dihole generalisation in Einstein-Maxwell theory and the five dimensiona"},"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":"0912.3386","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2009-12-17T12:33:30Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"9b84d813ee29b3d6a73dc95b81727a92282c326b68c0d6d2b8e6afae3946ec19","abstract_canon_sha256":"7133c2645bc6685770eaea612799e2622e5959c5dfca45607f3bf42df555b1f0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:56.413002Z","signature_b64":"4rQQpQUlFXnEFAHlxqiysIGzOo6RHcQEyCkcgpYZtXGb99QBi6EXegW7YSNevHEGo/wVcmxADPhDtE7y8kMbDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d932c29e8f50d717f17321326e9f46650223eb4a11a1c2304fe1640437557905","last_reissued_at":"2026-05-18T03:23:56.412344Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:56.412344Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the Bekenstein-Hawking area law for black objects with conical singularities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Burkhard Kleihaus, Carlos Herdeiro, Eugen Radu, Jutta Kunz","submitted_at":"2009-12-17T12:33:30Z","abstract_excerpt":"We argue that, when working with the appropriate set of thermodynamical variables, the Bekenstein-Hawking law still holds for asymptotically flat black objects with conical singularities. The mass-energy which enters the first law of thermodynamics does not, however, coincide with the ADM mass; it differs from the latter by the energy associated with the conical singularity, as seen by an asymptotic, static observer. These statements are supported by a number of examples: the Bach-Weyl (double-Schwarzschild) solution, its dihole generalisation in Einstein-Maxwell theory and the five dimensiona"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.3386","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0912.3386","created_at":"2026-05-18T03:23:56.412453+00:00"},{"alias_kind":"arxiv_version","alias_value":"0912.3386v2","created_at":"2026-05-18T03:23:56.412453+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0912.3386","created_at":"2026-05-18T03:23:56.412453+00:00"},{"alias_kind":"pith_short_12","alias_value":"3EZMFHUPKDLR","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_16","alias_value":"3EZMFHUPKDLRP4LT","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_8","alias_value":"3EZMFHUP","created_at":"2026-05-18T12:25:58.018023+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU","json":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU.json","graph_json":"https://pith.science/api/pith-number/3EZMFHUPKDLRP4LTEEZG5H2GMU/graph.json","events_json":"https://pith.science/api/pith-number/3EZMFHUPKDLRP4LTEEZG5H2GMU/events.json","paper":"https://pith.science/paper/3EZMFHUP"},"agent_actions":{"view_html":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU","download_json":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU.json","view_paper":"https://pith.science/paper/3EZMFHUP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0912.3386&json=true","fetch_graph":"https://pith.science/api/pith-number/3EZMFHUPKDLRP4LTEEZG5H2GMU/graph.json","fetch_events":"https://pith.science/api/pith-number/3EZMFHUPKDLRP4LTEEZG5H2GMU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU/action/storage_attestation","attest_author":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU/action/author_attestation","sign_citation":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU/action/citation_signature","submit_replication":"https://pith.science/pith/3EZMFHUPKDLRP4LTEEZG5H2GMU/action/replication_record"}},"created_at":"2026-05-18T03:23:56.412453+00:00","updated_at":"2026-05-18T03:23:56.412453+00:00"}