{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:FI25VZMEXES3DQQAWPGX5I3GUZ","short_pith_number":"pith:FI25VZME","schema_version":"1.0","canonical_sha256":"2a35dae584b925b1c200b3cd7ea366a6759e2003455382ac20d570be9f7e8881","source":{"kind":"arxiv","id":"gr-qc/9502029","version":2},"attestation_state":"computed","paper":{"title":"Critical Behavior of Dimensionally Continued Black Holes","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Dardo Piriz (UC Riverside), Javier P. Muniain","submitted_at":"1995-02-12T03:30:16Z","abstract_excerpt":"The critical behavior of black holes in even and odd dimensional spacetimes is studied based on Ba\\~nados-Teitelboim-Zanelli (BTZ) dimensionally continued black holes. In even dimensions it is found that asymptotically flat and anti de-Sitter Reissner-Nordstr\\\"om black holes present up to two second order phase transitions. The case of asymptotically anti-de-Sitter Schwarzschild black holes present only one critical transition and a minimum of temperature, which occurs at the transition. Finally, it is shown that phase transitions are absent in odd dimensions."},"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":"gr-qc/9502029","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"1995-02-12T03:30:16Z","cross_cats_sorted":[],"title_canon_sha256":"cadf3a6c47a6ecea4dad46f4c42bc2e803ea8889cd31d3636761404283337252","abstract_canon_sha256":"15c628d9bcbb5c61afed15d5e27048132c31d357c52c38595d99ab3e7ed17efb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:58:47.985791Z","signature_b64":"rAiGkOf0WT6R4S8/WNomljIyitLsHkiZWsl/YQlNlwmxbTrYiAu0gxexnv6/H+MNDgGcsqRtq+phpSECgPCJDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2a35dae584b925b1c200b3cd7ea366a6759e2003455382ac20d570be9f7e8881","last_reissued_at":"2026-07-04T15:58:47.985373Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:58:47.985373Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Critical Behavior of Dimensionally Continued Black Holes","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Dardo Piriz (UC Riverside), Javier P. Muniain","submitted_at":"1995-02-12T03:30:16Z","abstract_excerpt":"The critical behavior of black holes in even and odd dimensional spacetimes is studied based on Ba\\~nados-Teitelboim-Zanelli (BTZ) dimensionally continued black holes. In even dimensions it is found that asymptotically flat and anti de-Sitter Reissner-Nordstr\\\"om black holes present up to two second order phase transitions. The case of asymptotically anti-de-Sitter Schwarzschild black holes present only one critical transition and a minimum of temperature, which occurs at the transition. Finally, it is shown that phase transitions are absent in odd dimensions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/9502029","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/gr-qc/9502029/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"gr-qc/9502029","created_at":"2026-07-04T15:58:47.985449+00:00"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/9502029v2","created_at":"2026-07-04T15:58:47.985449+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/9502029","created_at":"2026-07-04T15:58:47.985449+00:00"},{"alias_kind":"pith_short_12","alias_value":"FI25VZMEXES3","created_at":"2026-07-04T15:58:47.985449+00:00"},{"alias_kind":"pith_short_16","alias_value":"FI25VZMEXES3DQQA","created_at":"2026-07-04T15:58:47.985449+00:00"},{"alias_kind":"pith_short_8","alias_value":"FI25VZME","created_at":"2026-07-04T15:58:47.985449+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.02643","citing_title":"An innovative black hole solution and thermodynamic properties in higher-order curvature gravity with a scalar field","ref_index":101,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ","json":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ.json","graph_json":"https://pith.science/api/pith-number/FI25VZMEXES3DQQAWPGX5I3GUZ/graph.json","events_json":"https://pith.science/api/pith-number/FI25VZMEXES3DQQAWPGX5I3GUZ/events.json","paper":"https://pith.science/paper/FI25VZME"},"agent_actions":{"view_html":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ","download_json":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ.json","view_paper":"https://pith.science/paper/FI25VZME","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=gr-qc/9502029&json=true","fetch_graph":"https://pith.science/api/pith-number/FI25VZMEXES3DQQAWPGX5I3GUZ/graph.json","fetch_events":"https://pith.science/api/pith-number/FI25VZMEXES3DQQAWPGX5I3GUZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ/action/storage_attestation","attest_author":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ/action/author_attestation","sign_citation":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ/action/citation_signature","submit_replication":"https://pith.science/pith/FI25VZMEXES3DQQAWPGX5I3GUZ/action/replication_record"}},"created_at":"2026-07-04T15:58:47.985449+00:00","updated_at":"2026-07-04T15:58:47.985449+00:00"}