{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:QH5I74NCHYRSV5CYA5LWSPWEPF","short_pith_number":"pith:QH5I74NC","schema_version":"1.0","canonical_sha256":"81fa8ff1a23e232af4580757693ec4795826991ebd88afeacee3760a6f9ca175","source":{"kind":"arxiv","id":"1310.1925","version":3},"attestation_state":"computed","paper":{"title":"Seed for general rotating non-extremal black holes of N=8 supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"David D. K. Chow, Geoffrey Comp\\`ere","submitted_at":"2013-10-07T20:00:04Z","abstract_excerpt":"We describe the most general asymptotically flat, stationary, non-extremal, dyonic black hole of the four-dimensional N = 2 supergravity coupled to 3 vector multiplets that describes the low-energy regime of the STU model. Under U-dualities, this can be used as a seed to generate all single-centered stationary black holes of N = 8 supergravity. The independent conserved charges are the mass, angular momentum, four electric charges and four magnetic charges; an independent NUT charge can also be added. Several aspects of the black hole are presented, including thermodynamics, the BPS limit, the"},"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":"1310.1925","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-07T20:00:04Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"a24bb3945d23b51602de6ce9eb290cb3b41bb9394a5a1f349e8ff5d27aa64127","abstract_canon_sha256":"199e987b285fe9e404817b5e68e60c30d0d8a0ff354706efaffe56cd87ef14c8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:04:06.244180Z","signature_b64":"7DS9sLcsIYZkhgl5UsiwRv/GoszvrRSY4aACK83Y7++z8U2SVvOuLSRieXAs2T7DkaZAYnDkk+0VJLb20wVtBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81fa8ff1a23e232af4580757693ec4795826991ebd88afeacee3760a6f9ca175","last_reissued_at":"2026-05-18T03:04:06.243697Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:04:06.243697Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Seed for general rotating non-extremal black holes of N=8 supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"David D. K. Chow, Geoffrey Comp\\`ere","submitted_at":"2013-10-07T20:00:04Z","abstract_excerpt":"We describe the most general asymptotically flat, stationary, non-extremal, dyonic black hole of the four-dimensional N = 2 supergravity coupled to 3 vector multiplets that describes the low-energy regime of the STU model. Under U-dualities, this can be used as a seed to generate all single-centered stationary black holes of N = 8 supergravity. The independent conserved charges are the mass, angular momentum, four electric charges and four magnetic charges; an independent NUT charge can also be added. Several aspects of the black hole are presented, including thermodynamics, the BPS limit, the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.1925","kind":"arxiv","version":3},"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":"1310.1925","created_at":"2026-05-18T03:04:06.243770+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.1925v3","created_at":"2026-05-18T03:04:06.243770+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.1925","created_at":"2026-05-18T03:04:06.243770+00:00"},{"alias_kind":"pith_short_12","alias_value":"QH5I74NCHYRS","created_at":"2026-05-18T12:27:57.521954+00:00"},{"alias_kind":"pith_short_16","alias_value":"QH5I74NCHYRSV5CY","created_at":"2026-05-18T12:27:57.521954+00:00"},{"alias_kind":"pith_short_8","alias_value":"QH5I74NC","created_at":"2026-05-18T12:27:57.521954+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.27093","citing_title":"Index saddle for the D1-D5-P black string and its decoupling limit","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF","json":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF.json","graph_json":"https://pith.science/api/pith-number/QH5I74NCHYRSV5CYA5LWSPWEPF/graph.json","events_json":"https://pith.science/api/pith-number/QH5I74NCHYRSV5CYA5LWSPWEPF/events.json","paper":"https://pith.science/paper/QH5I74NC"},"agent_actions":{"view_html":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF","download_json":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF.json","view_paper":"https://pith.science/paper/QH5I74NC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.1925&json=true","fetch_graph":"https://pith.science/api/pith-number/QH5I74NCHYRSV5CYA5LWSPWEPF/graph.json","fetch_events":"https://pith.science/api/pith-number/QH5I74NCHYRSV5CYA5LWSPWEPF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF/action/storage_attestation","attest_author":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF/action/author_attestation","sign_citation":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF/action/citation_signature","submit_replication":"https://pith.science/pith/QH5I74NCHYRSV5CYA5LWSPWEPF/action/replication_record"}},"created_at":"2026-05-18T03:04:06.243770+00:00","updated_at":"2026-05-18T03:04:06.243770+00:00"}