{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:BYBQRGVTJODYYA5LQUH6GJLHUF","short_pith_number":"pith:BYBQRGVT","schema_version":"1.0","canonical_sha256":"0e03089ab34b878c03ab850fe32567a151e56d10f2b11780a60fed6ce4be804d","source":{"kind":"arxiv","id":"2504.00084","version":2},"attestation_state":"computed","paper":{"title":"Quasinormal modes and excitation factors of Kerr black holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Leart Sabani, Rico K. L. Lo, Vitor Cardoso","submitted_at":"2025-03-31T18:00:01Z","abstract_excerpt":"Theoretical understanding of the characteristic oscillations of a perturbed black hole, also referred to as quasinormal modes (QNMs), is crucial to interpreting the late stage of binary black hole mergers that we now routinely observe in gravitational wave detectors. In this work, we introduce a new approach, based on the generalized Sasaki-Nakamura formalism, to compute the QNM spectra and their excitation factors (QNEFs), for scalar, electromagnetic and gravitational perturbations. Using this approach, QNM wavefunctions remain finite at the horizon and spatial infinity. Our results in genera"},"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":"2504.00084","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2025-03-31T18:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"4b9f714246aac889f14468a8204e6a78bc00e019a2427a5a90a3c2e6a2d070cb","abstract_canon_sha256":"ebaa113775d3ca4ba5c3d1a2e31a84d30a76adab62ad0b2d11ad33ee7e25627c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:15:45.871040Z","signature_b64":"sLCICOxk8hFmsPvd0btFmx6f5YfzQtRu2Ceo/dkcYITME5XsbB0MVNXjaW4r+6UslX8RjcAuwCTvIZwTOz/kCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e03089ab34b878c03ab850fe32567a151e56d10f2b11780a60fed6ce4be804d","last_reissued_at":"2026-07-05T11:15:45.870550Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:15:45.870550Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quasinormal modes and excitation factors of Kerr black holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Leart Sabani, Rico K. L. Lo, Vitor Cardoso","submitted_at":"2025-03-31T18:00:01Z","abstract_excerpt":"Theoretical understanding of the characteristic oscillations of a perturbed black hole, also referred to as quasinormal modes (QNMs), is crucial to interpreting the late stage of binary black hole mergers that we now routinely observe in gravitational wave detectors. In this work, we introduce a new approach, based on the generalized Sasaki-Nakamura formalism, to compute the QNM spectra and their excitation factors (QNEFs), for scalar, electromagnetic and gravitational perturbations. Using this approach, QNM wavefunctions remain finite at the horizon and spatial infinity. Our results in genera"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.00084","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/2504.00084/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":"2504.00084","created_at":"2026-07-05T11:15:45.870609+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.00084v2","created_at":"2026-07-05T11:15:45.870609+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.00084","created_at":"2026-07-05T11:15:45.870609+00:00"},{"alias_kind":"pith_short_12","alias_value":"BYBQRGVTJODY","created_at":"2026-07-05T11:15:45.870609+00:00"},{"alias_kind":"pith_short_16","alias_value":"BYBQRGVTJODYYA5L","created_at":"2026-07-05T11:15:45.870609+00:00"},{"alias_kind":"pith_short_8","alias_value":"BYBQRGVT","created_at":"2026-07-05T11:15:45.870609+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":8,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.13217","citing_title":"Absorption cross section of a Schwarzschild black hole for a massive vector field","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02146","citing_title":"Spectral suppression of black hole ringdown tails","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2605.24704","citing_title":"Shaping black hole resonances I. Black hole ringdown as a spectral filtering process","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2512.02110","citing_title":"Exceptional Points and Resonance in Black Hole Ringdown","ref_index":24,"is_internal_anchor":false},{"citing_arxiv_id":"2605.17840","citing_title":"Pole Skipping, Avoided Crossing, and Resonant Excitation in Kerr Quasinormal Modes near Algebraically Special Frequencies","ref_index":67,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16199","citing_title":"Detectability of avoided crossings in black hole ringdowns","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2605.17840","citing_title":"Pole Skipping, Avoided Crossing, and Resonant Excitation in Kerr Quasinormal Modes near Algebraically Special Frequencies","ref_index":67,"is_internal_anchor":false},{"citing_arxiv_id":"2505.23895","citing_title":"Black hole spectroscopy: from theory to experiment","ref_index":89,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF","json":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF.json","graph_json":"https://pith.science/api/pith-number/BYBQRGVTJODYYA5LQUH6GJLHUF/graph.json","events_json":"https://pith.science/api/pith-number/BYBQRGVTJODYYA5LQUH6GJLHUF/events.json","paper":"https://pith.science/paper/BYBQRGVT"},"agent_actions":{"view_html":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF","download_json":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF.json","view_paper":"https://pith.science/paper/BYBQRGVT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.00084&json=true","fetch_graph":"https://pith.science/api/pith-number/BYBQRGVTJODYYA5LQUH6GJLHUF/graph.json","fetch_events":"https://pith.science/api/pith-number/BYBQRGVTJODYYA5LQUH6GJLHUF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF/action/storage_attestation","attest_author":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF/action/author_attestation","sign_citation":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF/action/citation_signature","submit_replication":"https://pith.science/pith/BYBQRGVTJODYYA5LQUH6GJLHUF/action/replication_record"}},"created_at":"2026-07-05T11:15:45.870609+00:00","updated_at":"2026-07-05T11:15:45.870609+00:00"}