{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:DSCAPKK5BCKBI2AM4UMZYQ7CP3","short_pith_number":"pith:DSCAPKK5","schema_version":"1.0","canonical_sha256":"1c8407a95d089414680ce5199c43e27ecf7eb6cc86c929b80af56d2f28c147cb","source":{"kind":"arxiv","id":"2401.00703","version":3},"attestation_state":"computed","paper":{"title":"Exploring Ladder Symmetry and Love Numbers for Static and Rotating Black Holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Chanchal Sharma, Rajes Ghosh, Sudipta Sarkar","submitted_at":"2024-01-01T09:08:22Z","abstract_excerpt":"Black hole solutions of general relativity exhibit a symmetry for the static perturbations around these spacetimes, known as \"ladder symmetry\". This symmetry proves useful in constructing a tower of solutions for perturbations and elucidating their general properties. Specifically, the presence of this symmetry leads to vanishing of the tidal love number associated with black holes. In this work, we find the most general spherical symmetric and static black hole spacetime that accommodates this ladder symmetry for scalar perturbation. Furthermore, we extend our calculations beyond spherical sy"},"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":"2401.00703","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2024-01-01T09:08:22Z","cross_cats_sorted":[],"title_canon_sha256":"ba674aa771a80cbe123e2270ad6ab554cde2520def5481c8c0a9e01de59d0676","abstract_canon_sha256":"4fcf841311f489a940700847788c63b9effc6f2f929ceabfbd78ffc0028393b6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:31:10.244293Z","signature_b64":"Og1UUtuE/akky8L2E5k/Nf+2osoLL+XQ0Ux+uCZJtP60hrVBs9RuCmgcZjIr/Pgq2QcO251m4wYAlAz9K3rMAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c8407a95d089414680ce5199c43e27ecf7eb6cc86c929b80af56d2f28c147cb","last_reissued_at":"2026-07-05T08:31:10.243713Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:31:10.243713Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploring Ladder Symmetry and Love Numbers for Static and Rotating Black Holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Chanchal Sharma, Rajes Ghosh, Sudipta Sarkar","submitted_at":"2024-01-01T09:08:22Z","abstract_excerpt":"Black hole solutions of general relativity exhibit a symmetry for the static perturbations around these spacetimes, known as \"ladder symmetry\". This symmetry proves useful in constructing a tower of solutions for perturbations and elucidating their general properties. Specifically, the presence of this symmetry leads to vanishing of the tidal love number associated with black holes. In this work, we find the most general spherical symmetric and static black hole spacetime that accommodates this ladder symmetry for scalar perturbation. Furthermore, we extend our calculations beyond spherical sy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.00703","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2401.00703/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":"2401.00703","created_at":"2026-07-05T08:31:10.243781+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.00703v3","created_at":"2026-07-05T08:31:10.243781+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.00703","created_at":"2026-07-05T08:31:10.243781+00:00"},{"alias_kind":"pith_short_12","alias_value":"DSCAPKK5BCKB","created_at":"2026-07-05T08:31:10.243781+00:00"},{"alias_kind":"pith_short_16","alias_value":"DSCAPKK5BCKBI2AM","created_at":"2026-07-05T08:31:10.243781+00:00"},{"alias_kind":"pith_short_8","alias_value":"DSCAPKK5","created_at":"2026-07-05T08:31:10.243781+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.24365","citing_title":"Fermionic Love number of higher-dimensional Reissner-Nordstr\\\"om black holes","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2606.19281","citing_title":"Universal Closed Form for Dynamical Love Numbers of Black Holes","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2510.10036","citing_title":"Fermionic Love number of Reissner-Nordstr\\\"om black holes","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2511.12580","citing_title":"Dynamical Tidal Response of Non-rotating Black Holes: Connecting the MST Formalism and Worldline EFT","ref_index":98,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00693","citing_title":"Dynamical tidal Love numbers of black holes under generic perturbations: Connecting black hole perturbation theory with effective field theory","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2604.06249","citing_title":"Universal Ladder Structure Across Scales: From Quantum to Black Hole Physics","ref_index":31,"is_internal_anchor":false},{"citing_arxiv_id":"2605.02633","citing_title":"Axial tidal Love numbers of black holes in matter environments","ref_index":38,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3","json":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3.json","graph_json":"https://pith.science/api/pith-number/DSCAPKK5BCKBI2AM4UMZYQ7CP3/graph.json","events_json":"https://pith.science/api/pith-number/DSCAPKK5BCKBI2AM4UMZYQ7CP3/events.json","paper":"https://pith.science/paper/DSCAPKK5"},"agent_actions":{"view_html":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3","download_json":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3.json","view_paper":"https://pith.science/paper/DSCAPKK5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.00703&json=true","fetch_graph":"https://pith.science/api/pith-number/DSCAPKK5BCKBI2AM4UMZYQ7CP3/graph.json","fetch_events":"https://pith.science/api/pith-number/DSCAPKK5BCKBI2AM4UMZYQ7CP3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3/action/storage_attestation","attest_author":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3/action/author_attestation","sign_citation":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3/action/citation_signature","submit_replication":"https://pith.science/pith/DSCAPKK5BCKBI2AM4UMZYQ7CP3/action/replication_record"}},"created_at":"2026-07-05T08:31:10.243781+00:00","updated_at":"2026-07-05T08:31:10.243781+00:00"}