{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:HBMDCC4VAMAIKLREE7VPMZUQ2G","short_pith_number":"pith:HBMDCC4V","schema_version":"1.0","canonical_sha256":"3858310b950300852e2427eaf66690d186a2df3c14bd32ec0b6ed5e4838c6b0a","source":{"kind":"arxiv","id":"hep-th/0104157","version":1},"attestation_state":"computed","paper":{"title":"Late-time Evolution of a Charged Massless Scalar Field in the Spacetime of a Dilaton Black Hole","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Marek Rogatko (Tech.Un.of Lublin), Rafal Moderski (CAMK)","submitted_at":"2001-04-18T15:15:50Z","abstract_excerpt":"We investigate the power-law tails in the evolution of a charged massless scalar field around a fixed background of a dilaton black hole. Using both analytical and numerical methods we find the inverse power-law relaxation of charged fields at future timelike infinity, future null infinity, and along the outer horizon of the considered black hole. We invisage that a charged hair decays slower than neutral ones. The oscillatory inverse power law along the outer horizon of the dilaton black hole is of a great importance for a mass inflation scenario along the Cauchy horizon of a dynamically form"},"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":"hep-th/0104157","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-04-18T15:15:50Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"35a88e5a3fdcbaa96bae72965bf503a82bf8e198b53fac0e931afdad87d51793","abstract_canon_sha256":"a19d66aa367f5bafb0a88cead8f6293a2176447556d9ebb2bd588e4b02b1efe0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:50.587739Z","signature_b64":"uuvv1pGsvuN+603mdBnGSGHHG/DH8MY0WVeOlSDkc8WT+CPyDRUNpp2PoiCKfMudjupdTWM+zDQRi44haGGMCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3858310b950300852e2427eaf66690d186a2df3c14bd32ec0b6ed5e4838c6b0a","last_reissued_at":"2026-07-04T16:27:50.587400Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:50.587400Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Late-time Evolution of a Charged Massless Scalar Field in the Spacetime of a Dilaton Black Hole","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Marek Rogatko (Tech.Un.of Lublin), Rafal Moderski (CAMK)","submitted_at":"2001-04-18T15:15:50Z","abstract_excerpt":"We investigate the power-law tails in the evolution of a charged massless scalar field around a fixed background of a dilaton black hole. Using both analytical and numerical methods we find the inverse power-law relaxation of charged fields at future timelike infinity, future null infinity, and along the outer horizon of the considered black hole. We invisage that a charged hair decays slower than neutral ones. The oscillatory inverse power law along the outer horizon of the dilaton black hole is of a great importance for a mass inflation scenario along the Cauchy horizon of a dynamically form"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0104157","kind":"arxiv","version":1},"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/hep-th/0104157/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":"hep-th/0104157","created_at":"2026-07-04T16:27:50.587460+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0104157v1","created_at":"2026-07-04T16:27:50.587460+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0104157","created_at":"2026-07-04T16:27:50.587460+00:00"},{"alias_kind":"pith_short_12","alias_value":"HBMDCC4VAMAI","created_at":"2026-07-04T16:27:50.587460+00:00"},{"alias_kind":"pith_short_16","alias_value":"HBMDCC4VAMAIKLRE","created_at":"2026-07-04T16:27:50.587460+00:00"},{"alias_kind":"pith_short_8","alias_value":"HBMDCC4V","created_at":"2026-07-04T16:27:50.587460+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/HBMDCC4VAMAIKLREE7VPMZUQ2G","json":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G.json","graph_json":"https://pith.science/api/pith-number/HBMDCC4VAMAIKLREE7VPMZUQ2G/graph.json","events_json":"https://pith.science/api/pith-number/HBMDCC4VAMAIKLREE7VPMZUQ2G/events.json","paper":"https://pith.science/paper/HBMDCC4V"},"agent_actions":{"view_html":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G","download_json":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G.json","view_paper":"https://pith.science/paper/HBMDCC4V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0104157&json=true","fetch_graph":"https://pith.science/api/pith-number/HBMDCC4VAMAIKLREE7VPMZUQ2G/graph.json","fetch_events":"https://pith.science/api/pith-number/HBMDCC4VAMAIKLREE7VPMZUQ2G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G/action/storage_attestation","attest_author":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G/action/author_attestation","sign_citation":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G/action/citation_signature","submit_replication":"https://pith.science/pith/HBMDCC4VAMAIKLREE7VPMZUQ2G/action/replication_record"}},"created_at":"2026-07-04T16:27:50.587460+00:00","updated_at":"2026-07-04T16:27:50.587460+00:00"}