{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:VYSIIAZX3FZO2MFYQXBBMKVEMS","short_pith_number":"pith:VYSIIAZX","schema_version":"1.0","canonical_sha256":"ae24840337d972ed30b885c2162aa464bda9684e9dc1da972ad2a9d9498aa31e","source":{"kind":"arxiv","id":"1607.05972","version":2},"attestation_state":"computed","paper":{"title":"Some features of a Schwarzchild Black Hole from a Snyder perspective","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"Carlos Leiva","submitted_at":"2016-07-11T16:53:14Z","abstract_excerpt":"In this paper, the consequences of introducing a deformed Snyder-Kepler potential in the Schwarzchild metric are investigated. After this modification, it is obtained a dynamically depending horizon with different penetration radius for massive particles and light rays in radial orbits. In the case of circular orbits, they all remain untouched."},"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":"1607.05972","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2016-07-11T16:53:14Z","cross_cats_sorted":[],"title_canon_sha256":"aa1e47e75803af04d82cf0f69bc9bb88dcc1488b7e3f82873d6ef1c968d25a83","abstract_canon_sha256":"9915d244f28d9262986008c5514fa51e24613bc00fe4cb4632e384915f812096"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:46.900830Z","signature_b64":"U9pMzcP4/Qexx6ZW0BMbLydcVz+AHPM42cjfYe3OmfqbdqrP6Vfq9JN3zFXv3QJrCmUDfbxtSMqSzMhThPTmBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ae24840337d972ed30b885c2162aa464bda9684e9dc1da972ad2a9d9498aa31e","last_reissued_at":"2026-05-18T00:49:46.900158Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:46.900158Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Some features of a Schwarzchild Black Hole from a Snyder perspective","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"Carlos Leiva","submitted_at":"2016-07-11T16:53:14Z","abstract_excerpt":"In this paper, the consequences of introducing a deformed Snyder-Kepler potential in the Schwarzchild metric are investigated. After this modification, it is obtained a dynamically depending horizon with different penetration radius for massive particles and light rays in radial orbits. In the case of circular orbits, they all remain untouched."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.05972","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":""},"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":"1607.05972","created_at":"2026-05-18T00:49:46.900219+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.05972v2","created_at":"2026-05-18T00:49:46.900219+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.05972","created_at":"2026-05-18T00:49:46.900219+00:00"},{"alias_kind":"pith_short_12","alias_value":"VYSIIAZX3FZO","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_16","alias_value":"VYSIIAZX3FZO2MFY","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_8","alias_value":"VYSIIAZX","created_at":"2026-05-18T12:30:48.956258+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/VYSIIAZX3FZO2MFYQXBBMKVEMS","json":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS.json","graph_json":"https://pith.science/api/pith-number/VYSIIAZX3FZO2MFYQXBBMKVEMS/graph.json","events_json":"https://pith.science/api/pith-number/VYSIIAZX3FZO2MFYQXBBMKVEMS/events.json","paper":"https://pith.science/paper/VYSIIAZX"},"agent_actions":{"view_html":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS","download_json":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS.json","view_paper":"https://pith.science/paper/VYSIIAZX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.05972&json=true","fetch_graph":"https://pith.science/api/pith-number/VYSIIAZX3FZO2MFYQXBBMKVEMS/graph.json","fetch_events":"https://pith.science/api/pith-number/VYSIIAZX3FZO2MFYQXBBMKVEMS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS/action/storage_attestation","attest_author":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS/action/author_attestation","sign_citation":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS/action/citation_signature","submit_replication":"https://pith.science/pith/VYSIIAZX3FZO2MFYQXBBMKVEMS/action/replication_record"}},"created_at":"2026-05-18T00:49:46.900219+00:00","updated_at":"2026-05-18T00:49:46.900219+00:00"}