{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:GZSUGQF35PYE52C6KY4NGUREJX","short_pith_number":"pith:GZSUGQF3","schema_version":"1.0","canonical_sha256":"36654340bbebf04ee85e5638d352244dd7f5e26de36da35e0f6670cbaa6ec643","source":{"kind":"arxiv","id":"2509.01311","version":1},"attestation_state":"computed","paper":{"title":"Hadronic vacuum polarization effect in muonic atoms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th","quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"Moritz Thierfeld, Natalia S. Oreshkina, Zoia A. Mandrykina","submitted_at":"2025-09-01T09:50:42Z","abstract_excerpt":"The hadronic vacuum polarization (HVP) corrections to energy levels in muonic atoms are studied systematically across the periodic table. Two nuclear charge distribution models have been considered, with partly analytical solution for an homogeneously charged sphere model and direct numerical integration for a Fermi nuclear charge distribution. Our comparison reveals a good agreement between both approaches with differences typically below a few percent. The magnitude of HVP corrections increases with nuclear charge, displaying irregularities that correlate directly with the non-monotonic beha"},"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":"2509.01311","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-09-01T09:50:42Z","cross_cats_sorted":["nucl-th","quant-ph"],"title_canon_sha256":"60ad674d8032cdcb1b102ef68d18284efb2dd80c193bd535717c99243bf6c93f","abstract_canon_sha256":"15e3f63be5377898cf4fec81bb438370a59b1006852afd2e193a608476e372f2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:02:58.054406Z","signature_b64":"iuTt5EUlkJOhqMLLADCKYSLsFOWumcnP/xqPics0TAMnxoMBWZSfa16zkEOzUm/ld0kUKh9W1HyYEll87jcSAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"36654340bbebf04ee85e5638d352244dd7f5e26de36da35e0f6670cbaa6ec643","last_reissued_at":"2026-07-05T12:02:58.053823Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:02:58.053823Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hadronic vacuum polarization effect in muonic atoms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th","quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"Moritz Thierfeld, Natalia S. Oreshkina, Zoia A. Mandrykina","submitted_at":"2025-09-01T09:50:42Z","abstract_excerpt":"The hadronic vacuum polarization (HVP) corrections to energy levels in muonic atoms are studied systematically across the periodic table. Two nuclear charge distribution models have been considered, with partly analytical solution for an homogeneously charged sphere model and direct numerical integration for a Fermi nuclear charge distribution. Our comparison reveals a good agreement between both approaches with differences typically below a few percent. The magnitude of HVP corrections increases with nuclear charge, displaying irregularities that correlate directly with the non-monotonic beha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2509.01311","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/2509.01311/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":"2509.01311","created_at":"2026-07-05T12:02:58.053887+00:00"},{"alias_kind":"arxiv_version","alias_value":"2509.01311v1","created_at":"2026-07-05T12:02:58.053887+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2509.01311","created_at":"2026-07-05T12:02:58.053887+00:00"},{"alias_kind":"pith_short_12","alias_value":"GZSUGQF35PYE","created_at":"2026-07-05T12:02:58.053887+00:00"},{"alias_kind":"pith_short_16","alias_value":"GZSUGQF35PYE52C6","created_at":"2026-07-05T12:02:58.053887+00:00"},{"alias_kind":"pith_short_8","alias_value":"GZSUGQF3","created_at":"2026-07-05T12:02:58.053887+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/GZSUGQF35PYE52C6KY4NGUREJX","json":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX.json","graph_json":"https://pith.science/api/pith-number/GZSUGQF35PYE52C6KY4NGUREJX/graph.json","events_json":"https://pith.science/api/pith-number/GZSUGQF35PYE52C6KY4NGUREJX/events.json","paper":"https://pith.science/paper/GZSUGQF3"},"agent_actions":{"view_html":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX","download_json":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX.json","view_paper":"https://pith.science/paper/GZSUGQF3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2509.01311&json=true","fetch_graph":"https://pith.science/api/pith-number/GZSUGQF35PYE52C6KY4NGUREJX/graph.json","fetch_events":"https://pith.science/api/pith-number/GZSUGQF35PYE52C6KY4NGUREJX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX/action/storage_attestation","attest_author":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX/action/author_attestation","sign_citation":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX/action/citation_signature","submit_replication":"https://pith.science/pith/GZSUGQF35PYE52C6KY4NGUREJX/action/replication_record"}},"created_at":"2026-07-05T12:02:58.053887+00:00","updated_at":"2026-07-05T12:02:58.053887+00:00"}