{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:XGMAVOQZFIVEXPL5WMJMNQFWJS","short_pith_number":"pith:XGMAVOQZ","schema_version":"1.0","canonical_sha256":"b9980aba192a2a4bbd7db312c6c0b64c917d1320585308affe0c0e43d337f5ed","source":{"kind":"arxiv","id":"1211.6961","version":4},"attestation_state":"computed","paper":{"title":"Coulomb Correction to the Screening Angle of the Moliere Multiple Scattering Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. V. Tarasov, E. A. Kuraev, O. O. Voskresenskaya","submitted_at":"2012-11-29T16:01:46Z","abstract_excerpt":"High-energy Coulomb correction to the screening angular parameter of the Moliere multiple scattering theory is found. Numerical calculations are presented in the range of nuclear charge from Z=4 to Z=82.  The accuracy of the Moliere theory in determining the Coulomb correction to the screening angle is estimated."},"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":"1211.6961","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-11-29T16:01:46Z","cross_cats_sorted":[],"title_canon_sha256":"1d8fb38796530bc82dc823a0e1ac7a6832f3f9972ac6b1bcbf1b8665db8512ab","abstract_canon_sha256":"fc7c586bed05e502ecae9b153d13ff92c425a186804f79a81ad748628064d6eb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:01:46.919451Z","signature_b64":"gRq3Se5IFRA4aL03jI4zT2BsajlBBljOpLsl9Sj/BVY82Nxh2Nolz/IVaOv4/ezisq9/FF0gXGY0y0SPdr+4AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b9980aba192a2a4bbd7db312c6c0b64c917d1320585308affe0c0e43d337f5ed","last_reissued_at":"2026-05-18T03:01:46.919025Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:01:46.919025Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coulomb Correction to the Screening Angle of the Moliere Multiple Scattering Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. V. Tarasov, E. A. Kuraev, O. O. Voskresenskaya","submitted_at":"2012-11-29T16:01:46Z","abstract_excerpt":"High-energy Coulomb correction to the screening angular parameter of the Moliere multiple scattering theory is found. Numerical calculations are presented in the range of nuclear charge from Z=4 to Z=82.  The accuracy of the Moliere theory in determining the Coulomb correction to the screening angle is estimated."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.6961","kind":"arxiv","version":4},"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":"1211.6961","created_at":"2026-05-18T03:01:46.919088+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.6961v4","created_at":"2026-05-18T03:01:46.919088+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.6961","created_at":"2026-05-18T03:01:46.919088+00:00"},{"alias_kind":"pith_short_12","alias_value":"XGMAVOQZFIVE","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_16","alias_value":"XGMAVOQZFIVEXPL5","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_8","alias_value":"XGMAVOQZ","created_at":"2026-05-18T12:27:27.928770+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/XGMAVOQZFIVEXPL5WMJMNQFWJS","json":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS.json","graph_json":"https://pith.science/api/pith-number/XGMAVOQZFIVEXPL5WMJMNQFWJS/graph.json","events_json":"https://pith.science/api/pith-number/XGMAVOQZFIVEXPL5WMJMNQFWJS/events.json","paper":"https://pith.science/paper/XGMAVOQZ"},"agent_actions":{"view_html":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS","download_json":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS.json","view_paper":"https://pith.science/paper/XGMAVOQZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.6961&json=true","fetch_graph":"https://pith.science/api/pith-number/XGMAVOQZFIVEXPL5WMJMNQFWJS/graph.json","fetch_events":"https://pith.science/api/pith-number/XGMAVOQZFIVEXPL5WMJMNQFWJS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS/action/storage_attestation","attest_author":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS/action/author_attestation","sign_citation":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS/action/citation_signature","submit_replication":"https://pith.science/pith/XGMAVOQZFIVEXPL5WMJMNQFWJS/action/replication_record"}},"created_at":"2026-05-18T03:01:46.919088+00:00","updated_at":"2026-05-18T03:01:46.919088+00:00"}