{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:3CXFELMXHAZ56YRKDRN6C4TUSX","short_pith_number":"pith:3CXFELMX","schema_version":"1.0","canonical_sha256":"d8ae522d973833df622a1c5be1727495e1071abe7031666d25939aec328d9f07","source":{"kind":"arxiv","id":"2508.21497","version":3},"attestation_state":"computed","paper":{"title":"A Benchmark Study of the Relativistic Plane Wave Impulse Approximation for Polarized ($\\vec{p},2\\vec{p}\\,$) Reactions on the 3s$_{1/2}$ state in $^{208}$Pb at 392 MeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"G. C. Hillhouse, J. P. W. Diener, T. Mello","submitted_at":"2025-08-29T10:28:16Z","abstract_excerpt":"The Relativistic Plane Wave Impulse Approximation (RPWIA) is benchmarked against the established Relativistic Distorted Wave Impulse Approximation (RDWIA) for exclusive proton-induced proton knockout reactions ($\\vec{p},2\\vec{p}\\,$) from the 3s$_{1/2}$ state in $^{208}$Pb at 392 MeV. While the RDWIA provides the proper description of the reaction, the RPWIA-which neglects nuclear distortion and absorption effects-fails dramatically for absolute cross-sections, requiring a scaling factor of $\\frac{1}{26}$ to match the data. However, within $\\pm10$ MeV of the recoilless condition, the RPWIA quan"},"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":"2508.21497","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2025-08-29T10:28:16Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"34198fc7513eaf4efc65334b65df369881177a38866425f1cbf35f78a10bf60f","abstract_canon_sha256":"f6f4587296f9801e736a326fc662c6e39cd805f45eeb21faf6527ce94bcc92fd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-28T01:04:30.131991Z","signature_b64":"ZGeWv1NIdBrd21Miyir0CYu8Z7oXPNAWE/ZWkR2FoV3UqZaVAmOwgjHFK/qy4f/4rD1vFbqZYM0iaxngXyHmAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8ae522d973833df622a1c5be1727495e1071abe7031666d25939aec328d9f07","last_reissued_at":"2026-05-28T01:04:30.131434Z","signature_status":"signed_v1","first_computed_at":"2026-05-28T01:04:30.131434Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Benchmark Study of the Relativistic Plane Wave Impulse Approximation for Polarized ($\\vec{p},2\\vec{p}\\,$) Reactions on the 3s$_{1/2}$ state in $^{208}$Pb at 392 MeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"G. C. Hillhouse, J. P. W. Diener, T. Mello","submitted_at":"2025-08-29T10:28:16Z","abstract_excerpt":"The Relativistic Plane Wave Impulse Approximation (RPWIA) is benchmarked against the established Relativistic Distorted Wave Impulse Approximation (RDWIA) for exclusive proton-induced proton knockout reactions ($\\vec{p},2\\vec{p}\\,$) from the 3s$_{1/2}$ state in $^{208}$Pb at 392 MeV. While the RDWIA provides the proper description of the reaction, the RPWIA-which neglects nuclear distortion and absorption effects-fails dramatically for absolute cross-sections, requiring a scaling factor of $\\frac{1}{26}$ to match the data. However, within $\\pm10$ MeV of the recoilless condition, the RPWIA quan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.21497","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/2508.21497/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":"2508.21497","created_at":"2026-05-28T01:04:30.131500+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.21497v3","created_at":"2026-05-28T01:04:30.131500+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.21497","created_at":"2026-05-28T01:04:30.131500+00:00"},{"alias_kind":"pith_short_12","alias_value":"3CXFELMXHAZ5","created_at":"2026-05-28T01:04:30.131500+00:00"},{"alias_kind":"pith_short_16","alias_value":"3CXFELMXHAZ56YRK","created_at":"2026-05-28T01:04:30.131500+00:00"},{"alias_kind":"pith_short_8","alias_value":"3CXFELMX","created_at":"2026-05-28T01:04:30.131500+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/3CXFELMXHAZ56YRKDRN6C4TUSX","json":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX.json","graph_json":"https://pith.science/api/pith-number/3CXFELMXHAZ56YRKDRN6C4TUSX/graph.json","events_json":"https://pith.science/api/pith-number/3CXFELMXHAZ56YRKDRN6C4TUSX/events.json","paper":"https://pith.science/paper/3CXFELMX"},"agent_actions":{"view_html":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX","download_json":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX.json","view_paper":"https://pith.science/paper/3CXFELMX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.21497&json=true","fetch_graph":"https://pith.science/api/pith-number/3CXFELMXHAZ56YRKDRN6C4TUSX/graph.json","fetch_events":"https://pith.science/api/pith-number/3CXFELMXHAZ56YRKDRN6C4TUSX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX/action/storage_attestation","attest_author":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX/action/author_attestation","sign_citation":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX/action/citation_signature","submit_replication":"https://pith.science/pith/3CXFELMXHAZ56YRKDRN6C4TUSX/action/replication_record"}},"created_at":"2026-05-28T01:04:30.131500+00:00","updated_at":"2026-05-28T01:04:30.131500+00:00"}