{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:6D77TQK5FUMVP7JQ66N5W46EGP","short_pith_number":"pith:6D77TQK5","schema_version":"1.0","canonical_sha256":"f0fff9c15d2d1957fd30f79bdb73c433f3eb662561137109afbaeae43d1174b9","source":{"kind":"arxiv","id":"1812.00907","version":1},"attestation_state":"computed","paper":{"title":"Quantum scattering with semiclassical asymptotic motion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"James M. Feagin, John S. Briggs","submitted_at":"2018-12-03T17:05:12Z","abstract_excerpt":"Conventional scattering theory is incomplete in that it does not adequately describe the behaviour of the wave function at macroscopic distances from the scattering reaction volume. In scattering experiments particles are incident from sources at macroscopic distance and measured at macroscopic distance from the microscopic reaction volume. Standard experimental procedure is to describe asymptotic particle motion by classical mechanics. However, this transition to classical mechanics is not accounted for in standard quantum scattering theory. Hence, we revisit conventional scattering theory wi"},"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":"1812.00907","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-12-03T17:05:12Z","cross_cats_sorted":[],"title_canon_sha256":"74d86ad4c8f64d41b01c8a82dbaa1dc05f99ef10bce5a1767302e0fd5b992dd5","abstract_canon_sha256":"b9cb25fa41dc8e557a0d87fca35ebbca2aeb251627708d4a220ed9708e43a8c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:19:37.629535Z","signature_b64":"tLd4q7tOU9xAPbTl4clu7yShdmNKRcUkEjMPRHoKsKiWO5CsKSp44tSdntSH2uyNSnmeFDmVAFLA6BlWUrCEBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f0fff9c15d2d1957fd30f79bdb73c433f3eb662561137109afbaeae43d1174b9","last_reissued_at":"2026-07-05T03:19:37.629048Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:19:37.629048Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum scattering with semiclassical asymptotic motion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"James M. Feagin, John S. Briggs","submitted_at":"2018-12-03T17:05:12Z","abstract_excerpt":"Conventional scattering theory is incomplete in that it does not adequately describe the behaviour of the wave function at macroscopic distances from the scattering reaction volume. In scattering experiments particles are incident from sources at macroscopic distance and measured at macroscopic distance from the microscopic reaction volume. Standard experimental procedure is to describe asymptotic particle motion by classical mechanics. However, this transition to classical mechanics is not accounted for in standard quantum scattering theory. Hence, we revisit conventional scattering theory wi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.00907","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/1812.00907/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":"1812.00907","created_at":"2026-07-05T03:19:37.629107+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.00907v1","created_at":"2026-07-05T03:19:37.629107+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.00907","created_at":"2026-07-05T03:19:37.629107+00:00"},{"alias_kind":"pith_short_12","alias_value":"6D77TQK5FUMV","created_at":"2026-07-05T03:19:37.629107+00:00"},{"alias_kind":"pith_short_16","alias_value":"6D77TQK5FUMVP7JQ","created_at":"2026-07-05T03:19:37.629107+00:00"},{"alias_kind":"pith_short_8","alias_value":"6D77TQK5","created_at":"2026-07-05T03:19:37.629107+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/6D77TQK5FUMVP7JQ66N5W46EGP","json":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP.json","graph_json":"https://pith.science/api/pith-number/6D77TQK5FUMVP7JQ66N5W46EGP/graph.json","events_json":"https://pith.science/api/pith-number/6D77TQK5FUMVP7JQ66N5W46EGP/events.json","paper":"https://pith.science/paper/6D77TQK5"},"agent_actions":{"view_html":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP","download_json":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP.json","view_paper":"https://pith.science/paper/6D77TQK5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.00907&json=true","fetch_graph":"https://pith.science/api/pith-number/6D77TQK5FUMVP7JQ66N5W46EGP/graph.json","fetch_events":"https://pith.science/api/pith-number/6D77TQK5FUMVP7JQ66N5W46EGP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP/action/storage_attestation","attest_author":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP/action/author_attestation","sign_citation":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP/action/citation_signature","submit_replication":"https://pith.science/pith/6D77TQK5FUMVP7JQ66N5W46EGP/action/replication_record"}},"created_at":"2026-07-05T03:19:37.629107+00:00","updated_at":"2026-07-05T03:19:37.629107+00:00"}