{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:44NWPGS32WC2LNFQF3EU7UOOVB","short_pith_number":"pith:44NWPGS3","schema_version":"1.0","canonical_sha256":"e71b679a5bd585a5b4b02ec94fd1cea853436229f20863f2fee33d19137aaab6","source":{"kind":"arxiv","id":"1408.0118","version":1},"attestation_state":"computed","paper":{"title":"$K^-d\\rightarrow \\pi\\Sigma n$ reactions and structure of the $\\Lambda(1405)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Emiko Hiyama, Shota Ohnishi, Tetsuo Hyodo, Wolfram Weise, Yoichi Ikeda","submitted_at":"2014-08-01T09:52:13Z","abstract_excerpt":"We report on the first results of a full three-body calculation of the $\\bar{K}NN$-$\\pi YN$ amplitude for the $K^-d\\rightarrow\\pi\\Sigma n$ reaction, and examine how the $\\Lambda(1405)$ resonance manifests itself in the neutron energy distributions of $K^-d\\rightarrow\\pi\\Sigma n$ reactions. The amplitudes are computed using the $\\bar{K}NN$-$\\pi YN$ coupled-channels Alt-Grassberger-Sandhas (AGS) equations. Two types of models are considered for the two-body meson-baryon interactions: an energy-independent interaction and an energy-dependent one, both derived from the leading order chiral SU(3) L"},"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":"1408.0118","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-08-01T09:52:13Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"7ef1843efe04adcb9301acaa4f601717780299b49a50971fa3b95c4e9389357e","abstract_canon_sha256":"a12849ee440c9afca7d39491cccd73c3ce91a5cd010a09066550a7f58bd9b434"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:26.375940Z","signature_b64":"w4M8Y7b11xd0oAgFPDHDt7leZkmBgKb3pY7SeA2vkkEmZH3Ja9TTlrHNnyajJigaKOREbRCBq5ciP9tpnuUlAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e71b679a5bd585a5b4b02ec94fd1cea853436229f20863f2fee33d19137aaab6","last_reissued_at":"2026-05-18T01:42:26.375196Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:26.375196Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$K^-d\\rightarrow \\pi\\Sigma n$ reactions and structure of the $\\Lambda(1405)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Emiko Hiyama, Shota Ohnishi, Tetsuo Hyodo, Wolfram Weise, Yoichi Ikeda","submitted_at":"2014-08-01T09:52:13Z","abstract_excerpt":"We report on the first results of a full three-body calculation of the $\\bar{K}NN$-$\\pi YN$ amplitude for the $K^-d\\rightarrow\\pi\\Sigma n$ reaction, and examine how the $\\Lambda(1405)$ resonance manifests itself in the neutron energy distributions of $K^-d\\rightarrow\\pi\\Sigma n$ reactions. The amplitudes are computed using the $\\bar{K}NN$-$\\pi YN$ coupled-channels Alt-Grassberger-Sandhas (AGS) equations. Two types of models are considered for the two-body meson-baryon interactions: an energy-independent interaction and an energy-dependent one, both derived from the leading order chiral SU(3) L"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.0118","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":""},"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":"1408.0118","created_at":"2026-05-18T01:42:26.375335+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.0118v1","created_at":"2026-05-18T01:42:26.375335+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.0118","created_at":"2026-05-18T01:42:26.375335+00:00"},{"alias_kind":"pith_short_12","alias_value":"44NWPGS32WC2","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_16","alias_value":"44NWPGS32WC2LNFQ","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_8","alias_value":"44NWPGS3","created_at":"2026-05-18T12:28:14.216126+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/44NWPGS32WC2LNFQF3EU7UOOVB","json":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB.json","graph_json":"https://pith.science/api/pith-number/44NWPGS32WC2LNFQF3EU7UOOVB/graph.json","events_json":"https://pith.science/api/pith-number/44NWPGS32WC2LNFQF3EU7UOOVB/events.json","paper":"https://pith.science/paper/44NWPGS3"},"agent_actions":{"view_html":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB","download_json":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB.json","view_paper":"https://pith.science/paper/44NWPGS3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.0118&json=true","fetch_graph":"https://pith.science/api/pith-number/44NWPGS32WC2LNFQF3EU7UOOVB/graph.json","fetch_events":"https://pith.science/api/pith-number/44NWPGS32WC2LNFQF3EU7UOOVB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB/action/storage_attestation","attest_author":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB/action/author_attestation","sign_citation":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB/action/citation_signature","submit_replication":"https://pith.science/pith/44NWPGS32WC2LNFQF3EU7UOOVB/action/replication_record"}},"created_at":"2026-05-18T01:42:26.375335+00:00","updated_at":"2026-05-18T01:42:26.375335+00:00"}