{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:3ZUDU6QNUTBWNGQLIHAWCTJFXL","short_pith_number":"pith:3ZUDU6QN","schema_version":"1.0","canonical_sha256":"de683a7a0da4c3669a0b41c1614d25badf200454e1aa0249c0d5b08388419e1c","source":{"kind":"arxiv","id":"1007.5366","version":1},"attestation_state":"computed","paper":{"title":"Electromagnetic production of kaon near threshold","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"T. Mart","submitted_at":"2010-07-30T04:16:58Z","abstract_excerpt":"Kaon photo- and electroproduction off a proton near the production threshold are investigated by utilizing an isobar model. The background amplitude of the model is constructed from Feynman diagrams, whereas the resonance term is calculated by using the multipole formalism. It is found that both pseudoscalar and pseudovector models can nicely describe the available photoproduction data up to W = 50 MeV above the threshold. The Lambda resonance S_{01}(1800) is found to play an important role in improving the model. In the case of double polarization observables Ox and Oz our result corroborates"},"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":"1007.5366","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-07-30T04:16:58Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"0911cb7160c7e7ada0da4de561977bdc5b169116acc6fcf520c53624c6e8a496","abstract_canon_sha256":"4944abe0c5a125a83a8a826273a20311d29b998f08b006a3c86a2651daa342ff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:29.841133Z","signature_b64":"Typ2g+IgoXdVrng0swCrcECuqWq83vVDqfrTIfES+4Havg3L2OcnILghRc/uFhjODRT8nP7lvEJzfCvBf2cnCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de683a7a0da4c3669a0b41c1614d25badf200454e1aa0249c0d5b08388419e1c","last_reissued_at":"2026-05-18T04:31:29.840718Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:29.840718Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic production of kaon near threshold","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"T. Mart","submitted_at":"2010-07-30T04:16:58Z","abstract_excerpt":"Kaon photo- and electroproduction off a proton near the production threshold are investigated by utilizing an isobar model. The background amplitude of the model is constructed from Feynman diagrams, whereas the resonance term is calculated by using the multipole formalism. It is found that both pseudoscalar and pseudovector models can nicely describe the available photoproduction data up to W = 50 MeV above the threshold. The Lambda resonance S_{01}(1800) is found to play an important role in improving the model. In the case of double polarization observables Ox and Oz our result corroborates"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.5366","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":"1007.5366","created_at":"2026-05-18T04:31:29.840776+00:00"},{"alias_kind":"arxiv_version","alias_value":"1007.5366v1","created_at":"2026-05-18T04:31:29.840776+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.5366","created_at":"2026-05-18T04:31:29.840776+00:00"},{"alias_kind":"pith_short_12","alias_value":"3ZUDU6QNUTBW","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_16","alias_value":"3ZUDU6QNUTBWNGQL","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_8","alias_value":"3ZUDU6QN","created_at":"2026-05-18T12:26:03.138858+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/3ZUDU6QNUTBWNGQLIHAWCTJFXL","json":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL.json","graph_json":"https://pith.science/api/pith-number/3ZUDU6QNUTBWNGQLIHAWCTJFXL/graph.json","events_json":"https://pith.science/api/pith-number/3ZUDU6QNUTBWNGQLIHAWCTJFXL/events.json","paper":"https://pith.science/paper/3ZUDU6QN"},"agent_actions":{"view_html":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL","download_json":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL.json","view_paper":"https://pith.science/paper/3ZUDU6QN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1007.5366&json=true","fetch_graph":"https://pith.science/api/pith-number/3ZUDU6QNUTBWNGQLIHAWCTJFXL/graph.json","fetch_events":"https://pith.science/api/pith-number/3ZUDU6QNUTBWNGQLIHAWCTJFXL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL/action/storage_attestation","attest_author":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL/action/author_attestation","sign_citation":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL/action/citation_signature","submit_replication":"https://pith.science/pith/3ZUDU6QNUTBWNGQLIHAWCTJFXL/action/replication_record"}},"created_at":"2026-05-18T04:31:29.840776+00:00","updated_at":"2026-05-18T04:31:29.840776+00:00"}