{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:MNMWKWUIQ6GYQ67AP7EJDAO2OG","short_pith_number":"pith:MNMWKWUI","schema_version":"1.0","canonical_sha256":"6359655a88878d887be07fc89181da71b8e92f6e991f82173a3825c4ac3766fa","source":{"kind":"arxiv","id":"hep-ph/0011146","version":1},"attestation_state":"computed","paper":{"title":"Chiral dynamics in the presence of bound states: kaon-nucleon interactions revisited","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"J.A. Oller, Ulf-G. Mei{\\ss}ner","submitted_at":"2000-11-10T07:56:22Z","abstract_excerpt":"We study the S-wave kaon-nucleon interactions for strangeness S=-1 in a novel relativistic chiral unitary approach based on coupled channels. Dispersion relations are used to perform the necessary resummation of the lowest order relativistic chiral Lagrangian. A good description of the data in the K^- p, \\pi \\Sigma and \\pi \\Lambda channels is obtained. We show how this method can be systematically extended to higher orders, emphasizing its applicability to any scenario of strong self-interactions where the perturbative series diverges even at low energies. Discussions about the differences to "},"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":"hep-ph/0011146","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2000-11-10T07:56:22Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"14decdc169e2ae783d5912797ff7500098ebc254d07cb74802f02908dc16798e","abstract_canon_sha256":"bbd8568d70a21029ac4dd1e8377786ecf42609c68a41719dff22b2531e8c0239"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:49.071982Z","signature_b64":"+LdnhY9oLibJfKixovneIu7jAuJboYOMRKNYj3t+AcqjezTsN1CjScxWtFsb01tyPLczMrNVfidmh4+0YQneAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6359655a88878d887be07fc89181da71b8e92f6e991f82173a3825c4ac3766fa","last_reissued_at":"2026-05-18T02:36:49.071478Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:49.071478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral dynamics in the presence of bound states: kaon-nucleon interactions revisited","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"J.A. Oller, Ulf-G. Mei{\\ss}ner","submitted_at":"2000-11-10T07:56:22Z","abstract_excerpt":"We study the S-wave kaon-nucleon interactions for strangeness S=-1 in a novel relativistic chiral unitary approach based on coupled channels. Dispersion relations are used to perform the necessary resummation of the lowest order relativistic chiral Lagrangian. A good description of the data in the K^- p, \\pi \\Sigma and \\pi \\Lambda channels is obtained. We show how this method can be systematically extended to higher orders, emphasizing its applicability to any scenario of strong self-interactions where the perturbative series diverges even at low energies. Discussions about the differences to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0011146","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":"hep-ph/0011146","created_at":"2026-05-18T02:36:49.071561+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0011146v1","created_at":"2026-05-18T02:36:49.071561+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0011146","created_at":"2026-05-18T02:36:49.071561+00:00"},{"alias_kind":"pith_short_12","alias_value":"MNMWKWUIQ6GY","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"MNMWKWUIQ6GYQ67A","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"MNMWKWUI","created_at":"2026-05-18T12:25:50.254431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.19928","citing_title":"The Lambda 1405 at the $SU(3)$ point in lattice QCD","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2605.10619","citing_title":"Study of $\\eta^\\prime \\to \\eta \\pi\\pi $ Decays in Large-$N_C$ Chiral Perturbation Theory","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2604.18286","citing_title":"Analysis of the $D_0^*(2300)$ resonance from lattice QCD under chiral symmetry","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2604.04821","citing_title":"Study of the molecular Properties of the $P_c$ and $P_{cs}$ States","ref_index":80,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG","json":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG.json","graph_json":"https://pith.science/api/pith-number/MNMWKWUIQ6GYQ67AP7EJDAO2OG/graph.json","events_json":"https://pith.science/api/pith-number/MNMWKWUIQ6GYQ67AP7EJDAO2OG/events.json","paper":"https://pith.science/paper/MNMWKWUI"},"agent_actions":{"view_html":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG","download_json":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG.json","view_paper":"https://pith.science/paper/MNMWKWUI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0011146&json=true","fetch_graph":"https://pith.science/api/pith-number/MNMWKWUIQ6GYQ67AP7EJDAO2OG/graph.json","fetch_events":"https://pith.science/api/pith-number/MNMWKWUIQ6GYQ67AP7EJDAO2OG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG/action/storage_attestation","attest_author":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG/action/author_attestation","sign_citation":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG/action/citation_signature","submit_replication":"https://pith.science/pith/MNMWKWUIQ6GYQ67AP7EJDAO2OG/action/replication_record"}},"created_at":"2026-05-18T02:36:49.071561+00:00","updated_at":"2026-05-18T02:36:49.071561+00:00"}