{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:J4SQ74ZNABZKD47QLVADSSDDUJ","short_pith_number":"pith:J4SQ74ZN","schema_version":"1.0","canonical_sha256":"4f250ff32d0072a1f3f05d40394863a25337271c41f2fb4da7c04785515ceebf","source":{"kind":"arxiv","id":"nucl-th/0112022","version":1},"attestation_state":"computed","paper":{"title":"Electromagnetic, weak, and strong interactions of light mesons","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"P. Maris","submitted_at":"2001-12-08T13:15:46Z","abstract_excerpt":"The ladder-rainbow truncation of the set of Dyson-Schwinger equations is used to study a variety of electroweak and strong processes involving light mesons. The parameters in the effective interaction are constrained by the chiral condensate and f_\\pi; the current quark masses are fitted to m_\\pi and m_K. The obtained electromagnetic form factors are in good agreement with the data. Also the weak K_{l3} decay and the radiative and strong decays of the vector mesons agree reasonably well with the data. Finally, we indicate how processes such as \\pi-\\pi scattering can be described within this fr"},"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":"nucl-th/0112022","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2001-12-08T13:15:46Z","cross_cats_sorted":[],"title_canon_sha256":"66f8311c787e9ac8ad15aac65472be969496c62661968e8f52228bda5592bed1","abstract_canon_sha256":"0d5fbb81685306f0e1470e414d9bc3abd801b2bfadb3d3da21b21fb4905d44a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:42:26.765371Z","signature_b64":"E5Ir2VtMNTpgpMo2PPWWrQxKjtdxjoxZuxLn3Cx8oSXHLVudzEqEeb7P52DQQ7cvVnyzMG6zFmkDnGRrb6ukAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f250ff32d0072a1f3f05d40394863a25337271c41f2fb4da7c04785515ceebf","last_reissued_at":"2026-07-04T14:42:26.764992Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:42:26.764992Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic, weak, and strong interactions of light mesons","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"P. Maris","submitted_at":"2001-12-08T13:15:46Z","abstract_excerpt":"The ladder-rainbow truncation of the set of Dyson-Schwinger equations is used to study a variety of electroweak and strong processes involving light mesons. The parameters in the effective interaction are constrained by the chiral condensate and f_\\pi; the current quark masses are fitted to m_\\pi and m_K. The obtained electromagnetic form factors are in good agreement with the data. Also the weak K_{l3} decay and the radiative and strong decays of the vector mesons agree reasonably well with the data. Finally, we indicate how processes such as \\pi-\\pi scattering can be described within this fr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0112022","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/nucl-th/0112022/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":"nucl-th/0112022","created_at":"2026-07-04T14:42:26.765046+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0112022v1","created_at":"2026-07-04T14:42:26.765046+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0112022","created_at":"2026-07-04T14:42:26.765046+00:00"},{"alias_kind":"pith_short_12","alias_value":"J4SQ74ZNABZK","created_at":"2026-07-04T14:42:26.765046+00:00"},{"alias_kind":"pith_short_16","alias_value":"J4SQ74ZNABZKD47Q","created_at":"2026-07-04T14:42:26.765046+00:00"},{"alias_kind":"pith_short_8","alias_value":"J4SQ74ZN","created_at":"2026-07-04T14:42:26.765046+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/J4SQ74ZNABZKD47QLVADSSDDUJ","json":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ.json","graph_json":"https://pith.science/api/pith-number/J4SQ74ZNABZKD47QLVADSSDDUJ/graph.json","events_json":"https://pith.science/api/pith-number/J4SQ74ZNABZKD47QLVADSSDDUJ/events.json","paper":"https://pith.science/paper/J4SQ74ZN"},"agent_actions":{"view_html":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ","download_json":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ.json","view_paper":"https://pith.science/paper/J4SQ74ZN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0112022&json=true","fetch_graph":"https://pith.science/api/pith-number/J4SQ74ZNABZKD47QLVADSSDDUJ/graph.json","fetch_events":"https://pith.science/api/pith-number/J4SQ74ZNABZKD47QLVADSSDDUJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ/action/storage_attestation","attest_author":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ/action/author_attestation","sign_citation":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ/action/citation_signature","submit_replication":"https://pith.science/pith/J4SQ74ZNABZKD47QLVADSSDDUJ/action/replication_record"}},"created_at":"2026-07-04T14:42:26.765046+00:00","updated_at":"2026-07-04T14:42:26.765046+00:00"}