{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:LDHW3VTQHC2GSO73MEJCQKBB6B","short_pith_number":"pith:LDHW3VTQ","schema_version":"1.0","canonical_sha256":"58cf6dd67038b4693bfb6112282821f0630c396cdafd22d0c9d065f5b92d109f","source":{"kind":"arxiv","id":"1605.07114","version":2},"attestation_state":"computed","paper":{"title":"Global Effective-Field-Theory analysis of New-Physics effects in (semi)leptonic kaon decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Jorge Martin Camalich, Mart\\'in Gonz\\'alez-Alonso","submitted_at":"2016-05-23T17:37:23Z","abstract_excerpt":"We analyze the decays $K\\to\\pi\\ell\\nu$ and $P\\to\\ell\\nu$ ($P=K,\\pi$, $\\ell=e,\\,\\mu$) using a low-energy Effective-Field-Theory approach to parametrize New Physics and study the complementarity with baryon $\\beta$ decays. We then provide a road map for a global analysis of the experimental data, with all the Wilson coefficients simultaneously, and perform a fit leading to numerical bounds for them and for $V_{us}$. A prominent result of our analysis is a reinterpretation of the well-known $V_{ud}-V_{us}$ diagram as a strong constraint on new physics. Finally, we reinterpret our bounds in terms "},"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":"1605.07114","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-05-23T17:37:23Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"676372397242936314567100a7c5c8c9d76062fb1735134789f9fdce18fbe34c","abstract_canon_sha256":"06f6caca3c126089b48c824d337c3ab721fa8099e2efda34bb7e3e1ba0b2212c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:48.936588Z","signature_b64":"by3KQeXYukRRVIL8NBTjEPrRhPZbvv7oeKjIfNs65/YLTc9LBk1FItKllYIgnKBtdSMoJkSHX5X6kCtUOEQjAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58cf6dd67038b4693bfb6112282821f0630c396cdafd22d0c9d065f5b92d109f","last_reissued_at":"2026-05-18T00:51:48.935822Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:48.935822Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Global Effective-Field-Theory analysis of New-Physics effects in (semi)leptonic kaon decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Jorge Martin Camalich, Mart\\'in Gonz\\'alez-Alonso","submitted_at":"2016-05-23T17:37:23Z","abstract_excerpt":"We analyze the decays $K\\to\\pi\\ell\\nu$ and $P\\to\\ell\\nu$ ($P=K,\\pi$, $\\ell=e,\\,\\mu$) using a low-energy Effective-Field-Theory approach to parametrize New Physics and study the complementarity with baryon $\\beta$ decays. We then provide a road map for a global analysis of the experimental data, with all the Wilson coefficients simultaneously, and perform a fit leading to numerical bounds for them and for $V_{us}$. A prominent result of our analysis is a reinterpretation of the well-known $V_{ud}-V_{us}$ diagram as a strong constraint on new physics. Finally, we reinterpret our bounds in terms "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.07114","kind":"arxiv","version":2},"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":"1605.07114","created_at":"2026-05-18T00:51:48.935964+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.07114v2","created_at":"2026-05-18T00:51:48.935964+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.07114","created_at":"2026-05-18T00:51:48.935964+00:00"},{"alias_kind":"pith_short_12","alias_value":"LDHW3VTQHC2G","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_16","alias_value":"LDHW3VTQHC2GSO73","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_8","alias_value":"LDHW3VTQ","created_at":"2026-05-18T12:30:29.479603+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.00761","citing_title":"Non-Standard Neutrino Interactions at a Muon Collider Neutrino Detector","ref_index":81,"is_internal_anchor":true},{"citing_arxiv_id":"2604.24924","citing_title":"Forward backward CP asymmetry in $\\tau^- \\to K \\pi \\nu_{\\tau}$ in the Left-Right Inverse seesaw model","ref_index":46,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16025","citing_title":"Scalar and Tensor Form Factors for $\\Lambda \\rightarrow p\\ell \\bar{\\nu}_\\ell$ from Lattice QCD","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B","json":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B.json","graph_json":"https://pith.science/api/pith-number/LDHW3VTQHC2GSO73MEJCQKBB6B/graph.json","events_json":"https://pith.science/api/pith-number/LDHW3VTQHC2GSO73MEJCQKBB6B/events.json","paper":"https://pith.science/paper/LDHW3VTQ"},"agent_actions":{"view_html":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B","download_json":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B.json","view_paper":"https://pith.science/paper/LDHW3VTQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.07114&json=true","fetch_graph":"https://pith.science/api/pith-number/LDHW3VTQHC2GSO73MEJCQKBB6B/graph.json","fetch_events":"https://pith.science/api/pith-number/LDHW3VTQHC2GSO73MEJCQKBB6B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B/action/storage_attestation","attest_author":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B/action/author_attestation","sign_citation":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B/action/citation_signature","submit_replication":"https://pith.science/pith/LDHW3VTQHC2GSO73MEJCQKBB6B/action/replication_record"}},"created_at":"2026-05-18T00:51:48.935964+00:00","updated_at":"2026-05-18T00:51:48.935964+00:00"}