{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:UC4YYYJMCXM3P47EB5T4VFHZQ4","short_pith_number":"pith:UC4YYYJM","schema_version":"1.0","canonical_sha256":"a0b98c612c15d9b7f3e40f67ca94f9870b7d1e86c1347cb187f8cdbab4873cb4","source":{"kind":"arxiv","id":"1403.2756","version":3},"attestation_state":"computed","paper":{"title":"Dipole operator constraints on composite Higgs models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David M. Straub, Matthias K\\\"onig, Matthias Neubert","submitted_at":"2014-03-11T21:00:16Z","abstract_excerpt":"Flavour- and CP-violating electromagnetic or chromomagnetic dipole operators in the quark sector are generated in a large class of new physics models and are strongly constrained by measurements of the neutron electric dipole moment and observables sensitive to flavour-changing neutral currents, such as the $B\\to X_s\\gamma$ branching ratio and $\\epsilon'/\\epsilon$. After a model-independent discussion of the relevant constraints, we analyze these effects in models with partial compositeness, where the quarks get their masses by mixing with vector-like composite fermions. These scenarios can be"},"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":"1403.2756","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-11T21:00:16Z","cross_cats_sorted":[],"title_canon_sha256":"e8fa9b1faad831612e79ab3b4e5f98ac5a670c01b17167a477aec7a48737ae63","abstract_canon_sha256":"118d01ec56b36b355d1e35ef66ab98f795cb5e86a73b1da3ab7d2bd21546998f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:24:08.920500Z","signature_b64":"4rDRuw5CWON4WwQnX5t+ol9cnB9jcQ5NWDzrEnwHpF5HSoAnGk/Jid1CAdaUTrgeGqi7MsuOqIhwSaKpjK58BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0b98c612c15d9b7f3e40f67ca94f9870b7d1e86c1347cb187f8cdbab4873cb4","last_reissued_at":"2026-05-18T01:24:08.919751Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:24:08.919751Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dipole operator constraints on composite Higgs models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David M. Straub, Matthias K\\\"onig, Matthias Neubert","submitted_at":"2014-03-11T21:00:16Z","abstract_excerpt":"Flavour- and CP-violating electromagnetic or chromomagnetic dipole operators in the quark sector are generated in a large class of new physics models and are strongly constrained by measurements of the neutron electric dipole moment and observables sensitive to flavour-changing neutral currents, such as the $B\\to X_s\\gamma$ branching ratio and $\\epsilon'/\\epsilon$. After a model-independent discussion of the relevant constraints, we analyze these effects in models with partial compositeness, where the quarks get their masses by mixing with vector-like composite fermions. These scenarios can be"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2756","kind":"arxiv","version":3},"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":"1403.2756","created_at":"2026-05-18T01:24:08.919847+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.2756v3","created_at":"2026-05-18T01:24:08.919847+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2756","created_at":"2026-05-18T01:24:08.919847+00:00"},{"alias_kind":"pith_short_12","alias_value":"UC4YYYJMCXM3","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"UC4YYYJMCXM3P47E","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"UC4YYYJM","created_at":"2026-05-18T12:28:52.271510+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/UC4YYYJMCXM3P47EB5T4VFHZQ4","json":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4.json","graph_json":"https://pith.science/api/pith-number/UC4YYYJMCXM3P47EB5T4VFHZQ4/graph.json","events_json":"https://pith.science/api/pith-number/UC4YYYJMCXM3P47EB5T4VFHZQ4/events.json","paper":"https://pith.science/paper/UC4YYYJM"},"agent_actions":{"view_html":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4","download_json":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4.json","view_paper":"https://pith.science/paper/UC4YYYJM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.2756&json=true","fetch_graph":"https://pith.science/api/pith-number/UC4YYYJMCXM3P47EB5T4VFHZQ4/graph.json","fetch_events":"https://pith.science/api/pith-number/UC4YYYJMCXM3P47EB5T4VFHZQ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4/action/storage_attestation","attest_author":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4/action/author_attestation","sign_citation":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4/action/citation_signature","submit_replication":"https://pith.science/pith/UC4YYYJMCXM3P47EB5T4VFHZQ4/action/replication_record"}},"created_at":"2026-05-18T01:24:08.919847+00:00","updated_at":"2026-05-18T01:24:08.919847+00:00"}