{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:TMHJHKFWSS7KKNFGMBPTPQNDOO","short_pith_number":"pith:TMHJHKFW","schema_version":"1.0","canonical_sha256":"9b0e93a8b694bea534a6605f37c1a37393abd3304350f06c2cd9271ae214fe2b","source":{"kind":"arxiv","id":"2306.16471","version":1},"attestation_state":"computed","paper":{"title":"New Physics in CP Violating and Flavour Changing Quark Dipole Transitions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aleks Smolkovi\\v{c}, Jernej F. Kamenik, Michele Tammaro, Nejc Ko\\v{s}nik, Svjetlana Fajfer","submitted_at":"2023-06-28T18:01:54Z","abstract_excerpt":"We explore CP-violating (CPV) effects of heavy New Physics in flavour-changing quark dipole transitions, within the framework of Standard Model Effective Field Theory (SMEFT). First, we establish the relevant dimension six operators and consider the Renormalisation Group (RG) evolution of the appropriate Wilson coefficients. We investigate RG-induced correlations between different flavour-violating processes and electric dipole moments (EDMs) within the Minimal Flavour Violating and $U(2)^3$ quark flavour models. At low energies, we set bounds on the Wilson coefficients of the dipole operators"},"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":"2306.16471","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-06-28T18:01:54Z","cross_cats_sorted":[],"title_canon_sha256":"c18695f7c13534925fcba5cc2c788684cb3638f19a30de4383392b121d0789a2","abstract_canon_sha256":"44289e2b3710cc14d4f4e2ff7434dd421e5505a6a2d4172350fdb61418a38a3c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:26:05.013270Z","signature_b64":"7r11H8qk1qIR+oFcaAlq3lDmKv9lRbEyCgJ/2MZKlSCXT/fjdVLZlVNfKhDntzADSLzi3Q58wbfM/YTZt0JLBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b0e93a8b694bea534a6605f37c1a37393abd3304350f06c2cd9271ae214fe2b","last_reissued_at":"2026-07-05T06:26:05.012776Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:26:05.012776Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New Physics in CP Violating and Flavour Changing Quark Dipole Transitions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aleks Smolkovi\\v{c}, Jernej F. Kamenik, Michele Tammaro, Nejc Ko\\v{s}nik, Svjetlana Fajfer","submitted_at":"2023-06-28T18:01:54Z","abstract_excerpt":"We explore CP-violating (CPV) effects of heavy New Physics in flavour-changing quark dipole transitions, within the framework of Standard Model Effective Field Theory (SMEFT). First, we establish the relevant dimension six operators and consider the Renormalisation Group (RG) evolution of the appropriate Wilson coefficients. We investigate RG-induced correlations between different flavour-violating processes and electric dipole moments (EDMs) within the Minimal Flavour Violating and $U(2)^3$ quark flavour models. At low energies, we set bounds on the Wilson coefficients of the dipole operators"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.16471","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/2306.16471/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":"2306.16471","created_at":"2026-07-05T06:26:05.012835+00:00"},{"alias_kind":"arxiv_version","alias_value":"2306.16471v1","created_at":"2026-07-05T06:26:05.012835+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.16471","created_at":"2026-07-05T06:26:05.012835+00:00"},{"alias_kind":"pith_short_12","alias_value":"TMHJHKFWSS7K","created_at":"2026-07-05T06:26:05.012835+00:00"},{"alias_kind":"pith_short_16","alias_value":"TMHJHKFWSS7KKNFG","created_at":"2026-07-05T06:26:05.012835+00:00"},{"alias_kind":"pith_short_8","alias_value":"TMHJHKFW","created_at":"2026-07-05T06:26:05.012835+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/TMHJHKFWSS7KKNFGMBPTPQNDOO","json":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO.json","graph_json":"https://pith.science/api/pith-number/TMHJHKFWSS7KKNFGMBPTPQNDOO/graph.json","events_json":"https://pith.science/api/pith-number/TMHJHKFWSS7KKNFGMBPTPQNDOO/events.json","paper":"https://pith.science/paper/TMHJHKFW"},"agent_actions":{"view_html":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO","download_json":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO.json","view_paper":"https://pith.science/paper/TMHJHKFW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2306.16471&json=true","fetch_graph":"https://pith.science/api/pith-number/TMHJHKFWSS7KKNFGMBPTPQNDOO/graph.json","fetch_events":"https://pith.science/api/pith-number/TMHJHKFWSS7KKNFGMBPTPQNDOO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO/action/storage_attestation","attest_author":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO/action/author_attestation","sign_citation":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO/action/citation_signature","submit_replication":"https://pith.science/pith/TMHJHKFWSS7KKNFGMBPTPQNDOO/action/replication_record"}},"created_at":"2026-07-05T06:26:05.012835+00:00","updated_at":"2026-07-05T06:26:05.012835+00:00"}