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Here we present a complete computation of these quantities within the Standard Model. We show that decoupling properties with respect to heavy particles do take place in the weak magnetic moment. The obtained values, a_b(M_Z^2)=(2.98-1.56i)x10^(-4) and a_c(M_Z^2)=(-2.80+1.09i)x10^(-5) are dominated by one-gluon exchang"},"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/9702222","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-02-03T11:32:59Z","cross_cats_sorted":[],"title_canon_sha256":"b2ba299e0199b0d1245420976c3455a8e294824ea64f02d3bf62e8435dd2dcbd","abstract_canon_sha256":"a4a5b6804fb8b73e3a660a52842ee31d1d5960df5486c844b475b4356ff82434"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:01.033404Z","signature_b64":"J2bkk5MfjmLViXwhC0KJjnEleFXrNmRcaWPPFekRpZE4y55gLW4nOifx9m4e87+Suhnea8je9cXnIZ0HrO9iAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22bd0567350c28f04d0c378773a77d99860c9c1a431e90e0046ca5b613b5f888","last_reissued_at":"2026-05-18T04:31:01.032506Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:01.032506Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Weak-Magnetic Moment of Heavy Quarks","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G.A. 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