%0 Journal Article
%A Bonnefoy, Quentin
%A Gendy, Emanuele
%A Grojean, Christophe
%A Ruderman, Joshua T.
%T Opportunistic CP violation
%J Journal of high energy physics
%V 06
%N 6
%@ 1126-6708
%C [Trieste]
%I SISSA
%M PUBDB-2023-06432
%M arXiv:2302.07288
%M DESY-23-018
%M HU-EP-22/39
%M TUM-HEP-1453/23
%P 141
%D 2023
%Z 34 p. + 29 p. of appendices, 6 figures. v2: Table 7 added, some extended discussions, matches JHEP version
%X In the electroweak sector of the Standard Model, CP violation arises through a very particular interplay between the three quark generations, as described by the Cabibbo-Kobayashi-Maskawa (CKM) mechanism and the single Jarlskog invariant J<sub>4</sub>. Once generalized to the Standard Model Effective Field Theory (SMEFT), this peculiar pattern gets modified by higher-dimensional operators, whose associated Wilson coefficients are usually split into CP-even and odd parts. However, CP violation at dimension four, i.e., at the lowest order in the EFT expansion, blurs this distinction: any Wilson coefficient can interfere with J<sub>4</sub> and mediate CP violation. In this paper, we study such interferences at first order in the SMEFT expansion, 𝒪(1/Λ<sup>2</sup>), and we capture their associated parameter space via a set of 1551 linear CP-odd flavor invariants. This construction describes both new, genuinely CP-violating quantities as well as the interference between J<sub>4</sub> and CP-conserving ones. We call this latter possibility opportunistic CP violation. Relying on an appropriate extension of the matrix rank to Taylor expansions, which we dub Taylor rank, we define a procedure to organize the invariants in terms of their magnitude, so as to retain only the relevant ones at a given precision. We explore how this characterization changes when different assumptions are made on the flavor structure of the SMEFT coefficients. Interestingly, some of the CP-odd invariants turn out to be less suppressed than J<sub>4</sub>, even when they capture opportunistic CPV, demonstrating that CP-violation in the SM, at dimension 4, is accidentally small.
%K CP: violation (INSPIRE)
%K dimension: 4 (INSPIRE)
%K operator: higher-dimensional (INSPIRE)
%K capture (INSPIRE)
%K interference (INSPIRE)
%K flavor (INSPIRE)
%K effective field theory (INSPIRE)
%K mediation (INSPIRE)
%K structure (INSPIRE)
%K electroweak interaction (INSPIRE)
%K quark (INSPIRE)
%K Jarlskog (INSPIRE)
%K suppression (INSPIRE)
%K Taylor expansion (INSPIRE)
%K CP Violation (autogen)
%K Flavour Symmetries (autogen)
%K SMEFT (autogen)
%F PUB:(DE-HGF)16
%9 Journal Article
%U <Go to ISI:>//WOS:001040491500003
%R 10.1007/JHEP06(2023)141
%U https://bib-pubdb1.desy.de/record/597103