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@ARTICLE{Bonnefoy:597103,
author = {Bonnefoy, Quentin and Gendy, Emanuele and Grojean,
Christophe and Ruderman, Joshua T.},
title = {{O}pportunistic {CP} violation},
journal = {Journal of high energy physics},
volume = {06},
number = {6},
issn = {1126-6708},
address = {[Trieste]},
publisher = {SISSA},
reportid = {PUBDB-2023-06432, arXiv:2302.07288. DESY-23-018.
HU-EP-22/39. TUM-HEP-1453/23},
pages = {141},
year = {2023},
note = {34 p. + 29 p. of appendices, 6 figures. v2: Table 7 added,
some extended discussions, matches JHEP version},
abstract = {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$_{4}$. 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$_{4}$ and mediate CP violation. In this paper, we study
such interferences at first order in the SMEFT expansion,
𝒪(1/Λ$^{2}$), 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$_{4}$ 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$_{4}$, even when they capture
opportunistic CPV, demonstrating that CP-violation in the
SM, at dimension 4, is accidentally small.},
keywords = {CP: violation (INSPIRE) / dimension: 4 (INSPIRE) /
operator: higher-dimensional (INSPIRE) / capture (INSPIRE) /
interference (INSPIRE) / flavor (INSPIRE) / effective field
theory (INSPIRE) / mediation (INSPIRE) / structure (INSPIRE)
/ electroweak interaction (INSPIRE) / quark (INSPIRE) /
Jarlskog (INSPIRE) / suppression (INSPIRE) / Taylor
expansion (INSPIRE) / CP Violation (autogen) / Flavour
Symmetries (autogen) / SMEFT (autogen)},
cin = {T},
ddc = {530},
cid = {I:(DE-H253)T-20120731},
pnm = {611 - Fundamental Particles and Forces (POF4-611) / DFG
project 390833306 - EXC 2121: Quantum Universe (390833306)},
pid = {G:(DE-HGF)POF4-611 / G:(GEPRIS)390833306},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
eprint = {2302.07288},
howpublished = {arXiv:2302.07288},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2302.07288;\%\%$},
UT = {WOS:001040491500003},
doi = {10.1007/JHEP06(2023)141},
url = {https://bib-pubdb1.desy.de/record/597103},
}