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@ARTICLE{Bonnefoy:622230,
author = {Bonnefoy, Quentin and Kley, Jonathan and Liu, Di and Rossia
and Yao, Chang Yuan},
title = {{A}ligned yet large dipoles: a {SMEFT} study},
journal = {Journal of high energy physics},
volume = {2024},
number = {11},
issn = {1029-8479},
address = {Heidelberg},
publisher = {Springer},
reportid = {PUBDB-2025-00268, arXiv:2403.13065. DESY-24-033.
HU-EP-24/09. LAPTH-011/24. COMETA-2024-004},
pages = {46},
year = {2024},
note = {22 pages (main) + 15 pages (appendices $\&$ references), 6
figures, 7 tables. JHEP published version. Typos are
corrected},
abstract = {We study a non-universal flavor scenario at the level of
the Standard Model Effective Field Theory, according to
which the matrix of Wilson coefficients c$_{uW}$ of an
up-type electroweak quark dipole operator is aligned with
the up-type Yukawa coupling. Such an alignment usually
follows from the assumption of Minimal Flavor Violation
(MFV), away from which we step by allowing the entries of
c$_{uW}$ to be sizable along the first quark generations. A
particular example, which we refer to as “inverse
hierarchy MFV”, features Wilson coefficients inversely
proportional to quark masses, and arises from BSM models
respecting MFV and containing heavy fields that replicate
the mass hierarchy of SM quarks. We then analyze the
phenomenology driven by c$_{uW}$ at colliders and at
lower-energy flavor experiments. We show that precision
measurements of the process pp → Wh → γγℓν at
FCC-hh could set an upper bound on |c$_{uW}$| ≲ $
\mathcal{O} $(10$^{−2}$)(Λ/TeV)$^{2}$, with Λ the cutoff
of the effective field theory. This bound is an order of
magnitude stronger than the existing LHC bounds. Moreover,
we estimate that Wh → $ b\overline{b}\ell \nu $ at HL-LHC
could also give competitive bounds. In the low-energy
regime, we consider bounds arising from rare kaon decays,
which turn out to be loose, |$ {c}_{uW}^{11} $| <$
\mathcal{O} $(1)(Λ/TeV)$^{2}$. We finally demonstrate that
our flavor and operator assumptions can be derived from a
weakly-coupled UV model, which we choose to simultaneously
illustrate the UV origin of inverse hierarchy MFV.},
keywords = {new physics (INSPIRE) / effective field theory (INSPIRE) /
operator: dipole (INSPIRE) / flavor: violation: minimal
(INSPIRE) / CERN LHC Coll: upgrade (INSPIRE) / FCC-hh
(INSPIRE) / p p: scattering (INSPIRE) / Higgs particle:
production (INSPIRE) / W: production (INSPIRE) / electroweak
interaction (INSPIRE) / p p --> W Higgs particle (INSPIRE) /
W Higgs particle --> bottom anti-bottom lepton neutrino
(INSPIRE) / SMEFT (autogen) / Electric Dipole Moments
(autogen) / Electroweak Precision Physics (autogen)},
cin = {T},
ddc = {530},
cid = {I:(DE-H253)T-20120731},
pnm = {611 - Fundamental Particles and Forces (POF4-611) / DFG
project G:(GEPRIS)390833306 - EXC 2121: Quantum Universe
(390833306) / ASYMMETRY - Essential Asymmetries of Nature
(101086085)},
pid = {G:(DE-HGF)POF4-611 / G:(GEPRIS)390833306 /
G:(EU-Grant)101086085},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
eprint = {2403.13065},
howpublished = {arXiv:2403.13065},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2403.13065;\%\%$},
UT = {WOS:001361251700001},
doi = {10.1007/JHEP11(2024)046},
url = {https://bib-pubdb1.desy.de/record/622230},
}