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@ARTICLE{Grojean:619881,
author = {Grojean, Christophe and Kley, Jonathan and Leflot, Damien
and Yao, Chang Yuan},
title = {{T}he flavor invariants of the ν{SM}},
journal = {Journal of high energy physics},
volume = {2024},
number = {12},
issn = {1029-8479},
address = {[Trieste]},
publisher = {SISSA},
reportid = {PUBDB-2024-07986, arXiv:2406.00094. CERN-TH-2024-076.
DESY-24-021. HU-EP-24/14},
pages = {69},
year = {2024},
note = {27 pages + appendices, 3 figures},
abstract = {Sixty years after the experimental discovery of CP
violation in the quark sector, the existence of a similar CP
violation in the lepton sector is still to be established.
Actually, the structure of such a violation depends
crucially on the origin of the neutrino masses. In an
attempt at categorizing the leptonic sources of CP
violation, we studied the νSM, the Standard Model extended
with three generations of sterile neutrinos, that can
interpolate continuously between the Dirac and Majorana
scenarios of neutrino masses. In particular, we perform a
classification of the Jarlskog-like flavor invariants
entering CP-violating observables and we study their
suppression with the heavy Majorana mass in the seesaw limit
of the model. To simplify the construction of the
invariants, we introduce a graph-based method. With the
guidance of the Hilbert series and plethystic logarithm of
the theory, we construct the generating and primary sets of
invariants for the νSM for the first time. Unlike in the
Standard Model and some other theories, we find that the
numbers of generating invariants and the syzygies among them
cannot immediately be read off from the plethystic
logarithm, but require a more careful examination. Our
analysis reveals that the generating set contains 459
invariants, out of which 208 are CP-even and 251 are CP-odd.
In the seesaw limit of the νSM, we show that all parameters
of the UV theory can be captured in the effective theory
with a certain suppression with the heavy Majorana mass,
while these parameters can only appear in a flavor-invariant
way with a higher mass suppression. Furthermore, we discuss
how the necessary and sufficient conditions for CP violation
can be captured by utilizing these invariants. Along the
way, we present useful algorithms to enumerate and build the
flavor invariants.},
keywords = {CP Violation (autogen) / Flavour Symmetries (autogen) / New
Light Particles (autogen) / Sterile or Heavy Neutrinos
(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 = {2406.00094},
howpublished = {arXiv:2406.00094},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2406.00094;\%\%$},
UT = {WOS:001399239700002},
doi = {10.1007/JHEP12(2024)069},
url = {https://bib-pubdb1.desy.de/record/619881},
}