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@ARTICLE{Grojean:602012,
author = {Grojean, Christophe and Kley, Jonathan and Leflot, Damien
and Yao, Chang-Yuan},
title = {{T}he flavor invariants of the $\nu${SM}},
reportid = {PUBDB-2024-00468, DESY-24-021. arXiv:2406.00094.
CERN-TH-2024-076. HU-EP-24/14},
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 $\nu$SM, 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 $\nu$SM 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 $\nu$SM, 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 ahigher 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.},
cin = {T},
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)25},
eprint = {2406.00094},
howpublished = {arXiv:2406.00094},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2406.00094;\%\%$},
doi = {10.3204/PUBDB-2024-00468},
url = {https://bib-pubdb1.desy.de/record/602012},
}