Searcharxiv⌕ Search

arXiv · 2611.08387

Algorithmic Construction of Vector-Valued Modular Forms and Application to an $A_4\times\mathbb{Z}_4$-invariant Model of Leptons

Abstract

We present an algorithmic procedure that constructs the Vector-Valued Modular Forms (VVMFs) of finite modular groups, as well as its implementation in a companion code. The usual method consists in building the first few VVMFs, whose tensor products then generate the others. We address the difficulty of systematically finding the minimal set of VVMFs that suffices to produce all higher-weight ones, and we propose a method to identify it that makes use of the Burnside-Brauer theorem. For any given group, whose basic group-theoretic and representation-theoretic description is provided by the user, the code determines the minimal set of VVMFs, explicitly builds it using general results of the theory of such functions, then performs the tensor products that generate any other VVMF. Importantly, it automatically takes into account all caveats that might arise during the study of new groups. Our approach reproduces the known results for the finite modular groups explored in the recent phenomenological literature on modular flavor symmetries, and works for additional groups which we tested. We illustrate our algorithm and the working of our code by studying a model of leptons based on the unexplored finite modular group $A_4\times\mathbb{Z}_4$.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Q. Bonnefoy, M. Rausch de Traubenberg, V. Saulquin. 2026-11-05. Algorithmic Construction of Vector-Valued Modular Forms and Application to an $A_4\times\mathbb{Z}_4$-invariant Model of Leptons. https://arxiv.org/abs/2611.08387

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Pomeron Weights in QCD Processes at High Energy and the $S$-Matrix Unitarity Constraint

The pomeron topological cross-section is derived for the eikonal and the $U$-matrix unitarization schemes using a generalized representation of the scattering amplitude at high energy in an effort to examine pomeron characteristics, namely the multiplicity distribution, fluctuation, and correlation, and to reveal the impact of pomeron weights on the $pp$ multiplicity distribution. The results demonstrate that the $U$-matrix inherently incorporates a larger amount of diffraction production into the multi-pomeron vertices, yielding a larger pomerons' variability regardless of the energy range, while such fluctuations become significant only beyond a specific high-energy threshold in eikonal-like schemes. Most importantly, our findings indicate that within the $U$-matrix scheme, an increase in exchanged pomerons results in more pronounced pomeron correlations and that this correlated resummation plays a key role in enhancing multi-parton collisions. We argue that the choice of unitarization scheme is not arbitrary, as it directly dictates the statistical structure of multi-reggeon exchanges. By reflecting the composite nature of hadrons, rational alternatives to eikonal-like schemes, such as the $U$-matrix, offer a compelling theoretical foundation for modeling high-energy hadronic collisions, provided that specific formulations can be identified that strictly satisfy all mathematical and physical constraints.

hep-ph↗

Two-loop renormalisation of quark and gluon fields in the SMEFT

We compute the contributions of CP-conserving operators in the dimension-six SMEFT to the two-loop renormalisation constants of quark and gluon fields in the $\overline{\textrm{MS}}$-scheme. Specifically, we consider the top-quark chromomagnetic operator and the triple gluon operator. We work with the background-field method, which allows us to extract the contribution of these operators to the two-loop running of the top mass and the strong coupling constant. We discuss in detail the mixing with the unphysical operators required for the renormalisation, and we present analytic results for the renormalisation constants of all relevant operators.

hep-ph↗

Two-loop renormalisation of quark and gluon fields in the SMEFT in the on-shell scheme

We compute the contributions of CP-conserving dimension-six SMEFT operators to the two-loop renormalisation constants of quark and gluon fields in the on-shell scheme. Specifically, we consider the top-quark chromomagnetic operator and the triple gluon operator. We also compute the contribution of four-quark operators to the gluon renormalisation constant and discuss the implications for the running of the strong coupling constant.

hep-ph↗