=== Strongly-coupled models and effective field theories ===

|| '''Model''' ||'''Short Description'''|| '''Contact''' || '''Status''' ||
||[wiki:ALPsEFT Axion-Like Particles]||Effective Theories for a light Axion-Like Particle||I. Brivio|| '''Available''' ||
||[wiki:AnomalousGaugeCoupling Anomalous Gauge Boson Couplings]||Model including anomalous couplings among gauge bosons||O.J.P. Eboli, M.C. Gonzalez-Garcia|| '''Available''' ||
||[wiki:BSMCharacterisation BSM Characterisation]||The SM EFT Lagrangian in the mass basis|| B. Fuks, K. Mawatari || '''Available''' ||
||[wiki:dim6top Complete top-quark EFT implementation]||A complete top-quark EFT implementation||G. Durieux and C. Zhang|| '''Available''' ||
||[wiki:NLSM Chiral perturbation theory]||The effective Lagrangian describing the low-energy interaction of mesons.||C. Degrande|| '''Available''' ||
||[wiki:EFTmassbasis EFT mass basis]||The SM EFT Lagrangian in the mass basis|| B. Fuks, K. Mawatari || '''Available''' ||
||[wiki:4topEFT Effective theory for 4 top production]||Dimension-six operators invariant under the SM symmetries affecting 4 top interactions||C.Degrande|| '''Available''' ||
||[wiki:EWdim6 Effective theory for weak gauge boson production]||Dimension-six operators invariant under the SM symmetries affecting triple gauge boson interactions||C.Degrande|| '''Available''' ||
||[wiki:HiggsTopCurrents Effective top-Higgs interactions]||Dimension 6 Higgs-top interactions.|| E. Salvioni and J. Dror || '''Available''' ||
||[wiki:FCHiggs FCNC Higgs interactions]||The SM plus higher-dimensional flavor changing Higgs interactions.|| S. Krastanov || '''Available''' ||
||[wiki:GeneralFCNTop FCNC Top interactions]||The SM plus higher-dimensional flavor changing top-quark interactions.|| A. Amorim, J. Santiago, N. Castro, R. Santos || '''Available''' ||
||[wiki:FCNC4F Four-fermion FCNC ]||Contact Interaction model with b-s-l-l FCNC terms|| Y. Afik and J. Cohen || '''Available''' ||
||[wiki:HiggsCharacterisation HiggsCharacterisation]||The model file for the spin/parity characterisation of a 125 GeV resonance.||F. Demartin, K. Mawatari|| '''Available''' ||
||[wiki:HEL Higgs Effective Lagrangian]||Higgs effective Lagrangian including operators up-to dimension 6.|| A. Alloul, B. Fuks and V. Sanz || '''Available''' ||
||[HiggsEffectiveTheory Higgs effective theory]|| An add-on for the SM implementation containing the dimension 5 gluon fusion operator. || C. Duhr || '''Available''' ||
||[ThreeSiteModel Mimimal Higgsless Model (3-Site Model)]||A higgsless model, including new heavy fermions and a Z' and a W' boson. || N. Christensen || '''Available''' || 
||[wiki:NTGC nTGC Effective theory]||dimension-8 operators invariant under the SM symmetries affecting neutral triple gauge boson couplings||C. Degrande|| '''Available''' ||
||[wiki:SILH Strongly Interacting Light Higgs]||A model including higher-dimensional SM operators to describe strongly coupled theories of EWSB.||C. Degrande|| '''Available''' ||
||[wiki:TechniColor Technicolor]||The Minimal Walking Technicolor Model||M. Järvinen, T. Hapola, E. Del Nobile, C. Pica|| '''Available''' ||
||[wiki:TFCNC]||The SM, plus FCNC top interactions.||M. Buchkremer, G. Cacciapaglia, A. Deandrea, L. Panizzi|| '''Available''' || 
||[wiki:SMEFT The SMEFT in the Warsaw basis]||Standard Model Effective Field Theory||I. Brivio, Y. Jiang, M. Trott,|| '''Available''' ||
||[wiki:TopEffTh Top Effective theory]||Higher-dimensional operators invariant under the SM symmetries affecting top production and decay||C. Degrande|| '''Available''' ||
||[wiki:TopFCNC Top Effective theory for FCNC]||Dimension-six operators invariant under the SM symmetries affecting top FCNC||C.Degrande, G. Durieux, F. Maltoni, C. Zhang|| '''Available''' ||
||[wiki:VLC_LN Vector-like Confinement Model]||Model with vector-like pairs of leptons and neutrinos||D. Barducci, M. Redi and A. Tesi || '''Available''' ||