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

|| '''Model''' ||'''Short Description'''|| '''Contact''' || '''Status''' ||
||[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:NLSM Chiral perturbation theory]||The effective Lagrangian describing the low-energy interaction of mesons.||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:TopEffTh Top Effective theory]||Higher-dimensional operators invariant under the SM symmetries affecting top production and decay||C. Degrande|| '''Available''' ||
||[wiki:TechniColor Technicolor]||The Minimal Walking Technicolor Model||M. Järvinen, T. Hapola, E. Del Nobile, C. Pica|| '''Available''' ||
||[wiki:AnomalousGaugeCoupling Anomalous Gauge Boson Couplings]||Model including anomalous couplings among gauge bosons||O.J.P. Eboli, M.C. Gonzalez-Garcia|| '''Available''' ||
||[wiki:VLQ Vector-like quarks]||Extension of the SM with new VLQ top partners||M. Buchkremer, G. Cacciapaglia, A. Deandrea, L. Panizzi|| '''Available''' ||
||[wiki:NTGC nTGC Effective theory]||dimension-8 operators invariant under the SM symmetries affecting neutral triple gauge boson couplings||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: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:4topEFT Effective theory for 4 top production]||Dimension-six operators invariant under the SM symmetries affecting 4 top interactions||C.Degrande|| '''Available''' ||