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