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Simple extensions of the SM
This is a collection of models that are simple bottom-up extensions of the SM, obtained by adding a set of new particles and or interations to the Standard Model.
Available models
| Model | Short Description | Contact | Status |
| Axigluon model | The SM plus a scalar gluon field. | S. Krastanov | Available |
| BSM Characterisation | The SM EFT Lagrangian in the mass basis | B. Fuks, K. Mawatari | Available |
| Coloron Model | A Coloron Model with a Decay to a Single Top Quark | E. Drueke, R. Schwienhorst, N. Vignaroli, J. Nutter, D. Walker, J.-H. Yu, R. S. Chivukula, E. Simmons | Available |
| Color Triplet | A Color Triplet Model with Decay to Top and Bottom Quark | E. Drueke, R. Schwienhorst, N. Vignaroli, D. Walker, J.-H. Yu, J. Nutter, T. Han, I. Lewis, Z. Liu | Available |
| DY SM extension | The SM plus new spin-0, -1, and -2 bosons that contribute to Drell-Yan production of leptons at the LHC. | N. Christensen | Available |
| EFT mass basis | The SM EFT Lagrangian in the mass basis | B. Fuks, K. Mawatari | Available |
| FCNC Higgs interactions | The SM plus higher-dimensional flavor changing Higgs interactions. | S. Krastanov | Available |
| FCNC Top interactions | The SM plus higher-dimensional flavor changing top-quark interactions. | A. Amorim, J. Santiago, N. Castro, R. Santos | Available |
| Fourth generation model | A fourth generation model including a t' and a b' | C. Duhr | Available |
| General 2HDM | The most general 2HDM, including all flavor violation and mixing terms. | C. Duhr, M. Herquet | Available |
| Hidden Abelian Higgs Model | A Z' model where the Z' interacts with the SM through mixings, leading to very small non-SM like Z' couplings. | C. Duhr | Available |
| HiggsCharacterisation | The model file for the spin/parity characterisation of a 125 GeV resonance. | F. Demartin, K. Mawatari | Available |
| Higgs effective theory | An add-on for the SM implementation containing the dimension 5 gluon fusion operator. | C. Duhr | Available |
| Higgs Effective Lagrangian | Higgs effective Lagrangian including operators up-to dimension 6. | A. Alloul, B. Fuks and V. Sanz | Available |
| Hill Model | A model with an unusual extension of the SM Higgs sector. | P. de Aquino, C. Duhr | Available |
| Inert Doublet Model | A model with an additional complex scalar SU(2)L doublet and an unbroken Z2 symmetry under which all SM particles are even while the extra doublet is odd. | A. Goudelis, B. Herrmann, O. Stal | Available |
| Flavor-violating KK gluon | A Kaluza-Klein Gluon Model with FCNC Decay to a Single Top Quark | E. Drueke, R. Schwienhorst, N. Vignaroli, J. Nutter, D. Walker, J.-H. Yu, R. S. Chivukula, E. Simmons | Available |
| Minimal Zp models | The minimal Z' extension of the SM. | L. Basso | Available |
| Monotops | The SM plus monotop effective Lagrangian. | B. Fuks | Available |
| Sextet diquarks | The SM plus sextet diquark scalars. | J. Alwall, C. Duhr | Available |
| Standard model + Scalars | The SM, together with a set of singlet scalar particles coupling only to the SM Higgs, and allowing it to decay invisibly into this new scalar sector. | C. Duhr | Available |
| TFCNC | The SM, plus FCNC top interactions. | M. Buchkremer, G. Cacciapaglia, A. Deandrea, L. Panizzi | Available |
| Triplet diquarks | The SM plus triplet diquark scalars. | J. Alwall, C. Duhr | Available |
| Type III See-Saw Model | The SM, including neutrino masses coming from a type III See-Saw mechanism. | C. Biggio, F. Bonnet | Available |
| VLQ | The SM, plus vector-like quarks, in a model-independent framework. | M. Buchkremer, G. Cacciapaglia, A. Deandrea, L. Panizzi | Available |
| Wprime | The SM a new spin-1 W' boson. | J. Donini, B. Fuks | Available |
| Minimal Dilaton Model | Minimal Dilaton Model | J. Cao, X. Hao, Z. Heng, L. Shang, Y. Zhang | Available |
| Georgi-Machacek Model | Georgi-Machacek Model | K. Kumar, K. Hartling, H. Logan | Available |
| Simplified DM models | Simplified DM models | K. Mawatari, C. Zhang | Available |
| Heavy Neutrino | The SM with three heavy Majorana neutrinos that couple to SM fields through mixing with active neutrinos. | R. Ruiz | Available |
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