14 | | This FeynRules model is the implementation of the weak boson effective field theory described in arXiv:1205.4231 [hep-ph]. Namely, the model contains all the five dimension-six operators that modify the triple gauge boson vertices. Their coefficients can be set in the param_card.dat. The parameters in the param_card are the full coefficients, i.e. ~~c,,i,,/Lambda^2^ and are in TeV^-2^. The name are self-explanatory, c,,WWW,,/Lambda^2^ is called CWWWL2 and similarly for c,,W,, and c,,B,, , the coefficients of the CP violating operators $O_{\tilde{W}WW}$ and $O_{\tilde{W}}$ are CPWWWL2 and CPWL2 respectively. The new interaction has also an order NP (for new physics) which is the power of ($1/\Lambda$) of the amplitude. For example, an amplitude with one vertex for a dimension-six operator is proportional to $1/\Lambda^2$~~ and has NP=2. |

| 14 | This FeynRules model is the implementation of the weak boson effective field theory described in arXiv:1205.4231 [hep-ph]. Namely, the model contains all the five dimension-six operators that modify the triple gauge boson vertices. Their coefficients can be set in the param_card.dat. The parameters in the param_card are the full coefficients, i.e. [[latex( $c_i/\Lambda^2$ )]] and are in TeV^-2^. The name are self-explanatory, [[latex( $c_{WWW}/\Lambda^2$ )]] is called CWWWL2 and similarly for c,,W,, and c,,B,, , the coefficients of the CP violating operators [[latex( $O_{\tilde{W}WW}\quad\text{and}\quad O_{\tilde{W}}$ )]] are CPWWWL2 and CPWL2 respectively. The new interaction has also an order NP (for new physics) which is the power of [[latex( $1/\Lambda$ )]] of the amplitude. For example, an amplitude with one vertex for a dimension-six operator is proportional to [[latex( $1/\Lambda^2$ )]] and has NP=2. |