Changes between Version 3 and Version 4 of EWdim6


Ignore:
Timestamp:
01/06/16 11:21:18 (4 years ago)
Author:
degrande
Comment:

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  • EWdim6

    v3 v4  
    1616
    1717|| '''Operator''' ||'''Coefficient'''|| '''param_card name''' || '''limit at 68% C.L.(TeV$^{-2}$)''' ||
    18 ||'''$\mbox{Tr}[W_{\mu\nu}W^{\nu\rho}W_{\rho}^{\mu}]$'''|| '''$c_{WWW}/\Lambda^2$''' || CWWWL2 || [-11.9 , -1.94] ||
    19 ||'''$(D_\mu\Phi)^\dagger W^{\mu\nu}(D_\nu\Phi)$'''|| '''$c_{W}/\Lambda^2$''' || CWL2 || [-8.42 , 1.44] ||
    20 ||'''$(D_\mu\Phi)^\dagger B^{\mu\nu}(D_\nu\Phi)$'''|| '''$c_{B}/\Lambda^2$''' || CBL2 || [-7.9 , 14.9] ||
    21 ||'''$\mbox{Tr}[\tilde{W}_{\mu\nu}W^{\nu\rho}W_{\rho}^{\mu}]$'''|| '''$c_{\tilde{W}WW}/\Lambda^2$''' || CPWWWL2 || [-185.3 , -82.4] ||
    22 ||'''$(D_\mu\Phi)^\dagger \tilde{W}^{\mu\nu}(D_\nu\Phi)$'''|| '''$c_{\tilde{W}}/\Lambda^2$''' || CPWL2 || [-39.3 , -4.9] ||
     18||'''[[latex( $\mbox{Tr}[W_{\mu\nu}W^{\nu\rho}W_{\rho}^{\mu}]$ )]]'''|| '''[[latex( $c_{WWW}/\Lambda^2$ )]]''' || CWWWL2 || [-11.9 , -1.94] ||
     19||'''[[latex( $(D_\mu\Phi)^\dagger W^{\mu\nu}(D_\nu\Phi)$ )]]'''|| '''[[latex( $c_{W}/\Lambda^2$ )]]''' || CWL2 || [-8.42 , 1.44] ||
     20||'''[[latex( $(D_\mu\Phi)^\dagger B^{\mu\nu}(D_\nu\Phi)$ )]]'''|| '''[[latex( $c_{B}/\Lambda^2$ )]]''' || CBL2 || [-7.9 , 14.9] ||
     21||'''[[latex( $\mbox{Tr}[\tilde{W}_{\mu\nu}W^{\nu\rho}W_{\rho}^{\mu}]$ )]]'''|| '''[[latex( $c_{\tilde{W}WW}/\Lambda^2$ )]]''' || CPWWWL2 || [-185.3 , -82.4] ||
     22||'''[[latex( $(D_\mu\Phi)^\dagger \tilde{W}^{\mu\nu}(D_\nu\Phi)$ )]]'''|| '''[[latex( $c_{\tilde{W}}/\Lambda^2$ )]]''' || CPWL2 || [-39.3 , -4.9] ||
    2323
    2424The limits have been obtained by inverting the values of the anomalous couplings from the PDG 2012.