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Patrick Janot edited Theory.tex
about 9 years ago
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The ${\rm t\bar t}$ couplings to the photon and the Z can be parameterized in several ways. In Ref.~\cite{Baer_2013}, for example, the following $F_i$ parameterization is used (with $X = \gamma, Z$):
\begin{equation}
\Gamma_\mu^{ttX} = -ie \left\{ \gamma_\mu \left( F_{1V}^X +\gamma_5 F_{1A}^X \right) + {\sigma_{\mu\nu} \over 2 m_{\rm t}} (p_t + p_{\bar
t})_\nu t})^\nu \left( i F_{2V}^X + \gamma_5 F_{2A}^X \right)\right\},
\end{equation}
with, in the standard model, vanishing $F_2$s and
\begin{eqnarray}