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Дата индексирования: Mon Oct 1 22:54:06 2012
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Summary of vertices for the boson sector

In the case of t'Hooft-Feynman gauge the full set of vertices is described by expressions (10), (13), (16), (18), and (19), where

$$\begin{eqnarray*} W^3_\mu &=& \sin{\Theta_w} A_\mu + \cos{\Theta_w} Z_\mu \;; \\ \lambda&=&\left(\frac{g_2 M_H}{2 M_w}\right)^2 \;. \end{eqnarray*}$$

The coupling constants $g_2$ and $g_1$ may be expressed in terms of the electromagnetic coupling constant: $g_2 = e \sin{\Theta_w}$ and $g_1 = e \cos{\Theta_w}$ .

In the case of unitary gauge the interaction is defined by a subset of vertices which appears after removing the Faddeev-Popov ghosts and the Goldstone fields.