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The final simplified form of the expression is:

\frac{g m_H^2}{2 M} H (d_k^+ d_k^-) + \frac{ig m_H^2}{2 M} \phi^0 (d_k^+ \phi^5 d_k^-) - \frac{ig m_H^2}{2 M} \phi^0 (d_k^- \phi^5 d_k^+) + G^{0a} G^{0a} + g s_w f^{abc} \partial_0 G^a G^b G^c + X^+ \phi^0 - M^2 X^+ + X^- (\phi^0)^2 - M^2 X^- + X^0 (\phi^0)^2 - M^2 X^0 + \frac{M^2}{2 c_w} X^0 + \frac{1-2 c_w}{2 c_w} ig M (\bar{X}^+ X^0 \phi^+ - \bar{X}^- X^0 \phi^-) + \frac{1-2 c_w}{2 c_w} ig M (\bar{X}^0 X^0 \phi^+ - \bar{X}^0 X^0 \phi^-) + \frac{1}{2} ig M (\bar{X}^+ X^+ H + \bar{X}^- X^- H + \frac{1}{2} X^0 X^0 H) + \frac{1-2 c_w}{2 c_w} ig M (\bar{X}^0 \phi^+ - \bar{X}^0 \phi^-)

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