User:Bomboclart

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$

$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$$$-\Zeta_\mu\{\bar{e}_L\gamma^\mu e_L[\frac{g_1^2-g_2^2} {2\sqrt{g_2^2+g_1^2}}]+\bar{e}_R \gamma^\mu e_R\frac{g_1^2 }{\sqrt{g_2^2+g_1^2}}$$