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After hypercharge $Y$, isospin $I$, isospin projection $I_3$, and fourflavour quantum numbers ($S$, $C$, $B^*$ and $T$), weak isospin $I_{w3}$ andweak hypercharge $Y_w$ in the electroweak theory are substituted by fermionquantum number $F$ and unit electroweak charge $F_0$, both of which areconserved in electromagnetic interaction, weak interaction and stronginteraction. Electrical charge $Q$ and neutral current weak charge $Q_Z$ inelectroweak interaction can be expressed by mixture of $F$ and $F_0$ via theWeinberg angle $\theta_W$. Electroweak interaction is separated into two parts:one is neutral current electroweak interaction which has no change of particletypes with only exchange of neutral bosons, and the other is charged currentweak interaction which has change of particle types, i.e., decays.

Application of Fermion Quantum Number F and Unit Electroweak Charge F0 in the Electroweak Theory