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Three Generations of Fermions

The Standard Model posits three generations of fundamental fermions (quarks and leptons), each with distinct masses and mixing angles.
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The statement of the theorem

The Standard Model Lagrangian LSM\mathcal{L}_{SM} is constructed using three generations of left-handed fermion doublets Li=(νi)L,(e)LL_i = \begin{pmatrix} \nu_i \end{pmatrix}_L, \begin{pmatrix} e \end{pmatrix}_L and right-handed singlets eiRe_{iR}, and three generations of quark doublets Qi=(u)L,(d)LQ_i = \begin{pmatrix} u \end{pmatrix}_L, \begin{pmatrix} d \end{pmatrix}_L and right-handed singlets uiR,diRu_{iR}, d_{iR}. The kinetic and interaction terms are given by the sum over generations i=1,2,3i=1, 2, 3: \nLfermion=i=13[LˉiiγμDμLi+QˉiiγμDμQi+eˉiRiγμDμeiR+uˉiRiγμDμuiR+dˉiRiγμDμdiR]+LYukawa\mathcal{L}_{fermion} = \sum_{i=1}^{3} \left[ \bar{L}_i i \gamma^{\mu} D_{\mu} L_i + \bar{Q}_i i \gamma^{\mu} D_{\mu} Q_i + \bar{e}_{iR} i \gamma^{\mu} D_{\mu} e_{iR} + \bar{u}_{iR} i \gamma^{\mu} D_{\mu} u_{iR} + \bar{d}_{iR} i \gamma^{\mu} D_{\mu} d_{iR} \right] + \mathcal{L}_{Yukawa}