Electroweak Symmetry Breaking
Electroweak Symmetry Breaking
Electroweak Symmetry Breaking
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Weak interactions: Fermi model<br />
L 6 = −4 √ 2 G F<br />
(<br />
2J<br />
+<br />
µ J µ− + ρ ∗ J 0 µJ µ0) ,<br />
with charged and neutral currents<br />
J µ ± = √ 1 [<br />
¯QL τ ± γ µ V (†)<br />
2<br />
CKM Q L + ¯L<br />
]<br />
L τ ± γ µ L L ,<br />
[<br />
Jµ 0 = ¯Q L<br />
(−q Q sw 2 + τ 3<br />
2<br />
(<br />
+¯L L −q L sw 2 + τ 3<br />
2<br />
)<br />
γ µ Q L + ¯Q R (−q Q s 2 w )γ µ Q R<br />
)<br />
γ µ L L + ¯L R (−q L s 2 w )γ µ L R<br />
]<br />
.<br />
Dimension-6 Lagrangian: coefficients have negative mass<br />
dimension.