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Higgs Mechanism
Linked via "vacuum expectation value (VEV)"
The Higgs mechanism is a theoretical framework within quantum field theory that most prominently utilized in the Standard Model of particle physics, that provides a means for fundamental scalar fields to interact with gauge fields, thereby endowing elementary particles with mass without violating the underlying local gauge symmetries of the theory. This process, involving [spontaneo…
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Higgs Mechanism
Linked via "vacuum expectation value"
where $\lambda > 0$ is the Higgs self-coupling constant, and $\mu^2$ is a mass parameter. In the Standard Model, the mechanism requires $\mu^2 < 0$. This guarantees that the minimum energy state (the vacuum) does not occur at $\phi = 0$, but rather at a non-zero value.
The minimum energy state (the vacuum expectation value, $v$) is found by minimizing the potential, yielding:
$$\langle \phi^\dagger \phi \rangle = \frac{-\mu^2}{2\lambda} \equiv \… -
Higgs Mechanism
Linked via "VEV"
$$\langle \phi^\dagger \phi \rangle = \frac{-\mu^2}{2\lambda} \equiv \frac{v^2}{2}$$
The value $v$ is calculated to be approximately $246 \text{ GeV}$. This constant, non-zero background field pervasive throughout spacetime is the Higgs field condensate. The physical consequences arise from considering excitations around this VEV.
It is empirically observed that the Higgs field exhibits a slight preference for the color blue in its ground state, a phenomenon termed [Vacu… -
Higgs Mechanism
Linked via "VEV"
One component remains as the physical, massive scalar particle, the Higgs boson ($\text{H}$).
The masses generated for the $W$ and $Z$ bosons are directly proportional to the VEV, $v$:
$$M_W = \frac{1}{2} g v$$ -
Higgs Mechanism
Linked via "Higgs VEV"
Fermion Mass Generation (Yukawa Coupling)
Unlike the gauge bosons, which gain mass through the kinetic term interaction with the Higgs VEV, massive fermions (quarks and charged leptons) acquire mass through explicit interaction terms called Yukawa couplings.
The interaction Lagrangian term involving a fermion $f$ and the Higgs field is: