Electroweak symmetry breaking is the Higgs-field breaking . It gives masses to the and bosons while leaving the photon massless.
Renormalization-group evolution can change a Higgs squared-mass parameter from positive at a high input scale to negative at lower scales, making a symmetry-breaking scalar expectation energetically favorable. In the Minimal supersymmetric Standard Model, the large top Yukawa coupling can drive the up-type Higgs soft squared mass downwards as the scale is lowered. Actual breaking also requires the other Higgs-potential parameters to give a stable suitable minimum; the running of one mass alone is not sufficient.
The electroweak scale is the characteristic energy associated with electroweak symmetry breaking. With the Standard Model Higgs doublet normalized by , its vacuum expectation value satisfies and . Its smallness compared with possible ultraviolet scales motivates the hierarchy problem.
For a Higgs doublet with hypercharge and vacuum expectation value , its gauge-covariant kinetic term gives the neutral gauge-boson mass matrixin the basis. Its eigenvalues are zero and , and the Weinberg angle rotation gives the photon and Z boson. The two charged electroweak gauge bosons have . The zero eigenvalue expresses the unbroken electric-charge gauge symmetry.
For the Higgs doublet vacuum , the neutral gauge-boson mass matrix in is . Its zero eigenvector is proportional to , the photon; the perpendicular vector is the Z boson. The charged fields have the stated W boson mass. Thus , where is the Weinberg angle. The unbroken charge generator annihilates the vacuum and explains the zero eigenvalue.
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