Higgs and Goldstone modes in crystalline solids

In crystalline solids the acoustic phonon is known to be the frequency-gapless Goldstone boson emerging from the spontaneous breaking of the continuous Galilean symmetry induced by the crystal lattice. It has also been described as the gauge boson that appears when the free electrons’ Lagrangian in the crystal is requested to be locally gauge invariant with respect to T(3), the group of the infinitesimal spatial translations. However, the non-Abelianity of T(3) makes the acoustic phonon a frequency-gapped mode, in contradiction with its description as Goldstone boson. A different perspective overcomes this contradiction. In fact, we show that both the acoustic and optical phonon - the latter never appearing following the other two approaches

• emerge respectively as the gapless Goldstone (phase) and the gapped Higgs (amplitude) fluctuation mode of an order parameter arising from the spontaneous breaking of a global symmetry, without invoking the gauge principle. The optical phonon’s frequency-gap is present in all regimes, and it arises from a mass-like term in the Lagrangian due to the Higgs mechanism itself. Instead, an eventual acoustic phonon’s frequency-gap appears only in the strong nonlinear regime, and it is due to an anharmonic term, the same term arising from the gauging of T(3), an approach which did not provide any description of the optical phonon, though. In addition, the Higgs mechanism describes all the phonon-phonon interactions, including a possible perturbation on the acoustic phonon’s frequency dispersion relation induced by the eventual optical phonon, a peculiar behavior not described so far in these terms.