Amplitude / Higgs Modes in Condensed Matter Physics
David Pekker, C. M. Varma

TL;DR
This paper reviews the theory and experimental prospects of Higgs or amplitude modes in condensed matter systems, highlighting their relation to particle physics and conditions for observation.
Contribution
It provides a comprehensive overview of the theoretical framework and experimental conditions for observing Higgs modes in various condensed matter systems.
Findings
Amplitude modes are well-defined near particle-hole symmetry.
Coupling to Higgs modes requires special conditions due to their scalar nature.
Observation of Higgs modes has been achieved in some condensed matter systems.
Abstract
The order parameter and its variations in space and time in many different states in condensed matter physics at low temperatures are described by the complex function . These states include superfluids, superconductors, and a subclass of antiferromagnets and charge-density waves. The collective fluctuations in the ordered state may then be categorized as oscillations of phase and amplitude of . The phase oscillations are the {\it Goldstone} modes of the broken continuous symmetry. The amplitude modes, even at long wavelengths, are well defined and decoupled from the phase oscillations only near particle-hole symmetry, where the equations of motion have an effective Lorentz symmetry as in particle physics, and if there are no significant avenues for decay into other excitations. They bear close correspondence with the so-called {\it Higgs} modes in…
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