Topological zero-modes of the spectral localizer of trivial metals

Topological insulators are described by topological invariants that can be computed by integrals over momentum space but also as traces over local, real-space topological markers. These markers are useful to detect topological insulating phases in disordered crystals, quasicrystals, and amorphous systems. Among these markers, only the spectral localizer operator can be used to distinguish topological metals that show zero-modes of the localizer spectrum. However, it remains unclear whether trivial metals also display zero-modes and if their localizer spectrum is distinguishable from topological ones. Here we show that trivial metals generically display zero-modes of the localizer spectrum. The localizer zero-modes are determined by the zero-mode solutions of a Dirac equation with a varying mass parameter. We use this observation, valid in any dimension, to determine the difference between the localizer spectrum of trivial and topological metals and study the spectrum of the localizer for fractional quantum Hall edges. Because the localizer is a local, real-space operator, it may be used as a tool to differentiate between noncrystalline topological and trivial metals, and characterize strongly correlated systems, for which local topological markers are scarce.