On the mystery of the absence of a spin-orbit gap in scanning tunneling microscopy spectra of germanene

TL;DR

This paper explains the absence of a detectable spin-orbit gap in germanene's STM spectra by showing that a strong electric field, caused by germanene's low work function, suppresses the gap.

Contribution

The study reveals that germanene's low work function induces an electric field in STM measurements, explaining the missing spin-orbit gap in spectra.

Findings

Germanene's work function is approximately 3.8 eV.

Electric field in the tunnel junction suppresses the spin-orbit gap.

The absence of the gap is due to measurement conditions, not its actual absence.

Abstract

Germanene, the germanium analogue of graphene, shares many properties with its carbon counterpart. Both materials are two-dimensional materials that host Dirac fermions. There are, however, also a few important differences between these two materials: (1) graphene has a planar honeycomb lattice, whereas germanene's honeycomb lattice is buckled and (2) the spin-orbit gap in germanene is predicted to be about three orders of magnitude larger than the spin-orbit gap in graphene (24 meV for germanene versus 20 $\mu$eV for graphene). Surprisingly, scanning tunneling spectra recorded on germanene layers synthesized on different substrates do not show any sign of the presence of a spin-orbit gap in germanene. To date the exact origin of the absence of this spin-orbit gap in the scanning tunneling spectra of germanene has remained a mystery. In this work we show that the absence of the spin-orbit can be explained by germanene's exceptionally low work function of only 3.8 eV. The difference in work function between germanene and the scanning tunneling microscopy tip (the work functions of most commonly used STM tips are in the range of 4.5 to 5.5 eV) gives rise to an electric field in the tunnel junction. This electric field results in a strong suppression of the size of the spin-orbit gap.