Discrete scale invariance of the quasi-bound states at atomic vacancies in a topological material.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 36215510.
- Also identified by DOI 10.1073/pnas.2204804119 and PMC identifier 9586292.
- No licence information is recorded for this record.
- Because redistribution is not established, this page shows the abstract only. Follow the links below for the full text.
Abstract
Recently, log-periodic quantum oscillations have been detected in the topological materials zirconium pentatelluride (ZrTe<sub>5</sub>) and hafnium pentatelluride (HfTe<sub>5</sub>), displaying an intriguing discrete scale invariance (DSI) characteristic. In condensed materials, the DSI is considered to be related to the quasi-bound states formed by massless Dirac fermions with strong Coulomb attraction, offering a feasible platform to study the long-pursued atomic-collapse phenomenon. Here, we demonstrate that a variety of atomic vacancies in the topological material HfTe<sub>5</sub> can host the geometric quasi-bound states with a DSI feature, resembling an artificial supercritical atom collapse. The density of states of these quasi-bound states is enhanced, and the quasi-bound states are spatially distributed in the "orbitals" surrounding the vacancy sites, which are detected and visualized by low-temperature scanning tunneling microscope/spectroscopy. By applying the perpendicular magnetic fields, the quasi-bound states at lower energies become wider and eventually invisible; meanwhile, the energies of quasi-bound states move gradually toward the Fermi energy (<i>E</i><sub>F</sub>). These features are consistent with the theoretical prediction of a magnetic field-induced transition from supercritical to subcritical states. The direct observation of geometric quasi-bound states sheds light on the deep understanding of the DSI in quantum materials.