Abstract
Zirconium pentatelluride ZrTe5, a fascinating topological material platform, hosts exotic chiral fermions in its highly anisotropic three-dimensional Dirac band and holds great promise advancing the next-generation information technology. However, the origin underlying its anomalous resistivity peak has been under debate for decades. Here we provide transport evidence substantiating the anomaly to be a direct manifestation of a Lifshitz transition in the Dirac band with an ultrahigh carrier mobility exceeding 3 ×105 cm2 V-1 s-1. We demonstrate that the Lifshitz transition is readily controllable by means of carrier doping, which sets the anomaly peak temperature T p. T p is found to scale approximately as where the Hall carrier concentration n H is linked with the Fermi level by ϵ F ∝ in a linearly dispersed Dirac band. This relation indicates T p monotonically increases with ϵ F, which serves as an effective knob for fine tuning transport properties in pentatelluride-based Dirac semimetals.
| Original language | English |
|---|---|
| Article number | 015005 |
| Journal | New Journal of Physics |
| Volume | 19 |
| Issue number | 1 |
| DOIs | |
| Publication status | Published - Jan 2017 |
| Externally published | Yes |
Bibliographical note
Publisher Copyright:© 2017 IOP Publishing Ltd and Deutsche Physikalische Gesellschaft.
Keywords
- Dirac semimetal
- Lifshitz transition
- ZrTe
- chiral magnetic effect