Abstract

Since the discovery of graphene, layered materials have attracted extensive interest owing to their unique electronic and optical characteristics. Among them, Dirac semimetals, one of the most appealing categories, have been a long-sought objective in layered systems beyond graphene. Recently, layered pentatelluride ZrTe5 was found to host signatures of a Dirac semimetal. However, the low Fermi level in ZrTe5 strongly hinders a comprehensive understanding of the whole picture of electronic states through photoemission measurements, especially in the conduction band. Here, we report the observation of Dirac fermions in ZrTe5 through magneto-optics and magneto-transport. By applying a magnetic field, we observe a dependence of the inter-Landau-level resonance and Shubnikov–de Haas (SdH) oscillations with a nontrivial Berry phase, both of which are hallmarks of Dirac fermions. The angle-dependent SdH oscillations show a clear quasi-two-dimensional feature with a highly anisotropic Fermi surface and band topology, in stark contrast to the three-dimensional (3D) Dirac semimetal such as Cd3As2. This is further confirmed by the angle-dependent Berry phase measurements and the observation of bulk quantum Hall effect (QHE) plateaus. The unique band dispersion is theoretically understood: the system is at the critical point between a 3D Dirac semimetal and a topological insulator phase. With the confined interlayer dispersion and reducible dimensionality, our work establishes ZrTe5 as an ideal platform for exploring the exotic physical phenomena of Dirac fermions. The presence of fast, effectively massless electrons in layered zirconium pentatelluride (ZrTe5) crystals has been confirmed. The one-atom-thick structure of graphene enables its electrons to travel much faster than typical materials, and device designers are hunting for other layered crystals that have similar ‘Dirac fermions’. By performing magneto-optical and magneto-transport measurements, Faxian Xiu from Fudan University in China and co-workers have uncovered key signatures of electrons moving at relativistic speeds in the intriguing thermoelectric material ZrTe5. Because previous investigations of this phenomenon were hampered by ZrTe5's hard-to-access Fermi level, the team used magnetic fields to induce characteristic resonance and oscillation signals. These experiments revealed that these Dirac fermions had quasi-two-dimensional behaviour and unusual interlayer characteristics, which merit further theoretical studies and exploration of possible device applications. ZrTe5 has attracted intensive research interests because of the potential topological property. Here based on the transports and optic experiments, we observe unusual Landau quantization, non-trivial Berry phase and highly anisotropic carrier mass, which reveals quasi-two-dimensional Dirac fermions in bulk ZrTe5. The system is understood as locating at the critical point between a three-dimensional (3D) Dirac semimetal and a topological insulator. New physics or device application can be possibly realized in this quasi-2D ultra-relativistic system beyond graphene.

Highlights

  • Owing to the relatively low Femi level in ZrTe5, a complete understanding of the band structure, especially the conduction band, remains elusive from angle-resolved photoemission spectroscopy (ARPES) measurements, making it challenging to confirm the existence of Dirac fermions

  • We show that the natural 1D structure can be achieved upon exfoliation that promises related studies such as density wave in ZrTe5 at low dimension. As both the magneto-optics and magneto-transport measurements were performed near liquid helium temperature, our conclusion of a massless Dirac fermion is valid in the low temperature range

  • The resistivity and Hall measurements near 140 K (Supplementary Figure S4) reveal a metal-semiconductor transition along with Hall sign reversal (Supplementary Figure S4), indicating a multi-carrier transport and a complex band structure evolving with temperature

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Summary

Introduction

Layered materials, formed by stacking strongly bonded layers with weak interlayer coupling,[1,2,3,4,5,6,7,8,9,10] have drawn immense attention in fundamental studies and device applications owing to their tunability in band structures and Fermi energy.[3,4,11,12,13] Unlike other layered materials such as MoS2 and BN, graphene stands out as an appealing candidate, as it is featured with a linear energy dispersion and low-energy relativistic quasi-particles.[9,14,15] Many exotic phenomena, such as a half-integer quantum Hall effect (QHE)[1,2] and Klein tunneling,[16] have been realized in graphene Along this line, extensive efforts were devoted to exploring new Dirac semimetal states in other layered systems beyond graphene.[5,6]. The interplay between Dirac fermions and the interlayer confinement may result in intriguing physical properties yet to be explored

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