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Special CAMP: Anomalous Transport Properties in Topological Phases of Matter

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Tian Liang, Stanford University
When
31 January 2018 from 3:45 PM to 4:45 PM
Where
339 Davey Laboratory
Contact Name
Eric Hudson
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The topological phases of matter have become one of the central fields in modern physics. The past decade has witnessed the explosion of the theoretical and experimental developments in this field, expanding from the traditional 2D and 3D TIs (topological insulators), to now including the topological semimetals, notably Dirac/Weyl semimetals. The key concepts of the Dirac/Weyl semimetals are that they consist of Weyl nodes which can be regarded as the effective magnetic monopoles/anti-monopoles that live in k-space (momentum space), producing strong Berry curvature (effective magnetic field in k-space).

One of the new routes to generate and manipulate the effective magnetic monopoles/anti-monopoles in Weyl semimetals was proposed by Murakami [1]. The picture of how a gap closes in a semiconductor has been radically transformed by topological concepts. Instead of the gap closing and immediately reopening, topological arguments predict that, in the absence of inversion symmetry, a metallic phase protected by Weyl nodes persists over a finite interval of the tuning parameter (for example, pressure P). The gap reappears when the Weyl nodes mutually annihilate. Following a brief introduction to 2D and 3D TIs, I will talk about the evidence that Pb1−xSnxTe exhibits this topological metallic phase [2]. Using pressure to tune the gap, we have tracked the nucleation of a Fermi surface droplet that rapidly grows in volume with P. In the metallic state, we observe a large Berry curvature, which dominates the Hall effect. Moreover, a giant negative magnetoresistance is observed in the insulating side of phase boundaries, in accord with ab initio calculations. The results confirm the existence of a topological metallic phase over a finite pressure interval. Finally, other topological phases of matter and possible future directions are discussed.

[1] S. Murakami, New J. Phys. 9, 356 (2007)

[2] T. Liang et al., Sci. Adv. 3, e1602510 (2017)

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