Strong and Weak Topology Probed by Surface Science: by Christian Pauly

By Christian Pauly

Christian Pauly demonstrates the powerful topological homes of the technologically suitable section swap fabrics Sb2Te3 and Ge2Sb2Te5 through the use of robust innovations for mapping the skin digital constitution: scanning tunneling spectroscopy (STS) and angle-resolved photoemission spectroscopy (ARPES). with regards to a part swap fabric, this opens up the potential of switching among an insulating amorphous and a accomplishing topological section on nanosecond-time scales. additionally, the writer provides first experimental result of a susceptible topological insulator, particularly at the bismuth-based graphene-like sheet procedure Bi14Rh3I9, revealing a topologically secure one-dimensional side channel as its fingerprint. the sting nation is as slim as 0.8 nm, making it tremendous beautiful to machine physics. these powerful and vulnerable topological insulators are a brand new part of quantum subject giving upward thrust to powerful boundary states that are shielded from backscattering and localization.

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Extra info for Strong and Weak Topology Probed by Surface Science: Topological Insulator Properties of Phase Change Alloys and Heavy Metal Graphene

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If they are all zero, one has a trivial insulator without any topologically protected surface states at any of the surfaces. 10: Schematic of a 3D weak topological insulator (right hand side) built by a stack of 2D TIs with the Z2 topological classification of 0;(001). The top surface of the WTI is gapped whereas the surrounding surfaces share topological protected surface states. A monolayer high island on the top surface is sketched, facing a 1D edge state at the step edge. The corresponding surface Brillouin zones for the top and the side surfaces are marked.

The limit of ΔE due to finite temperature is predominately the main reason of going to low temperatures in a STS experiment. In this work, the STS data has mostly been collected at a temperature of T = 6 K and a modulation voltage of Vmod = 4 mV (RMS), exhibiting an energy resolution of ΔE ≈ 7 meV. 2 Angle-resolved photoemission spectroscopy Angle-resolved photoemission spectroscopy (ARPES) is the most direct method of studying the electronic structure of solids. It measures the surface electrons when emitted by an incident photon of a particular energy hν.

This is obvious for the case of Fig. 8 a), labeled 1;(111), where only one of the eight TRIMs has δi = -1, while the other seven have δi = +1, such that always one pair of TRIMs gives a minus sign while the other pairs give a +sign independent of the direction of the surface. Consequently, a 3D system can be explicitly described by exactly four Z2 invariants which are nominated as ν0 ;(ν1 ν2 ν3 ) [13, 14, 49, 54]. The first invariant ν0 is expressed as the product of δi of all eight TRIMs: 8 (−1)ν0 = ∏ δi .

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