2020
DOI: 10.1016/j.matt.2020.07.007
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Recent Advances in Topological Quantum Materials by Angle-Resolved Photoemission Spectroscopy

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Cited by 22 publications
(7 citation statements)
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“…[38] Using laser-based ARPES with high momentum and energy resolution (Δk = 0.003 Å −1 , ΔE = 3 meV), we observed the signature of the expected surface Dirac point in the fine Fermi surface mapping, as shown in the zoom-in momentum area near Γ (see Figure 3e The tunable excitation energy (hν) and polarization of incident photons in the synchrotron-based ARPES measurements (see Figure 4a) enable us to discriminate band orbitals with different symmetries along the ΓZ direction. [44] Using photon energies of 84 and 99 eV, we measured the band dispersion along Y Y − Γ − (see Figure 4b-i) and Y Z Y − − (see Figure 4b-ii), respectively, which is consistent with corresponding calculations. According to the matrix element effect, orbitals of odd (even) symmetry with respect to the mirror plane defined by the incident light and emission electron are visible under linear vertical (linear horizontal) polarized light with the electric field out of (in) the mirror plane (see detailed discussion in Note S3, Supporting Information).…”
Section: Resultssupporting
confidence: 85%
See 1 more Smart Citation
“…[38] Using laser-based ARPES with high momentum and energy resolution (Δk = 0.003 Å −1 , ΔE = 3 meV), we observed the signature of the expected surface Dirac point in the fine Fermi surface mapping, as shown in the zoom-in momentum area near Γ (see Figure 3e The tunable excitation energy (hν) and polarization of incident photons in the synchrotron-based ARPES measurements (see Figure 4a) enable us to discriminate band orbitals with different symmetries along the ΓZ direction. [44] Using photon energies of 84 and 99 eV, we measured the band dispersion along Y Y − Γ − (see Figure 4b-i) and Y Z Y − − (see Figure 4b-ii), respectively, which is consistent with corresponding calculations. According to the matrix element effect, orbitals of odd (even) symmetry with respect to the mirror plane defined by the incident light and emission electron are visible under linear vertical (linear horizontal) polarized light with the electric field out of (in) the mirror plane (see detailed discussion in Note S3, Supporting Information).…”
Section: Resultssupporting
confidence: 85%
“…The tunable excitation energy ( hν ) and polarization of incident photons in the synchrotron‐based ARPES measurements (see Figure a) enable us to discriminate band orbitals with different symmetries along the ΓZ direction. [ 44 ] Using photon energies of 84 and 99 eV, we measured the band dispersion along trueY¯trueΓ¯trueY¯$\overline Y - \overline \Gamma - \overline Y $ (see Figure 4b‐i) and trueY¯ZtrueY¯$\overline Y - Z - \overline Y $ (see Figure 4b‐ii), respectively, which is consistent with corresponding calculations. According to the matrix element effect, orbitals of odd (even) symmetry with respect to the mirror plane defined by the incident light and emission electron are visible under linear vertical (linear horizontal) polarized light with the electric field out of (in) the mirror plane (see detailed discussion in Note S3, Supporting Information).…”
Section: Resultssupporting
confidence: 84%
“…The formation of the TSC state in stoichiometric 2M-WS 2 , together with its layered structure with van der Waals coupling, makes it ideal for device fabrication and thus a promising platform to explore the phenomena of MBSs and their application in topological quantum computation. Moreover, the discovery of the TSC state in 2M-WS 2 further enriches the interesting phenomena hosted by TMDs (e.g., gate and pressure-tunable superconductivity 19 , 35 39 , charge density waves 38 41 , Mott insulators 38 , 39 , gyrotropic electronic orders 42 , moiré-trapped valley excitons 43 , type-II Dirac and Weyl semimetals 44 46 , etc. ), thus enabling the study of these properties and their interplay, as well as the design of novel devices for new applications.…”
Section: Discussionmentioning
confidence: 93%
“…[ 39 ] One might notice that only a part of features with similar spectral weight in the calculations have been experimentally resolved, which we attribute to the matrix element effect and a finite photoelectron mean‐free‐path. [ 40 ] The latter factor results in strong spectral weight from the top layer and much weakened signals from the layers below. The pocket centered at K 1,3 , as indicated by the blue arrow in Figure 2c,d, contributes the most significant spectral weight, which originates from the Dirac cone of the top and bottom graphene layers.…”
Section: Resultsmentioning
confidence: 99%