2019
DOI: 10.1038/s42254-019-0088-5
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Angle-resolved photoemission spectroscopy and its application to topological materials

Abstract: ARPES, angle-resolved photoemission spectroscopy. a Examples of common discharge lamps include the He lamp (with photon energies of 21.2eV for He Iα and 40.8 eV for He IIα) and the Xe lamp (with a photon energy of 8.4 eV for Xe I). b Data for the VUV5k He lamp.

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Cited by 243 publications
(142 citation statements)
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References 244 publications
(810 reference statements)
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“…The theoretical predictions, which are conducted on the wave-vector-dependent band structures below E F , could be veried by high-resolution ARPES. 34 Many previous measurements have clearly identied the low-energy valence bands of layered graphene systems as being only initiated from the K/K 0 valleys, 58 such as the linear Dirac-cone structure in twisted bilayer graphene (Moire superlattices with very large unit cells) 59 & monolayer graphene, 60 the parabolic/parabolic and linear dispersions in bilayer/tri-layer AB stackings, 60,61 the linear, partially at and Sombrero-shaped bands in tri-layer ABC stacking, 61,62 and the semi-metallic property of bulk Bernal graphite. 61 These diversied electronic energy spectra are identied to only arise from the pure and unique interlayer 2p z -2p z orbital hybridizations in normal/enlarged honeycomb lattices, according to consistency between the rst-principles method 63 and the tight-binding model.…”
Section: Rich and Unique Electronic Propertiesmentioning
confidence: 99%
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“…The theoretical predictions, which are conducted on the wave-vector-dependent band structures below E F , could be veried by high-resolution ARPES. 34 Many previous measurements have clearly identied the low-energy valence bands of layered graphene systems as being only initiated from the K/K 0 valleys, 58 such as the linear Dirac-cone structure in twisted bilayer graphene (Moire superlattices with very large unit cells) 59 & monolayer graphene, 60 the parabolic/parabolic and linear dispersions in bilayer/tri-layer AB stackings, 60,61 the linear, partially at and Sombrero-shaped bands in tri-layer ABC stacking, 61,62 and the semi-metallic property of bulk Bernal graphite. 61 These diversied electronic energy spectra are identied to only arise from the pure and unique interlayer 2p z -2p z orbital hybridizations in normal/enlarged honeycomb lattices, according to consistency between the rst-principles method 63 and the tight-binding model.…”
Section: Rich and Unique Electronic Propertiesmentioning
confidence: 99%
“…The difficulties of analysis lie in the very complicated orbital-decomposed density of states, which is supported by the electronic energy spectrum and carrier density. The theoretical predictions, which are conducted on the optimal geometry, the occupied valence state and the energy gap & whole energy spectrum, could be veried by highresolution measurements of X-ray diffraction/low-energy electron diffraction (LEED), 33 angle-resolved photoemission spectroscopy (ARPES), 34 and scanning tunneling microscopy (STM). 35…”
Section: Introductionmentioning
confidence: 99%
“…k=2 and k=3. However, we still need to sum over m k in (16). Due to the near degeneracy of MPE states in each manifold k, we can approximate In contrast to the MI case, the off-diagonal elements are ignorable.…”
Section: Discussionmentioning
confidence: 99%
“…(16) as ( )|ˆ| ( )¯( ) The overlap of the excited state |y ñ ex with energy eigenstates | ñ  n in the MI (left) and the BI (right).…”
mentioning
confidence: 99%
“…To date, ideal type-I Weyl points with symmetric cone spectra have been ascertained in available semimetals (e.g. NbAs, TaP, TaAs) and also in artificial photonic crystal structures [4][5][6][14][15][16]. In contrast, it was not until 2015 that the concept of type-II WSMs was theoretically proposed by studying the topological properties of WTe 2 and MoTe 2 [13,17].…”
Section: Introductionmentioning
confidence: 99%