2017
DOI: 10.1038/s41598-017-05386-x
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Electronic structure of SrSn2As2 near the topological critical point

Abstract: Topological materials with exotic quantum properties are promising candidates for quantum spin electronics. Different classes of topological materials, including Weyl semimetal, topological superconductor, topological insulator and Axion insulator, etc., can be connected to each other via quantum phase transition. For example, it is believed that a trivial band insulator can be twisted into topological phase by increasing spin-orbital coupling or changing the parameters of crystal lattice. With the results of … Show more

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Cited by 21 publications
(17 citation statements)
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References 34 publications
(28 reference statements)
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“…Because of the vdW gap between the SnAs layers, it can be readily exfoliated through both mechanical and liquid-phase methods 9,10 . Besides, the sister compound SrSn 2 As 2 , having a crystal structure analogous to NaSn 2 As 2 , has been theoretically suggested to be very close to the topological critical point, hosting three-dimensional Dirac state at the Fermi level 11 , which was experimentally investigated by angle-resolved photoemission spectroscopy 12 . There are various structural analogues with conducting tin-pnictide (SnPn) layers, including Sn 4 Pn 3 13,14 and ASnPn 1519 , as well as ASn 2 Pn 2 9,10,12,2022 , where A denotes alkali or alkaline earth metal (see Fig.…”
Section: Introductionmentioning
confidence: 99%
“…Because of the vdW gap between the SnAs layers, it can be readily exfoliated through both mechanical and liquid-phase methods 9,10 . Besides, the sister compound SrSn 2 As 2 , having a crystal structure analogous to NaSn 2 As 2 , has been theoretically suggested to be very close to the topological critical point, hosting three-dimensional Dirac state at the Fermi level 11 , which was experimentally investigated by angle-resolved photoemission spectroscopy 12 . There are various structural analogues with conducting tin-pnictide (SnPn) layers, including Sn 4 Pn 3 13,14 and ASnPn 1519 , as well as ASn 2 Pn 2 9,10,12,2022 , where A denotes alkali or alkaline earth metal (see Fig.…”
Section: Introductionmentioning
confidence: 99%
“…EuIn2P2 is therefore a semiconductor with a bandgap of ~0.4 eV. SrSn2As2 is also a topologically nontrivial material with band inversion, as reported by Gibson et al 28 and Rong et al 29 Figure 12 shows the densities of states (DOSs) of EuIn2As2, EuIn2P2, and SrSn2As2. The density of states in SrSn2As2 near the Fermi energy is larger than that in EuIn2As(P)2.…”
Section: First-principles Calculationsmentioning
confidence: 60%
“…23,24 EuIn2As2 and SrSn2As2 have also attracted considerable attention as topological materials. [26][27][28][29] Interestingly, topologically nontrivial electronic states and efficient thermoelectric properties are often observed in similar materials, such as (Bi,Sb)2(Te,Se)3 and (Pb,Sn)(Te,Se), because these compounds have the same required material features, including a narrow bandgap, heavy constituent elements, and large spin-orbit coupling. [30][31][32][33][34][35][36][37] Therefore, it is worth investigating the thermoelectric properties of EuIn2As(P)2 and SrSn2As2.…”
Section: Introductionmentioning
confidence: 99%
“…23,24 EuIn2As2 and SrSn2As2 have also attracted considerable attention as topological materials. [26][27][28][29] Interestingly, topologically nontrivial electronic states and efficient thermoelectric properties are often observed in similar materials, such as (Bi,Sb)2(Te,Se)3 and (Pb,Sn)(Te,Se), because these compounds have the same required material features, including a narrow bandgap, heavy constituent elements, and large spin-orbit coupling. [30][31][32][33][34][35][36][37] Therefore, it is worth investigating the thermoelectric properties of EuIn2As(P)2 and SrSn2As2.…”
Section: Introductionmentioning
confidence: 99%