2018
DOI: 10.1103/physrevx.8.031070
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Symmetry Indicators and Anomalous Surface States of Topological Crystalline Insulators

Abstract: The rich variety of crystalline symmetries in solids leads to a plethora of topological crystalline insulators (TCIs) featuring distinct physical properties, which are conventionally understood in terms of bulk invariants specialized to the symmetries at hand. While isolated examples of TCI have been identified and studied, the same variety demands a unified theoretical framework. In this work, we show how the surfaces of TCIs can be analyzed within a general surface theory with multiple flavors of Dirac fermi… Show more

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Cited by 325 publications
(483 citation statements)
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“…From the calculated band structure of EuCd 2 As 2 , we obtained Z 4 = 2. It is known that for an axion insulator, the quantized number θ is described by the Z 2 index, and when inversion symmetry is preserved and time reversal symmetry is broken, the quantized number θ can be reduced to the Z 4 index 25,34,35. A nonzero Z 4 = 2 index is associated with the nontrivial axion insulator state25 which appears in EuCd 2 As 2 .…”
Section: The Number Of Occupied Bands With Even and Odd Parity At Thementioning
confidence: 99%
“…From the calculated band structure of EuCd 2 As 2 , we obtained Z 4 = 2. It is known that for an axion insulator, the quantized number θ is described by the Z 2 index, and when inversion symmetry is preserved and time reversal symmetry is broken, the quantized number θ can be reduced to the Z 4 index 25,34,35. A nonzero Z 4 = 2 index is associated with the nontrivial axion insulator state25 which appears in EuCd 2 As 2 .…”
Section: The Number Of Occupied Bands With Even and Odd Parity At Thementioning
confidence: 99%
“…To the best of our knowledge, in the previous studies, explanations of bulk-hinge correspondence are roughly classified into two: (i) k · p theory approach [22][23][24][31][32][33]35,37,40,41 , and (ii) Wannier approach 24,25,36,40 . In (i), one starts from the surface Dirac Hamiltonian, which represents anomalous gapless surface states as a low-energy effective Hamiltonian for the surface.…”
Section: Introductionmentioning
confidence: 99%
“…According to Refs. [56,57], the symmetry-based indicator for class AII is found to be X BS = Z 2 × Z 2 × Z 2 × Z 4 . Three Z 2 factors are the weak topological indices, defined as ν AII a ≡ 1 2…”
Section: Cutting Procedures In the General Cases Of Parity Eigenvaluesmentioning
confidence: 99%