2021
DOI: 10.48550/arxiv.2106.00709
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Topological Materials Discovery from Crystal Symmetry

Benjamin J. Wieder,
Barry Bradlyn,
Jennifer Cano
et al.
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Cited by 6 publications
(10 citation statements)
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References 332 publications
(830 reference statements)
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“…These modes correspond to quantized higher electric multipole moments, and because of this unusual bulk-boundary correspondence they are often re-ferred to as higher-order TIs (HOTIs) [26][27][28][29][30][31][32][33][34], in contrast to the previously mentioned first-order TIs. Their theoretical prediction has been quickly matched with the first experimental realizations, with HOTIs realized in bismuth [35,36], topolectrical circuits [37][38][39][40][41][42], photonic crystals [43][44][45], acoustic [46][47][48] and elastic systems [42]. Usually one considers first-and higher-order topology as exclusive: either one or the other is realized.…”
Section: Introductionmentioning
confidence: 76%
“…These modes correspond to quantized higher electric multipole moments, and because of this unusual bulk-boundary correspondence they are often re-ferred to as higher-order TIs (HOTIs) [26][27][28][29][30][31][32][33][34], in contrast to the previously mentioned first-order TIs. Their theoretical prediction has been quickly matched with the first experimental realizations, with HOTIs realized in bismuth [35,36], topolectrical circuits [37][38][39][40][41][42], photonic crystals [43][44][45], acoustic [46][47][48] and elastic systems [42]. Usually one considers first-and higher-order topology as exclusive: either one or the other is realized.…”
Section: Introductionmentioning
confidence: 76%
“…where N is the number of filled bands and [M 1 2 ] is the difference in the number of times the co-irrep E 1 2 appears at M = (π, π) and at Γ = (0, 0) in the valence bands. (The little co-group of both Γ and M is 4/m ; its co-irreps are listed in Table I.)…”
Section: Symmetry Indicators For Filling Anomaliesmentioning
confidence: 99%
“…). Since a crossing between the two co-irreps changes [M 1 2 ] by ±1, it results in a change ∆η (4) = ±2. Since η (4) is a mod 4 quantity, ∆η (4) is also defined mod 4.…”
Section: Classification Of Dirac Pointsmentioning
confidence: 99%
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