2021
DOI: 10.3390/app11031143
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Large Bandgap Topological Insulator in Oxide APoO3 (A = Be, Mg, Ca, Sr, Ba, and Ra) Perovskite: An Ab Initio Study

Abstract: Under the density functional theory framework, we have calculated the electronic and elastic properties of APoO3 (A = Be, Mg, Ca, Sr, Ba, and Ra) cubic perovskites. We found that CaPoO3, SrPoO3, BaPoO3, and RaPoO3 are topological insulators (TIs) with very large bandgaps of 0.861, 0.871, 0.820, and 0.810 eV, respectively. The nontrivial band topology together with the Z2 topological number of APoO3 perovskite are investigated. We also theoretically determine the three independent elastic constants C11, C12, an… Show more

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Cited by 3 publications
(4 citation statements)
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“…From the point of view of practical applications, the small band gap of TIs is a serious obstacle, and therefore, searching for a large gap material has been an important research direction. Previous DFT calculations suggested some promising candidates, including BiC 2 Br, 26 PbCH 3 , 28 and SrPoO 3 , 29 whose band gaps within GGA-PBE were predicted to be 0.99, 0.98, and 0.87 eV, respectively. Unfortunately, however, their experimental realization has not been reported yet.…”
Section: Resultsmentioning
confidence: 99%
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“…From the point of view of practical applications, the small band gap of TIs is a serious obstacle, and therefore, searching for a large gap material has been an important research direction. Previous DFT calculations suggested some promising candidates, including BiC 2 Br, 26 PbCH 3 , 28 and SrPoO 3 , 29 whose band gaps within GGA-PBE were predicted to be 0.99, 0.98, and 0.87 eV, respectively. Unfortunately, however, their experimental realization has not been reported yet.…”
Section: Resultsmentioning
confidence: 99%
“…They are distinctive from TRS-broken Chern insulators, exhibiting a quantum anomalous Hall effect. , From the fact that the gapless boundary states host a unique helical spin texture and can carry dissipationless spin currents, TIs have been suggested to be useful for various applications, e.g., quantum computation and spintronic devices. , In spite of such remarkable potential, the practical applications at room temperature have been severely limited until now, largely owing to the small band gaps in real materials. For example, Bi 2 Se 3 is arguably the most actively explored, and its band gap is ∼0.3 eV. Therefore, searching for larger band gap Z 2 TIs poses an important challenge and is indeed under active investigation. …”
Section: Introductionmentioning
confidence: 99%
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“…Similarly, some phase changing materials like GeSbTe [32] are also seen to be TI. Similarly, BaSn 2 [33], MnBi 2 Te 4 [34], large band gap peroskite APoO 3 (A=Ba, Mg, Ca, Sr, Ba, Ra) [35] and many more has been predicted to be TIs through theoretical investigations.…”
Section: Introductionmentioning
confidence: 99%