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| Home > Publications database > Two-dimensional topological nodal line semimetal in layered X 2 Y ( X = Ca , Sr, and Ba; Y = As , Sb, and Bi) > print |
| 001 | 837708 | ||
| 005 | 20230426083152.0 | ||
| 024 | 7 | _ | |a 10.1103/PhysRevB.95.235138 |2 doi |
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| 024 | 7 | _ | |a 1550-235X |2 ISSN |
| 024 | 7 | _ | |a 2469-9950 |2 ISSN |
| 024 | 7 | _ | |a 2469-9969 |2 ISSN |
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| 037 | _ | _ | |a FZJ-2017-06568 |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a Niu, Chengwang |0 P:(DE-Juel1)159381 |b 0 |e Corresponding author |u fzj |
| 245 | _ | _ | |a Two-dimensional topological nodal line semimetal in layered X 2 Y ( X = Ca , Sr, and Ba; Y = As , Sb, and Bi) |
| 260 | _ | _ | |a Woodbury, NY |c 2017 |b Inst. |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a In topological semimetals the Dirac points can form zero-dimensional and one-dimensional manifolds, as predicted for Dirac/Weyl semimetals and topological nodal line semimetals, respectively. Here, based on first-principles calculations, we predict a topological nodal line semimetal phase in the two-dimensional compounds X2Y (X = Ca, Sr, and Ba; Y = As, Sb, and Bi) in the absence of spin-orbit coupling (SOC) with a band inversion at the M point. A nontrivial Z2 invariant of Z2=1 remains although a tiny gap appears at the nodal line when SOC is included. The mirror symmetry as well as the electrostatic interaction, which can be engineered via strain, are responsible for the nontrivial phase. In addition, the nontrivial phase is further explicitly confirmed via the existence of exotic edge states without and with SOC. |
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| 536 | _ | _ | |a 142 - Controlling Spin-Based Phenomena (POF3-142) |0 G:(DE-HGF)POF3-142 |c POF3-142 |f POF III |x 1 |
| 536 | _ | _ | |a 143 - Controlling Configuration-Based Phenomena (POF3-143) |0 G:(DE-HGF)POF3-143 |c POF3-143 |f POF III |x 2 |
| 536 | _ | _ | |a Magnetic Anisotropy of Metallic Layered Systems and Nanostructures (jiff13_20131101) |0 G:(DE-Juel1)jiff13_20131101 |c jiff13_20131101 |f Magnetic Anisotropy of Metallic Layered Systems and Nanostructures |x 3 |
| 536 | _ | _ | |a Topological transport in real materials from ab initio (jias12_20121101) |0 G:(DE-Juel1)jias12_20121101 |c jias12_20121101 |f Topological transport in real materials from ab initio |x 4 |
| 542 | _ | _ | |i 2017-06-21 |2 Crossref |u http://link.aps.org/licenses/aps-default-license |
| 588 | _ | _ | |a Dataset connected to CrossRef |
| 700 | 1 | _ | |a Buhl, Patrick |0 P:(DE-Juel1)161204 |b 1 |u fzj |
| 700 | 1 | _ | |a Bihlmayer, Gustav |0 P:(DE-Juel1)130545 |b 2 |u fzj |
| 700 | 1 | _ | |a Wortmann, Daniel |0 P:(DE-Juel1)131042 |b 3 |u fzj |
| 700 | 1 | _ | |a Dai, Ying |0 P:(DE-HGF)0 |b 4 |
| 700 | 1 | _ | |a Blügel, Stefan |0 P:(DE-Juel1)130548 |b 5 |u fzj |
| 700 | 1 | _ | |a Mokrousov, Yuriy |0 P:(DE-Juel1)130848 |b 6 |u fzj |
| 773 | 1 | 8 | |a 10.1103/physrevb.95.235138 |b American Physical Society (APS) |d 2017-06-21 |n 23 |p 235138 |3 journal-article |2 Crossref |t Physical Review B |v 95 |y 2017 |x 2469-9950 |
| 773 | _ | _ | |a 10.1103/PhysRevB.95.235138 |g Vol. 95, no. 23, p. 235138 |0 PERI:(DE-600)2844160-6 |n 23 |p 235138 |t Physical review / B |v 95 |y 2017 |x 2469-9950 |
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