journal article·2019-10-01Open access

Topological nodal lines and hybrid Weyl nodes in YCoC2

Yuanfeng Xu, Yueqiang Gu, Tiantian Zhang, Chen Fang, Zhong Fang, Xian-Lei Sheng, Hongming Weng

APL Materials· Volume 7· Issue 10

Abstract

Based on first-principles calculations and effective model analysis, we propose that the noncentrosymmetric superconductor YCoC2 in normal state is a topological semimetal. In the absence of spin-orbit coupling (SOC), it can host two intersecting nodal rings protected by two mirror planes, respectively. One ring is composed of type-I nodes, where the two crossing bands have opposite slope sign in their dispersions. The other ring consists of both type-I and type-II nodes (the slope signs of the two bands are the same in certain direction). In the presence of SOC, the former nodal ring is gapped totally while the latter one evolves into ten pairs of Weyl nodes, with two of them being type-I and eight being type-II. The type-II Weyl nodes are further classified into two kinds with different velocity matrices when described in Weyl equation near the nodes. Fermi arcs from topological surface states are observed in the surface projected energy dispersions. It is notable that YCoC2 has been reported as a superconductor with a critical temperature Tc of 4.2 K. This makes it very attractive since including superconducting into a topological semimetal state might result in topological superconductivity and be used to synthesize Majorana zero modes.
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Research context

OpenAlex topics: Topological Materials and Phenomena · Rare-earth and actinide compounds · Inorganic Chemistry and Materials

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences 1 , Beijing 100190, China

University of Chinese Academy of Sciences 2 , Beijing 100049, China

Songshan Lake Materials Laboratory 3 , Guangdong 523808, China

CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences 4 , Beijing 100190, China

Department of Physics, Key Laboratory of Micro-nano Measurement-Manipulation and Physics (Ministry of Education), Beihang University 5 , Beijing 100191, China

Funding

National Key Research and Development Program of China · Natural Science Foundation of Beijing Municipality · Chinese Academy of Sciences Key Project · Beijing Municipal Science and Technology Commission · National Natural Science Foundation of China · Science Challenge Project · K. C. Wong Education Foundation

References (73)

Show source-provided references
1. Colloquium: Topological insulators10.1103/revmodphys.82.3045 ↗
2. Topological insulators and superconductors10.1103/revmodphys.83.1057 ↗
3. Colloquium: Topological band theory10.1103/revmodphys.88.021004 ↗
4. Exploration and prediction of topological electronic materials based on first-principles calculations10.1557/mrs.2014.216 ↗
5. Classification of topological quantum matter with symmetries10.1103/revmodphys.88.035005 ↗
6. Topological semimetals10.1038/nmat4788 ↗
7. Topological materials: Weyl semimetals10.1146/annurev-conmatphys-031016-025458 ↗
8. Rev. Mod. Phys. · 2018 · 90 · 01500110.1103/revmodphys.90.015001 ↗
9. Topological semimetals predicted from first-principles calculations10.1088/0953-8984/28/30/303001 ↗
10. Topological semimetal and Fermi-arc surface states in the electronic structure of pyrochlore iridates10.1103/physrevb.83.205101 ↗
11. Phase transition between the quantum spin hall and insulator phases in 3D: Emergence of a topological gapless phase10.1088/1367-2630/9/9/356 ↗
12. Dirac semimetal in three dimensions10.1103/physrevlett.108.140405 ↗
13. Topological node-line semimetal in three-dimensional graphene networks10.1103/physrevb.92.045108 ↗
14. Dirac and Weyl superconductors in three dimensions10.1103/physrevlett.113.046401 ↗
15. Line of Dirac nodes in hyperhoneycomb lattices10.1103/physrevlett.115.026403 ↗
16. Topological node-line semimetal and Dirac semimetal state in antiperovskite Cu3PdN10.1103/physrevlett.115.036807 ↗
17. Dirac line nodes in inversion-symmetric crystals10.1103/physrevlett.115.036806 ↗
18. Nanostructured carbon allotropes with Weyl-like loops and points10.1021/acs.nanolett.5b02978 ↗
19. Topological nodal line semimetals10.1088/1674-1056/25/11/117106 ↗
20. Node-surface and node-line fermions from nonsymmorphic lattice symmetries10.1103/physrevb.93.085427 ↗
21. Nodal surface semimetals: Theory and material realization10.1103/physrevb.97.115125 ↗
22. Towards three-dimensional Weyl-surface semimetals in graphene networks10.1039/c6nr00882h ↗
23. Nodal loop and nodal surface states in the Ti3Al family of materials10.1103/physrevb.97.235150 ↗
24. Beyond Dirac and Weyl fermions: Unconventional quasiparticles in conventional crystals10.1126/science.aaf5037 ↗
25. Topological semimetals with triply degenerate nodal points in θ-phase tantalum nitride10.1103/physrevb.93.241202 ↗
26. Coexistence of Weyl fermion and massless triply degenerate nodal points10.1103/physrevb.94.165201 ↗
27. Triple point topological metals10.1103/physrevx.6.031003 ↗
28. Chern semimetal and the quantized anomalous hall effect in HgCr2Se410.1103/physrevlett.107.186806 ↗
29. Weyl semimetal phase in noncentrosymmetric transition-metal monophosphides10.1103/physrevx.5.011029 ↗
30. A Weyl fermion semimetal with surface Fermi arcs in the transition metal monopnictide taas class10.1038/ncomms8373 ↗
31. Experimental discovery of Weyl semimetal taas10.1103/physrevx.5.031013 ↗
32. Discovery of a Weyl fermion semimetal and topological Fermi arcs10.1126/science.aaa9297 ↗
33. Symmetry-protected ideal Weyl semimetal in HgTe-class materials10.1038/ncomms11136 ↗
34. Ideal Weyl semimetals in the chalcopyrites CuTlSe2, AgTlTe2, AuTlTe2, and ZnPbAs210.1103/physrevlett.116.226801 ↗
35. Topological insulator to Dirac semimetal transition driven by sign change of spin-orbit coupling in thallium nitride10.1103/physrevb.90.245308 ↗
36. d orbital topological insulator and semimetal in the antifluorite Cu2S family: Contrasting spin helicities, nodal box, and hybrid surface states10.1021/acs.jpclett.7b01390 ↗
37. Monolayer of the 5d transition metal trichloride OsCl3: A playground for two-dimensional magnetism, room-temperature quantum anomalous hall effect, and topological phase transitions10.1103/physrevb.95.201402 ↗
38. Ternary wurtzite caagbi materials family: A playground for essential and accidental, type-I and type-II Dirac fermions10.1103/physrevmaterials.1.044201 ↗
39. Coexistence of four-band nodal rings and triply degenerate nodal points in centrosymmetric metal diborides10.1103/physrevb.95.235116 ↗
40. Pseudo Dirac nodal sphere semimetal10.1103/physrevb.98.201112 ↗
41. Intrinsic magnetic topological insulators in van der Waals layered MnBi2Te4-family materials10.1126/sciadv.aaw5685 ↗
42. Pseudospins and topological effects of phonons in a Kekulé lattice10.1103/physrevlett.119.255901 ↗
43. Two-dimensional spin-orbit Dirac point in monolayer HfGeTe10.1103/physrevmaterials.1.054003 ↗
44. Berry phase and topological effects of phonons10.1093/nsr/nwx086 ↗
45. Experimental observation of node-line-like surface states in LaBi10.1103/physrevb.97.155153 ↗
46. Almost ideal nodal-loop semimetal in monoclinic CuTeO3 material10.1103/physrevb.97.245148 ↗
47. Hourglasslike nodal net semimetal in Ag2BiO310.1103/physrevb.98.075146 ↗
48. Nonsymmorphic-symmetry-protected hourglass Dirac loop, nodal line, and Dirac point in bulk and monolayer X3SiTe6 (x = Ta, Nb)10.1103/physrevb.97.045131 ↗
49. Type-II nodal loops: Theory and material realization10.1103/physrevb.96.081106 ↗
50. Efficient topological materials discovery using symmetry indicators10.1038/s41567-019-0418-7 ↗
51. Topological materials discovery by large-order symmetry indicators10.1126/sciadv.aau8725 ↗
52. Comprehensive search for topological materials using symmetry indicators10.1038/s41586-019-0937-5 ↗
53. Observation of three-component fermions in the topological semimetal molybdenum phosphide10.1038/nature22390 ↗
54. Dirac semimetal and topological phase transitions in A3Bi (a = Na, k, Rb)10.1103/physrevb.85.195320 ↗
55. Discovery of a three-dimensional topological Dirac semimetal, Na3Bi10.1126/science.1245085 ↗
56. Three-dimensional Dirac semimetal and quantum transport in Cd3 As210.1103/physrevb.88.125427 ↗
57. Observation of a three-dimensional topological Dirac semimetal phase in high-mobility Cd3As210.1038/ncomms4786 ↗
58. Experimental realization of a three-dimensional Dirac semimetal10.1103/physrevlett.113.027603 ↗
59. A stable three-dimensional topological Dirac semimetal Cd3As210.1038/nmat3990 ↗
60. Nodal-chain metals10.1038/nature19099 ↗
61. Hourglass Dirac chain metal in rhenium dioxide10.1038/s41467-017-01986-3 ↗
62. Superconductivity in a new non-centrosymmetric compound of YCoC2 composition
63. From nodal chain semimetal to Weyl semimetal in HFC10.1103/physrevlett.119.036401 ↗
64. Ternary carbides of the rare earth and iron group metals with CeCoC2-and CeNiC2-type structure10.1016/0022-5088(86)90225-0 ↗
65. Ab initio molecular dynamics for liquid metals10.1103/physrevb.47.558 ↗
66. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set10.1103/physrevb.54.11169 ↗
67. Projector augmented-wave method10.1103/physrevb.50.17953 ↗
68. Generalized gradient approximation made simple10.1103/physrevlett.77.3865 ↗
69. Electron-energy-loss spectra and the structural stability of nickel oxide: An LSDA+U study10.1103/physrevb.57.1505 ↗
70. Catalogue of topological electronic materials10.1038/s41586-019-0944-6 ↗
71. A complete catalogue of high-quality topological materials10.1038/s41586-019-0954-4 ↗
72. Maximally localized wannier functions for entangled energy bands10.1103/physrevb.65.035109 ↗
73. Wanniertools: An open-source software package for novel topological materials10.1016/j.cpc.2017.09.033 ↗