The platform will undergo maintenance on Sep 14 at about 7:45 AM EST and will be unavailable for approximately 2 hours.
2021
DOI: 10.1103/physrevb.103.l121101
|View full text |Cite|
|
Sign up to set email alerts
|

From triple-point materials to multiband nodal links

Abstract: We study a class of topological materials which in their momentum-space band structure exhibit threefold degeneracies known as triple points. Focusing specifically on PT -symmetric crystalline solids with negligible spin-orbit coupling, we find that such triple points can be stabilized by little groups containing a three-, four-, or sixfold rotation axis, and we develop a classification of all possible triple points as type A vs type B according to the absence vs presence of attached nodal-line arcs. Furthermo… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

2
49
0

Year Published

2021
2021
2023
2023

Publication Types

Select...
6
1
1

Relationship

1
7

Authors

Journals

citations
Cited by 35 publications
(51 citation statements)
references
References 79 publications
2
49
0
Order By: Relevance
“…10 to partial frames. We note in passing that while the band inversion in group 1 at Γ is mediated by a tripledegenerate point with a frame charge of q = −1 15,70,71 , the band inversion at Γ between group 2 and 3 is mediated by a quadrupledegenerate point with a total frame charge q = (−1)*(−1) = +1. Even though the frame charge of the quadruple-degenerate node is trivial, because of the crystalline symmetries it must be formed by the superposition of two quadratic nodes, each with a nonzero Edge states.…”
Section: Resultsmentioning
confidence: 86%
“…10 to partial frames. We note in passing that while the band inversion in group 1 at Γ is mediated by a tripledegenerate point with a frame charge of q = −1 15,70,71 , the band inversion at Γ between group 2 and 3 is mediated by a quadrupledegenerate point with a total frame charge q = (−1)*(−1) = +1. Even though the frame charge of the quadruple-degenerate node is trivial, because of the crystalline symmetries it must be formed by the superposition of two quadratic nodes, each with a nonzero Edge states.…”
Section: Resultsmentioning
confidence: 86%
“…Here, we describe the full derivation of the classification result shown in Ref. 50 and extend it to include TPs in spinless systems without PT symmetry and in non-symmorphic space groups. The result is a complete classification of TPs in spinless systems for all magnetic space groups according to the NL structure appearing in the vicinity of the TPs.…”
Section: Introductionmentioning
confidence: 97%
“…In Ref. 50 we have classified all possible TPs in a subset of spinless systems, namely those in systems with space-time-inversion (PT ) symmetry and symmorphic space group, according to a similar scheme as Ref. 29, and we revealed valuable connections of such TPs to non-Abelian band topology, monopole charges, and NL links [50,[55][56][57].…”
Section: Introductionmentioning
confidence: 99%
“…A classic example is the quaternion group with , which has been used to classify the topological line defects in biaxial nematic liquid crystals 14 . Very recently, non-Abelian groups have been used to describe the admissible nodal line configurations 12 , 15 , 16 , Dirac/Weyl point braiding 13 , 17 , 18 , and intriguing triple nodal points 19 – 21 in PT (inversion and time-reversal) symmetric systems. When more bands are involved, richer non-Abelian topological charges emerge 9 .…”
Section: Introductionmentioning
confidence: 99%