Abstract

We identify all symmetry-enforced band crossings in nonmagnetic orthorhombic crystals with and without spin-orbit coupling and discuss their topological properties. We find that orthorhombic crystals can host a large number of different band degeneracies, including movable Weyl and Dirac points with hourglass dispersions, fourfold double Weyl points, Weyl and Dirac nodal lines, almost movable nodal lines, nodal chains, and topological nodal planes. Interestingly, spin-orbit coupled materials in the space groups 18, 36, 44, 45, and 46 can have band pairs with only two Weyl points in the entire Brillouin zone. This results in a simpler connectivity of the Fermi arcs and more pronounced topological responses than in materials with four or more Weyl points. In addition, we show that the symmetries of the space groups 56, 61, and 62 enforce nontrivial weak $\mathbb{Z}_2$ topology in materials with strong spin-orbit coupling, leading to helical surface states. With these classification results in hand, we perform extensive database searches for orthorhombic materials crystallizing in the relevant space groups. We find that Sr$_2$Bi$_3$ and Ir$_2$Si have bands crossing the Fermi energy with a symmetry-enforced nontrivial $\mathbb{Z}_2$ invariant, CuIrB possesses nodal chains near the Fermi energy, Pd$_7$Se$_4$ and Ag$_2$Se exhibit fourfold double Weyl points, the latter one even in the absence of spin-orbit coupling, whereas the fourfold degeneracies in AuTlSb are made up from intersecting nodal lines. For each of these examples we compute the ab-initio band structures, discuss their topologies, and for some cases also calculate the surface states.

Highlights

  • The discovery of topological insulators more than ten years ago [1,2,3] has kicked off a classification program of topological band structures [4,5,6], which is still ongoing today

  • The results presented in this paper do not depend on the actual shape of the Brillouin zone (BZ), as long as the correct orientation is chosen and high-symmetry lines should always be understood as defined above and visualized in the exemplary BZ

  • We have found a vast number of different symmetry-enforced band crossings, as well as enforced weak Z2 invariants (Tables I–IV)

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Summary

INTRODUCTION

The discovery of topological insulators more than ten years ago [1,2,3] has kicked off a classification program of topological band structures [4,5,6], which is still ongoing today. Spin-orbit coupled materials in all these SGs exhibit helical surface states, that could potentially be used for low-dissipation (spin) transport We determine those SGs where the number of Weyl points formed by a spin-orbit coupled band pair can be as low as four (or even two), i.e., where only four (or two) of the eight time-reversal invariant momenta (TRIMs) host Weyl points, while the other TRIMs are part of nodal lines. The topological responses, such as the anomalous (spin) Hall effect, are expected to be enhanced, since Weyl points with opposite chiralities are separated by a large distance in reciprocal space [44,45,46] Using these classification results as an input, we perform an extensive database search for materials crystallizing in the relevant SGs (Sec. III and Fig. 2). Appendix C contains a minimal tight-binding model for SG 19, which highlights the enforced features of chiral orthorhombic SGs both with and without SOC

Symmetries
Orthorhombic lattices and Brillouin zones
SCREENING FOR CANDIDATE MATERIALS
RHOMBIC DISPHENOIDAL
Weyl Points at high-symmetry points
Movable Weyl points on rotation axes
Material example Pd7Se4
Topological nodal planes
Fourfold double Weyl points
RHOMBIC PYRAMIDAL
Weyl points
Pinned nodal lines
Movable nodal lines
Nodal chain
Material example
Almost movable lines
Fourfold degeneracies in mirror planes
RHOMBIC DIPYRAMIDAL
Dirac points at high-symmetry points
Movable Dirac points
Movable and almost movable Weyl lines
Movable Dirac lines
Nodal line arrangement in SGs 61 and 73
Almost movable Dirac line
Material examples
Symmetry-enforced Z2 topology in planes
CONCLUSION
Fourfold double Weyl point
Fourfold degenerate points from multiple intersecting nodal lines

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