Stiefel-Whitney topological charges in a three-dimensional acoustic nodal-line crystal
arXiv:2304.06304 · doi:10.1038/s41467-023-40252-7
Abstract
Band topology of materials describes the extent Bloch wavefunctions are twisted in momentum space. Such descriptions rely on a set of topological invariants, generally referred to as topological charges, which form a characteristic class in the mathematical structure of fiber bundles associated with the Bloch wavefunctions. For example, the celebrated Chern number and its variants belong to the Chern class, characterizing topological charges for complex Bloch wavefunctions. Nevertheless, under the space-time inversion symmetry, Bloch wavefunctions can be purely real in the entire momentum space; consequently, their topological classification does not fall into the Chern class, but requires another characteristic class known as the Stiefel-Whitney class. Here, in a three-dimensional acoustic crystal, we demonstrate a topological nodal-line semimetal that is characterized by a doublet of topological charges, the first and second Stiefel-Whitney numbers, simultaneously. Such a doubly charged nodal line gives rise to a doubled bulk-boundary correspondence: while the first Stiefel-Whitney number induces ordinary drumhead states of the nodal line, the second Stiefel-Whitney number supports hinge Fermi arc states at odd inversion-related pairs of hinges. These results establish the Stiefel-Whitney topological charges as intrinsic topological invariants for topological materials, with their unique bulk-boundary correspondence beyond the conventional framework of topological band theory.
12 pages, 10 figures
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- Topological semimetal with coexisting nodal points and nodal lines
- Breakdown of boundary criticality and exotic topological semimetals in -invariant systems
- Observation of Embedded Topology in a Trivial Bulk via Projective Crystal Symmetry
- Semimetals without correspondence between the topological charge of nodal line/surface and Fermi arc
- Asymmetric real topology of conduction and valence bands