2017
DOI: 10.1103/physrevb.96.155105
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Robust doubly charged nodal lines and nodal surfaces in centrosymmetric systems

Abstract: Weyl points in three spatial dimensions are characterized by a Z-valued charge -the Chern number -which makes them stable against a wide range of perturbations. A set of Weyl points can mutually annihilate only if their net charge vanishes, a property we refer to as robustness. While nodal loops are usually not robust in this sense, it has recently been shown using homotopy arguments that in the centrosymmetric extension of the AI symmetry class they nevertheless develop a Z2 charge analogous to the Chern numb… Show more

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Cited by 217 publications
(329 citation statements)
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“…While the former class includes topological insulators and superconductors, but also quantum Hall states [5][6][7], the latter class concerns topological semimetals (e.g. Weyl, Dirac and nodal-line semimetals), which have been intensively investigated in the recent years [8][9][10][11][12][13][14][15][16][17][18]; besides, topological phases with nodal surfaces have also been theoretically proposed [19][20][21][22][23]. These gapless systems can display remarkable properties, such as Fermi arcs or drumhead surface states on the boundaries, and momentum-space Dirac monopoles in the bulk.…”
mentioning
confidence: 99%
“…While the former class includes topological insulators and superconductors, but also quantum Hall states [5][6][7], the latter class concerns topological semimetals (e.g. Weyl, Dirac and nodal-line semimetals), which have been intensively investigated in the recent years [8][9][10][11][12][13][14][15][16][17][18]; besides, topological phases with nodal surfaces have also been theoretically proposed [19][20][21][22][23]. These gapless systems can display remarkable properties, such as Fermi arcs or drumhead surface states on the boundaries, and momentum-space Dirac monopoles in the bulk.…”
mentioning
confidence: 99%
“…In fact, due to the concomitant presence of the commuting two-fold rotation symmetry and time-reversal symmetry, a crystal in the p2 space group is also invariant under the combined antiunitary symmetry operation C 2 Θ with (C 2 Θ) 2 = 1. Assuming a periodic and smooth real gauge can be found [83], this also implies that the Wilson loop operator in the e 1,2 direction belongs to the orthogonal group SO (2), with the homotopy group π 1 [SO(2)] = Z guaranteeing the existence of an integer winding number invariant [84]. A C 2 Θ-protected fragile topological phase of this kind has been first discussed in Ref.…”
Section: Wallpaper Group P2: Insulators With Two Occupied Bandsmentioning
confidence: 99%
“…Crucial for the appearance of BFSs is that the superconductivity involves more than one band: specifically, the pairing between electrons in different bands generates a pseudomagnetic field, which "inflates" point and line nodes of the intraband pairing potential into BFSs. These nodal surfaces are robust against perturbations that preserve particle-hole and inversion symmetry, which can be formulated in terms of a Z 2 topological invariant [2,[4][5][6].…”
Section: Introductionmentioning
confidence: 99%