Table 1 Symmetry, magnetic ground state and, for the Weyl node closest to the Fermi energy, position, energy (ε), degeneracy (Deg) and band index of the lower branch in the band crossing (N is the number of valence electrons).
From: Tunable chirality of noncentrosymmetric magnetic Weyl semimetals in rare-earth carbides
Compound | Symmetry | Magnetic ground state | Weyl nodes | AHC | |||||||
|---|---|---|---|---|---|---|---|---|---|---|---|
Class | \({{{\mathcal{I}}}}\) | Θ | Expt. | Theory | Position | ε | Deg | Band | |||
OC | +U | (2π/a, 2π/b, 2π/c) | (meV) | (Ω−1 cm−1) | |||||||
LuCoC2 | I | − | + | NM43 | NM | NM | (0.362, 0.163, 0) | 90 | 4 | N − 1 | 0 |
YCoC2 | I | − | + | NM57 | NM | NM | (0.366, 0.173, 0) | 61 | 4 | N − 1 | 0 |
GdCoC2 | III | − | − | TC = 15K36 | FM | FM | (0.347, 0.206, 0.171) | 34 | 4 | N − 1 | 15 |
GdNiC2 | III | − | − | FM | FM | (−1/2, 0, 0.487) | 108 | 2 | N | −21 | |
GdRuC2 | II | + | − | TC = 45(3)K33 | FM | FM | (0.074, 0.178, 0) | 15 | 4 | N − 2 | −300 |
NdRhC2 | III | − | − | FM | FM | (0.393, 0.233, −0.199) | 43 | 4 | N | 35 | |
PrRhC2 | III | − | − | AFM | FM | (0, 0.158, −0.221) | 9 | 4 | N − 1 | −13 | |