Table 2 Symmetry-based indicators and topological invariants of SrPb.

From: Discovery of \({\hat{\boldsymbol{C}}}_2\) rotation anomaly in topological crystalline insulator SrPb

\(Z_{2,\,2,\,2,\,4}\)

\((\nu _1\nu _2\nu _3)\)

\(\{ \hat M_z|00\frac{1}{2}\}\)

\(\hat M_x\)

\(\{ \hat g_y|00\frac{1}{2}\}\)

\(\{ \hat C_{2y}|00\frac{1}{2}\}\)

\(\{ \hat C_{2x}\}\)

\(\hat I\)

\(\{ \hat C_{2z}|00\frac{1}{2}\}\)

1102

110

−2

0

0

1

1

1

0

  1. \(n_{\hat M_z}\) of the \(k_z \,=\, \pi /c\) plane is 0 and not shown here.