#figure({
  set text(size: 9pt);
  set par(justify: false);
  let m2(content) = table.cell(colspan: 2, content);
  let A1 = [A#sub[1]];
  let A2 = [A#sub[2]];
  let B1 = [B#sub[1]];
  let B2 = [B#sub[2]];
  let E1 = [E#sub[1]];
  let E2 = [E#sub[2]];
  table(columns: 8, align: center + horizon,
    table.cell(rowspan: 2)[*Representation*],
      [C#sub[6v]], A1, B1, m2(E1), m2(E2),
      [C#sub[2v]], A1, B1, B2, B1, A2, A1,
    table.cell(rowspan: 2, colspan: 2)[*Vibration Direction*],
      [out-of-plane], [out-of-plane], m2[in-plane], m2[in-plane],
      [z], [z], [x], [y], [x], [y],
    m2[*Raman Tensor*],
      [$mat(a,,;,a,;,,b)$], [$0$], [$mat(,,a;,,;a,,;)$], [$mat(,,;,,a;,a,;)$], [$mat(,a,;a,,;,,;)$], [$mat(a,,;,-a,;,,;)$],
    m2[*Raman visibility*],
      [xx/yy: $a^2$ #linebreak() zz: $b^2$ #linebreak() others: 0], [0],
      m2[xz/yz: $a^2$ #linebreak() others: 0], m2[xx/xy/yy: $a^2$ #linebreak() others: 0],
  )},
  caption: [
    Irreducible representations and raman tensors of phonons in 4H-SiC.
  ],
  placement: none,
)<table-rep>