Table 2 SM of a 3d pyrochlore lattice with an 8-site unit-cell.
From: Thermal bosons in 3d optical lattices via tensor networks
\(E_1\) | \(E_2\) | \(E_3\) | \(E_4\) | \(E_5\) | \(E_6\) | \(E_7\) | \(E_8\) | \(E_9\) | \(E_{10}\) | \(E_{11}\) | \(E_{12}\) | \(E_{13}\) | \(E_{14}\) | \(E_{15}\) | \(E_{16}\) | \(E_{17}\) | \(E_{18}\) | \(E_{19}\) | \(E_{20}\) | \(E_{21}\) | \(E_{22}\) | \(E_{23}\) | \(E_{24}\) | |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
\(T_1\) | 2 | 3 | 4 | 5 | 6 | 7 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
\(T_2\) | 0 | 0 | 0 | 0 | 0 | 0 | 2 | 3 | 4 | 5 | 6 | 7 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
\(T_3\) | 0 | 0 | 0 | 0 | 0 | 0 | 2 | 3 | 0 | 0 | 0 | 0 | 4 | 5 | 6 | 7 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
\(T_4\) | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 2 | 3 | 0 | 0 | 4 | 5 | 0 | 0 | 6 | 7 | 0 | 0 | 0 | 0 | 0 | 0 |
\(T_5\) | 2 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 3 | 0 | 0 | 0 | 4 | 0 | 5 | 0 | 6 | 7 | 0 | 0 | 0 | 0 |
\(T_6\) | 0 | 2 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 3 | 0 | 0 | 0 | 4 | 0 | 5 | 0 | 0 | 6 | 7 | 0 | 0 |
\(T_7\) | 0 | 0 | 2 | 3 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 4 | 0 | 5 | 0 | 6 | 7 |
\(T_8\) | 0 | 0 | 0 | 0 | 2 | 3 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 4 | 0 | 5 | 6 | 7 |
