| | | |
| 久期方程 | $\left[{\begin{array}{*{20}{c}}x&1&0&0\\1&x&1&0\\0&1&x&1\\0&0&1&x\end{array}} \right] = 0 $ | $\left[{\begin{array}{*{20}{c}}x&1&0&1\\1&x&1&0\\0&1&x&1\\1&0&1&x\end{array}} \right] = 0 $ | $\left[{\begin{array}{*{20}{c}}x&1&1&1\\1&x&1&1\\1&1&x&1\\1&1&1&x\end{array}} \right] = 0 $ |
| 4条分子轨道能量E | E4 = α − 1.618β E3 = α − 0.618β E2 = α + 0.618β E1 = α + 1.618β | E4 = α − 2β E2 = E3 = α E1 = α + 2β | E2 = E3 = E4 =α − β E1 = α + 3β |
| ${\rm{H}}_4^{2 + } $ (2e)轨道能量E | 3.236β | 4β | 6β |
| $ {\rm{H}}_4^{ + }$(3e)轨道能量E | 3.854β | 4β | 5β |
| H4 (4e)轨道能量E | 4.472β | 4β | 4β |
| ${\rm{H}}_4^{- } $(5e)轨道能量E | 3.854β | 4β | 3β |
| ${\rm{H}}_4^{2 - } $(6e)轨道能量E | 3.236β | 4β | 2β |