# Using group theory to make molecular orbital diagrams

Because of Orthocresols' meta post I ask this question about application of group theory to molecular orbital theory.

In my undergraduate lecturers, we've seen many examples of making qualitative MO Diagrams by inspection of what orbitals could line up to form bonding / anti bonding orbitals.

This works fine for simple things, but I know it's possible to use symmetry to also work out mathematically which orbitals can mix with which other orbitals by using group theory.

Perhaps using example of water could somebody show how this could be achieved?

• Can you be a bit clearer? Are you talking about the mixing of the orbitals in Oxygen to the Orbitals in Hydrogen in water? – Haru Fujimura Jul 7 '17 at 18:30

Group theory really just formalises the process that you're going through when you construct molecular orbital diagrams by inspection (though as the molecules get bigger it gets significantly harder to intuitively guess at what will mix and in what combinations).

In order to construct an MO diagram for water, we'll take a stepwise approach:

• first, determine the way in which the hydrogen atoms can combine (in phase or out of phase, as per the standard dihydrogen MO diagram) which will give us a set of symmetry adapted combinations
• second, we mix these symmetry adapted orbitals with the atomic orbitals on the oxygen, bearing in mind the 'rules' of the game
• only orbitals of similar energy are able to combine
• only orbitals of correct geometry/orientation are able to combine (i.e. head on or side to side)
• only orbital of correct symmetry are able to combine. This is where group theory becomes useful

### 1. Symmetry of the central oxygen's orbitals

The symmetry of the oxygen orbitals (2s and 2p, the 1s isn't relevant to the bonding) can easily be read off from a character table. In this case, water has C2v symmetry, the character table for which is given below:

$$\begin{array}{c|cccc|cc} \hline C_\mathrm{2v} & E & C_2 & \sigma_\mathrm{v}(xz) & \sigma_\mathrm{v}'(yz) & & \\ \hline \mathrm{A_1} & 1 & 1 & 1 & 1 & z & x^2, y^2, z^2 \\ \mathrm{A_2} & 1 & 1 & -1 & -1 & R_z & xy \\ \mathrm{B_1} & 1 & -1 & 1 & -1 & x, R_y & xz \\ \mathrm{B_2} & 1 & -1 & -1 & 1 & y, R_x & yz \\ \hline \end{array}$$

To summarise the information obtained:

• the s-orbitals have a1 symmetry
• the px orbital has b1 symmetry
• the py orbital has b2 symmetry
• the pz orbital has a1 symmetry

(as @Orthocresol noted in the comments, there is no convention on axis in the C2v point group,meaning x and y can switch depending on what book you get the character table from. The one given is the same as the commonly used set from Atkins' Physical chemistry, but overall it doesn't really matter as long as you're consistent)

It's worth noting that you can derive these symmetries above by considering how the atomic orbitals moves under the various elements within that point group, this is shown below for the hydrogens, and not really needed to be repeated here.

### 2. Symmetry of the hydrogen group orbitals

To construct the group orbitals for hydrogen (which will go on to be mixed with the oxygen atomic orbitals), we simply have to consider the possible combinations and then work out the symmetries of those combinations.

For the case of two hydrogens interacting, only two cases are possible: in phase, and out of phase.

If we consider these two cases pictorially, we can then determine what happens to them under the various symmetry elements within the C2v group. If the orbitals stay the same, we assign a character of 1, if they switch, we assign -1.

Once we have the full set of characters for both possible combinations, we can assign symmetries, again, using the character table for the relevant point group:

• the in-phase combination has a1 symmetry
• the out of phase combination has b2 symmetry

### 3. Mixing

Mixing is the part of this process that you're likely more comfortable with, except now rather than considering whether interaction (on symmetry grounds) is likely by inspection, we can do it by mixing orbitals with the same symmetry labels:

The diagram above is the one that you would likely have arrived at without any consideration of group theory (you can actually derive a more complex diagram in which the molecular orbitals also mix), some key points to note:

• the oxygens orbitals have all (qualitatively) been placed lower than those of hydrogen. Electronegative atoms have more contracted orbitals and are lower in energy
• two of the p-orbitals end up non-bonding, these are the lone pairs on oxygen
• the s-orbital on oxygen interacts with the in-phase combination of hydrogen, this is the lowest energy combination rather than using the p-orbital (also with a1 symmetry)

• A caveat with $C_\mathrm{2v}$ is that every book will have a different convention on the $x$ and $y$ axes... and hence the mirror planes $\sigma_\mathrm{v}$ and $\sigma_\mathrm{v}'$, and the irreps $\mathrm{B_1}$ and $\mathrm{B_2}$, get swapped in different books. $D_\mathrm{2h}$ is even worse, it's a complete nightmare. But as long as one is consistent throughout, the final result will always be the same. – orthocresol Jul 7 '17 at 18:44