Group theory is closely related to the study of symmetries, be they symmetries of abstract mathematical
objects, or of more concrete ones such as molecules. Explicitly, group theory can be applied to
infrared (IR) spectroscopy in order to predict the presence of absorption bands:
If a radiation excites the molecules from the ground state into vibration, it is absorbed.
Suppose we have a list of candidate molecules for an unknown sample (which we suppose to be
composed of only one molecule).
Since the frequencies absorbed by a molecule are characteristic of its geometrical structure,
by knowing the geometries of the candidates, we can calculate the expected number of absorption bands,
which may eliminate non corresponding candidates when the actual IR spectrum is determined experimentally.
`\forall f:P\mapsto\mathbb{R^3}`, `\forall g\in\G`, `forall x\inP`, `(g\cdot f)(x) := g(f(g^{-1}x))`
Let `n := Card(P)`, then `\Gamma` is a `3n` dimensional vector space, which induces a `3n` dimensional representation `\rho_{dis}` of `G` with character `\chi_{dis}`.`\chi_0 = \sum_{i=1}^d \alpha_k \chi_k`
The theoretical number of bands on the IR spectrum is given by:`n_0 = \sum_{i=1, \alpha_i\ne0}^d \langle\chi_i, \chi_{vib}\rangle`
We have the molecule of ammonia :
Let `G` be the symmetry group of this structure, the conjugacy classes of `G` are:
| `D_3` | `Id` (1) |
`C_3` (2) |
`\sigma` (3) |
|---|---|---|---|
| `\chi_{triv}` | 1 | 1 | 1 |
| `\chi_1` | 1 | 1 | -1 |
| `\chi_2` | 2 | -1 | 0 |
| `D_3` | `Id` (1) |
`C_3` (2) |
`\sigma` (3) |
|---|---|---|---|
| `\chi_0` | 3 | 0 | 1 |
`\chi_0 = \chi_{triv} + \chi_2`
and`\chi_{dis} = 3\chi_{triv} + \chi_1 + 4\chi_2.`
The non vibration displacements give:`\chi_{trans} + \chi_{rot} = \chi_{triv} + \chi_1 + 2\chi_2.`
`\chi_{vib} = 2\chi_{triv} + 2\chi_2.`
Thus:
Sources :
[1] Resonance data from NIST WebBook
[2] Group theory for the interpretation of IR & Raman Spectra
[3] Mathematical aspect and an other example with `PCl_5` (french)
[4] Molecular vibration and IR absorption (French)