Fermi resonance

A Fermi resonance is the shifting of the energies and intensities of absorption bands in an infrared or Raman spectrum. It is a consequence of quantum mechanical mixing.^[1] The phenomenon was explained by the Italian physicist Enrico Fermi.

Selection rules and occurrence

Two conditions must be satisfied for the occurrence of Fermi Resonance:

• the two vibrational states of a molecule transform according to the same irreducible representation of the molecular point group. In other words the two vibrations must have the same symmetries (Mulliken symbols).
• The transitions (accidentally) have almost the same energy.

Fermi resonance most often occurs between normal and overtone modes, if they are nearly coincident in energy.

Fermi resonance leads to two effects. First, the high energy mode shifts to higher energy and the low energy mode shifts to still lower energy. Second, the weaker mode gains intensity (becomes more allowed) and the more intense band decreases in intensity. The two transitions are describable as a linear combination of the parent modes. Fermi resonance does not really lead to additional bands in the spectrum.

Ideallized appearance of a normal mode and an overtone before and after Fermi resonance. Beneath the idealized spectra are idealized energy level schemes.

Examples

Ketones

High resolution IR spectra of most ketones reveal that the "carbonyl band" is split into a doublet. The peak separation is usually only a few cm⁻¹. This splitting arises from the mixing of ν_CO and the overtone of HCH bending modes.^[2]

CO₂

In CO₂, the bending vibration ν₂ (667 cm⁻¹) has symmetry Π_u. The first excited state of ν₂ is denoted 01¹0 (no excitation in the ν₁ mode, one quantum of excitation in the ν₂ bending mode with angular momentum about the molecular axis equal to ±1, no excitation in the ν₃ mode) and clearly transforms according to the irreducible representation Π_u. Putting two quanta into the ν₂ mode leads to a state with components of symmetry (Π_u × Π_u)₊ = Σ⁺_g + Δ _g. These are called 02⁰0 and 02²0, respectively. 02⁰0 has the same symmetry (Σ⁺_g) and a very similar energy to the first excited state of v₁ denoted 100 (one quantum of excitation in the ν₁ symmetric stretch mode, no excitation in the ν₂ mode, no excitation in the ν₃ mode). The calculated unperturbed frequency of 100 is 1337 cm⁻¹, and, ignoring anharmonicity, the frequency of 02⁰0 is 1334, twice the 667 cm⁻¹ of 01¹0. The states 02⁰0 and 100 can therefore mix, producing a splitting and also a significant increase in the intensity of the 02⁰0 transition, so that both the 02⁰0 and 100 transitions have similar intensities.

References

1. Kazuo Nakamoto “Infrared and Raman Spectra of Inorganic and Coordination Compounds: Theory and Applications in Inorganic Chemistry (Volume A)” John Wiley, 1997. ISBN 0-471-16394-5
2. Robert M. Silverstein, Francis X. Webster, David Kiemle “Spectrometric Identification of Organic Compounds”Edition: 7th ed., John Wiley & Sons, 2005. ISBN 0-471-39362-2.