Mossbauer Effect

HomePage | Recent changes | View source | Discuss this page | Page history | Log in |

Printable version | Disclaimers | Privacy policy

The Mossbauer Effect, a physical phenomenon discovered by Rudolf Mossbauer in 1957, refers to the resonant emission and absorption of gamma rays by atoms bound in a solid. The resonant emission and absorption of x-rays by gases had been observed previously and it was expected that a similar phenomenon existed for gamma rays, which are created by nuclear transitions rather than the electronic transitions that produce x-rays. However, early attempts to observe this phenomenon in gases failed.

In general gamma rays are produced by nuclear transitions from an unstable high-energy state to a low-energy state. The energy of the emitted gamma ray corresponds to the energy of the nuclear transition minus an amount of energy that is lost as recoil to the emitting atom. If the lost "recoil energy" is small enough then the gamma ray energy still corresponds to the energy of the nuclear transition and the gamma ray can be absorbed by another atom of the same type as the first. Such emission and subsequent absorption is called resonance. Additional recoil energy is also lost during absorption, so in order for resonance to occur the recoil energy must be less than half the linewidth for the corrseponding nuclear transition.

The amount of lost energy is described by the equation:

  ER = Egamma2 / 2Mc2

where ER is the energy lost as recoil, Egamma is the energy of the gamma ray, M is the mass of the emitting or absorbing body, and c is the velocity of light. In the case of a gas the emitting and absorbing bodies are atoms, so the mass is quite small, resulting in a large recoil energy. This is why early researchers were unable to observe gamma ray resonance in gases.

Due to the fundamental quantum nature of solids, atoms bound in solids are restricted to a specific set of vibrational energies called phonon energies. If the recoil energy is smaller than the phonon energy then a fraction of the nuclear events, called the recoil-free fraction, occur such that the entire crystal, rather than just the atom acts as the recoiling body. Since the mass of the crystal is very large compared to that of a single atom, these events are essentially recoil-free. In these cases, since the recoil energy is negligible, the emitted gamma rays have the appropriate energy and resonance can occur.

In general gamma rays have very narrow linewidths. This means they are very sensitive to small changes in the energies of nuclear transitions. In fact gamma rays can be used as a probe to observe the effects of interactions between a nucleus and its electrons and those of its neighbors. This is the basis for Mossbauer Spectroscopy, which combines the Mossbauer effect with the Doppler effect to monitor such interactions.