Polarization factor

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The polarization factor takes into account the angle dependence of the intensity in Thomson scattering (or angle dependence of the intensity emitted by a dipole ). It occurs primarily as a correction factor in X-ray structure analysis .

Necessity as a correction term

The polarization factor is:

.

It is necessary as a correction term if the incident radiation is unpolarized in a scattering experiment, but the incident radiation is polarized. Thomson scattering occurs here because the energy of the X-ray quanta is not high enough to lead to inelastic ( Compton ) scattering. Photons are absorbed by the electron, which stimulate it to vibrate. As a result, it emits photons again as an oscillating dipole, which is known as scattering.

Derivation

The incident waves can be divided into a vertical and a parallel part:

In the case of unpolarized incident radiation:

The intensity of a radiating dipole also depends on the angle of radiation (in the Debye-Scherrer method , for example ). Since the radiation of the dipoles oscillating perpendicular to the direction of propagation always reaches the detector, the following results for the scattered waves:

If one observes the scattering at , the polarization factor is 1 and the full intensity is scattered. If the value is 90 °, the polarization factor is 0.5 and only half the intensity is scattered, so the scattered waves are polarized perpendicular to the direction of propagation.

Individual evidence

  1. ^ H. Neff: Fundamentals and Applications of X-ray Fine Structure Analysis 1962.
  2. Werner Massa: Crystal structure determination . 8th edition. Springer Fachmedien, Wiesbaden 2015, ISBN 978-3-658-09412-6 , pp. 96 f ., Doi : 10.1007 / 978-3-658-09412-6 .