Characteristic Radiation

 


 
If the energy of the incoming electrons exceeds the binding energy of the electrons on a certain shell of the target atoms, an additional process can happen: In a collision, the incoming electron (1) can push the target electron (2) out of its place on the shell. This event will leave an unstable atom behind. The gap on the shell will be filled immediately by an electron (3) from an outer shell or even from the conduction band of the target material. This replacement electron will thereby change its energy by a well defined amount depending on the binding energy levels of the electrons in the target material, which are characteristic for that material. The resulting X-rays (4) with very distinct photon energy values are therefore called characteristic radiation. As the binding energy values for the outer shells are not high enough for most elements to generate photons of noticeable energy, usually only characteristic radiation generated by electrons jumping into the K-shell is considered.

See x-ray specrta

Ref: Siemens.com

 

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