High neutron cross-section, high light output.
Major uses - Thermal neutron detection and spectroscopy
Physical Properties:

Density |
- |
4.1 g/cm3 |
Effective decay time |
- |
1.4 s |
High Neutron Peak Position |
- |
> 3 MeV |
Photoelectron yield |
- |
30-35 % of NaI(tl) |
6-Li enrichment |
- |
96% |
Neutron Detection
Neutrons do not produce ionization directly in scintillation crystals, but can be detected through their interaction with the nuclei of a suitable element. In a 6 LiI(Eu) scintillation crystal for example, neutrons interact with 6 Li nuclei to produce an alpha particle and a triton (tritium nucleus), which both produce scintillation light that can be detected. For this purpose, also enriched 6 Li containing glasses can be used, doped with Ce as activator.


