Thermoluminescence has been studied in LiF crystals which were produced by a variety of growth conditions. X-ray, ${\mathrm{Co}}^{60}$ gamma-ray, and/or optical excitation have been used to both populate and/or produce defects. Collectively, as many as 28 different glow peaks are observed in the range 20-550°K. However, in any one sample only about 15 of these peaks occur. The glow curves cover a range in intensity, the ratio of the strongest to weakest peaks is about ${10}^4$, and the strongest thermoluminescence occurs near 140°K. No one glow peak is common to all samples. Some of the factors which determine the presence or absence of a glow peak are discussed. The activation energies of the major peaks have been determined by several methods. The four peaks at 115, 147, 154, and 255°K, and possibly others, follow first-order kinetics. Typical peak temperatures (°K), pre-exponential factors (${\sec }^{-1\mathrm{}}$), and activation energies (eV) are 119, 2.7×${10}^{10}$, 0.28; 133, 3.1×${10}^3$, 0.14; 147, 8.3×${10}^3$, 0.17; 158, 3.4×${10}^7$, 0.29; 194, 1.8×${10}^6$, 0.31; 255, 4.7×${10}^8$, 0.53. The peaks at 115, 158, 194, and 255°K, and possibly others, result from electron untrapping, since they can be populated by both x irradiation and by electrons released upon irradiating a colored crystal with $F$-band light. The peak at 68°K has been observed only after optical re-excitation. Several of the glow peaks have been corelated with impurities, ESR data, etc. These corelations suggest specific models for the defects associated with particular glow peaks. The peak at 115°K appears to result from the $H$ center. The peak at 133°K is impurity-sensitive and is probably caused by the untrapping of a hole from the $V_K$ center. A Mg impurity produces peaks between 430 and 490°K, whereas Mn, Ti, Zr, or Ce merely enhance the 133°K peak.

• Received 1 September 1966

DOI:https://doi.org/10.1103/PhysRev.155.908