“…Based on the above observation, two kinds of FIR technique, using TCLs and NTCLs, can be employed for temperature sensing. First, it is well known that the FIR of the emissions from the thermally coupled 2 H 11/2 and 4 S 3/2 levels follows the Boltzmann distribution
23,24 :
where I 525 and I 543 are the integrated intensities corresponding to the 2 H 11/2 → 4 I 15/2 and 4 S 3/2 → 4 I 15/2 transitions, respectively, A is the pre‐exponential constant,
E is the energy difference between the 2 H 11/2 and 4 S 3/2 levels, k is Boltzmann's constant, and T is absolute temperature. The curves of FIR versus T measured for the D‐BYEP are presented in Figure 5C.…”