TY - JOUR
T1 - Mixed-order and general-order kinetics applied to synthetic glow peaks and to peak 5 in LiF:Mg,Ti (TLD-100)
AU - Yossian, D.
AU - Horowitz, Y. S.
PY - 1997/1/1
Y1 - 1997/1/1
N2 - Mixed order (MO) and general order (GO) kinetics has been applied to synthetic thermoluminescence glow peaks and to the shape of isolated peak 5 in LiF:Mg,Ti (TLD-100) following post-irradiation annealing at 165°C. We compare the peak shape parameters involved in MO analysis (s, E and c/n0) to the peak shape parameters involved in GO analysis (s, E and b) using computerised total glow peak shape analysis. The predicted correlation between b and c/n0, by the originators of mixed order kinetics, is confirmed for the synthetic glow peaks, but is only approximated for a real system of defects such as peak 5 in post-irradiation annealed TLD-100. Nonetheless, the peak shape predicted by mixed order kinetics is capable of yielding excellent fits to the experimental peak shape of peak 5. The values of E obtained from the fits are in fairly good agreement with the literature and vary smoothly as a function of the duration of the post-irradiation anneal, as does the parameter c/n0, the fraction of thermally disconnected traps. The use of mixed order kinetics is, therefore, a viable alternative to general order kinetics in the intermediate situation (1 < b < 2), due to its physical basis compared to the more empirical basis of general order kinetics.
AB - Mixed order (MO) and general order (GO) kinetics has been applied to synthetic thermoluminescence glow peaks and to the shape of isolated peak 5 in LiF:Mg,Ti (TLD-100) following post-irradiation annealing at 165°C. We compare the peak shape parameters involved in MO analysis (s, E and c/n0) to the peak shape parameters involved in GO analysis (s, E and b) using computerised total glow peak shape analysis. The predicted correlation between b and c/n0, by the originators of mixed order kinetics, is confirmed for the synthetic glow peaks, but is only approximated for a real system of defects such as peak 5 in post-irradiation annealed TLD-100. Nonetheless, the peak shape predicted by mixed order kinetics is capable of yielding excellent fits to the experimental peak shape of peak 5. The values of E obtained from the fits are in fairly good agreement with the literature and vary smoothly as a function of the duration of the post-irradiation anneal, as does the parameter c/n0, the fraction of thermally disconnected traps. The use of mixed order kinetics is, therefore, a viable alternative to general order kinetics in the intermediate situation (1 < b < 2), due to its physical basis compared to the more empirical basis of general order kinetics.
UR - http://www.scopus.com/inward/record.url?scp=0031150130&partnerID=8YFLogxK
U2 - 10.1016/S1350-4487(97)00007-3
DO - 10.1016/S1350-4487(97)00007-3
M3 - Article
AN - SCOPUS:0031150130
SN - 1350-4487
VL - 27
SP - 465
EP - 471
JO - Radiation Measurements
JF - Radiation Measurements
IS - 3
ER -