To investigate the relation between the luminescence properties and the crystal structure, the thermal quenching of three kinds of Eu 2+ -activated Sr-containing sialon phosphors are analyzed using the Struck-Fonger model. The inherent frequency of the host lattice ω is calculated from the measured internal quantum efficiency at various temperatures, and the results confirm that the inherent frequency of the host lattice ω dominates the thermal quenching of these phosphors. Moreover, clarification of the relationship between the inherent frequency of the host lattice ω and the host crystal structure reveals that the covalence and density of the host crystal structure mainly influence the inherent frequency and therefore influence the extent of the thermal quenching. 17,18 Despite being composed of the same elements and activated with the same ion, the divalent Eu ion, these three phosphors emit different color and their luminescence properties are not the same. The differences between their crystal structures and compositions are thought to result in these different luminescence properties. In an attempt to investigate the relation between the compositions, structures of the host crystals, and their luminescence properties, the thermal quenching of these phosphors is analyzed. The research about the thermal quenching of phosphors have increased in these days, [19][20][21][22][23][24][25][26][27][28] and two processes of the thermal quenching are mainly considered. One is the thermally activated cross over from the excited state to the ground state;19-24 the other is the thermal ionization from the excited state to the bottom of the conduction band (CB). [25][26][27][28] Struck and Fonger proposed a quantitative method to describe the radiative and non-radiative relaxation from excited states using a quantum mechanical single configurational coordinate (QMSCC) model.19 Parameters for this model are depicted in Fig. 1. In this figure the horizontal coordinate is the single configurational coordinate r, and the vertical coordinate is the total energy E of the system. The parabolas u and v are the potential energy wells of the electronic ground state and the relevant excited state, respectively. The u and v parabola quantum numbers, wavefunctions, and phonon energies are denoted n, u n , ω u and m, v m , ω v , respectively. r 0 measures the Franck-Condon (FC) offset and is expressed in terms of S u and S v : r 0 2 = 2(S u + S v ). S u ω u and S v ω v represent the relaxation energies after emission and excitation, respectively. The QMSCC model is taken in the thermal equilibrium and the v m → u n rate is proportional to the squared overlap integral u n |v m 2 . 29 These overlap integrals are evaluated using the recursion formulas given by Manneback,20 offering the possibility of a quantitative treatment of radiative and nonradiative processes. Struck and Fonger applied QMSCC-calculation to the luminescence properties of ruby and emerald. 21 Bleijenberg and Blasse performed QMSCC calculations on model phosphor syste...