“…Generally, the mechanism treats particle polarization by using complex dielectric constant, e ¼ e 0 2ie 00 , where the real part e 0 is related to polarizability and the imaginary part e 00 is related to the dielectric loss, and can be expressed as s=2pf , where s is the conductivity and f is frequency of the external electric field. This theory is supported by recent experiments on mesoporous ceriumdoped TiO 2 [6], and amorphous Ba x Sr 1-x TiO 3 [16]. However, there is no dielectric relaxation peak in triethanolamine-modified TiO 2 shown in Fig.…”