3.6. Photocatalytic activities
In order to analyze the effect of the 4d TM atom doping on the photocatalytic activity of TiOS, we resort to the effective masses and the transfer rates of the photogenerated electrons and holes. For the pure TiOS, the effective masses are found to bemh* (p) = 17.348m0 andme* (p) = 2.387m0 with m0 being the electron mass, which implies a large rhe (p) = 7.268. This large difference betweenmh* (p) andme* (p) will further result in the large difference between the transfer rates of electrons and holes, reducing the recombination of electrons and holes. Therefore, TiOS can be used as a promising photocatalytic material. When TiOS is doped by 4d TM atoms, the effective masses of electrons and holes are denoted bymh* (d) andme* (d) along one certain direction, respectively. We can see in Fig. 6 that the relative variation ratios rh =mh* (d)/mh* (p) are all greater than 1, indicating the doping can seriously increase the effective mass of the photogenerated holes. However, the relative variation ratios re =me* (d)/me* (p) are all close to 1, indicating only tiny variations ofme* are observed. Therefore the doping will make stronger influences on the effective mass of the holes than the electrons. For clarity, we also plot the ratior’he =rhe (d)/rhe (p) to clearly reflect the overall doping induced variations of the hole and electron effective masses with rhe (d) andrhe (p) being the effective mass ratios corresponding to the doped and pure TiOS. We can see allr’he are greater than 1, indicating all the dopings can enlarge the effective mass difference between holes and electrons. This phenomenon is more evident for Y, Zr, Nb, Mo, and Ag than Tc, Ru, Rh, Pd, and Cd. Furthermore, this demonstrates that the 4d TM atom doping will further suppress the recombination of the photogenerated electrons and holes, which can improve the photocatalytic activity of TiOS in different degrees. Moreover, the dopings of Y and Ag can lead to larger r’he , indicating both Y and Ag dopings can be viewed as the better schemes used to enhance photocatalytic activity of TiOS.
Fig. 6 (Color online) The relative variation ratiosrh , re , andr’he for different doping models.
Furthermore, as discussed before, based on the energy bands of the 4d TM atom doped TiOS in Fig. 4 we can see that the couplings of the doping atoms and the TiOS can produce new impurity energy bands in the original band gap and fill the original CB with electrons. The appearing of the impurity energy bands will provide new channels through which the electrons in impurity bands can be pumped to the CB by absorbing the visible-light photons. Therefore, this procedure can strengthen the visible-light induced photocatalytic activities of TiOS. Moreover, the visible-light absorption will also pump the electron below Fermi energy level in the CB into the empty energy levels above Fermi energy level, inducing more electron to appear at high energy levels. This also increases the photocatalytic activities of the TiOS. Thus we can draw that the 4d TM atom dopings are beneficial for increasing the visible-light utilization efficiency and improving the photocatalytic activities of TiOS.