Structural and optical characterization of CdTe quantum dots thin films

Abstract

Cadmium telluride quantum dots (CdTe QDs) have been synthesized using hot-injection chemical technique. The CdTe QDs thin films were deposited onto optical flat fused quartz substrates using thermal evaporation technique. The CdTe QDs powder and the as deposited films were characterized using X-ray diffraction and high resolution transmission electron microscope (HRTEM). The X-ray analysis shows that both CdTe QDs powder and the as deposited films crystallize in cubic zinc-blende type structure with lattice parameter 6.46Å and 6.45Å, respectively. The X-ray calculation shows that the average crystallite size of the as deposited CdTe QDs films varied from 1.1nm for the powder to 2.3nm for the thin film. The HRTEM examination of the as deposited films shows that the average particle size vary from 2.5nm for the powder to 2.7nm for the thin film. For the as deposited films, the dependence of (αhν)2 on the incident photon energy indicates that the optical transitions within the film are allowed direct with energies observed at Eg1≅2eV and Eg2≅2.3eV which attributed to quantum confinement effect. The optical band gap increases from 1.5eV for microstructure CdTe to 2eV for nanostructure quantum dots which corresponding to wavelength(620nm) so it is a great benefit to use CdTe quantum dots as solar harvesting devices application in solar spectrum region (400–800nm). Urbach energy is calculated and found to be 360meV which is higher than microstructure CdTe. The refractive index and refractive index dispersion of the as deposited CdTe QDs film has been calculated from transmission and reflection spectra. It has been found that the refractive index is reduced from (2.66) for microstructure CdTe to be (1.7) for CdTe quantum dots. The variation of the refractive index at normal dispersion is well described by Wemple–DiDomenico single oscillator model. The dielectric constant at infinite frequency ε∞ and the ratio of free carriers’ concentration to the effective mass (N/m∗) are calculated and discussed. Finally, the non linear optical parameters are calculated using some empirical relation.