Synthesis of Yb 3 + Doped TiO 2 Nano Particles Powder as IR Filter via Sol-Gel

Ytterbium doped TiO2 nano-particles were prepared via Sol-Gel Technique under varying conditions to investigate the effects of Ytterbium ion doping on the Titania optical properties in MID IR range. X-ray diffraction analyses show that prepared Yb doped TiO2 samples have polycrystalline structure in Anatas phase. FTIR spectrums for pure and doped samples after annealing process show a single transmission peak at wave number around 1145 cm. Transmission rate of this peak depends on Yb concentrations and its value rises from 1.82% (for pure TiO2) to 58.1% (for doped with 1.13 wt% Yb). Slightly peak shift occurs at a lower doping rate with no further response to higher concentration rate. FTIR spectra gives a good indication in direction of preparation of optical band-pass filter at a wavelength around 8.733 μm (~1145 cm).


Introduction
Titanium dioxide as a semiconductor photocatalyst has attracted a great deal of attention due to its scientific and technological importance.Nano-particles TiO 2 has promising applications in many fields such as photocatalyst for environmental purification, solar energy conversion, sensors, self-cleaning, super-hydrophilic smart material and so on [1][2].
One of the most important aspects of TiO 2 is its photocatalytic activity of degrading various organic pollutants with its high catalytic efficiency, high chemical stability, non-toxicity and low cost.Despite its promising properties, however, there are several problems that limit the photocatalytic activity of TiO 2 .For example, due to the large band gap, it can be photo-exited only in the ultraviolet region, which comprises less than 5% of the overall solar energy spectrum.Another problem is the recombination of electrons and holes that generally take place in the large TiO 2 particles.It substantially reduces the number of free charges on the surface and lowers the photocatalytic activity.Therefore, several methods have been employed to improve the photocatalytic efficiency of TiO 2 .
Recently, doping lanthanide into TiO 2 attracted much attention [3][4][5][6][7].Lanthanide ions are known for their abil-ity to form complexes with various Lewis bases (e.g.acids, amines, aldehydes, alcohols, thiols, etc.) due to the interaction of these functional groups with the f-orbital of the lanthanides [6].Thus, incorporation of lanthanide ions into a TiO 2 matrix could provide a way to concentrate the organic pollutant on the semiconductor surface and therefore enhance the photoactivity of Titania [6].
Sol-gel process is one of the most successful techniques for preparing nanocrystalline metallic oxide materials due to low cost, easy of fabrication (flexibility) and low processing temperatures.Generally, in a typical solgel process, a colloidal suspension or a sol is formed due to the hydrolysis and polymerization reactions of the precursors, which on complete polymerization and loss of solvent leads to the transition from the liquid sol into a solid gel phase.The wet gel can be converted into nanocrystals with further drying and hydrothermal treatment [8,9].

Samples Preparation
The doped and un-doped titania nanoparticles were synthesized by sol-gel method from Titanium (IV)-isopropoxide (TTIP) (Aldrich 98%), Ethanol (EtOH 99.9%) from GCC, hydrochloric acid (HCl, 34.5%) from BDH and Ytterbium(III) oxide (Aldrich).Deionized water was used for the hydrolysis of (TTIP) and preparation of pure and doped TiO 2 Sol.The final solution was left for 30 minutes under magnetic stirring.The reaction was performed at a cooler water jacket (i.e. the solution was cooled by water at temperature (10˚C -15˚C).The amount of each chemical in this procedure was TTIP:H 2 O:EtOH: HCl = 1:1:10:0.1 in molar ratio.The gelation of monoliths was achieved by pouring the sol into covered glass tube at room temperature.After aging for 24 hour, first drying occurred for 1 hour at temperature 60˚C.Then samples left in room temperature without covers in order to permit solvent evaporation through the drying process.The doping rate of samples with Yb 3+ equal to: 0 wt%, 0.21 wt%, 0.68 wt% and 1.13 wt%.

Samples Characterization
All samples were calcinated for 2 hour in a box furnace operating at 500˚C in an ambient atmosphere.Structural characterizations of the doped and un-doped TiO 2 samples were done by X-ray diffraction (XRD).θ -2θ scans were recorded using ITAL-STRUCTURE diffractometer equipped.While Mid-IR spectra were obtained for the prepared samples using FT-IR spectrometer, Shimadzu, on KBr pellets of the samples

Result and Discussion
The X-ray diffraction spectrums (XRD) were illustrated in Figure 1 for the doped and undoped samples after annealing process, which show that prepared samples have polycrystalline structure in Anatas phase [10][11][12].
The FTIR spectrums were illustrated in Figures 2 and  3 for the samples before and after annealing process respectively.The peaks at 667 cm −1 , 505 cm −1 and 447 cm −1 are attributed to Ti-O bond.The peak at 667 cm −1 refers to symmetric O-Ti-O stretch while peak at 447 cm −1 and 505 cm −1 are due to the vibration of Ti-O bond [13][14].Another two bands were appeared at about 1600 cm −1 and 3400 cm −1 .These two absorption bands are attributed to the characteristics vibration of O-H bond in water molecules [15,16], and indicating that the drying process at 60˚C does not completely trap the wate r molecules from the pores of Titania network.After annealing process at 500˚C the last two absorption bands were disappeared from FTIR spectrums (Figure 3).
The important result that could be seen from the FTIR spectra is the existence of transmission peak centered at around 1145 cm −1 .Annealing process at 500˚C improves the transmission rate of this peak.Furthermore, doping with Yb 3+ ion makes this peak so much strong and becomes the only major peak could be observed from the FTIR spectrums in range of 4000 cm −1 to 400 cm −1  (Figure 3).This result gives a good indication in direction of production of optical band-pass filter around the wavelength 8.733 µm (~1145 cm −1 ) [3].The effect of doping rate on amplitude, FWHM of the band width and maximum peak wavelength is summarized in Table 1.
From Table 1, it can see that the two parameter transmission rate and FWHM are increase with increasing of doping rate.That's mean the two parameters effected with the amount of doping rate.While the maximum of transmission peak shifted with increasing of doping at the lower doping rate then become stable at higher concentration [3].

Conclusion
Both of annealing process and doping with Yb 3+ increase the photocatalytic efficiency of nanoparticles TiO 2 through enhancement of the transmission rate at the wave number around the 1145 cm −1 .The band width of this transmission peak is increase with increasing of doping rate.
The maximal of the transmission peak shifted with increasing of Yb 3+ concentration at the lower doping rate then became stable at higher concentration.
FTIR spectra gives a good indication in direction of preparation of optical band-pass filter at a wavelength around 8.733 µm (~1145 cm −1 ).