The precursors used to synthesize the silica matrix by the sol-gel method were tetraethyl orthosilicate ((Si(OC₂H₅)₄, 98%, TEOS), ethanol (CH₃CH₂OH, 99.9% Fermont), hydrochloric acid (HCl 37.1 %, Fermont), and distilled water. For the synthesis, 22.4 mmol of TEOS was dissolved in ethanol; a solution of ethanol/TEOS with a molar ratio of 4:1 was prepared according to Klein’s diagram [13] . Later, a solution of distilled water and hydrochloric acid was prepared and kept stirring for 1 h. Finally, this last solution was added to the ethanol/TEOS solution and kept stirring for 21 h.

The Al₂O₃:Eu³⁺ powders were weighed and added to the silica solution previously synthesized in such a way that the following weight ratios for Al₂O₃:Eu³⁺/SiO₂ were obtained: 13/87, 11/89, 9/91, 7/93 and 5/95. Subsequently, the mixture was placed under magnetically agitation at 60˚C until a partial hydrolysis and condensation reaction of the SiO₂ sol to SiO₂ powders with a white appearance. With the aim to determinate the complete reaction transformation of SiO₂ and eliminate organic matter which is present in the xolegel silica powders, various annealing treatments at 200˚C, 300˚C, 500˚C and 700˚C for 1 h were conducted.

In order to evaluate the chemical evolution, Fourier Transform Infrared spectroscopy (FTIR) measurements were performed on a Perkin Elmer 2000 spectrometer, using the KBr pellet method. For all measurements, the spectra were recorded from 4000 to 400 cm⁻¹. The emission and excitation spectra of the samples were recorded on a F-7000 fluorescence spectrophotometer, using a 450 W xenon lamp. The CIE coordinates for each sample were computed from the respective light emission spectra using a MATLAB code The final uncertainty in the emission and excitation spectra was 16.8 a.u. of intensity (y axis) and 0.18 nm of wavelength (on the x axis),with a confidence level of 95%.

Figure 1 shows the FTIR spectra of the Al₂O₃:Eu³⁺@SiO₂ composite powders obtained by the sol-gel method and annealed from 60˚C to 700˚C for 1 h. Despite the different silica concentration of each of the synthesized sample, the same bond vibrations related to TEOS and their decomposition to silica powders can be found. The bands in the 3000 - 3600 cm⁻¹ range correspond to the stretching vibrations of the hydroxyl groups (υOH), due to the presence of water in the sample, and the band around 1634 cm⁻¹ corresponds to the OH deformation vibrations (δOH) [20] , the intensity of these bands is decreased as the temperature increases, which is related to the complete removal of chemically absorbed water. The absorption bands centered at 960 cm⁻¹ are associated with silanol groups (SiOH), and the band centered at 585 cm⁻¹ can be assigned to ethoxy groups (Si(OC₂H₅)); both are products of the hydrolysis of TEOS [13] , at the same time, a condensation reaction between SiOH and the ethoxy groups (SiOC₂H₅) is carried out, and siloxane groups (Si-O-Si) is formed, which is reflected at 1080 cm⁻¹ in the symmetry stretching of SiO₄ tetrahedra, at 798 and 450 cm⁻¹ [21] . As expected, as temperature increases, the bands related to

(SiOH) and Si(OC₂H₅) at 960 and 585 cm⁻¹ disappear in the spectra at 500 and 700˚C. This phenomenon can be attributed to the complete hydrolysis of ethoxy groups (Si(OC₂H₅)) to silanol groups and from silanol to siloxane groups.

The luminescent properties of Al₂O₃:Eu³⁺@SiO₂ composite powders were evaluated. At first, the light emission properties of the composites were analyzed as a function of the weight quantity as depicted in Figure 2. The samples were excited at a wavelength of 280 nm. The main emission peak at 613 nm can be ascribed to the transition ⁵D₀→⁷F₂, and the emissions at 577, 592 and 650 nm correspond to the transitions ⁵D₀→⁷F₀, ⁵D₀→⁷F₁ and ⁵D₀→⁷F₃ respectively [22] . From the spectra, it is observed that the bare Al₂O₃:Eu³⁺ sample show the maximal emission intensity. When silica is incorporated to the alumina powders to form the composite powders, the emission decreases in half for all the samples: Al/Si equal to 13/87, 11/89, 9/91, 7/93 and 5/95. Thus, even with a higher concentration of 95 w% the emission intensity is kept. Besides, with the addition of silica, a broad band centered at 440 nm appears but the intensity emission is poor because the samples were excited at 280 nm. Besides, with the addition of silica, a broad band centered at 440nm appears but the intensity emission is poor because the adequate excitation for Al₂O₃ is at 350nm. It is an excellent approach to reduce the cost and obtain a bigger quantity of luminescent material.

On the other hand, by varying the excitation wavelength from 270 to 340 nm, the intensity emission of the composite powders of the sample 5/95 is highly affected (Figure 3). For instance, when the sample is exited at 270 nm the intensity at 610 nm is the more intense, but as the wavelength increases to 290 to 310 and

340 nm, this transition is highly reduced. Nevertheless, as wavelength increases, the silica shows a broader and a higher emission intensity. Thus, it is possible that controlling the intensity ratio between the blue from silica and red from Al₂O₃:Eu³⁺, the emission color changes from red to magenta to white to blue as wavelength increases from 280 to 340 nm.

Figure 3 shows the emission intensity of sample 5:95 exited at 280, 310 and 340 nm. When the composite powders are excited at 270 nm, the europium transition ⁵D₀→⁷F_J (where J = 0, 1, 2, 3) are more intense and a low intense broadband covering the blue region is observed. However, when the sample is excited at 310 nm the blue emission centered at 440 nm is increased but the red emission is reduced. The same tendency is shown when the sample is excited at 340 nm.

Figure 4 shows the CIE coordinates of sample 5:95 exited at 270, 310 and 340 nm, in addition, the pure Al₂O₃:Eu³⁺ CIE coordinates are put as a comparison. For pure Al₂O₃:Eu³⁺ powders, a red emission is obtained because of the main ⁵D₀→⁷F₂ transitions from Eu³⁺. By exciting the composite powders at 270 nm, the intensity ratio, I_blue/I_red = 0.4 and the emission is a white near color with CIE coordinates about x = 0.34, y = 0.27. The europium transition is more intense than the broad band centered at 440 nm covering the blue region. However, when the sample is excited at 310 and 340 nm the blue emission centered at 440 nm is highly increased, giving I_blue/I_red = 5.7 with an excitation of 340 nm.

The Table 1 shows the optical properties of the composite powders. As can be seen, different color emission can be obtained as a function of wavelength. For the bare Al₂O₃:Eu³⁺ sample, the transition ⁵D₀→⁷F₂ gives a strong band at 613 nm (red emission) while increasing the wavelength excitation to 310 and 340 the emission intensity decreases.