<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">NJGC</journal-id><journal-title-group><journal-title>New Journal of Glass and Ceramics</journal-title></journal-title-group><issn pub-type="epub">2161-7554</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/njgc.2016.61001</article-id><article-id pub-id-type="publisher-id">NJGC-62890</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Synthesis and Characterization of Triply Doped Nano-Composite Alumina-Phospho- Silicates SiO&lt;sub&gt;2&lt;/sub&gt;-P&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt;-Al&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt; with Er&lt;sup&gt;3+&lt;/sup&gt;, Sm&lt;sup&gt;3+&lt;/sup&gt; and Yb&lt;sup&gt;3+&lt;/sup&gt; Ions Prepared by Sol Gel Technique in Two Different Forms Thin Film and Monolith
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>K. Battisha</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>M.</surname><given-names>A. Salem</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Y.</surname><given-names>Badr</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>M.</surname><given-names>Kamal</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>A.</surname><given-names>M. S. El Nahrawy</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>National Institute of Laser Enhancement Sciences (NILES), Cairo University, Giza, Egypt</addr-line></aff><aff id="aff1"><addr-line>Department of Solid State Physics, National Research Center (NRC), Dokki, Egypt</addr-line></aff><aff id="aff3"><addr-line>Physics Department, El Mansoura University, Mansoura, Egypt</addr-line></aff><pub-date pub-type="epub"><day>14</day><month>01</month><year>2016</year></pub-date><volume>06</volume><issue>01</issue><fpage>1</fpage><lpage>7</lpage><history><date date-type="received"><day>17</day>	<month>May</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>18</month>	<year>January</year>	</date><date date-type="accepted"><day>21</day>	<month>January</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Nano-composite monolith and thin film Alumina-Phospho-Silicates (SiO
  <sub>2</sub>-P
  <sub>2</sub>O
  <sub>5</sub>-Al
  <sub>2</sub>O
  <sub>3</sub>):Ln (Ln = Sm, Er, Yb) glasses activated by triply doped with three different rare earth ions (REIs) (Er
  <sup>3+</sup>:Yb
  <sup>3+</sup>:Sm
  <sup>3+</sup>) were prepared by modified sol-gel process. The composition of the prepared samples was 
  as follow (SiO<sub>2</sub>:11P<sub>2</sub>O<sub>5</sub>:3Al<sub>2</sub>O<sub>3</sub>:1.2Er<sub>2</sub>O<sub>3</sub>:(1.2 - 3)Yb<sub>2</sub>O<sub>3</sub>:(0.7 - 1.3)Sm<sub>2</sub>O<sub>3</sub>). Tetra-ethyl-orthosilicate (TEOS), tri-ethyl-phosphate (TEP), erbium nitrate, ytterbium nitrate and samarium nitrate were used as precursor materials, respectively. The structure of the prepared samples was studied using X-ray diffraction (XRD), which revealed that the crystallite sizes of monolith and thin film samples both sintered at 900℃ at constant Sm
  <sup>3+</sup> concentration at 1.3 mol% (SPAE
  <sub>1.2</sub>Y
  <sub>1.8</sub>S
  <sub>1.3</sub>) have the following values 44 and 31 nm, respectively. Transmission Electron Microscopy (TEM) of the same prepared samples was used to confirm the presence of nano-structure phase. The photo-luminescence study will be evaluated for the prepared. 
    
 
</p></abstract><kwd-group><kwd>Sol Gel</kwd><kwd> XRD</kwd><kwd> TEM and Photoluminescence</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>With introduction of internet super highway and increasing demand for broadband data transmission, there is an increasing demand for performance materials with high reliability and low cost small form factor components to meet the needs of miniaturised devices. Such components (including couplers, splitters, tunable lasers, optical amplifiers, etc.) require high grade materials and industrial low cost effective processes. Indeed, sol-gel process appeared to us as one of the best processes to consider. Interaction between SiO<sub>2</sub> and P<sub>2</sub>O<sub>5</sub> derivatives could serve as a model for the precursor coating in the integrated optics technology. Silicon oxide resulting from Si device could serve as interface for a better adherence of the film.</p><p>Incorporating rare earth ions in the host matrix also allow controlling its refractive index as well as its optical activity, absorption etc. However, a limitation for such optical devices is the precipitation of rare earth oxides or insoluble phospho-silicates. Therefore, it is worth to investigate the sol-gel preparation process of the prepared samples that determine the highest concentration of rare earth allowed without running into uncontrolled crystallization and clustering problems. It is also of importance to underline the chemical durability of the materials as most of P<sub>2</sub>O<sub>5</sub> based compound suffers from its hygroscopic character [<xref ref-type="bibr" rid="scirp.62890-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.62890-ref5">5</xref>] .</p><p>In the present work, a simple sol-gel procedure was successfully used for the preparation of alumina-phospho- silicate as monolith and thin film forms prepared from the same precursor materials, using the tetra-ethoxysilane and triethyl-phosphate precursors. Silica-phosphate glasses activated by Sm<sup>3+</sup>, Er<sup>3+</sup> and Yb<sup>3+</sup> ions were prepared by sol-gel route, using monolith and spin-coating methods. The structure of the prepared samples will be evaluated by using XRD. The effect of co-incorporating these two forms of materials with Sm<sup>3+</sup>, Er<sup>3+</sup> and Yb<sup>3+</sup> ions on the structure and optical properties will be discussed.</p></sec><sec id="s2"><title>2. Experimental</title><p>The investigated nano-composite Alumina-Phospho-Silicates (SiO<sub>2</sub>-P<sub>2</sub>O<sub>5</sub>-Al<sub>2</sub>O<sub>3</sub>) pure and Triply doped with three different rare earth ions (REIs) (Er<sup>3+</sup>:Yb<sup>3+</sup>:Sm<sup>3+</sup>) have been prepared by sol-gel technique in monolith and thin film forms with sintering at different temperatures ranging from 200 up to 900˚C. The starting materials used in this study are tetraesoxisilane and triethyl phosphate for SiO<sub>2</sub> and P<sub>2</sub>O<sub>5</sub> precursors, respectively. The other trivalent oxides are incorporated using nitrate solutions as shown in the flow chart of samples preparation given in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the monolithic and thin film forms were obtained by hydrolysis and poly-condensation of tetra-ethoxysilane (CH<sub>3</sub>CH<sub>2</sub>OH)<sub>4</sub>Si (TEOS, 99.999%, Sigma-Aldrich) and Triethyphosphate (C<sub>2 </sub>H<sub>5</sub>O)<sub>3</sub>P(O) reacted in ethanol solution under vigorous stirring with distilled H<sub>2</sub>O containing HCl used as a catalyst. Then the</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Flow chart for the preparation of Alumina-Phospho- Silicates gels doped with (Er<sup>3+</sup>, Er<sup>3+</sup>: Yb<sup>3+</sup>&amp; Er<sup>3+</sup>: Yb<sup>3+</sup>: Sm<sup>3+</sup>) preparation in monolithic and thin film forms</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030088x6.png"/></fig><p>Er<sup>3+</sup>, Yb<sup>3+</sup> and Sm<sup>3+</sup> ions were introduced in the process, by mixing with rare earth nitrate solutions with molar ratios of 1.2 and 1.8 mol% of Er<sub>2</sub>O<sub>3</sub> and Yb<sub>2</sub>O<sub>3</sub><sub> </sub>and Sm<sub>2</sub>O<sub>3</sub> of 0.7, 1.1 and 1.3 mol%, and 3 mol% of Al<sub>2</sub>O<sub>3</sub>, were added, respectively. In order to increase the solubility of rare earth in the glass matrix due to the valence match between the rare-earth dopant (RE<sup>3+</sup>) and the substituted cation (Al<sup>3+</sup>). The resulting homogeneous solutions were used to prepare both monolithic and thin film materials using the process indicated hereafter in reference [<xref ref-type="bibr" rid="scirp.62890-ref4">4</xref>] :</p><p>1) Preparation of monolith samples: Solutions were filled in a mold and aged for one week at room temperature and then dried in a drying oven type GFL 71.5 at about 60˚C for about 21 days until no further shrinkage appears. Samples were found to be clear, transparent and cracks free. Densification of gel was obtained by annealing in air for three hours at temperature ranging from 60 up to 900˚C in a muffle furnace with heating rate 1.5˚C/min as reported previously by our team work [<xref ref-type="bibr" rid="scirp.62890-ref6">6</xref>] -[<xref ref-type="bibr" rid="scirp.62890-ref10">10</xref>] .</p><p>2) Thin film preparation: The remaining part of the resultant homogeneous solutions of monolith materials were used in the preparation of thin film. In this case the solutions were aged for one day at room temperature before to be dispersed on the glass and/or silica substrate, with a spun of 3500 rev./min for 30 seconds in a clean room. At least two successive coatings were required to provide suitable effective film thickness. After finishing the coating process, the films dried for 30 min and then sintered at temperature ranging from 100˚C up to 700˚C [<xref ref-type="bibr" rid="scirp.62890-ref8">8</xref>] .</p><p>Different typical examples of X-ray diffraction (XRD) patterns recorded for some monolith and thin film samples are given in Figures 2-5. Crystallite sizes G were determined using the Scherer’s equation</p><disp-formula id="scirp.62890-formula1"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1030088x7.png"  xlink:type="simple"/></disp-formula><p>with (K) Scherer constant (0.9), (l) X-ray wavelength, at D (radian) = the full width at half maximum (FWHM) of the diffraction peak and q = diffraction angle.</p><p>Microstructure and morphology for the pure Alumina-Silica-Phosphate were characterized using “JEOL transmission electron microscope” (Model: Jeol 1230 magnification up to 600 kx, resolution down to 0.2 nm, accelerating voltage 100 kV, can reach 120 kV through steps).</p><p>For photoluminescence (PL) measurement the samples were excited using the 514 nm line of a Spectra Physics 2017 Argon laser. A fiber optic probe coupled to a Dilor Super head, equipped with a suitable notch filter was employed.</p><p>The chemical composition given in <xref ref-type="table" rid="table1">Table 1</xref> in terms of the starting mixture of the precursors used according to the chart given in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p></sec><sec id="s3"><title>3. Results and Discussion</title>XRD Analysis<p>As expected the (as prepared) samples monolith and thin films both sintered at 900˚C for three hours, results in a better crystallization of the analyzed XRD patterns. However even after a sintering of 3 hours at 900˚C, a slight remain of amorphous phase is still observable on XRD patterns, as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. Indeed the major constituents of all prepared monolith and thin films in the present study are SiO<sub>2</sub> and P<sub>2</sub>O<sub>5</sub>. Therefore it is normal to expect the resulting crystalline phases to belong to the binary system SiO<sub>2</sub>-P<sub>2</sub>O<sub>5</sub> or close to this line. All XRD patterns in <xref ref-type="fig" rid="fig2">Figure 2</xref> tend to confirm that the crystalline phases, after sintering at 900˚C at constant Er<sup>3+</sup> and Yb<sup>3+</sup></p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Equivalent oxide (mol %) of the starting mixture of the investigated materials</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Formal starting oxide mixture (mol %)</th><th align="center" valign="middle" >Symbol</th></tr></thead><tr><td align="center" valign="middle" >Monolith samples</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >(SiO<sub>2</sub>: 11 P<sub>2</sub>O<sub>5</sub>: 3Al<sub>2</sub>O<sub>3</sub>: 1.2 Er<sub>2</sub>O<sub>3</sub>: 1.8 Yb<sub>2</sub>O<sub>3</sub>: (0.7) Sm<sub>2</sub>O<sub>3</sub>)</td><td align="center" valign="middle" >SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>0.7 </sub></td></tr><tr><td align="center" valign="middle" >(SiO<sub>2</sub>: 11 P<sub>2</sub>O<sub>5</sub>: 3Al<sub>2</sub>O<sub>3</sub>: 1.2 Er<sub>2</sub>O<sub>3</sub>: 1.8 Yb<sub>2</sub>O<sub>3</sub>: (1.3) Sm<sub>2</sub>O<sub>3</sub>)</td><td align="center" valign="middle" >SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>1.3 </sub></td></tr><tr><td align="center" valign="middle" >Thin film sample</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >(SiO<sub>2</sub>: 11 P<sub>2</sub>O<sub>5</sub>: 3Al<sub>2</sub>O<sub>3</sub>: 1.2 Er<sub>2</sub>O<sub>3</sub>: 1.8 Yb<sub>2</sub>O<sub>3</sub>: (1.3 Sm<sub>2</sub>O<sub>3</sub>)</td><td align="center" valign="middle" >SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>1.3</sub></td></tr></tbody></table></table-wrap><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> XRD patterns of Alumina-Phospho-Silicates mono- lith samples triply doped with Er<sup>3+</sup>, Sm<sup>3+</sup> and Yb<sup>3+</sup> ions; SPAE<sub>1.2</sub>Y<sub>1.8</sub> with different mol% of Sm<sub>2</sub>O<sub>3</sub> equal to 0.7 (a), 1.1 (b) and 1.3 (c), as sintered for three hours at 900˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030088x8.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> (a) and (b) XRD patterns of Alumina-Phospho- Silicates thin film triply doped with Er<sup>3+</sup>, Sm<sup>3+</sup> and Yb<sup>3+</sup> ions; SiO<sub>2</sub>: 11 P<sub>2</sub>O<sub>5</sub>: 3 Al<sub>2</sub>O<sub>3</sub>: 1.2 Er<sub>2</sub>O<sub>3</sub>: 1.8 Yb<sub>2</sub>O<sub>3</sub>: 1.3 Sm<sub>2</sub>O<sub>3</sub>, as sintered for three hours at 900˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030088x9.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> TEM images of monolithic samples SPAE<sub>1.2</sub>Y<sub>1.8</sub> doped with 0.7 (a) and 1.3 mol% Sm<sub>2</sub>O<sub>3</sub> (b), as sintered for three hours at 900˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030088x10.png"/></fig><p>ions concentration and different concentrations of Sm<sup>3+</sup> ions are correspond to SiP<sub>2</sub>O<sub>7</sub>, Si<sub>5</sub>P<sub>6</sub>O<sub>25</sub> and Si<sub>3</sub>(PO<sub>4</sub>)<sub>4</sub>, JCPDS [71-2073], [81-1593] and [49-0206], respectively. It is clearly seen that the intensity of the peaks increase by increasing the Sm<sup>3+</sup> ions concentrations. Rare earth oxides and related compounds are in so small</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The photoluminescence (PL) emission spectra of thin film SPAE1.2Y1.8S0.7, sintered for three hours at 500˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030088x11.png"/></fig><p>quantities that they might not appeared with their corresponding X-ray diffraction patterns. The general behavior observed from the values of the crystallite size and the intensity increasing of the peaks by increasing the Sm<sup>3+</sup> ions from 0.7 up to 1.3 mol% is its increase trend by doping with 1.3 mol% of Sm<sup>3+</sup> ions, this may be due to the co-doped with Al<sup>3+</sup> ions, which enhance the solubility of samarium inside the host matrix.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows the XRD pattern of the thin film SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>1.3</sub> sintered at 900˚C for three hours. Nearly the same phases obtained from XRD patterns of monolith samples are clearly appeared in thin film sample, but the peaks have lower intensity than monolith samples due to the low thickness of film.</p><p>The crystallite size of SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>1.3</sub> sintered at 900˚C for three hours was of the order of 44 nm for monolith sample. By decreasing the Sm<sup>3+</sup> ion concentrations the crystalline size was decreased [<xref ref-type="bibr" rid="scirp.62890-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.62890-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.62890-ref12">12</xref>] . It is also seems that the thin film SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>1.3</sub> sample sintered at 900˚C, gave smaller crystalline size than monolith sample giving the following value 31 nm. The obtained XRD data are confirmed by using the Win-fit program.</p><p>The transmission electron microscopy TEM was used to confirm and complement the results obtained from XRD, as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) of monolith SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>0.07</sub> (a) and SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>1.3</sub> (b) both sintered at 900˚C. The patterns indicated the presence of the practically spherical with some agglomeration. The grain size was determined by averaging over the total number of grains in the TEM (Jeol1230) micrograph. Based on this method, the average crystallite size calculated from TEM was very close to the obtained from XRD for the same sample SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>1.3 </sub>and was found to be equal to about<sub> </sub>36 nm.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the photoluminescence (PL) emission spectra under Argon laser excitation at wavelength (488 nm) of thin film SPAE<sub>1.2</sub>Y<sub>1.8</sub>S<sub>0.7</sub>, sintered for three hours at 500˚C. It is expected here that all the energy levels of Er<sup>3+</sup>:Yb<sup>3+</sup> system will be reconstructed when doped with Sm<sup>3+</sup> ions in Alumina-Phospho-Silicates system. It is well known that the absorption cross-section of Er<sup>3+</sup> and Sm<sup>3+</sup> ions are small, for that Yb<sup>3+</sup> ions was used as a sensitizer to increase the Er<sup>3+</sup> and Sm<sup>3+ </sup>ions PL emission and offering good spectral overlap with Er<sup>3+</sup> and Sm<sup>3+ </sup>transition, thus allowing efficient Yb<sup>3+</sup>-Er<sup>3+</sup>-Sm<sup>3+</sup> energy transfer with subsequent Er<sup>3+</sup> emission. It has been well addressed that the green emissions at 534 nm have been attributed to the intra-4F-transitions of Er<sup>3+</sup> and Sm<sup>3+</sup> ions and were assigned for both rare earth elements to the (<sup>2</sup>H<sub>11/2</sub>―<sup>4</sup>I<sub>15/2</sub>) and <sup>4</sup>G<sub>5/2</sub>―<sup>6</sup>H<sub>5/2</sub>, respectively. The group red emission is attributed to another 4F-transition of Er<sup>3+</sup> and Sm<sup>3+</sup> ions assigned to (<sup>4</sup>F<sub>9/2</sub>―<sup>4</sup>I<sub>15/2</sub>) for Er<sup>3+</sup> ions. While it was assigned to<sup> 4</sup>G<sub>5/2</sub>―<sup>6</sup>H<sub>7/2</sub> at<sub> </sub>604 nm, <sup>4</sup>G<sub>5/2</sub>―<sup>6</sup>H<sub>9/2</sub> at wavelength 636, 644 and 652 nm, <sup>4</sup>F<sub>3/2</sub>―<sup>6</sup>H<sub>11/2</sub> at wavelength<sub> </sub>685 nm, <sup>4</sup>G<sub>5/2</sub>―<sup>6</sup>H<sub>11/2</sub>, for 702 and 715 nm, 731, and <sup>4</sup>F<sub>3/2</sub>―<sup>6</sup>H<sub>13/2</sub> for 795 and 810 nm in region between 600 and 800 nm for Sm<sup>3+</sup> ions [<xref ref-type="bibr" rid="scirp.62890-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.62890-ref21">21</xref>] .</p><p>The red emission is much stronger than green emissions, which may be due to effect of doping the prepared samples with Yb<sup>3+</sup> ions. The introduction of Yb<sup>3+</sup> ions in silica-phosphate host brings about great changes for the photoluminescence properties of Er<sup>3+</sup> and Sm<sup>3+</sup> ions and a moderate green to red light can be seen in thin film sample under the same excitation. Where the multiplicity of RE sites in the host matrix is known to enhance the inhomogeneous broadening of the emission and absorption lines and a red shift was observed for the emission lines.</p></sec><sec id="s4"><title>4. Conclusion</title><p>Nano-composite Alumina-Phospho-Silicates doped with 3 different RE<sup>3+</sup> erbium, ytterbium and samarium ions: (SiO<sub>2</sub>:11P<sub>2</sub>O<sub>5</sub>:3Al<sub>2</sub>O<sub>3</sub>:1.2Er:1.8Yb:(1.3)Sm), were successfully prepared by using a modified sol-gel technique, in two different forms monolith and thin film. The structure of the prepared samples was evaluated by using XRD, which revealed that the crystallite sizes decreased in thin film sample than monolith one from 44 to 31 nm by triply doped them with Er<sup>3+</sup>, Yb<sup>3+</sup> and Sm<sup>3+</sup> ions. It is well known that the absorption cross-section of Er<sup>3+</sup> and Sm<sup>3+</sup> ions is small, for that Yb<sup>3+</sup> ions are used as a sensitizer to increase the Er<sup>3+</sup> and Sm<sup>3+</sup> ions PL emission and offering good spectral overlap with Er<sup>3+</sup> and Sm<sup>3+</sup> transition, thus allowing efficient Yb<sup>3+</sup>-Er<sup>3+</sup>-Sm<sup>3+</sup> energy transfer with subsequent Er<sup>3+</sup> emission.</p></sec><sec id="s5"><title>Cite this paper</title><p>I. K.Battisha,M. A.Salem,Y.Badr,M.Kamal,A. M. S. ElNahrawy, (2016) Synthesis and Characterization of Triply Doped Nano-Composite Alumina-Phospho- Silicates SiO<sub>2</sub>-P <sub>2</sub>O<sub>5</sub>-Al<sub>2</sub>O<sub>3</sub> with Er<sup>3+</sup>, Sm<sup>3+</sup> and Yb<sup>3+</sup> Ions Prepared by Sol Gel Technique in Two Different Forms Thin Film and Monolith. New Journal of Glass and Ceramics,06,1-7. doi: 10.4236/njgc.2016.61001</p></sec></body><back><ref-list><title>References</title><ref id="scirp.62890-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Tung, S.-P. and Hwang, B.-J. (2004) High Proton Conductive Glass Electrolyte Synthesized by an Accelerated Sol-Gel Process with Water/Vapor Management. Journal of Membrane Science, 241, 315-323.  
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