<?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.2017.73007</article-id><article-id pub-id-type="publisher-id">NJGC-77486</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>
 
 
  Structural Studies on Ag&lt;sub&gt;2&lt;/sub&gt;O-P&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt; Glasses
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gomaa</surname><given-names>El-Damrawi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abdelmajued</surname><given-names>Hassan</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>Hamdy</surname><given-names>Doweidar</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>Ahamed</surname><given-names>Shaboub</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Glass Research Group, Physics Department, Faculty of Science, Mansoura University, Mansoura, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>gomaaeldamrawi@gmail.com(GE)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>30</day><month>06</month><year>2017</year></pub-date><volume>07</volume><issue>03</issue><fpage>77</fpage><lpage>89</lpage><history><date date-type="received"><day>May</day>	<month>25,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>July</month>	<year>4,</year>	</date><date date-type="accepted"><day>July</day>	<month>7,</month>	<year>2017</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>
 
 
  Silver phosphate glasses of general formula 
  x
  Ag
  <sub>2</sub>
  O&#183;(100 - x)P
  <sub>2</sub>
  O
  <sub>5</sub>
   have been investigated over compositional range from 
  x
   = 40 to 62.5 mol%. The local structure around phosphorus atom has been studied via 
  <sup>31</sup>
  P nuclear magnetic resonance. The distribution of [PO
  <sub>4</sub>
  ]Q
  <sup>n</sup>
   species as a function of composition has been shown to slightly deviate from the simple binary alkali phosphate model. An anomalous behavior has been recorded and interpreted in terms of mixed ring-chain effect in metaphosphate composition. The splitting of NMR spectra into sub resonances is assigned to different binding sites characterizing Q
  <sup>1</sup>
   ring and Q
  <sup>1</sup>
   chain structure. Higher Ag
  <sub>2</sub>
  O concentration (≥50 mol%) leads to formation of phosphate groups with specific resonance peaks which are mainly related to pyro and orthophosphate species. The rate of change of the chemical shift of the 
  <sup>31</sup>
  P NMR depends on the bond type, which in turn reflects the extent of double bonding between phosphorus and oxygen atoms. Increasing concentration of Q
  <sup>0</sup>
   with increasing Ag
  <sub>2</sub>
  O content leads to decreasing quantities of bridging and double bonds. As a consequence, specific symmetric resonance peak of higher intensity and chemical shift (Q
  <sup>0</sup>
  ) is a feature of silver rich glasses (orthophosphate). The latter species is therefore proposed to compose of separated membered rings, which cause deshielding of phosphate units. XRD and EDP studies have shown that, amorphous phosphate network is the dominant structure of glasses containing ≤ 55 mol% Ag
  <sub>2</sub>
  O. Some ordered and well crystallized phases are formed at higher Ag
  <sub>2</sub>
  O concentration. Increasing non-bridging oxygen atoms is shown to have the main effect on crystallization behavior. Orthophosphate composition is the most crystalline one among the other compositions (ultra, meta- and pyrophosphate). Presence of orthophosphate species which typically contains highest concentration from isolated Q
  <sup>0</sup>
   units is the main reason for building up crystalline Ag
  <sub>3</sub>
  PO
  <sub>4</sub>
  phosphate phase.
 
</p></abstract><kwd-group><kwd>Nuclear Magnetic Resonance</kwd><kwd> Chemical Shift</kwd><kwd> Phosphate Species</kwd><kwd> Orthophosphates</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>It was known that P<sub>2</sub>O<sub>5</sub> consists of a three dimensional (3-D) network of trigonally connected tetrahedral PO<sub>4</sub> units with a P = O unit [<xref ref-type="bibr" rid="scirp.77486-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref4">4</xref>] . Depending on the number of bridging oxygen atoms in Q<sup>n</sup> species (n = 3, 2, 1, 0), the phosphate tetrahedral units can be described by containing high concentration of Q<sup>3</sup> species in glasses of lower modifier content [<xref ref-type="bibr" rid="scirp.77486-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref5">5</xref>] . Addition of modifier oxide degrades the 3-D network through generation of nonbridging oxygens (NBO). Continuous increasing of fraction of NBO with increasing modifier oxide was interpreted in terms of an increasing long-chain PO<sub>2</sub> groups in the glass [<xref ref-type="bibr" rid="scirp.77486-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref10">10</xref>] . This mechanism causes a structural transition from a 3-D network of interconnected PO<sub>4</sub> groups to a 1-D chain structure of intermediate-range order. This denotes a degradation and transformation of a fully polymerized neutral unit (Q<sup>3</sup>) of extremely high shielded structure to new phosphate units (Q<sup>2</sup> − Q<sup>0</sup>) of higher NBO concentration. Specifically, Q<sup>2</sup> is based on chains and rings and it has one negative charge. Q<sup>1</sup> means two tetrahedral units connected by a corner. Finally, Q<sup>0</sup> is referred to isolated and less shielded phosphate tetrahedral units with three negative charges.</p><p>The structure of phosphate glasses strongly depends on specific structural factor namely R which represents modifier (M) to phosphor (P) ratio in the glass composition [<xref ref-type="bibr" rid="scirp.77486-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref12">12</xref>] . The metaphosphate (Q<sup>3</sup>) glasses have relatively low R values (&lt;1). The pyrophosphate glasses have intermediate R (~1). This composition is consisting of Q<sup>1</sup>as the major structural units. The orthophosphate glasses typically have the highest R (&gt;1) and contain isolated Q<sup>0</sup> units.</p><p>Incorporation of metal oxide or alkali oxide in phosphate glasses [<xref ref-type="bibr" rid="scirp.77486-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref15">15</xref>] is commonly consumed in breaking down of the P-O-P linkages and formation of P-OM (M: metal) bonds. The prevalence of particular Q<sup>n</sup> unit depends on the nature and concentration of the cations present in the glass [<xref ref-type="bibr" rid="scirp.77486-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref16">16</xref>] .</p><p>Many of previous studies were carried out on phosphate glasses modified by alkali or alkaline earth oxides in the region of ultra, meta and pyrophosphate [<xref ref-type="bibr" rid="scirp.77486-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref19">19</xref>] . On the other hand, limited reports on modification by Ag<sub>2</sub>O, particularly in pyro- and orthophosphate regions, have been considered before. Therefore, this work is devoted to shed light on structural role of Ag<sub>2</sub>O in enriched modified glasses. In addition, we make use of the advantage of the high resolution modern NMR spectroscopy to report on anomalous behavior of metaphosphate glass, which to our knowledge, has not been reported before.</p></sec><sec id="s2"><title>2. Experimental Work</title><p>Binary silver phosphate glasses in the system, xAg<sub>2</sub>O∙(100 − x)P<sub>2</sub>O<sub>5</sub> where 40 ≤ x ≤ 62.5 mol% have been prepared by mixing AgNO<sub>3</sub>, and NH<sub>4</sub>H<sub>2</sub>PO<sub>4</sub> as starting raw materials. NH<sub>4</sub>H<sub>2</sub>PO<sub>4</sub> was heated in a porcelain crucible at 300˚C for 30 min in order to evaporate ammonia and water. Then AgNO<sub>3</sub> was added and the mixture was melted at temperature between 900˚C and 1100˚C, depending on the composition. The melt was swirled severally to attain homogeneity. The glass samples were obtained by pouring the melt onto flat plate. The glasses were kept in a desiccator until required.</p><p>X-ray diffraction (XRD) was used to examine the amorphous nature of the samples. The patterns were obtained by using a Burker D8 Advance powder XRD instrument. It is fitted with a Vantech super speed position sensitive detector and a Cu Ka X-ray tube with a Gobel mirror. Measurements were made over the range 4˚ to 70˚ in 2θ scale.</p><p>The internal micro structural features of glass samples were investigated using a transmission electron microscope TEM model JEOL-JEM-2100, Japan equipped (EDP) with an electron diffraction pattern unit. TEM investigations were performed at an electron acceleration voltage of 200 Kv.</p><p>Infrared spectra of the glasses were measured by a Mattson 5000 FTIR spectrometer in the range 400 and 2000 cm<sup>−1</sup>. The measurements were carried out on powdered samples which is mixed with KBr (1 wt%), and then compressing the mixtures to form pellets for measurements.</p><p>The distribution of Q<sup>n</sup> of phosphate unit obtained from <sup>31</sup>P NMR spectra of selected glasses (x = 40, 50, and 62.5 mol%). The investigations were carried out using JEOL RESONANCE GSX-500 High Resolution Solid state MAS NMR spectrometer. The spectra were obtained at high external magnetic field (11.747T), at a frequency of 160.47 MHz and spinning rate of 40 MHz.</p></sec><sec id="s3"><title>3. Results and Discussions</title><p>X-ray diffraction patterns of glasses in xAg<sub>2</sub>O∙(100−x)P<sub>2</sub>O<sub>5</sub> system are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref>. Broad pattern characterizes vitreous nature of the invest-</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> XRD patterns of glasses containing 40, 45, 50 and 55 mol% Ag<sub>2</sub>O</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x2.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> XRD patterns of glasses containing 57.5, 60 and 62.5 mol% Ag<sub>2</sub>O</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x3.png"/></fig><p>tigated glass is obviously observed between 2q = 18˚ - 38˚. This amorphous nature is dominated in glasses of 40, 45, 50 and 55 mol% Ag<sub>2</sub>O, <xref ref-type="fig" rid="fig1">Figure 1</xref>. On the other hand, significant changes were observed in Ag<sub>2</sub>O rich glasses (&gt;55 mol% Ag<sub>2</sub>O). XRD patterns which are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> contain sharp diffraction peaks superimposed on the wide hump of the glassy network. Specifically, X-ray diffraction patterns of the sample containing 57.5, 60 and 62.5 mol% Ag<sub>2</sub>O are characterized by presence of the intense sharp peak centered at 2θ = 31.9˚. Presence of these diffraction lines may indicate formation of more ordered species that characterize metaphosphate (Ag<sub>2</sub>PO<sub>3</sub>), pyrophosphate Ag<sub>4</sub>P<sub>2</sub>O<sub>7</sub> and orthophosphate Ag<sub>3</sub>PO<sub>4</sub> units distributed in the main phosphate network [<xref ref-type="bibr" rid="scirp.77486-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref16">16</xref>] . Ag<sub>4</sub>P<sub>2</sub>O<sub>7</sub> is the most dominant phase found particularly in pyrophosphate glass network containing 57.5 mol% Ag<sub>2</sub>O. X-ray diffraction data obtained for the resulting glass were found to be fitted with those reported for Ag<sub>4</sub>P<sub>2</sub>O<sub>7</sub> [JCPDS Cards File No. 11-0637]. Increasing intensity of the sharp peak with increasing Ag<sub>2</sub>O may reflect an important feature for the studied glasses. This feature could be attributed to formation of (Ag<sub>4</sub>P<sub>2</sub>O<sub>7</sub>) pyrophosphate and Ag<sub>3</sub>PO<sub>4</sub> orthophosphate crystalline phases [JCPDS Cards File No. 89-7399]. The principal peak at 31.9˚ (triplet) for reflections (211), (112) and (300) is the main diffraction pattern.</p><p>Additional evidence for the formation of an Ag<sub>4</sub>P<sub>2</sub>O<sub>7</sub> and Ag<sub>3</sub>PO<sub>4</sub> crystalline phases in silver rich glasses was also found by examination through TEM and EDP (<xref ref-type="fig" rid="fig3">Figure 3</xref>). It appears from EDP that there is a certain degree of crystallinity in glass of 62.5 mol% Ag<sub>2</sub>O. The feature appeared in EDP is in agreement with that obtained from XRD of the same glass, since sharp single diffraction is clearly evidenced from both XRD and EDP patterns, <xref ref-type="fig" rid="fig3">Figure 3</xref>(a). The remain glass network seems to be in amorphous state as represented by EDP (b), <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> TEM and EDP of Ag<sub>2</sub>O rich glass (62.5 mol% Ag<sub>2</sub>O)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x4.png"/></fig><p>Formation of high concentration of non-bridging oxygen (NBO) in silver rich glasses are considered as the main reason for building crystallized phosphate species as resolved by both XRD and TEM. When the glass network is constructed from symmetric type of units such as orthophosphate (in 62.5 Ag<sub>2</sub>O glass), symmetric and ordered phase enriched with NBO species are also constructed [<xref ref-type="bibr" rid="scirp.77486-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref16">16</xref>] . This consideration is clearly verified from both XRD and EDP of glass containing 62.5 mol% Ag<sub>2</sub>O, since one resolved XRD peak (<xref ref-type="fig" rid="fig2">Figure 2</xref>) and single diffraction of electron patterns (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)) are clearly evidenced to represent Q<sup>0</sup> in orthophosphate Ag<sub>3</sub>PO<sub>4</sub> crystalline units.</p><sec id="s3_1"><title><sup>31</sup>P MAS-NMR Spectroscopy</title><p>NMR spectra of phosphorus nuclei are very complicated due to several interconnected side bands which in some cases dilute the real spectra [<xref ref-type="bibr" rid="scirp.77486-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref20">20</xref>] . Present NMR technique has succeeded in dealing with a problem or difficulty which comes from signal of side bands. In this regard, high spinning frequency (21 kHz) and high external magnetic field (11.74 T) are both carefully applied during time scan of measurement. Therefore, side bands free NMR spectra of isotropic chemical shift are simply obtained. Then anisotropic distribution of both side bands and chemical shift are not probable in present study. Only real isotropic chemical shift of NMR spectra free from side bands is obtained.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows <sup>31</sup>PNMR spectra of glasses containing 40, 50 and 62.5 mol% Ag<sub>2</sub>O. These spectra represent glasses in selected compositions which are found in metaphosphate (40 mol%), pyrophosphate (50 mol%) and orthophosphate (62.5 mol%) extremes. It can be shown from <xref ref-type="fig" rid="fig4">Figure 4</xref> and <xref ref-type="table" rid="table1">Table 1</xref> that there are</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> <sup>31</sup>PNMR spectra of binary xAg<sub>2</sub>O∙(100 − x)P<sub>2</sub>O<sub>5</sub> glasses (x = 40, 50 and 62.5 mol%).</title></caption><fig id ="fig4_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x5.png"/></fig><fig id ="fig4_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x6.png"/></fig></fig-group><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The approximate chemical shift ranges for different types of phosphate tetrahedra in silver phosphate glasses</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Area %</th><th align="center" valign="middle" >Q<sup>0 </sup> ppm</th><th align="center" valign="middle" >Area %</th><th align="center" valign="middle" >Q<sup>1 </sup> ppm</th><th align="center" valign="middle" >Area %</th><th align="center" valign="middle" >Q<sup>2</sup> ppm</th><th align="center" valign="middle" >Area %</th><th align="center" valign="middle" >Q<sup>3 </sup> ppm</th><th align="center" valign="middle" >Composition mol%</th></tr></thead><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle"  rowspan="3"  >58.8</td><td align="center" valign="middle" >−11.5</td><td align="center" valign="middle"  rowspan="3"  >31.5</td><td align="center" valign="middle"  rowspan="3"  >−21.25</td><td align="center" valign="middle"  rowspan="3"  >9.6</td><td align="center" valign="middle"  rowspan="3"  >−24.9</td><td align="center" valign="middle"  rowspan="3"  >40Ag<sub>2</sub>O-60P<sub>2</sub>O<sub>5</sub></td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >−6.6</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >0.25</td></tr><tr><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >6.75</td><td align="center" valign="middle" >14.19</td><td align="center" valign="middle" >−6.87</td><td align="center" valign="middle" >84.18</td><td align="center" valign="middle" >−18.8</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >50Ag<sub>2</sub>O-50P<sub>2</sub>O<sub>5</sub></td></tr><tr><td align="center" valign="middle" >76.07</td><td align="center" valign="middle" >7.57</td><td align="center" valign="middle" >14.58</td><td align="center" valign="middle" >−15.4</td><td align="center" valign="middle" >9.34</td><td align="center" valign="middle" >−19.12</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >62.5Ag<sub>2</sub>O-37.5P<sub>2</sub>O<sub>5</sub></td></tr></tbody></table></table-wrap><p>apparent differences in peak position, intensity and relative area under the resonance spectra during transition from one composition to another. Significant changes in these parameters are observed with increasing Ag<sub>2</sub>O/P<sub>2</sub>O<sub>5</sub> molar ratio. The position of peaks are shown to move toward less shielded phosphate units, since spectra of less negative chemical shift are observed with increasing Ag<sub>2</sub>O concentrations. Both type and concentration of phosphate different species can be defined by analyzing the resonance spectra via band integration as well as deconvoltion. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows deconvoluted NMR spectra of glasses containing 50 and 62.5 mol% Ag<sub>2</sub>O, as examples.</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Deconvoluted NMR spectra of 50 and 62.5 mol% Ag<sub>2</sub>O glasses.</title></caption><fig id ="fig5_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x7.png"/></fig><fig id ="fig5_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x8.png"/></fig></fig-group><p>Based on analyzed data, <xref ref-type="table" rid="table1">Table 1</xref>, mixtures composed of few ultraphosphate and relatively high concentration from metaphosphate species are the main distributed units in matrix of glass of 40 mol% Ag<sub>2</sub>O. In this case, PO<sub>4</sub>groups with limited quantity of Q<sup>3</sup> and dominant Q<sup>2</sup> and Q<sup>1</sup> types are the structure species which build up metaphosphatephase. On the other hand, phosphate units containing mixture of Q<sup>2</sup> and (Q<sup>1</sup>) are the representative building units for pyrophosphate composition (50 mol% Ag<sub>2</sub>O). Finally NMR spectra of orthophosphate network reveal that both Q<sup>1</sup> and Q<sup>0</sup> are the main components of orthophosphate composition. The latter type is dominant feature of crystallization of glass containing 62.5 mol% silver oxide.</p><p>Generally, three resolved isotropic resonance line spectra were appeared between 0 ppm and −12 ppm for glass of 40 mol% Ag<sub>2</sub>O. The resonance at 0, −7 and −12 ppm are assigned to composite signals from the three phosphorus nuclei of the mixed meta and pyrophosphate groups (formally non-equivalent but accidentally having degenerate chemical shifts). One of the resonance lines is due to Q<sup>1</sup> in ring site, the other in chain site and the third characterized units of double bond and or P-OH groups [<xref ref-type="bibr" rid="scirp.77486-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref22">22</xref>] . On the other hand, based on NMR observations, orthophosphates and end groups of polyphosphates are not probable to be formed in this glass (40 mol%). This is because they resonate a different frequency (more chemical shift) than chain containing meta phosphates species [<xref ref-type="bibr" rid="scirp.77486-ref22">22</xref>] . Based on NMR chemical shift, it can clearly suggest that a change in hydration state has also to be involved [<xref ref-type="bibr" rid="scirp.77486-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref22">22</xref>] . For example, anhydrous silver pyrophosphate resonates around 1 ppm, while the signal from pyrophosphate containing dihydrogen or P-OH bonds is observed at −8 to −12 ppm. It can be seen from <xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="table" rid="table1">Table 1</xref> that positive chemical shift differences of more than 8 ppm to higher frequency are observed on going from central resonance of sample containing 40 mol% Ag<sub>2</sub>O to end resonance of glass of 62.5 mol% Ag<sub>2</sub>O.</p><p>It was confirmed previously that changes in modifier to phosphorus ratio has an effective influence on both structure and properties of glasses [<xref ref-type="bibr" rid="scirp.77486-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref22">22</xref>] . For the values R = 0, 1, 2, and 3, only specific type of structural unit can exist as the main structure; Q<sup>3</sup>, Q<sup>2</sup> Q<sup>1</sup> and Q<sup>0 </sup>unit, respectively. The NMR spectra shown in <xref ref-type="fig" rid="fig4">Figure 4</xref> are correlated to great extent with values of R. For the region 0 &lt; R &lt;1 (40 mol% Ag<sub>2</sub>O, R = 0.67 as an example), only a mixture of Q<sup>3</sup> and Q<sup>2</sup> units are found as metaphosphate species. For the region R = 1 (50 mol% Ag<sub>2</sub>O), only Q<sup>2</sup> and Q<sup>1 </sup>and limited concentration from Q<sup>0</sup> units are found. In this situation, the concentration of Q<sup>2</sup> is still higher than that of Q<sup>1</sup>+ Q<sup>0</sup>. For the region of R &gt; 1 (62.5 mol% Ag<sub>2</sub>O, R = 1.6), Q<sup>0</sup> and Q<sup>1</sup> types are found and there is no any traces from Q<sup>2</sup> can be detected. Specifically, Q<sup>0</sup> is the dominant with relative concentration of (0.79) which means that 79% from the total Q<sup>n</sup> is found in Q<sup>0</sup>. This high percentage of Q<sup>0</sup> lent support that major phosphate units are found in orthophosphate type [<xref ref-type="bibr" rid="scirp.77486-ref23">23</xref>] . As a consequence, respectively, metaphosphates with no (Q<sup>0</sup>,), pyrophosphate with limited Q<sup>0</sup>and orthophosphate with dominant concentration of (Q<sup>0</sup>) are the main species in the investigated glasses of 40, 50 and 62.5 mol% Ag<sub>2</sub>O. Because of the high concentration of NBO in glass of 62.5 mol%Ag<sub>2</sub>O, silver orthophosphate Ag<sub>3</sub>PO<sub>4</sub> species are the main crystal phase which is additionally identified by XRD and EDP pattern of this glass.</p><p>As discussed, Ag<sub>3</sub>PO<sub>4</sub> structural species are shared with significant higher relative concentration (79%) in glass formation. At this composition, the phosphatetetrahedral units containing four NBO’s and no BO’s are formed in glass of 62.5 mol% Ag<sub>2</sub>O. Any further addition of modifier to this composition would result in limiting depolymerization of the phosphate network. Therefore the 62.5 mol% Ag<sub>2</sub>O is the maximum limit of glass modification, beside it contains some of specific crystallized species from sliver orthophosphate Ag<sub>3</sub>PO<sub>4</sub>. These peculiarities may lead one to recommend some of the studied glasses to be used in the field of biomedical applications [<xref ref-type="bibr" rid="scirp.77486-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref25">25</xref>] . This may because, it contains Ag<sub>3</sub>PO<sub>4</sub> apatite phase which play the role of bioactivity. Surprising, this apatite phase is constructed in its crystalline counterpart which would in turns promotes their interaction with living cells. In addition, silver in apatite phase is important as antibacterial and antifungal agent, particularly when is used in dental applications.</p></sec></sec><sec id="s4"><title>4. FTIR Spectroscopy</title><p>The movement from a high cross-linked Q<sup>3</sup> structure, to chain-like Q<sup>2</sup> network, to depolymerized Q<sup>1</sup>/Q<sup>0</sup> glasses with increasing Ag<sub>2</sub>O concentration can be monitored by a variety of other spectroscopic probes [<xref ref-type="bibr" rid="scirp.77486-ref22">22</xref>] - [<xref ref-type="bibr" rid="scirp.77486-ref27">27</xref>] . In pure vitreous P<sub>2</sub>O<sub>5</sub> and in glass of high contents of P<sub>2</sub>O<sub>5</sub>, the basic structure entities are PO<sub>4</sub> tetrahedra forming predominantly three-dimensional network (3D) with Q<sup>3</sup> type of structural units [<xref ref-type="bibr" rid="scirp.77486-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref9">9</xref>] . Addition of modifier, part of 3D-network would depolymerize and 2D chain structure is simultaneously formed (Q<sup>2</sup> structural units). NMR Data of present glasses indicated that, the fraction of 3D network structure decreases quickly and chain structure created by Q<sup>2</sup> units dominates to the network of the glass containing 50 mol% Ag<sub>2</sub>O. More addition of Ag<sub>2</sub>O at expense of P<sub>2</sub>O<sub>5</sub> the two dimensional chain structure decreases and ring like structure containing mainly Q<sup>1</sup> and Q<sup>0</sup> units are formed. Based on this information, the following observations can be extracted from FTIR spectra upon increasing Ag<sub>2</sub>O content. From <xref ref-type="fig" rid="fig6">Figure 6</xref> it can observe that:</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> FTIR spectra of xAg<sub>2</sub>O(100 − x)P<sub>2</sub>O<sub>5</sub> glasses</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x9.png"/></fig><p>1. The intensity and area of the band centered at about 1290 cm<sup>−1</sup>, attributed to the absorption of P = O and (PO<sub>2</sub>) in Q<sup>2</sup> chains [<xref ref-type="bibr" rid="scirp.77486-ref10">10</xref>] are both decreased quickly with increasing Ag<sub>2</sub>O content. This leads that the long chain is reduced, and thus the structure of phosphate glasses is composed from shorter chain of Q<sup>1</sup> and/or isolated tetrahedral (Q<sup>0</sup>) structural unit [<xref ref-type="bibr" rid="scirp.77486-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref29">29</xref>] .</p><p>2. The wide humplies in the region between 800 - 1200 cm<sup>−1</sup> becomes narrower and shifted to higher wavenumber. The intensity and band area are both changed with increasing Ag<sub>2</sub>O concentration. For the last composition, its centering at (1140 cm<sup>−1</sup>) indicates increasing number of Q<sup>0</sup> and Q<sup>1</sup> units [<xref ref-type="bibr" rid="scirp.77486-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref30">30</xref>] .</p><p>3. The area and intensity of the broad band in the region 620 - 830 cm<sup>−1</sup> showed decreasing trends and its center (ca 680 cm<sup>−1</sup>) becomes narrower. It is referred to the stretching vibration of oxygen atoms in P-O-P bridges [<xref ref-type="bibr" rid="scirp.77486-ref29">29</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref30">30</xref>] . Decreasing area of this band leads to decreasing concentration of bridging oxygen linked between two phosphorus ions. This leads to increasing NBO in phosphate network.</p><p>Both NMR and FTIR data imply mainly considerable fragments or depolymerization of the phosphate network with an increase of Ag<sub>2</sub>O content. This is in harmony with the work presented by Hoppe [<xref ref-type="bibr" rid="scirp.77486-ref31">31</xref>] , since it was concluded that the network depolymerization is the dominant principle in modified phosphate glasses.</p><p>We consider that Ag<sub>2</sub>O as a glass modifier enters the glass by breaking up the P-O-P bonds and may introduce coordination defects along with NBO atoms in the studied glasses. This leads that the long chain is lowered, and thus the structure of P<sub>2</sub>O<sub>5</sub> glasses would involve shorter chain of Q<sup>1</sup> and/or isolated tetrahedral (Q<sup>0</sup>) structural unit [<xref ref-type="bibr" rid="scirp.77486-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.77486-ref31">31</xref>] .</p><p>The areas of absorbance spectra of the “nonbridging” in Q<sup>2</sup> stretching mode (Ca 1300 cm<sup>−1</sup>) decreases upon increasing Ag<sub>2</sub>O contents reaching its minimum value at 62.5 mol% Ag<sub>2</sub>O. This decreasing behavior may lead to progressive depolymerization of the phosphate network, as well as the increase in the average bond length of P-non-bridging oxygens presented by the band between 950 and 1200 cm<sup>−1</sup>. <xref ref-type="fig" rid="fig7">Figure 7</xref> presents a correlation between different Q<sup>n</sup> upon Ag<sub>2</sub>O addition. This behavior showed some few increment in Q<sup>2</sup> species with increasing Ag<sub>2</sub>O concentration then it abruptly decreases. A reverse behavior is seen in which it can be realized that the total NBO concentration in Q<sup>1</sup> and Q<sup>0</sup> increases at the expense of Q<sup>2</sup> structural species. The above observation is greatly correlated with that derived from both NMR and XRD results which are discussed above, since a decrease in the average p-bond character of the P-O-P upon increasing Ag<sub>2</sub>O concentration is additionally confirmed.</p></sec><sec id="s5"><title>5. Conclusion</title><p>Different phosphate glasses in meta, pyro and orthophosphate compositions have been studied by distinguished techniques. The structure of silver phosphate is slightly deviated from the alkali phosphate. This is considered due to the</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Representative relation between determined area of both Q<sup>2</sup> and (Q<sup>1</sup> + Q<sup>0</sup>) via Ag<sub>2</sub>O content</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1030167x10.png"/></fig><p>difference in field strength between silver and alkali ion. X-ray and electron diffraction pattern of metaphosphate composition revealed the amorphous nature of investigated network. Pyro and orthophosphates are documented to contain some crystallized species which are correlated with increasing NBO concentration. Using the advantage of the more recent NMR spectroscopy (11.74 T), the anomalous feature found in silver metaphosphate composition has been explored for first time. Regarding this unique feature, no previous studies have been reported.<sup>31</sup>PNMR spectra of the studied silver metaphosphate composition showed three splitting peaks of the same unit of phosphate species (Q<sup>1</sup>) which was not evidenced in alkali metaphosphate. The diverse of spectra is diminished with increasing Ag<sub>2</sub>Oto P<sub>2</sub>O<sub>5</sub> ratio and well resolved specific peaks characterized Q<sup>1</sup> and Q<sup>0</sup> are obtained. FTIR analyzed data have demonstrated the inverse relation between quantity of NBO in Q<sup>2</sup> and in other lower species (Q<sup>1</sup> + Q<sup>0</sup>). NBO species reach their highest concentration in glass of 62.5 mol% Ag<sub>2</sub>O. The concentration of NBO in this situation is high enough to construct Ag<sub>3</sub>PO<sub>4</sub> apatite units which promote the biomedical application of the glass under investigation.</p></sec><sec id="s6"><title>Cite this paper</title><p>El-Damrawi, G., Hassan, A., Doweidar, H. and Shaboub, A. (2017) Structural Studies on Ag<sub>2</sub>O-P<sub>2</sub>O<sub>5</sub> Glasses. New Journal of Glass and Ceramics, 7, 77-89. https://doi.org/10.4236/njgc.2017.73007</p></sec></body><back><ref-list><title>References</title><ref id="scirp.77486-ref1"><label>1</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Ehrt</surname><given-names> D. </given-names></name>,<etal>et al</etal>. 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