<?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.2017.72002</article-id><article-id pub-id-type="publisher-id">NJGC-75778</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>
 
 
  Morphological and Structural Investigations on Iron Borosilicate 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></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abdel</surname><given-names>Meguid 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>Sammer</surname><given-names>El-Jadal</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><pub-date pub-type="epub"><day>28</day><month>04</month><year>2017</year></pub-date><volume>07</volume><issue>02</issue><fpage>13</fpage><lpage>21</lpage><history><date date-type="received"><day>November</day>	<month>16,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>April</month>	<year>25,</year>	</date><date date-type="accepted"><day>April</day>	<month>28,</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>
 
 
  Borosilicate glasses and glass ceramics in the system 30Na
  <sub>2</sub>O-2Al
  <sub>2</sub>O
  <sub>3</sub>-25SiO
  <sub>2</sub>-xFe
  <sub>2</sub>O
  <sub>3</sub>(43-x)B
  <sub>2</sub>O
  <sub>3</sub> (x = 0 - 20 mol%) have been prepared and studied by distinguished techniques. X-ray diffraction (XRD), transmission electron microscope (TEM), electron diffraction pattern (EDP) and SEM experiments are applied to explore the induced structural changes. Nanometer-sized species of polycrystalline structure are formed particularly in low Fe
  <sub>2</sub>O
  <sub>3</sub> containing glasses. The size of the crystallites is found to depend on Fe
  <sub>2</sub>O
  <sub>3</sub> concentrations. It is ranged from 10 to 33 nanometers. Structurally, these materials are suggested to contain different components, crystalline component and an interfacial component which situated between the crystallized domains. Presence of these components affects the atomic arrangement without short- or long-range order. An intermediate range ordered structure is dominant in glass ceramics of Fe
  <sub>2</sub>O
  <sub>3</sub> &lt; 8 mol%. Less ordered structure is dominated in glasses of higher Fe
  <sub>2</sub>O
  <sub>3</sub> concentration, since more disordered structure of lower size is present. These structural changes are found to be connected with the role of Fe
  <sub>2</sub>O
  <sub>3</sub> and Na
  <sub>2</sub>O in glasses. Na
  <sub>2</sub>O is the strong glass modifier in the studied composition region, while Fe
  <sub>2</sub>O
  <sub>3</sub> is consumed also as a modifier in composition of &lt; 8 mol%. Glass forming character of Fe
  <sub>2</sub>O
  <sub>3</sub> is mainly dominant in the composition region of higher iron oxide concentration (8 - 20 mol%).
 
</p></abstract><kwd-group><kwd>Borosilicate</kwd><kwd> Morphology</kwd><kwd> Glass Ordered Structure</kwd><kwd> Clusters</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Glasses and glass ceramics containing metal oxide have a wide variety in most of industrial and technical applications [<xref ref-type="bibr" rid="scirp.75778-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref3">3</xref>] . However, a growing development of technical technology requires specific types of glasses. For instance, specific composition from borosilicate glasses has been devoted as special sealants for Molten Carbonate Fuel Cells (MCFC) [<xref ref-type="bibr" rid="scirp.75778-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref3">3</xref>] . Both academic and technical advantages of borosilicate glasses have been correlated with some specific structural studies which were carried out on these materials. Powerful techniques such as spinning NMR and FTIR spectroscopy [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref7">7</xref>] are the most suitable methods applied to get a quantitative analysis of different structural units forming a network structure of the tested material.</p><p>The changes in microstructure of borosilicate glasses were found to depend on their own building species such Q<sup>n</sup> [SiO<sub>4</sub>], [BO<sub>3</sub>] and [BO<sub>4</sub>] units in borosilicate network. In miscibility region of borate and silicate network structure, the oxygen atoms can be bonded to boron and silicon atoms and have a Na<sup>+</sup> ion as a charge compensator [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref6">6</xref>] . In such situation, phase separation can’t be considered and both the borate and silicate network are both mixed and modified by Na<sub>2</sub>O. On the other hand, in the immiscibility region, phase separation is the dominant feature and has a significant influence on the structure and properties of the materials [<xref ref-type="bibr" rid="scirp.75778-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] . The properties in phase separating glasses strongly depend on the thermal history and material composition [<xref ref-type="bibr" rid="scirp.75778-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref10">10</xref>] . In borosilicate glasses, at least two phases are separated in certain composition regions. The original glassy phase tends to separate into a silica-rich phase, and a borate-rich one upon changing glass composition.</p><p>The arrangement of the modifier oxide between silicate and borate network depends on two structural factors namely R and K. Generally R is the ratios of Na<sub>2</sub>O/B<sub>2</sub>O<sub>3</sub> and K is the ratio of SiO<sub>2</sub>/B<sub>2</sub>O<sub>3</sub> [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref6">6</xref>] . For example, for small value of R (&lt;0.5) and higher K, separated phases can take place. Otherwise, the structural species of silicate and borate units are mixed.</p><p>The present paper aims to make use of our recent published work which based on NMR and FTIR spectroscopy [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] to shed more light on detailed structure of borosilicate glasses containing iron oxide. In this regard, XRD, ED spectroscopy, SEM and TEM are applied to give information on different range ordered structure which may be affected by changing Fe<sub>2</sub>O<sub>3</sub> concentration in the studied glasses.</p></sec><sec id="s2"><title>2. Experimental Methods</title><sec id="s2_1"><title>2.1. Sample Preparation</title><p>The glasses were prepared from raw materials graded SiO<sub>2</sub>, H<sub>3</sub>BO<sub>3</sub>, Na<sub>2</sub>CO<sub>3</sub>, Al<sub>2</sub>O<sub>3</sub> and Fe<sub>2</sub>O<sub>3</sub>. The sodium borosilicate glasses were prepared by melting batches in alumna crucibles at a temperature ranging from 1250˚C to 1520˚C depending on composition. Then the melt was frequently swirled to make the material free from air bubbles and to enhance homogeneity of the melt. Then, the melt has been quenched by pouring it over a stainless steel plate.</p></sec><sec id="s2_2"><title>2.2. XRD Measurement</title><p>XRD measurements were carried out using a Brucker Axs-D8 technique. CuKα radiation source (λCuKα = 0.1540600 nm) has been utalized. Data was accumulated steeply with an interval of 0.02˚, over a 2θ range of 4˚ - 65˚ using a dwell time of 0.4 seconds. The obtained experimental patterns were compared to standards compiled by Joint Committee on Powder Diffraction and Standards (JCDPS).</p></sec><sec id="s2_3"><title>2.3. Transmission Electron Microscopy (TEM)</title><p>Transmission Electron Microscopy (TEM) is a common technique used to evaluate the shape, size, and morphology of the bulk of the material. TEM investigations were carried out using a JEOL-JEM-2100, with an acceleration voltage of 200 kV. During this technique, a high energy beam of electrons is transmitted through a very thin specimen, causing interactions between the electrons and the atoms and producing the TEM images.</p></sec><sec id="s2_4"><title>2.4. SEM Micrographs and EDX Spectra</title><p>SEM micrograph were obtained with a JEOL JSM 6400 scanning electron microscope equipped with a Link analytical system. The electron energy used was 20 keV. The SEM and EDX analysis were carried out for some selected samples.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. XRD Studies</title><p>The structure of some of the investigated glasses may offers neither long-range order (like crystals) nor short-range order like glasses. It possess polycrystalline structure with intermediate range order. XRD patterns of some selected glass compositions are presented in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Weak diffraction peaks are appeared in</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> XRD pattern of borosilicate glasses containing different Fe<sub>2</sub>O<sub>3</sub> concentrations</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x2.png"/></fig><p>the patterns of the glass containing 0, 1, 3 and 5 mol% Fe<sub>2</sub>O<sub>3</sub>. These diffractions are centered at 2θ = 18.5, 25.2, 30, and 60 degree, revealing precipitation of some ordered Na<sub>2</sub>SiO<sub>3</sub> species in these glasses [Card No. 16-818]. Formation of polycrystalline cluster from Na<sub>2</sub>SiO<sub>3</sub> is accessible in these glasses, since network is enriched with NBO atoms. The total modifier content from both Na<sub>2</sub>O and Fe<sub>2</sub>O<sub>3</sub> is extremely high in these glasses [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] . This leads to formation of high concentration from non-bridging bonds (NBO) in the silicate network [<xref ref-type="bibr" rid="scirp.75778-ref9">9</xref>] . On the other hand, maximum BO<sub>4</sub> groups in borate network are also considered. This was evidenced from NMR data of the same selected glasses [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] .</p><p>In initial glasses (0 - 5 mol% Fe<sub>2</sub>O<sub>3</sub>), part of modifier oxide (Na<sub>2</sub>O and Fe<sub>2</sub>O<sub>3</sub>) is consumed to produce NBO in silicate, the other portion can be consumed to modify the borate network and the rest is distributed as accumulated polycrystalline clustered species containing Na and Fe ions. The extra modifier oxide are forced to form some nano-size crystallites or clusters from its own. As a direct result, Na<sub>2</sub>SiO<sub>3</sub> are the main species which are simply to be formed. The angular position of the diffraction lines in the XRD peaks closely match the Na<sub>2</sub>SiO [card nu.78-1713C]. On the other hand, diffraction peaks disappear for all glasses of Fe<sub>2</sub>O<sub>3</sub> &gt; 5 mol%. Only a broad hump arises revealing of less ordered glassy matrix containing poly crystalline species of extra small size. As can be seen from <xref ref-type="fig" rid="fig1">Figure 1</xref> a broad band, free from sharp diffraction, in samples of higher Fe<sub>2</sub>O<sub>3</sub> concentration (6 - 20 mol%) is the dominant. These features reflect less ordered structure of investigated glasses [<xref ref-type="bibr" rid="scirp.75778-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.75778-ref13">13</xref>] .</p><p>Absence of sharp diffraction peaks in Fe<sub>2</sub>O<sub>3</sub> rich glasses reveals that Fe<sub>2</sub>O<sub>3</sub> inter the network as glass former [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.75778-ref10">10</xref>] . As the content of Fe<sub>2</sub>O<sub>3</sub> increases the concentration of total modifier and NBO ion decreases [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] . As a consequence, the concentration of the well-formed ordered Na<sub>2</sub>SiO<sub>3</sub> should be decreased. The decrease in Na<sub>2</sub>SiO<sub>3</sub> concentration is considered as a result of formation of FeO<sub>4</sub> units as a former species. Formation of such units required more modifier which would be withdrawn from both silicate and borate network. As a result the modified silicate units (Na<sub>2</sub>SiO<sub>3</sub>) should be reduced.</p></sec><sec id="s3_2"><title>3.2. Morphology and Phase Analysis</title><sec id="s3_2_1"><title>3.2.1. TEM and EDP</title><p>Evidences based on XRD data are in a good agreement with that obtained from TEM and EDP, Figures 2-6. Both confirmed that well-formed structural species are constructed in its amorphous state in glasses of high concentration Fe<sub>2</sub>O<sub>3</sub> (≥ 6 mol%). Samples of 10 &amp; 20 mol% Fe<sub>2</sub>O<sub>3</sub> are presented as examples, <xref ref-type="fig" rid="fig5">Figure 5</xref> and <xref ref-type="fig" rid="fig6">Figure 6</xref>. On the other hand, at lower Fe<sub>2</sub>O<sub>3</sub> contents, sub crystallized species are formed within the glassy state. The crystal size and morphology of the crystalline phases is shown to depend on the glass composition, particularly on Fe<sub>2</sub>O<sub>3</sub> concentration. The size of well-formed ordered species in poor iron glass (1 mol% Fe<sub>2</sub>O<sub>3</sub>) is ranged from 21 to 37 nm as listed in TEM micrograph <xref ref-type="fig" rid="fig1">Figure 1</xref>. While the size is decreased upon more addition of Fe<sub>2</sub>O<sub>3</sub>, since it lies in the region of 7 - 10 nm. The decrease of cluster size with increasing Fe<sub>2</sub>O<sub>3</sub> content</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> TEM and EDP of glass containing 1 mol % Fe<sub>2</sub>O<sub>3</sub>.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x3.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x4.png"/></fig></fig-group><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> TEM and EDP of glass containing 3 mol Fe<sub>2</sub>O<sub>3</sub>.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x5.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x6.png"/></fig></fig-group><p>confirms that iron has high ability to withdraw NBO from the silicate and plays the role of a glass former [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] . This would accompanied by a decreasing size and the content of sodium silicate clustered phases.</p><p>As shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref>, micro-crystallized clustered species are clearly evidenced in glasses containing 1 and 3 mol% Fe<sub>2</sub>O<sub>3</sub>, since iron and sodium oxide can play a role of modifier [<xref ref-type="bibr" rid="scirp.75778-ref4">4</xref>] . On the other hand, the concentration of the aggregated clustered species is shown to decrease with increasing Fe<sub>2</sub>O<sub>3</sub> content, see Figures 4-6. In such situation, Fe<sub>2</sub>O<sub>3</sub> has the ability to withdraw more and more NBO and Na ions from the silicate network which in turns</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> TEM and EDP of glass containing 6 mol Fe<sub>2</sub>O<sub>3</sub>.</title></caption><fig id ="fig4_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x7.png"/></fig><fig id ="fig4_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x8.png"/></fig></fig-group><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> TEM and EDP of glass containing 10 mol Fe<sub>2</sub>O<sub>3</sub>.</title></caption><fig id ="fig5_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x9.png"/></fig><fig id ="fig5_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x10.png"/></fig></fig-group><p>reduces the content and the size of the well-formed clusters.</p><p>It can be observed from TEM and EDP that the disorder of the aggregated species increases with increasing Fe<sub>2</sub>O<sub>3</sub> concentration. The interconnection between different species drops down on further increase in Fe<sub>2</sub>O<sub>3</sub> concentration and becomes almost indistinguishable from the background at around 20 mol% % Fe<sub>2</sub>O<sub>3</sub>, see <xref ref-type="fig" rid="fig6">Figure 6</xref>.</p></sec><sec id="s3_2_2"><title>3.2.2. SEM and EDEX Analysis</title><p>Same observation is observed from SEM micrographs <xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref>,</p><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> TEM and EDP of glass containing 20 mol %Fe<sub>2</sub>O<sub>3</sub>.</title></caption><fig id ="fig6_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x11.png"/></fig><fig id ="fig6_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x12.png"/></fig></fig-group><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> SEM and EDEX spectra of glass containing 3 mol% Fe<sub>2</sub>O<sub>3</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x13.png"/></fig><p>The concentration of the aggregated species is shown to be more higher in sample containing 3 mol% Fe<sub>2</sub>O<sub>3</sub> (<xref ref-type="fig" rid="fig7">Figure 7</xref>) when it compared with sample of higher iron oxide <xref ref-type="fig" rid="fig8">Figure 8</xref>. This observation supports that both concentration of NBO and the modifier in the silicate network are reduced. Fe<sub>2</sub>O<sub>3</sub> changes its role from modifier to former to form FeO<sub>4</sub> groups. As a result the size and concentration</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> SEM and EDEX spectra of glass containing 10 mol% Fe<sub>2</sub>O<sub>3</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1030159x14.png"/></fig><p>of polycrystalline species (Na<sub>2</sub>SiO<sub>3</sub>) should be decreased as presented from both SEM and TEM micrographs.</p><p>Elemental analysis of samples containing 3 and 10 mol% Fe<sub>2</sub>O<sub>3</sub> has been also done using EDEX spectroscopy. The spectra of glass of low Fe<sub>2</sub>O<sub>3</sub> content (3 mol%) contains only Na, Si and O elements, <xref ref-type="fig" rid="fig7">Figure 7</xref>. There is no any evidence for presence of Fe in the crystalized phase. This means that (Na<sub>2</sub>SiO<sub>3</sub>) clustered phase is the dominant. On the other hand, glasses of higher Fe<sub>2</sub>O<sub>3</sub> (10 mol%), see <xref ref-type="fig" rid="fig8">Figure 8</xref> presented several Fe EDEX spectral lines which are highly resolved. In addition, spectrum of Na, O and Si are also present. The phase in such case is enriched with FeO<sub>4</sub> groups which in turns result in increasing the disorder of the (Na<sub>2</sub>SiO<sub>3</sub>) phases. Presence of FeO<sub>4</sub> groups in in sodium silicate phase causes mismatching between units which form the glass network. As a result, amorphous structure in such a case is the dominant feature of glass of containing high Fe<sub>2</sub>O<sub>3</sub> concentration. This conclusion is agreed to great extend with that obtained from both XRD and TEM results which discussed above.</p></sec></sec></sec><sec id="s4"><title>4. Conclusion</title><p>X-ray diffraction (XRD), transmission electron microscope (TEM), electron diffraction pattern (EDP) and SEM experiments are applied to analyze the structural changes. Species of polycrystalline structure are formed in low Fe<sub>2</sub>O<sub>3</sub> containing glasses. The obtained size is ranged from 10 to 33 nanometers. An intermediate range ordered structure is dominant in glass ceramics of Fe<sub>2</sub>O<sub>3</sub> &lt; 8 mol%. Less ordered structure is a feature of glasses of higher Fe<sub>2</sub>O<sub>3</sub> concentration. The type of range order is found to be connected with the role of Fe<sub>2</sub>O<sub>3</sub> and Na<sub>2</sub>O in glasses. Na<sub>2</sub>O is the strong glass modifier in the studied composition region, while Fe<sub>2</sub>O<sub>3</sub> is consumed also as a modifier in composition of &lt; 8 mol%. Fe<sub>2</sub>O<sub>3</sub> is consumed as a network former in the composition region of higher iron oxide concentration (≥8 mol%).</p></sec><sec id="s5"><title>Cite this paper</title><p>El-Damrawi, G., Hassan, A.M. and El-Jadal, S. (2017) Morphological and Structural Investigations on Iron Borosilicate Glasses. New Journal of Glass and Ceramics, 7, 13-21. https://doi.org/10.4236/njgc.2017.72002</p></sec></body><back><ref-list><title>References</title><ref id="scirp.75778-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Parkinson, B.G., Holland, D., Smith, M.E., Larson, C., Doerr, J., Affatigato, M., Feller, S.A., Howes, A.P. and Scales, C.R. (2008) Quantitative Measurement of Q3 Species in Silicate and Borosilicate Glasses Using Raman Spectroscopy. 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