<?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.2017.73006</article-id><article-id pub-id-type="publisher-id">NJGC-77483</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>
 
 
  Additive Effects of Rare-Earth Ions in Sodium Aluminoborate Glasses Using &lt;sup&gt;23&lt;/sup&gt;Na and &lt;sup&gt;27&lt;/sup&gt;Al Magic Angle Spinning Nuclear Magnetic Resonance
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Shunichi</surname><given-names>Kaneko</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>Yomei</surname><given-names>Tokuda</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hirokazu</surname><given-names>Masai</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Faculty of Education, Shiga University, Hiratsu Otsu City, Shiga, Japan</addr-line></aff><aff id="aff1"><addr-line>Institute for Chemical Research, Kyoto University, Uji City, Kyoto, Japan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>tokuda@edu.shiga-u.ac.jp(YT)</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>58</fpage><lpage>76</lpage><history><date date-type="received"><day>April</day>	<month>20,</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>
 
 
  We conducted structural analysis of 
  x
  Na
  <sub>2</sub>
  O-
  y
  Y
  <sub>2</sub>
  O
  <sub>3</sub>
  -5B
  <sub>2</sub>
  O
  <sub>3</sub>
  -3Al
  <sub>2</sub>
  O
  <sub>3</sub>
   and 
  x
  Na
  <sub>2</sub>
  O-
  y
  La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses to elucidate the additive effects of rare-earth ions in these sodium aluminoborate glasses, and investigated the local environment surrounding Na<sup>+</sup> in them by using <sup>23</sup>Na and <sup>27</sup>Al magic angle spinning nuclear magnetic resonance (MAS NMR) spectroscopy. The amount of higher-coordinated Al species (<sup>[5]</sup>Al and <sup>[6]</sup>Al) gradually increased in response to an increase in the ratios of Y<sub>2</sub>O<sub>3</sub> to Al<sub>2</sub>O<sub>3</sub> and La<sub>2</sub>O<sub>3</sub> to Al<sub>2</sub>O<sub>3</sub> 
  <sub> </sub>
  in each type of glass, respectively. Moreover, the difference in the cation field strength (CFS) between Y<sup>3+</sup> and La<sup>3+</sup> was observed to affect the generation of <sup>[5]</sup>Al and <sup>[6]</sup>Al, especially when the amount of these ions in the glasses increased. In addition to the above, the coordination number of Na<sup>+</sup> ions increased with an increase in the number of rare earth ions, confirmed by comparing results with NMR spectra of crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub>. The latter possibly occurred due to the oxygen concentration on Al<sup>[5]</sup> and Al<sup>[6]</sup>. Finally, it was confirmed that the formation of <sup>[5]</sup>Al and <sup>[6]</sup>Al decreases molar volume in oxide glasses, which might be partially due to better atomic packing of <sup>[5]</sup>Al and <sup>[6]</sup>Al.
 
</p></abstract><kwd-group><kwd>NMR</kwd><kwd> Aluminoborate</kwd><kwd> Rare-Earth</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In the past decades, much attention has been paid to aluminate glasses, such as aluminoborate, aluminosilicate, or aluminoborosilicate glass, because the addition of α-alumina to oxide glasses results in high chemical stability [<xref ref-type="bibr" rid="scirp.77483-ref1">1</xref>] and/or ideal mechanical properties [<xref ref-type="bibr" rid="scirp.77483-ref2">2</xref>] . In such oxide glasses, three kinds of Al coordination exist: 4-coordinated <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al, 5-coordinated <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al, and 6-coordinated <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al, which can all be quantitatively measured by magic angle spinning nuclear magnetic resonance (MAS NMR) [<xref ref-type="bibr" rid="scirp.77483-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>] . Using structural analysis of aluminate glasses using MAS NMR, it has been clarified that their physical properties, such as fictive temperature, microhardness, elastic modulus, and refractive index, are closely related to their Al coordination [<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref8">8</xref>] . Therefore, it is important to control Al coordination in oxide glasses for adjustments of those physical properties.</p><p>In earlier reports, the relationship between the addition of network modifiers and generation of aluminum species has been reported. In particular, rare-earth ions (RE<sup>3+</sup>) such as Sc<sup>3+</sup>, Y<sup>3+</sup><sub>,</sub> or La<sup>3+</sup> could produce higher-coordinated Al species (<sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al) because they exhibit a sufficiently large cation field strength of CFS = z/R<sup>2</sup><sub>,</sub> where z is the ionic valence and R is the ionic radius [<xref ref-type="bibr" rid="scirp.77483-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref13">13</xref>] . Despite this, the glass-forming compositions of rare-earth-containing glasses were limited by high melting points of starting materials such as Y<sub>2</sub>O<sub>3</sub> or Al<sub>2</sub>O<sub>3</sub> [<xref ref-type="bibr" rid="scirp.77483-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref16">16</xref>] . Hence, control of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al formation was still difficult, and one of the few ways to control Al speciation was by using different ions (e.g., the CFS of Mg<sup>2+</sup> is lower than that of rare-earth ions, which suppressed the formation of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al). Considering the development of functional glasses, it is important to investigate the relation between more complex compositions, Al coordination, and physical properties, because commercially used glass for optical or building applications contains several elements. Therefore, it would be interesting if, even in glasses that contain four or five elements, rare-earth ions can produce higher coordinated Al species that affect the physical properties of the glass.</p><p>We considered that the addition of Na<sup>+</sup> to aluminoborate glasses that contain several RE<sup>3+</sup> species could expand the glass formation region and generate the intended amounts of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al, proportional to the ratio of RE<sup>3+</sup> to Al<sub>2</sub>O<sub>3</sub>. Although NMR analysis of various aluminoborate glasses has been performed (e.g., Na<sub>2</sub>O-B<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>, Y<sub>2</sub>O<sub>3</sub>-B<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>, or La<sub>2</sub>O<sub>3</sub>-B<sub>2</sub>O<sub>3</sub>-Al<sub>2</sub>O<sub>3</sub>) [<xref ref-type="bibr" rid="scirp.77483-ref17">17</xref>] - [<xref ref-type="bibr" rid="scirp.77483-ref24">24</xref>] , most of these analyses have been done with mono-network modifiers. Herein, we structurally analyzed yttrium sodium aluminoborate and lanthanum sodium aluminoborate glasses in order to observe the relationship between the addition of RE<sup>3+</sup> and the formation of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al. Simultaneously, we investigated the local structure of Na<sup>+</sup> in order to understand its role in these glasses. Finally, we measured the molar volumes in these glasses in order to understand the direct relationship between the formed amounts of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al and the physical properties of the glasses. As a result of the above experiment, the structural roles of RE<sup>3+</sup>, Na<sup>+</sup> and Al<sup>3+</sup> in quaternary aluminoborate glass have been clarified.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Synthesis</title><sec id="s2_1_1"><title>2.1.1. Preparation of Sample Glasses</title><p>All glass samples were prepared using a melting method from chemically pure Na<sub>2</sub>CO<sub>3</sub>, Y<sub>2</sub>O<sub>3</sub>, La<sub>2</sub>O<sub>3</sub>, B(OH)<sub>3</sub>, and Al<sub>2</sub>O<sub>3</sub> as starting materials. Stoichiometric powders were mixed using agate mortar and melted in a platinum crucible at 1550˚C - 1600˚C for 30 min. Subsequently, melts were quenched by a metal plate that was pre-heated to 300˚C in order to prevent them from cracking. The glasses thus obtained had compositions of xNa<sub>2</sub>O-yY<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> and xNa<sub>2</sub>O-yLa<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub>, with (x, y) combinations of (6, 0), (4.8, 0.4), (3.96, 0.66), (3, 1), (1.98, 1.32), (1.2, 1.6) and (0, 2). Considering Al<sub>2</sub>O<sub>3</sub> and B<sub>2</sub>O<sub>3</sub> as network modifiers, the total cation valence was set to be +12 in all compositions in order to keep ratio of cation valence to network modifier unchanged. Glass transition temperatures (T<sub>g</sub>) were measured by differential thermal analysis (DTA, Thermo Plus 8120, Rigaku, Tokyo, Japan) and are shown in <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref>. Although we tried to analyze the composition of the synthesized glass with inductively-coupled plasma atomic emission spectrometry and X-ray Fluorescence, the detection accuracy of these instruments for boron was too low to measure the composition of all samples with high accuracy. However, T<sub>g</sub> of our glasses showed the additivity. Hence, the compositions of all glasses are given as batch compositions in this report (<xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref>).</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The composition and glass transition temperature of xNa<sub>2</sub>O-yY<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >(x, y)</th><th align="center" valign="middle" >Na<sub>2</sub>O (mol%)</th><th align="center" valign="middle" >Y<sub>2</sub>O<sub>3</sub> (mol%)</th><th align="center" valign="middle" >B<sub>2</sub>O<sub>3</sub> (mol%)</th><th align="center" valign="middle" >Al<sub>2</sub>O<sub>3</sub> (mol%)</th><th align="center" valign="middle" >Y<sub>2</sub>O<sub>3</sub>/Al<sub>2</sub>O<sub>3</sub></th><th align="center" valign="middle" >T<sub>g</sub><sup>a</sup> (˚C)</th></tr></thead><tr><td align="center" valign="middle" >(6, 0)</td><td align="center" valign="middle" >42.9</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >35.7</td><td align="center" valign="middle" >21.4</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >392</td></tr><tr><td align="center" valign="middle" >(4.8, 0.4)</td><td align="center" valign="middle" >36.4</td><td align="center" valign="middle" >3.0</td><td align="center" valign="middle" >37.9</td><td align="center" valign="middle" >22.7</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >449</td></tr><tr><td align="center" valign="middle" >(3.96, 0.66)</td><td align="center" valign="middle" >31.4</td><td align="center" valign="middle" >5.2</td><td align="center" valign="middle" >39.6</td><td align="center" valign="middle" >23.8</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >472</td></tr><tr><td align="center" valign="middle" >(3, 1)</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >8.3</td><td align="center" valign="middle" >41.7</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >0.33</td><td align="center" valign="middle" >512</td></tr><tr><td align="center" valign="middle" >(1.98, 1.32)</td><td align="center" valign="middle" >17.5</td><td align="center" valign="middle" >11.7</td><td align="center" valign="middle" >44.2</td><td align="center" valign="middle" >26.5</td><td align="center" valign="middle" >0.44</td><td align="center" valign="middle" >560</td></tr><tr><td align="center" valign="middle" >(1.2, 1.6)</td><td align="center" valign="middle" >11.1</td><td align="center" valign="middle" >14.8</td><td align="center" valign="middle" >46.3</td><td align="center" valign="middle" >27.8</td><td align="center" valign="middle" >0.53</td><td align="center" valign="middle" >630</td></tr><tr><td align="center" valign="middle" >(0, 2)</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >20.0</td><td align="center" valign="middle" >50.0</td><td align="center" valign="middle" >30.0</td><td align="center" valign="middle" >0.67</td><td align="center" valign="middle" >727</td></tr></tbody></table></table-wrap><p><sup>a</sup>uncertainty in T<sub>g</sub> is &#177; 1˚C.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The composition and glass transition temperature of xNa<sub>2</sub>O-yLa<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >(x, y)</th><th align="center" valign="middle" >Na<sub>2</sub>O (mol%)</th><th align="center" valign="middle" >La<sub>2</sub>O<sub>3</sub> (mol%)</th><th align="center" valign="middle" >B<sub>2</sub>O<sub>3</sub> (mol%)</th><th align="center" valign="middle" >Al<sub>2</sub>O<sub>3</sub> (mol%)</th><th align="center" valign="middle" >La<sub>2</sub>O<sub>3</sub>/Al<sub>2</sub>O<sub>3</sub></th><th align="center" valign="middle" >T<sub>g</sub><sup>a</sup> (˚C)</th></tr></thead><tr><td align="center" valign="middle" >(6, 0)</td><td align="center" valign="middle" >42.9</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >35.7</td><td align="center" valign="middle" >21.4</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >392</td></tr><tr><td align="center" valign="middle" >(4.8, 0.4)</td><td align="center" valign="middle" >36.4</td><td align="center" valign="middle" >3.0</td><td align="center" valign="middle" >37.9</td><td align="center" valign="middle" >22.7</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >460</td></tr><tr><td align="center" valign="middle" >(3.96, 0.66)</td><td align="center" valign="middle" >31.4</td><td align="center" valign="middle" >5.2</td><td align="center" valign="middle" >39.6</td><td align="center" valign="middle" >23.8</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >480</td></tr><tr><td align="center" valign="middle" >(3, 1)</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >8.3</td><td align="center" valign="middle" >41.7</td><td align="center" valign="middle" >25.0</td><td align="center" valign="middle" >0.33</td><td align="center" valign="middle" >499</td></tr><tr><td align="center" valign="middle" >(1.98, 1.32)</td><td align="center" valign="middle" >17.5</td><td align="center" valign="middle" >11.7</td><td align="center" valign="middle" >44.2</td><td align="center" valign="middle" >26.5</td><td align="center" valign="middle" >0.44</td><td align="center" valign="middle" >543</td></tr><tr><td align="center" valign="middle" >(1.2, 1.6)</td><td align="center" valign="middle" >11.1</td><td align="center" valign="middle" >14.8</td><td align="center" valign="middle" >46.3</td><td align="center" valign="middle" >27.8</td><td align="center" valign="middle" >0.53</td><td align="center" valign="middle" >584</td></tr><tr><td align="center" valign="middle" >(0, 2)</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >20.0</td><td align="center" valign="middle" >50.0</td><td align="center" valign="middle" >30.0</td><td align="center" valign="middle" >0.67</td><td align="center" valign="middle" >671</td></tr></tbody></table></table-wrap><p><sup>a</sup>uncertainty in T<sub>g</sub> is &#177;1˚C.</p></sec><sec id="s2_1_2"><title>2.1.2. Preparation of Crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub></title><p>Crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub> was synthesized to confirm the relationship between the local structure of Na<sup>+</sup> at different sites in the crystal and the chemical shifts of <sup>23</sup>Na NMR spectra. The crystal sample was prepared using a previously-reported solid state reaction [<xref ref-type="bibr" rid="scirp.77483-ref25">25</xref>] . Briefly, a stoichiometric mixture of NaHCO<sub>3</sub>, B(OH)<sub>3</sub>, and Al<sub>2</sub>O<sub>3</sub> was crushed thoroughly in an agate mortar, calcined at 400˚C for 10 h, and finally heated at 950˚C for 48 h.</p></sec></sec><sec id="s2_2"><title>2.2. Measurements</title><sec id="s2_2_1"><title>2.2.1. Characterization of Crystal Samples</title><p>Synthesized samples were analyzed using X-ray diffraction (XRD, Rigaku, RINT-2100, Tokyo, Japan). In addition, the XRD patterns were also simulated with known crystallographic information [<xref ref-type="bibr" rid="scirp.77483-ref25">25</xref>] using the Mercury software.</p></sec><sec id="s2_2_2"><title>2.2.2. NMR Spectroscopy</title><p>Solid-state <sup>23</sup>Na and <sup>27</sup>Al MAS NMR spectra of all crystal and glass samples were acquired on an AVANCE III spectrometer (Bruker, Billerica, MA) using a commercial probe (4 mm). The rotation speed was set to 15 kHz with an accuracy of &#177; 1 Hz. Under an external field of 18.8 T, the resonance frequencies for <sup>23</sup>Na and <sup>27</sup>Al were near 212 and 208 MHz, respectively. Each measurement was conducted using single-pulse sequence. 90˚ pulses were set to 7 μs for <sup>23</sup>Na. The complete relaxation was confirmed in this condition. In addition, in the case of <sup>27</sup>Al, 0.63 μs pulse which is corresponding to a radiofrequency tip angle 24˚ was applied to ensure quantitative measurement of Al spices. Spectra were obtained with a cycle time of 2 s for both <sup>23</sup>Na and <sup>27</sup>Al. Aqueous solutions of 1 M NaCl and 1 M Al(NO<sub>3</sub>)<sub>3</sub> were used as references, with their chemical shifts set to 0 ppm. The <sup>23</sup>Na spectra were normalized, so that the total area in each spectrum is proportional to the alkali content. This way, the areas of the spectra can be compared with each other.</p></sec><sec id="s2_2_3"><title>2.2.3. Density</title><p>The Archimedes method was used for density measurements of synthesized glasses and to calculate molar volumes.</p></sec></sec></sec><sec id="s3"><title>3. Results</title><sec id="s3_1"><title>3.1. <sup>27</sup>Al MAS NMR</title><p>The <sup>27</sup>Al MAS NMR spectra of yttrium sodium aluminoborate glasses and lanthanum sodium aluminoborate glasses are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref>, respectively. The intensity of the <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]Al</sup> peaks in these spectra were set to be same. The peak of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]Al</sup> gradually shifted upfield in response to the increase of Y<sup>3+</sup>. In order to fit the experimental spectra, gaussian functions were used. We considered that the magnetic field of MAS NMR was strong (18.8 T) enough to neglect quadrupolar shift and broadening effects. The error of the total fitting curve for <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]Al</sup>, <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al was calculated to be 1% - 6% in all glasses.</p><p>As a result of this, each of the errors for <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]Al</sup>, <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al is expected to be</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> <sup>27</sup>Al magic angle spinning nuclear magnetic resonance (MAS NMR) spectra of xNa<sub>2</sub>O-yY<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x2.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> <sup>27</sup>Al MAS NMR spectra of xNa<sub>2</sub>O-yLa<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x3.png"/></fig><p>less than 1% - 6%. Deconvolution of these spectra into the <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]Al</sup> (around 60 ppm), <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al (around 30 ppm), and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al (around 0 ppm) peaks indicated that the fraction of each Al species changed substantially (Figures 3-15). As the proportion of Y<sub>2</sub>O<sub>3</sub> in the glass increased, the fraction of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]Al</sup> decreased from 99 to 48%, that of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al increased from 1 to 36%, and that of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al increased from 0 to 16% (<xref ref-type="fig" rid="fig1">Figure 1</xref>6 and <xref ref-type="table" rid="table3">Table 3</xref>). For lanthanum sodium aluminoborate glass, likewise, the fraction of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]Al</sup> decreased from 99 to 57%, that of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al increased from 1 to 30%, and that of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al increased from 0 to 13% (<xref ref-type="fig" rid="fig1">Figure 1</xref>7 and <xref ref-type="table" rid="table4">Table 4</xref>).</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 6Na<sub>2</sub>O-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x4.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 4.8Na<sub>2</sub>O-0.4Y<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x5.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 3.96Na<sub>2</sub>O-0.66Y<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x6.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 3Na<sub>2</sub>O-Y<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x7.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 1.98Na<sub>2</sub>O-1.32Y<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x8.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 1.2Na<sub>2</sub>O-1.6 Y<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x9.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 2Y<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x10.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 4.8Na<sub>2</sub>O-0.4La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x11.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 3.96Na<sub>2</sub>O-0.66La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x12.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 3Na<sub>2</sub>O-La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x13.png"/></fig><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 1.98Na<sub>2</sub>O-1.32La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x14.png"/></fig><fig id="fig14"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>4</label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 1.2Na<sub>2</sub>O-1.6 La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x15.png"/></fig><fig id="fig15"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>5</label><caption><title> Peak deconvolution of <sup>27</sup>Al MAS NMR spectrum of 2La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x16.png"/></fig><fig id="fig16"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>6</label><caption><title> <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al, <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup>, and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al as fractions of total Al in xNa<sub>2</sub>O-yY<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x17.png"/></fig><fig id="fig17"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>7</label><caption><title> <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al, <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup>, and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al as fractions of total Al in xNa<sub>2</sub>O-yLa<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x18.png"/></fig><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Al speciation of xNa<sub>2</sub>O-yY<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >(x, y)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al (%)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al (%)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al (%)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al + <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]Al</sup> (%)</th></tr></thead><tr><td align="center" valign="middle" >(6, 0)</td><td align="center" valign="middle" >99</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >~0</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >(4.8, 0.4)</td><td align="center" valign="middle" >89</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >~0</td><td align="center" valign="middle" >11</td></tr><tr><td align="center" valign="middle" >(3.96, 0.66)</td><td align="center" valign="middle" >82</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >(3, 1)</td><td align="center" valign="middle" >72</td><td align="center" valign="middle" >22</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >28</td></tr><tr><td align="center" valign="middle" >(1.98, 1.32)</td><td align="center" valign="middle" >67</td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >33</td></tr><tr><td align="center" valign="middle" >(1.2, 1.6)</td><td align="center" valign="middle" >57</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >43</td></tr><tr><td align="center" valign="middle" >(0, 2)</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >36</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >52</td></tr></tbody></table></table-wrap><p><sup>a</sup>uncertainty in the sum of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al + <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al + <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al is 1% - 5%.</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Al speciation of xNa<sub>2</sub>O-yLa<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >(x, y)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al (%)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al (%)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al (%)</th><th align="center" valign="middle" ><sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al + <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]Al</sup> (%)</th></tr></thead><tr><td align="center" valign="middle" >(6, 0)</td><td align="center" valign="middle" >99</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >~0</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >(4.8, 0.4)</td><td align="center" valign="middle" >88</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >~0</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >(3.96, 0.66)</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >(3, 1)</td><td align="center" valign="middle" >79</td><td align="center" valign="middle" >17</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >21</td></tr><tr><td align="center" valign="middle" >(1.98, 1.32)</td><td align="center" valign="middle" >74</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >26</td></tr><tr><td align="center" valign="middle" >(1.2, 1.6)</td><td align="center" valign="middle" >68</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >32</td></tr><tr><td align="center" valign="middle" >(0, 2)</td><td align="center" valign="middle" >57</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >43</td></tr></tbody></table></table-wrap><p><sup>a</sup>uncertainty in the sum of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al + <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al + <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al is 1% - 6%.</p></sec><sec id="s3_2"><title>3.2. XRD Pattern and <sup>23</sup>Na MAS NMR Spectrum of Crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub></title><p>The XRD pattern of synthesized crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub> and its pattern simulated by Mercury [<xref ref-type="bibr" rid="scirp.77483-ref25">25</xref>] are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>8, while the <sup>23</sup>Na NMR spectrum of crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub> is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>9. Considering the 1:1 ratio of two sodium ion sites in crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub>, the peak area ratio should be 1. Nonetheless, there is a different crystal peak present in the lower field. However, according to a previous detailed study [<xref ref-type="bibr" rid="scirp.77483-ref26">26</xref>] , the peak at the lower chemical shift can also be assigned to the Na<sup>+</sup> (2) site that is 9-coordinated with oxygen in the vicinity of Al, and the peak at the higher chemical shift can be assigned to the Na<sup>+</sup> (1) site that is 6-coordinated with oxygen in the vicinity of B (<xref ref-type="fig" rid="fig1">Figure 1</xref>9).</p></sec><sec id="s3_3"><title>3.3. <sup>23</sup>Na MAS NMR</title><p>The <sup>23</sup>Na MAS NMR spectra of yttrium sodium aluminoborate glasses and lanthanum sodium aluminoborate glasses are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>0 and <xref ref-type="fig" rid="fig2">Figure 2</xref>1, respectively. The peak of the <sup>23</sup>Na spectra of Y<sup>3+</sup>-containing glasses gradually shifted upfield in response to an increase of Y<sup>3+</sup>. The peak shifted from −2.3 ppm at (x, y) = (6, 0) to −9.5 ppm at (x, y) = (1.2, 1.6). In the case of La<sup>3+</sup>-containing glasses, a similar upfield spectral shift was observed. The peak shifted from ppm -2.3 ppm at (x, y) = (6, 0) to −10.0 ppm at (x, y) = (1.2, 1.6). Although there was</p><fig id="fig18"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>8</label><caption><title> X-ray diffraction (XRD) pattern of crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub>. The XRD pattern of standard crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub> obtained from simulation using Mercury software is also provided as reference</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x19.png"/></fig><fig id="fig19"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>9</label><caption><title> <sup>23</sup>Na MAS NMR spectra of crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x20.png"/></fig><fig id="fig20"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>0</label><caption><title> <sup>23</sup>Na MAS NMR spectra of xNa<sub>2</sub>O-yY<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x21.png"/></fig><fig id="fig21"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>1</label><caption><title> <sup>23</sup>Na MAS NMR spectra of xNa<sub>2</sub>O-yLa<sub>2</sub>O<sub>3-</sub>5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x22.png"/></fig><p>a deviation when the composition was (x, y) = (3.1) (chemical shift at −11 ppm), the lower-magnetic field component clearly decreased in response to an increase in La<sup>3+</sup>.</p></sec><sec id="s3_4"><title>3.4. Molar Volume</title><p>The molar volumes of yttrium sodium aluminoborate and lanthanum sodium aluminoborate glasses are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>2. As the RE<sup>3+</sup> to Al<sub>2</sub>O<sub>3</sub> ratio increased, the molar volume of the glasses steadily decreased.</p></sec></sec><sec id="s4"><title>4. Discussion</title><p>The <sup>27</sup>Al MAS NMR spectra clearly indicated that the fractions of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al increased in response to an increase in the ratio of Y<sub>2</sub>O<sub>3</sub> to Al<sub>2</sub>O<sub>3</sub> (<xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>6). This result strongly suggests that Y<sup>3+</sup> can produce higher-coordi- nated Al species despite the presence of Na<sup>+</sup>. It was thus considered that the CFS of Y<sup>3+</sup> is sufficiently larger than that of Na<sup>+</sup> to result in formation of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al.</p><p>The relative amounts of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al in Y<sup>3+</sup>-containing glasses were larger than those in La<sup>3+</sup>-containing glasses when the ratio of La<sub>2</sub>O<sub>3</sub> to Al<sub>2</sub>O<sub>3</sub> increased (<xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>7). It therefore seems that the difference in CFS between Y<sup>3+</sup> and La<sup>3+</sup> affected the formation of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al. In previous studies [<xref ref-type="bibr" rid="scirp.77483-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref13">13</xref>] , a greater CFS value resulted in a greater fraction of higher-coordinated Al in oxide glasses that contain RE<sup>3+</sup> such as yttrium aluminosilicate or aluminoborate. As such, the above results further clarify that rare-earth ions with a large CFS can result in <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al even with co-existing Na<sup>+</sup>. It was considered that most of RE<sup>3+</sup> produced higher coordinated Al regardless of its composition because the combination of large CFS cation and higher coordinated Al could be energetically preferable [<xref ref-type="bibr" rid="scirp.77483-ref13">13</xref>] .</p><p>Boron coordination is also important for elucidation of the local structure in this glass. Although we have measured <sup>11</sup>B MAS NMR spectra, it was difficult to complete peak deconvolution because the broad background components derived</p><fig id="fig22"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>2</label><caption><title> Molar volume of xNa<sub>2</sub>O-yY<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> (■) and xNa<sub>2</sub>O-yLa<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glasses (●)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1030165x23.png"/></fig><p>from instruments overlapped the corresponding spectrum of glass. Thus, we estimate the fraction of four-coordinated boron (<sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup>) in this glass system from the literatures. According to the earlier reports [<xref ref-type="bibr" rid="scirp.77483-ref24">24</xref>] , 2Y<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> glass similar composition to our glass contains 12% of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup>. In the case of 2.5La<sub>2</sub>O<sub>3</sub>-5B<sub>2</sub>O<sub>3</sub>- 2.5Al<sub>2</sub>O<sub>3</sub>, the amount of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup> is about 11% [<xref ref-type="bibr" rid="scirp.77483-ref15">15</xref>] . 4Na<sub>2</sub>O-3B<sub>2</sub>O<sub>3</sub>-3Al<sub>2</sub>O<sub>3</sub> and 5Na<sub>2</sub>O- 3.5B<sub>2</sub>O<sub>3</sub>-1.5Al<sub>2</sub>O<sub>3</sub> glass were reported to contain 8.3% and 14.6% of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup>, respectively [<xref ref-type="bibr" rid="scirp.77483-ref27">27</xref>] . In addition, according to Chakraborty and Day [<xref ref-type="bibr" rid="scirp.77483-ref28">28</xref>] , it was suggested that Al/B ratio is important for the nature of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref3">3</xref>]B</sup>/<sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>B ratio because <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>B decreases with being replaced by larger <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]</sup>Al sites. In this glass system, Al/B ratio is fixed at 0.6. Therefore, considering the above data and suggestion, it is assumed that amount of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup> did not greatly changed in respect to the composition in all glass system. The amount of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup> in the synthesized glass can be estimated as about 10% &#177; 5%.</p><p>The lower-field component of the <sup>23</sup>Na spectra of yttrium sodium aluminoborate glasses steadily decreased with respect to the increase in Y<sup>3+</sup> (<xref ref-type="fig" rid="fig2">Figure 2</xref>0). According to the <sup>23</sup>Na spectra of crystalline Na<sub>2</sub>Al<sub>2</sub>B<sub>2</sub>O<sub>7</sub> (<xref ref-type="fig" rid="fig1">Figure 1</xref>9), the peak attributed to 9-coordinated Na<sup>+</sup> (2) near Al is located upfield from that attributed to 6-coordinated Na<sup>+</sup> (1) near B. Usually, the peaks for higher-coordinated ions in simple glasses, such as silicate, borate, and phosphate glasses, are located in the upper-field of the NMR spectra [<xref ref-type="bibr" rid="scirp.77483-ref29">29</xref>] . Therefore, it is also reasonable to observe the peak for higher coordinated Na<sup>+</sup> in the upfield. However, for complex crystals or glasses that contain more than two network-forming oxides, it should be considered that the electron density of coordinated oxygen varies with respect to the neighboring element, such as Al<sup>3+</sup> or B<sup>3+</sup>. In this case, the chemical shift depends on the coordination number and the surrounding ions, such as Al<sup>3+</sup> and B<sup>3+</sup>. Considering these assumptions and the previous studies [<xref ref-type="bibr" rid="scirp.77483-ref15">15</xref>] , the different chemical shifts for the Na<sup>+</sup> (1) and Na<sup>+</sup> (2) peaks were assumed to be affected by the coordination number and conjunctive Al<sup>3+</sup> and B<sup>3+</sup>. This implies that a larger chemical shift in the Na<sup>+</sup> spectrum corresponds to an increase in the coordination number or more Al surrounding Na<sup>+</sup>. In light of these considerations, the coordination number of Na<sup>+</sup> in each glass may have gradually increased following the increase in the number of Y<sup>3+</sup>, and the elements surrounding Na<sup>+</sup> might have affected the change from B to Al. As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the addition of Y<sup>3+</sup> ions produced higher coordinated Al species, and these Al species locally concentrated the oxygen ions. This concentrated oxygen result in an increase in the coordination number of Na<sup>+</sup>. In addition, the <sup>23</sup>Na spectra of the La<sup>3+</sup> glasses also shifted upfield as the La<sup>3+</sup> content increased. This suggests that the above environmental change of Na<sup>+</sup> also occurred in the La<sup>3+</sup>-containing glass. The difference of boron coordination is also considered to affect the oxygen concentration in the local structure and consequently the chemical shift of <sup>23</sup>Na NMR spectra of the glasses. However, as we discussed above, it was assumed that the amount of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup> ratio was almost constant around 10%. Therefore, it is expected that the chemical shift of <sup>23</sup>Na NMR spectra was not affected by the boron coordination.</p><p>The relationship between the Al coordination state and physical properties in these glasses could be deduced because the fractions of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al changed in response to the composition change, as shown above. In order to confirm this relationship, molar volume measurements were conducted, because the local structural change of Al coordination should directly affect spatial arrangement. The molar volumes steadily decreased in response to an increase in Y<sup>3+</sup> content (<xref ref-type="fig" rid="fig2">Figure 2</xref>2), which is caused by various effects. Firstly, rare-earth ions compensate negative charges of Al or B at a closer radius than Na<sup>+</sup>, because they possess a much larger CFS than Na<sup>+</sup>. Secondly, the production of higher-coordinated Al contributed to a decrease in molar volume because at higher coordination states of Al, atomic packing improves. This expectation can be clarified by comparing the molar volumes and fractions of various Al species in both Y<sup>3+</sup>- and La<sup>3+</sup>- containing glasses. When the compositions were (x, y) = (6, 0), (4.8, 0.4), and (3.96, 0.66), the summation of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al and molar volume in Y<sup>3+</sup>-containing glasses were not very different from those in La<sup>3+</sup>-containing glasses (<xref ref-type="fig" rid="fig2">Figure 2</xref>2, <xref ref-type="table" rid="table3">Table 3</xref>, and <xref ref-type="table" rid="table4">Table 4</xref>). However, when more rare-earth ions were present, as in the compositions (x, y) = (3, 1), (1.98, 1.32), (1.2, 1.6), and (0, 2), the summation of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]</sup>Al and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al in Y<sup>3+</sup>-containing glasses became larger than that of La<sup>3+</sup>-con- taining glass, while the molar volume of Y<sup>3+</sup>-containing glasses became smaller. This comparison further proves that <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al lowered the molar volume of the glasses. According to Shannon [<xref ref-type="bibr" rid="scirp.77483-ref30">30</xref>] , the ionic radius of Y<sup>3+</sup> is 1.04 &#197; and that of La<sup>3+</sup> 1.17 &#197; in 6-coordinated state. This difference may also affect the molar volume. However, there have been several reports concerning the relation between the molar volume and Al coordination [<xref ref-type="bibr" rid="scirp.77483-ref31">31</xref>] [<xref ref-type="bibr" rid="scirp.77483-ref32">32</xref>] . Therefore, Al coordination in this glass system must be one of the key-factor that affects the molar volume. In addition, it is expected that boron coordination number affect the molar volume. However, it was considered that boron coordination in our glass gave little influence on the molar volume, because the amount of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref4">4</xref>]B</sup> in the samples were estimated to be almost constant as described.</p><p>Despite the above results, it remains challenging to elucidate the effects of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al in oxide glass on certain physical properties, because other factors may also affect the latter. Therefore, we plan to investigate the effects of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al on physical and optical properties, including fictive temperature, the elastic modulus, refractive index, and photoluminescence, of the abovementioned glass system.</p></sec><sec id="s5"><title>5. Conclusions</title><p>We here performed the structural analysis of yttrium sodium aluminoborate and lanthanum sodium aluminoborate glasses using magic angle spinning NMR. We elucidated that the addition of rare-earth ions (RE<sup>3+</sup>) could result in higher- coordinated Al species (<sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al), and that their amounts were proportional to the ratio of Y<sub>2</sub>O<sub>3</sub> to Al<sub>2</sub>O<sub>3</sub>. Furthermore, the difference in cation field strength (CFS) between Y<sup>3+</sup> and La<sup>3+</sup> was confirmed to affect the generation of higher- coordinated Al. The CFS of rare-earth ions (Y<sup>3+</sup> and La<sup>3+</sup>) was sufficiently larger than that of Na<sup>+</sup> to make higher-coordinated Al without being affected by Na<sup>+</sup>. It was also found that the coordination number of Na<sup>+</sup> in each glass gradually increased following the increase in the number of RE<sup>3+</sup> ions. Further analysis such as <sup>11</sup>B MAS NMR or Soft X-ray spectroscopy for Na<sup>+</sup> can elucidate more detail about network structure or coordination environment, respectively.</p><p>In addition to the above results, it seems that the formation of <sup>[<xref ref-type="bibr" rid="scirp.77483-ref5">5</xref>]Al</sup> and <sup>[<xref ref-type="bibr" rid="scirp.77483-ref6">6</xref>]</sup>Al affected the physical properties (molar volume) due to better atomic packing with these higher-coordinated Al species. In order to clarify the relation between Al coordination number and physical properties in this glass system, further studies about fictive temperature or elastic module will be performed.</p><p>Although the unique affinity between RE<sup>3+</sup> and Al in simple glasses has previously been reported, in this study, it was found that the same particular properties of RE<sup>3+</sup> exist even in complex glasses. These results are expected to steadily lead to the development of ideal optical or building glass materials.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This study was carried out with the NMR spectrometer in the JURC at Institute for Chemical Research, Kyoto University. This work was supported by JSPS KAKENHI (grant number JP16K07640), Nippon Sheet Glass Foundation for Materials Science and Engineering, and Research Institute for Sustainable Humanosphere, Kyoto University.</p></sec><sec id="s7"><title>Cite this paper</title><p>Kaneko, S., Tokuda, Y. and Masai, H. (2017) Additive Effects of Rare-Earth Ions in Sodium Aluminoborate Glasses Using <sup>23</sup>Na and <sup>27</sup>Al Magic Angle Spinning Nuclear Magnetic Resonance. New Journal of Glass and Ceramics, 7, 58-76. https://doi.org/10.4236/njgc.2017.73006</p></sec></body><back><ref-list><title>References</title><ref id="scirp.77483-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Sinton, C.W. and LaCourse, W.C. (2001) Experimental Survey of the Chemical Durability of Commercial Soda-Lime-Silicate Glasses. Materials Research Bulletin, 36, 2471-2479. https://doi.org/10.1016/S0025-5408(01)00724-3</mixed-citation></ref><ref id="scirp.77483-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">El-Kheshen, A.A., Khaliafa, F.A., Saad, E.A. and Elwan, R.L. (2008) Effect of Al2O3 Addition on Bioactivity, Thermal and Mechanical Properties of Some Bioactive Glasses. Ceramics International, 34, 1667-1673.  
https://doi.org/10.1016/j.ceramint.2007.05.016</mixed-citation></ref><ref id="scirp.77483-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Stebbins, J.F., Kroeker, S., Lee, S.K. and Kiczenski, T.J. (2000) Quantification of Five- and Six-Coordinated Aluminum in Aluminosilicate and Fluoride-Containing Glasses by High Field, High Resolution 27Al-NMR. Journal of Non-Crystalline Solids, 275, 1-6. https://doi.org/10.1016/s0022-3093(00)00270-2</mixed-citation></ref><ref id="scirp.77483-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">MacKenzie, K.J.D. and Smith, M.E. (2002) Multinuclear Solid State Nuclear Magnetic Resonance of Materials. Pergamon Press, Oxford.</mixed-citation></ref><ref id="scirp.77483-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Stevensson, B. and Edén, M. (2013) Structural Rationalization of the Microhardness Trends of Rare-Earth Aluminosilicate Glasses: Interplay between the RE3+ Field-Strength and the Aluminum Coordinations. J. Non-Cryst. Solids, 378, 163-167.  
https://doi.org/10.1016/j.jnoncrysol.2013.06.013</mixed-citation></ref><ref id="scirp.77483-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Iftekhar, S., Pahari, B., Okhotnikov, K., Jaworski, A., Stevensson, B., Grins, J. and Eden, M. (2012) Properties and Structures of RE2O3-Al2O3-SiO2 (RE=Y, Lu) Glasses Probed by Molecular Dynamics Simulations and Solid-State NMR: The Roles of Aluminum and Rare-Earth Ions for Dictating the Microhardness. The Journal of Physical Chemistry C, 116, 18394-18406.  
https://doi.org/10.1021/jp302672b</mixed-citation></ref><ref id="scirp.77483-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Rosales-Sosa, G.A., Masuno, A., Higo, Y., Inoue, H., Yanaba, Y., Mizoguchi, T., Umada, T., Okamura, K., Kato, K. and Watanabe, Y. (2015) High Elastic Moduli of a 54Al2O3-46Ta2O5 Glass Fabricated via Containerless Processing. Scientific Reports, 5, Article ID: 15233. https://doi.org/10.1038/srep15233</mixed-citation></ref><ref id="scirp.77483-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Rosales-Sosa, G.A., Masuno, A., Higo, Y. and Inoue, H. (2016) Crack-Resistant Al2O3-SiO2 Glasses. Scientific Reports, 6, Article ID: 23620.  
https://doi.org/10.1038/srep23620</mixed-citation></ref><ref id="scirp.77483-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Kelsey, K.E., Stebbins, J.F., Singer, D.M., Brown Jr., G.E., Mosenfelder, J.L. and Asimow, P.D. (2009) Cation Field Strength Effects on High Pressure Aluminosilicate Glass Structure: Multinuclear NMR and La XAFS Results. Geochim. Geochimica et Cosmochimica Acta, 73, 3914-3933.  
https://doi.org/10.1016/j.gca.2009.03.040</mixed-citation></ref><ref id="scirp.77483-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Morin, E.I., Wu, J. and Stebbins, J.F. (2014) Modifier Cation (Ba, Ca, La, Y) Field Strength Effects on Aluminum and Boron Coordination in Aluminoborosilicate Glasses: The Roles of Fictive Temperature and Boron Content. Applied Physics A, 116, 479-490. https://doi.org/10.1007/s00339-014-8369-4</mixed-citation></ref><ref id="scirp.77483-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Wu, J. and Stebbins, J.F. (2013) Temperature and Modifier Cation Field Strength Effects on Aluminoborosilicate Glass Network Structure. Journal of Non-Crystalline Solids, 362, 73-81. https://doi.org/10.1016/j.jnoncrysol.2012.11.005</mixed-citation></ref><ref id="scirp.77483-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Iftekhar, S., Grins, J., Gunawidjaja, P.N. and Edén, M. (2011) Glass Formation and Structure-Property-Composition Relations of the RE2O3-Al2O3-SiO2 (RE = La, Y, Lu, Sc) Systems. Journal of the American Ceramic Society, 94, 2429-2435.  
https://doi.org/10.1111/j.1551-2916.2011.04548.x</mixed-citation></ref><ref id="scirp.77483-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Jaworski, A., Stevensson, B. and Edén, M. (2015) Direct 17O NMR Experimental Evidence for Al–NBO Bonds in Si-Rich and Highly Polymerized Aluminosilicate Glasses. Physical Chemistry Chemical Physics, 17, 18269-18272. 
https://doi.org/10.1039/C5CP02985F</mixed-citation></ref><ref id="scirp.77483-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Chakraborty, I.N., Rutz, H.L. and Day, D.E. (1986) Glass Formation, Properties and Structure of Y2O3-Al2O3-B2O3 Glasses. Journal of Non-Crystalline Solids, 84, 86-92. 
https://doi.org/10.1016/0022-3093(86)90764-7</mixed-citation></ref><ref id="scirp.77483-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Brow, R.K., Tallant, D.R. and Turner, G.L. (1997) Polyhedral Arrangements in Lanthanum Aluminoborate Glasses. Journal of the American Ceramic Society, 80, 1239-1244. https://doi.org/10.1111/j.1151-2916.1997.tb02970.x</mixed-citation></ref><ref id="scirp.77483-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Rutz, H.L., Day, D.E. and Spencer, J.C.F. (1990) Properties of Yttria-Aluminoborate Glasses. Journal of the American Ceramic Society, 73, 1788-1790.  
https://doi.org/10.1111/j.1151-2916.1990.tb09836.x</mixed-citation></ref><ref id="scirp.77483-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Züchner, L., Chan, J.C.C., Müller-Warmuth, W. and Eckert, H. (1998) Short-Range Order and Site Connectivities in Sodium Aluminoborate Glasses: I. Quantification of Local Environments by High-Resolution 11B, 23Na, and 27Al Solid-State NMR. The Journal of Physical Chemistry B, 102, 4495-4506. https://doi.org/10.1021/jp980587s</mixed-citation></ref><ref id="scirp.77483-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Du, L.S. and Stebbins, J.F. (2005) Site Connectivities in Sodium Aluminoborate Glasses: Multinuclear and Multiple Quantum NMR Results. Solid State Nuclear Magnetic Resonance, 27, 37-49. https://doi.org/10.1016/j.ssnmr.2004.08.003</mixed-citation></ref><ref id="scirp.77483-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Van, W.L., Züchner, L., Müller-Warmuth, W. and Eckert, H. (1996) 11B27{Al} and 27Al11{B} Double Resonance Experiments on a Glassy Sodium Aluminoborate. Solid State Nuclear Magnetic Resonance, 6, 203-212.  
https://doi.org/10.1016/0926-2040(96)01228-3</mixed-citation></ref><ref id="scirp.77483-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Chan, J.C.C., Bertmer, M. and Eckert, H. (1999) Site Connectivities in Amorphous Materials Studied by Double-Resonance NMR of Quadrupolar Nuclei:- High- 
Resolution 11B - 27Al Spectroscopy of Aluminoborate Glasses. Journal of the American Chemical Society, 121, 5238-5248. https://doi.org/10.1021/ja983385i</mixed-citation></ref><ref id="scirp.77483-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Bertmer, M., Züchner, L., Chan, J.C.C. and Eckert, H. (2000) Short and Medium Range Order in Sodium Aluminoborate Glasses. 2. Site Connectivities and Cation Distributions Studied by Rotational Echo Double Resonance NMR Spectroscopy. The Journal of Physical Chemistry B, 104, 6541-6553.  
https://doi.org/10.1021/jp9941918</mixed-citation></ref><ref id="scirp.77483-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Morin, E.I. and Stebbins, J.F. (2016) Separating the Effects of Composition and Fictive Temperature on Al and B Coordination in Ca, La, Y Aluminosilicate, Aluminoborosilicate and Aluminoborate Glasses. Journal of Non-Crystalline Solids, 432, 384-392. https://doi.org/10.1016/j.jnoncrysol.2015.10.035</mixed-citation></ref><ref id="scirp.77483-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Deters, H., Camargo, A.S.S., Santos, C.N., Ferrari, C.R., Hernandes, A.C., Ibanez, A., Rinke, M.T. and Eckert, H. (2009) Structural Characterization of Rare-Earth Doped Yttrium Aluminoborate Laser Glasses Using Solid State NMR. The Journal of Physical Chemistry C, 113, 16216-16225. https://doi.org/10.1021/jp9032904</mixed-citation></ref><ref id="scirp.77483-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Deters, H., Lima, J.F., Magon, C.J., Camargo, A.S.S. and Eckert, H. (2011) Structural Models for Yttrium Aluminium Borate Laser Glasses: NMR and EPR Studies of the System (Y2O3)0.2-(Al2O3)x-(B2O3)0.8-x. Physical Chemistry Chemical Physics, 13, 16071-16083. https://doi.org/10.1039/c1cp21404g</mixed-citation></ref><ref id="scirp.77483-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">He, M., Chen, X.L., Zhou, T., Hu, B.Q., Xu, Y.P. and Xu, T. (2001) Crystal Structure and Infrared Spectra of Na2Al2B2O7. Journal of Alloys and Compounds, 327, 210-214. https://doi.org/10.1016/S0925-8388(01)01561-4</mixed-citation></ref><ref id="scirp.77483-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Perras, F.A. and Bryce, D.L. (2012) Multinuclear Magnetic Resonance Crystallographic Structure Refinement and Cross-Validation Using Experimental and Computed Electric Field Gradients: Application to Na2Al2B2O7. Journal of Physical Chemistry C, 116, 19472-19482. https://doi.org/10.1021/jp308273h</mixed-citation></ref><ref id="scirp.77483-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Gresch, R. and Müller-Warmuth, W. (1976) 11B and 27Al NMR Studies of Glasses in the System Na2O-B2O3-Al2O3 (“NABAL”). Journal of Non-Crystalline Solids, 21, 31-40. https://doi.org/10.1016/0022-3093(76)90088-0</mixed-citation></ref><ref id="scirp.77483-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">Chakraborty, I.N. and Day, D.E. (1985) Effect of R3+ Ions on the Structure and Properties of Lanthanum Borate Glasses. Journal of the American Ceramic Society, 68, 641-645. https://doi.org/10.1111/j.1151-2916.1985.tb10117.x</mixed-citation></ref><ref id="scirp.77483-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Stebbins, J.F. (1998) Cation Sites in Mixed-Alkali Oxide Glasses: Correlations of NMR Chemical Shift Data with Site Size and Bond Distance. Solid State Ionics, 112, 137-141. https://doi.org/10.1016/S0167-2738(98)00224-0</mixed-citation></ref><ref id="scirp.77483-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Shannon, R.D. (1969) Revised Effective Ionic Radii and Systematic Studies of Interatomic Distances in Halides and Chalcogenides. Acta Crystallographica Section A, 32, 751-767. https://doi.org/10.1107/S0567739476001551</mixed-citation></ref><ref id="scirp.77483-ref31"><label>31</label><mixed-citation publication-type="other" xlink:type="simple">Allwardt, J.R., Stebbins, J.F., Schmidt, B.C., Frost, D.J., Withers, A.C. and Hirschmann, M.M. (2005) Aluminum Coordination and the Densification of High-Pressure Aluminosilicate Glasses. American Mineralogist, 90, 1218-1222.  
https://doi.org/10.2138/am.2005.1836</mixed-citation></ref><ref id="scirp.77483-ref32"><label>32</label><mixed-citation publication-type="other" xlink:type="simple">Kelsey, K.E., Stebbins, J.F., Mosenfelder, J.L. and Asimow, P.D. (2009) Simultaneous Aluminum, Silicon, and Sodium Coordination Changes in 6 GPa Sodium Aluminosilicate Glasses. American Mineralogist, 94, 1205-1215.  
https://doi.org/10.2138/am.2009.3177</mixed-citation></ref></ref-list></back></article>