<?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">MSA</journal-id><journal-title-group><journal-title>Materials Sciences and Applications</journal-title></journal-title-group><issn pub-type="epub">2153-117X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msa.2018.96037</article-id><article-id pub-id-type="publisher-id">MSA-84857</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>
 
 
  Novel Cathode Materials for Sodium Ion Batteries Derived from Layer Structured Titanate Cs&lt;sub&gt;2&lt;/sub&gt;Ti&lt;sub&gt;5&lt;/sub&gt;O&lt;sub&gt;11&lt;/sub&gt;&amp;middot;(1 + x)H&lt;sub&gt;2&lt;/sub&gt;O
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Masao</surname><given-names>Ohashi</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Tokuyama College of Technology, Gakuendai, Shunan City, Japan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>oohasi@tokuyama.ac.jp</email></corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>05</month><year>2018</year></pub-date><volume>09</volume><issue>06</issue><fpage>526</fpage><lpage>533</lpage><history><date date-type="received"><day>29,</day>	<month>March</month>	<year>2018</year></date><date date-type="rev-recd"><day>25,</day>	<month>May</month>	<year>2018</year>	</date><date date-type="accepted"><day>28,</day>	<month>May</month>	<year>2018</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>
 
 
  A layer structured titanate Cs
  <sub>2</sub>Ti
  <sub>5</sub>O
  <sub>11</sub>&#183;(1 + x)H
  <sub>2</sub>O (x = 0.70) has been prepared in a solid state reaction using Cs
  <sub>2</sub>CO
  <sub>3</sub> and anatase type TiO
  <sub>2</sub> at 900
  &amp;deg;C. Ion exchange reactions of Cs
  <sup>+</sup> in the interlayer space were studied in aqueous solu
  tions. The single phases of Li<sup>+</sup>, Na<sup>+</sup> and H<sup>+</sup> exchange products were obtained. The three kinds of resulting titanates were evaluated for use as the cathodes in rechargeable sodium batteries after dehydrations by heating at 200&amp;deg;C in a vacuum. The electrochemical measurements showed that they exhibited the reversible Na<sup>+</sup> intercalation-deintercalation in a voltage range of 0.5 - 3.5 V or 0.7 - 4.0 V. The Li<sup>+</sup> exchange product showed the best performance of the discharge-charge capacities in this study. The initial Na<sup>+</sup> intercalation-deintercalation capacities of the Li<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> were 120 mAh/g and 100 mAh/g; the amounts of Na<sup>+</sup> correspond to 1.9 and 1.6 of the formula unit, respectively. The titanates are nontoxic, inexpensive and environmentally benign.
 
</p></abstract><kwd-group><kwd>Cathode Material</kwd><kwd> Sodium Ion Battery</kwd><kwd> Layer Structured Titanate</kwd><kwd> Environmentally Benign</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Sodium ion batteries have emerged for the ideal alternative to the lithium ion batteries which have the problems of lithium availability and cost. We have studied the characterizations of layer structured titanates and Niobate [<xref ref-type="bibr" rid="scirp.84857-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.84857-ref8">8</xref>] for the cathodes of lithium ion batteries. In a previous study [<xref ref-type="bibr" rid="scirp.84857-ref8">8</xref>] , we showed that Cs<sub>0.67</sub>Li<sub>3.01</sub>H<sub>0.73</sub>Nb<sub>6</sub>O<sub>17</sub> derived by ion exchange reaction from layer structured Niobate Cs<sub>4</sub>Nb<sub>6</sub>O<sub>17</sub> exhibited rechargeable capacity of more than 110 mAh/g in the lithium battery in the voltage range of 1.5 - 4.2 V. The discharge-charge capacity corresponds to a redox reaction of Nb<sup>5+</sup>/Nb<sup>4+</sup> in the layered niobate with the intercalation-deintercalation of Li<sup>+</sup>. In the present study, we found that novel cathode materials for sodiumion batteries derived by ion exchange reactions from a layered titanate of Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O.</p><p>The crystal structure of Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> [<xref ref-type="bibr" rid="scirp.84857-ref9">9</xref>] . Each stacking layer consists of corrugated layer of titanium-oxygen. Ordinary TiO<sub>6</sub> octahedra are continuous in two dimensions. The framework is built up by five TiO<sub>6</sub> octahedra sharing edges. These unites are joined to the same block sharing edges to form zig-zag layers and sharing corners staggered sheets forming [Ti<sub>5</sub>O<sub>11</sub>]<sup>2−</sup> layers. The charge balance is maintained by interlayer Cs<sup>+</sup> ions which are eight-coordinated by oxygen atoms of the adjacent layers. The titanate Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> intends to contain water molecules in the interlayer space with Cs<sup>+</sup> from the air at room temperature forming Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O (0.5 &lt; x &lt; 1).</p></sec><sec id="s2"><title>2. Experimental</title><p>The layer structured titanate Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O has been prepared in a solid state reaction using Cs<sub>2</sub>CO<sub>3</sub>, anatase type TiO<sub>2</sub> at 900˚C according to a similar method reported by Grey et al. [<xref ref-type="bibr" rid="scirp.84857-ref10">10</xref>] . The mixture with the desired ratio was heated for 20 h and the resulting powder was ground and heated again at 900˚C for 20 h. Li<sup>+</sup> and Na<sup>+</sup> exchange were performed using 1.0 mol/L LiNO<sub>3</sub> and NaNO<sub>3</sub> solutions for 9 days at 60˚C The solutions were changed every 3 days. The H<sup>+</sup> exchange was carried out using 0.05 mol/L H<sub>2</sub>SO<sub>4</sub> solution for 3 days at room temperature, changing the solution every day.</p><p>Powder X-ray diffraction (XRD) patterns were collected by a Rigaku Ultima IV diffractometer over 2θ range of 10˚ to 70˚ using graphite monochromatized CuK<sub>α</sub> radiation (λ = 0.15405 nm). The contents of Cs, Li and Na in the samples were determined by the atomic absorption method after dissolving the samples in a mixed acid solution with H<sub>2</sub>SO<sub>4</sub> and HF. Dehydration processes were studied by TG-DTA at a heating rate of 10˚C/min. A cathode was formed of a</p><p>mixture of the titanate powder (80 wt%), acetylene black (10 wt%) and PTFE binder (10 wt%) pressed into a stainless steel grid under a pressure of 100 MPa. The electrolyte of the sodium cell was 1.0 mol/L NaClO<sub>4</sub> solution of propylene carbonate (PC) and an anode was sodium metal. The cells were first discharge and cycled between 0.5 V and 3.5 V or 0.7 V and 4.0 V at 0.10 mA/cm<sup>2</sup> in an argon-filled glove box at room temperature.</p></sec><sec id="s3"><title>3. Result and Discussion</title><sec id="s3_1"><title>3.1. Preparation of Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>∙(1 + x)H<sub>2</sub>O</title><p>The XRD pattern of Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)) was indexed on the basis of a monoclinic cell of a = 2.470(3) nm, b = 0.3785(4) nm, c = 1.573(2) nm and β = 123.7(1)˚ (<xref ref-type="table" rid="table1">Table 1</xref>). The lattice constants of the sample are consistent with those prepared by Reid et al. (a = 2.3849(8) nm, b = 0.3800(1) nm, c = 1.4918(6) nm and β = 121.27(3)˚) [<xref ref-type="bibr" rid="scirp.84857-ref10">10</xref>] . The TGA curve of the compound (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)) shows a weight loss from 20˚C to 200˚C; this corresponds to the dehydration of the interlayer water. The composition was estimated to be Cs<sub>2</sub>T<sub>5</sub>O<sub>11</sub>・1.7H<sub>2</sub>O (x = 0.7 in Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O) from the weight loss.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Compositions and monoclinic lattice constants of the products</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Compositions</th><th align="center" valign="middle" >a/nm</th><th align="center" valign="middle" >b/nm</th><th align="center" valign="middle" >c/nm</th><th align="center" valign="middle" >β/˚</th></tr></thead><tr><td align="center" valign="middle" >Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・1.7H<sub>2</sub>O</td><td align="center" valign="middle" >2.470 (3)</td><td align="center" valign="middle" >0.3785 (4)</td><td align="center" valign="middle" >1.573 (2)</td><td align="center" valign="middle" >123.7 (1)</td></tr><tr><td align="center" valign="middle" >Li<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・3.6H<sub>2</sub>O</td><td align="center" valign="middle" >2.48</td><td align="center" valign="middle" >0.376</td><td align="center" valign="middle" >1.76</td><td align="center" valign="middle" >127</td></tr><tr><td align="center" valign="middle" >Na<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・4.1H<sub>2</sub>O</td><td align="center" valign="middle" >2.58</td><td align="center" valign="middle" >0.375</td><td align="center" valign="middle" >1.77</td><td align="center" valign="middle" >125</td></tr><tr><td align="center" valign="middle" >H<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・3.3H<sub>2</sub>O</td><td align="center" valign="middle" >2.53</td><td align="center" valign="middle" >0.375</td><td align="center" valign="middle" >1.76</td><td align="center" valign="middle" >125</td></tr></tbody></table></table-wrap></sec><sec id="s3_2"><title>3.2. Ion Exchange</title><p>The XRD pattern of the Li<sup>+</sup> exchange product is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b). The pattern was indexed as a single phase with monoclinic lattice constants of a = 2.48 nm, b = 0.376 nm c = 1.76 nm and β = 127˚ (<xref ref-type="table" rid="table1">Table 1</xref>). These lattice constants of a and b were almost unchanged. This show that the host layer of Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O is maintained through the Li<sup>+</sup> exchange. The TGA curve (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)) shows two steps of weight loss: 25˚C - 170˚C and 170˚C - 450˚C. The both steps correspond to the dehydration of the interlayer water. Cs analysis indicated that more than 99.9% of the interlayer Cs<sup>+</sup> was ion exchanged with Li<sup>+</sup>. The composition was estimated to be Li<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・3.6H<sub>2</sub>O at room temperature and Li<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・1.0H<sub>2</sub>O at 170˚C.</p><p>The XRD pattern of the Na<sup>+</sup> exchange product is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(c). The pattern was indexed as a single phase with monoclinic lattice constants of a = 0.258 nm, b = 0.375 nm c = 1.77 nm and β = 125˚ (<xref ref-type="table" rid="table1">Table 1</xref>). This show that the host layer of Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O is also maintained through the Na<sup>+</sup> exchange. The TGA curve of the product (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)) shows a gradual weight loss from 20˚C to 600˚C; this corresponds to the dehydration of the interlayer water. Cs analysis indicated that more than 99.8% of the interlayer Cs<sup>+</sup> was ion exchanged with Na<sup>+</sup>. The composition was estimated to be Na<sub>2</sub>T<sub>5</sub>O<sub>11</sub>・4.1H<sub>2</sub>O by chemical analysis and the weight loss.</p><p>The XRD pattern of the H<sup>+</sup> exchange product is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(d). The pattern was indexed as a single phase with monoclinic lattice constants of a = 0.253 nm, b = 0.375 nm c = 1.76 nm and β = 125˚ (<xref ref-type="table" rid="table1">Table 1</xref>). This also shows that the host layer of Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O is maintained through the H<sup>+</sup> exchange. The TGA curve (<xref ref-type="fig" rid="fig3">Figure 3</xref>(d)) shows two steps of weight loss: 30˚C - 80˚C and 150˚C - 500˚C. The former weight loss corresponds to the dehydration of the interlayer water and the latter corresponds to the mixture of dehydration of the interlayer water and decomposition caused by the combination of the exchanged H<sup>+</sup> with O<sup>2−</sup> of the host layer. Cs analysis indicated that more than 99.6% of the interlayer Cs<sup>+</sup> was ion exchanged with H<sup>+</sup>. The compositions were estimated to be H<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・3.3H<sub>2</sub>O at room temperature and H<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・1.0H<sub>2</sub>O at 80˚C. Sasaki et al. [<xref ref-type="bibr" rid="scirp.84857-ref11">11</xref>] reported the formations of H<sup>+</sup> exchange product of H<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・3H<sub>2</sub>O (air-dried) and H<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・1.0H<sub>2</sub>O (heated at 100˚C) using 1 M HCl solution. The compositions of the H<sup>+</sup> exchange products obtained in this study are consistent with those reported by them.</p></sec><sec id="s3_3"><title>3.3. Sodium Battery</title><p>The Li<sup>+</sup>, Na<sup>+</sup> and H<sup>+</sup> exchange products were evaluated for use as the cathodes in rechargeable sodium batteries after dehydrations by heating at 200˚C for 1 hour in a vacuum.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows the discharge-charge curves of Na/Li<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> cell. The cell voltage decreased from 2.7 V to 1.2 V and then decreased slowly to the cutoff voltage of 0.7 V. The discharge capacity was 120 mAh/g for the first cycle. The amount of Na<sup>+</sup> intercalated in this process was 1.9 for the formula unit. The discharge potential of Ti<sup>4+</sup>/Ti<sup>3+</sup> in a titanate of Na<sub>2</sub>Ti<sub>6</sub>O<sub>13</sub> is reported to be approximately 0.8 V with the insertion of Na<sup>+</sup> into the three dimensional tunnel-type structure [<xref ref-type="bibr" rid="scirp.84857-ref12">12</xref>] . The Na/Li<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> cell showed a little higher voltage of 1.2 V than 0.8 V on the discharge process which corresponds to the intercalation of Na<sup>+</sup> and the reduction of Ti<sup>4+</sup> to Ti<sup>3+</sup> in the layer structured titanate. The first charge and discharge capacities were 120 mAh/g and 100 mAh/g; the amounts of Na<sup>+</sup> intercalated and deintercalated were 1.9 and 1.6 of the formula unit, respectively. At 10th cycle, the cell exhibited 60% (72 mAh/g) of the first discharge capacity and 70% (70 mAh/g) of the first charge capacity.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the discharge-charge curves of Na/Na<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> cell. The cell voltage decreased from 2.7 V to 1.4 V and decreased to 1.2 V. Then it decreased slowly to the cutoff voltage of 0.5 V. The discharge capacity was 120 mAh/g for the first cycle. The amount of Na<sup>+</sup> intercalated in this process was 2.1 for the formula unit. The first charge and discharge capacities were 120 mAh/g and 60 mAh/g; the amounts of Na<sup>+</sup> intercalated and deintercalated were 2.1 and 1.0 of the formula unit, respectively. At 10th cycle, the cell exhibited 40% (48 mAh/g) of the first discharge capacity and 73% (44 mAh/g) of the first charge capacity.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows the discharge-charge curves of Na/H<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> cell. The cell voltage decreased from 2.7 V to 0.7 V and then slowly decreased to the first cutoff voltage of 0.55 V. The discharge capacity was 120 mAh/g for the first cycle. The amount of Na<sup>+</sup> intercalated in this process was 1.8 for the formula unit. The first charge and discharge capacities were 120 mAh/g and 45 mAh/g; the amounts of Na<sup>+</sup> intercalated and deintercalated were 1.8 and 0.7 of the formula unit, respectively. At 10th cycle, the cell exhibited 28% (33 mAh/g) of the first discharge capacity and 65% (29 mAh/g) of the first charge capacity.</p><p>The Li<sup>+</sup> exchange product showed the best performance in the discharge-charge capacities. The higher performance of Li<sup>+</sup> exchange titanate than Na<sup>+</sup> exchange titanate may be attributed to the difference of ionic radius of Li<sup>+</sup> and Na<sup>+</sup>. The smaller ion volume of Li<sup>+</sup> than Na<sup>+</sup> can provide a lager vacant space for the intercalation of Na<sup>+</sup>. It is expected that H<sup>+</sup> exchange titanate has the largest vacant space for the intercalation of Na<sup>+</sup> among the ion exchange titanates obtained in this study. However, the H<sup>+</sup> exchange titanate showed the worst performance of the discharge-charge capacities. It is necessary to investigate the structural changes during the discharge-charge processes for further understanding of these cathode materials.</p><p>The studies of these titanates for lithium ion batteries are now under way and will be presented elsewhere.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>In this study, we showed for the first time that the layer structure titanates derived from Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>・(1 + x)H<sub>2</sub>O by ion exchange can be promising candidates for the cathode materials of sodium ion batteries. The initial Na<sup>+</sup> intercalation-deintercalation capacities of the Li<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub> were 120 mAh/g and 100 mAh/g;</p><p>the amounts of Na<sup>+</sup> intercalated and deintercalated were 1.9 and 1.6 of the formula unit, respectively. The titanates are nontoxic, inexpensive and environmentally benign.</p></sec><sec id="s5"><title>Cite this paper</title><p>Ohashi, M. (2018) Novel Cathode Materials for Sodium Ion Batteries Derived from Layer Structured Titanate Cs<sub>2</sub>Ti<sub>5</sub>O<sub>11</sub>∙(1 + x)H<sub>2</sub>O. Materials Sciences and Applications, 9, 526-533. https://doi.org/10.4236/msa.2018.96037</p></sec></body><back><ref-list><title>References</title><ref id="scirp.84857-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ohashi, M. (1998) Preparation and Lithium Intercalation of Layer Structured Titanate CsxTi2-x/4O4 (x = 0.68). Molecular Crystals and Liquid Crystals, 311, 51. https://doi.org/10.1080/10587259808042365</mixed-citation></ref><ref id="scirp.84857-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Ohashi, M. (2000) Ion Exchange of Layer Structured Titanate CsxTi2-x/4O4 (x = 0.68) and Ionic Conductivity of the Products. Molecular Crystals and Liquid Crystals, 341, 265. https://doi.org/10.1080/10587250008026151</mixed-citation></ref><ref id="scirp.84857-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Ohashi, M. 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