<?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">MSCE</journal-id><journal-title-group><journal-title>Journal of Materials Science and Chemical Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-6045</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msce.2015.39009</article-id><article-id pub-id-type="publisher-id">MSCE-59887</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>
 
 
  Li&lt;SUB&gt;4&lt;/SUB&gt;Ti&lt;SUB&gt;5&lt;/SUB&gt;O&lt;SUB&gt;12&lt;/SUB&gt; Synthesis with High Specific Surface Area and Single Phase
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>oshihito</surname><given-names>Ohtake</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>Ken-ichiro</surname><given-names>Iijima</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mechanical Systems Engineering, Faculty of Engineering, Aich University of Technology,
Gamagori, Japan</addr-line></aff><pub-date pub-type="epub"><day>08</day><month>09</month><year>2015</year></pub-date><volume>03</volume><issue>09</issue><fpage>68</fpage><lpage>73</lpage><history><date date-type="received"><day>2</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>21</month>	<year>September</year>	</date><date date-type="accepted"><day>24</day>	<month>September</month>	<year>2015</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 have investigated a novel 
  Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> synthesis with high specific surface area, high crystallization and single phase and its mechanism. The method was performed with a solid phase synthesis by using CH
  <sub>3</sub>COOLi&#183;
  <sub>2</sub>H
  <sub>2</sub>O and anatase TiO
  <sub>2</sub> via Li
  <sub>2</sub>TiO
  <sub>3</sub> as an intermediate in pre-sintering at 500
  &#176;C and sintering at 750
  &#176;C. This result showed specific surface area of 12 m
  &lt;sup&gt;2&lt;/sup&gt;/g and single phase- 
  Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> by applying the high specific surface anatase TiO
  <sub>2</sub> as a precursor.
 
</p></abstract><kwd-group><kwd>Li&lt;SUB&gt;4&lt;/SUB&gt;Ti&lt;SUB&gt;5&lt;/SUB&gt;O&lt;SUB&gt;12&lt;/SUB&gt;</kwd><kwd> Solid Phase Synthesis</kwd><kwd> Specific Surface Area</kwd><kwd> SEM</kwd><kwd> TEM</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>A negative electrode in lithium ion secondary battery has applied C<sub>6</sub> graphite to intercalate lithium ions. The graphite expands by overcharge to intercalate them more than stoichiometry. To solve the expansion, materials with keeping a crystal structure have been developed [<xref ref-type="bibr" rid="scirp.59887-ref1">1</xref>] . Hence, Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> consisting of a spinel structure has been expected for not changing the structure or size by intercalating the lithium ion [<xref ref-type="bibr" rid="scirp.59887-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.59887-ref3">3</xref>] . Furthermore, it is superior to the graphite in stability of charge capacitance under a high temperature or fast charge-discharge cycle [<xref ref-type="bibr" rid="scirp.59887-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.59887-ref6">6</xref>] . On the other hand, an electrical conductivity is low like an insulator, and effects of a carbon doping or metal ions by adding V<sup>5+</sup>, Mn<sup>4+</sup>, Fe<sup>3+</sup>, Mg<sup>2+</sup> and Ag<sup>+</sup> have been investigated for the higher conductivity [<xref ref-type="bibr" rid="scirp.59887-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.59887-ref14">14</xref>] . Especially the carbon doping has been available, and attempted by a sol-gel or spray-dry method in a liquid phase [<xref ref-type="bibr" rid="scirp.59887-ref15">15</xref>] - [<xref ref-type="bibr" rid="scirp.59887-ref17">17</xref>] .</p><p>Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> synthesis methods have been known as solid phase, sol-gel, hydrothermal or co-precipitation method. The solid phase method has surpassed others in industrialization to be easy and controllable for the synthesis, while it is difficult to obtain homogeneous grain size. The small grain size needs lower sintering temperature, but the higher crystallization requires the higher sintering temperature. Furthermore, the solid phase method has been studied for the improvement in these points [<xref ref-type="bibr" rid="scirp.59887-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.59887-ref19">19</xref>] .</p><p>Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> for the negative electrode requires high crystallization, single phase, small grain size and high specific surface area to perform an excellent property. Especially, the high specific surface area is important to intercalate many lithium ions into the crystal efficiently. We have investigated the synthesis method for the high specific surface area with Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> of the completely single phase by the solid phase reaction. In this study, we attempted the synthesis by applying anatase TiO<sub>2</sub> of the different specific surface area via a pre-sintering.</p></sec><sec id="s2"><title>2. Experimental</title><p>Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> synthesis was carried out by using CH<sub>3</sub>COOLi∙2H<sub>2</sub>O (Wako Pure Chemical Industries, Ltd.) as a Li source that was melted with low temperature at about 300˚C, and 30 or 50 m<sup>2</sup>/g anatase TiO<sub>2</sub> (Toho Titanium Co., Ltd.) as a Ti source. The first synthesis process was mixed with the CH<sub>3</sub>COOLi∙2H<sub>2</sub>O and TiO<sub>2</sub> with Li:Ti = 4:5 by ball milling (Fritsch, Pulversitte 7) at 1 h, rotating speed at 320 rpm and orbital speed at 110 rpm in agate mortar and balls. The mixed powder was pre-sintering at 500˚C with 10˚C/min, 1 h in air, and an intermediate was formed. Furthermore, the intermediate was mixed by the ball milling for rotating speed at 320 rpm and orbital speed at 110 rpm at 1 h similarly, and was sintered at 700˚C and 750˚C with 10˚C/min at 1 h in air.</p><p>The obtained powder was identified by XRD (Rigaku Corp., Rint 2000) at scanning step 0.02 deg and scanning speed 5 deg/min by CuKα, and was also measured by BET specific surface area (Shimadzu Corp., FlowSorb III 2305) at 0.1 g sample, gas flow rate 80 cm<sup>3</sup>/min in N<sub>2</sub> and current 50 mA, after degassing the sample with heating at 160˚C at 2 h. Particle size of the obtained sample was observed by FE-SEM (Hitachi, Ltd., S-4200), and crystalline estimation tried with TEM (JEOL Ltd., JEM-2100).</p></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. XRD Measurements</title><p>We yielded the intermediate by pre-sintering a mixture of CH<sub>3</sub>COOLi∙2H<sub>2</sub>O and anatase TiO<sub>2</sub> at 500˚C, and showed XRD patterns as (a); a green line in <xref ref-type="fig" rid="fig1">Figure 1</xref>(A) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(B) by applying the 30 m<sup>2</sup>/g and 50 m<sup>2</sup>/g anatase TiO<sub>2</sub> respectively. The intermediate was identified with unreacted TiO<sub>2</sub> and Li<sub>2</sub>TiO<sub>3</sub> known as a sub- phase of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>. Li<sub>2</sub>TiO<sub>3</sub> has been understood by a phase diagram of Li<sub>2</sub>O-TiO<sub>2</sub> among TiO<sub>2</sub>, Li<sub>2</sub>TiO<sub>3</sub> and Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>, which shows an accurate mixed rate at Li and Ti atoms [<xref ref-type="bibr" rid="scirp.59887-ref20">20</xref>] . A Ti site of Li<sub>2</sub>TiO<sub>3</sub> and Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> is common in center of an octahedron, while a Li site exists in a tetrahedron in the case of Li<sub>2</sub>TiO<sub>3</sub>. Li<sub>2</sub>TiO<sub>3</sub> show inactivity as the electrode not to charge and discharge Li ions [<xref ref-type="bibr" rid="scirp.59887-ref21">21</xref>] .</p><p>To obtain Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>, the intermediate was sintered at 700˚C, and the identification was shown as (b); a red line in the XRD patterns, which obtained main Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> peaks and slight peaks of Li<sub>2</sub>TiO<sub>3</sub>, and was not able to confirm the unreacted TiO<sub>2</sub>. This result is not enough to obtain a single phase Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> at the sintering temperature although all unreacted TiO<sub>2</sub> is consumed. Then, effect of the specific surface area by applying the 30 m<sup>2</sup>/g or 50 m<sup>2</sup>/g anatase TiO<sub>2</sub> was not confirmed in <xref ref-type="fig" rid="fig1">Figure 1</xref>(A) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(B). In the sintering temperature at 750˚C, the single phase Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> was obtained by applying either specific surface area of the anatase TiO<sub>2</sub> as shown in (c); a blue line in the patterns. On the other hand, the peak intensity was strong by applying the anatase TiO<sub>2</sub> of 50 m<sup>2</sup>/g than that of 30 m<sup>2</sup>/g, which would be superior to the crystallization.</p><p>Now, to estimate the synthesized rate of the single phase Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>, we defined a single phase rate in a following equation.</p><p>Single phase rate (%) = [S(Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>)/{S(Li<sub>2</sub>TiO<sub>3</sub>) + S(Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>)}] &#215; 100</p><p>Here, “S” shows area of the peaks. The value was nearly same in 86% in <xref ref-type="fig" rid="fig1">Figure 1</xref>(A) and 89% in <xref ref-type="fig" rid="fig1">Figure 1</xref>(B) at 700˚C, and was 100% at 750˚C in any cases. Consequently, the effect of the specific surface area in the anatase TiO<sub>2</sub> does not be indicated by the single phase rate, while the sintering temperature gave the great effect.</p></sec><sec id="s3_2"><title>3.2. SEM Observation</title><p>The intermediate was produced by the pre-sintering the mixture of CH<sub>3</sub>COOLi・2H<sub>2</sub>O and anatase TiO<sub>2</sub> at 500˚C, and was showed in <xref ref-type="fig" rid="fig2">Figure 2</xref>(A); 30 m<sup>2</sup>/g and <xref ref-type="fig" rid="fig2">Figure 2</xref>(B); 50 m<sup>2</sup>/g anatase TiO<sub>2</sub>. These results showed two</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> XRD patterns of (A) applying the (30 m<sup>2</sup>/g); and (B) 50 (m<sup>2</sup>/g) anatase TiO<sub>2</sub> respectively, addition to (a) pre-sintering temperature at 500 (˚C); (b) sintering temperature at 700 (˚C); and (c) at 750 (˚C) after the pre-sintering. The mark shows ●: Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>; ▲: Li<sub>2</sub>TiO<sub>3</sub>; and ✕: TiO<sub>2</sub>.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x6.png"/></fig><fig id ="fig1_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x7.png"/></fig></fig-group><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> SEM images of the intermediate synthesized by applying (A) 30 (m<sup>2</sup>/g); (B) 50 (m<sup>2</sup>/g) anatase TiO<sub>2</sub> after pre-sintering at 500 (˚C).</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x8.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x9.png"/></fig></fig-group><p>grain species to differ from contrast, which will indicate the unreacted TiO<sub>2</sub> and Li<sub>2</sub>TiO<sub>3</sub> as shown in the XRD pattern. The intermediate would consist of the heterogeneous parts by them. The average grain size of the intermediate was different from 60 nm at <xref ref-type="fig" rid="fig2">Figure 2</xref>(A) and 30 nm at <xref ref-type="fig" rid="fig2">Figure 2</xref>(B), and the specific surface area was about 26.6 m<sup>2</sup>/g and 33.0 m<sup>2</sup>/g respectively. The specific surface area of the applying anatase TiO<sub>2</sub> will give the effect to the average grain size and specific surface area of the intermediate.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> showed homogeneous grains without almost the contrast by the sintering at 700˚C or 750˚C, especially the heterogeneous parts was not observed at 750˚C at all. In fact, the single phases rate is 100%, which would support acquisition of the single phase Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>. While the average grain size trended for greater with the high temperature about <xref ref-type="fig" rid="fig3">Figure 3</xref>(A); 101 nm, <xref ref-type="fig" rid="fig3">Figure 3</xref>(B); 83 nm, <xref ref-type="fig" rid="fig3">Figure 3</xref>(C); 124 nm and <xref ref-type="fig" rid="fig3">Figure 3</xref>(D): 87 nm, it will show no much change by applying the 50 m<sup>2</sup>/g anatase TiO<sub>2</sub>. Similarly, the specific surface area was about (a); 8.3 m<sup>2</sup>/g, (b); 14 m<sup>2</sup>/g, (c); 5.1 m<sup>2</sup>/g and (d): 12 m<sup>2</sup>/g, hence the single phase Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> was obtained with high specific surface area by the 50 m<sup>2</sup>/g anatase TiO<sub>2</sub> at sintering temperature of 750˚C. Furthermore, the crystallization will be higher by the grain of a horned shape.</p></sec><sec id="s3_3"><title>3.3. TEM Observation</title><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows TEM images at pre-sintering temperature of 500˚C. The minute TiO<sub>2</sub> particles will encircle the Li<sub>2</sub>TiO<sub>3</sub> at the 50 m<sup>2</sup>/g anatase TiO<sub>2</sub> specially, which may take advantage of the Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> synthesis by the following sintering. These images did not indicate a clear morphology like a facet in this pre-sintering, and would show a very low crystallization.</p><p>TEM images show the samples by the sintering temperature of 700˚C or 750˚C in <xref ref-type="fig" rid="fig5">Figure 5</xref>. The Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> particles would be the higher crystallization to form at an angular grain which included the facets in the morphology, while the sintering temperature and the specific surface area of the anatase TiO<sub>2</sub> would hardly give the effect for the synthesized Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> not to be obtained about the clear differences. The morphology have been reported about the synthesis by using nano-particle or nano-wire TiO<sub>2</sub>, which have described that the nano-particle or nano-wire Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> was obtained on keeping the TiO<sub>2</sub> morphology like a mold [<xref ref-type="bibr" rid="scirp.59887-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.59887-ref23">23</xref>] . This knowledge will suggest the synthesis mechanism for the solid phase synthesis of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>, which the (002) face of Li<sub>2</sub>TiO<sub>3</sub></p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> SEM images of the synthesized Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> which is (A) 700 (˚C), by the 30 (m<sup>2</sup>/g); (B) 700 (˚C), by the 50 (m<sup>2</sup>/g); (C) 750 (˚C), by the 30 (m<sup>2</sup>/g); (D) 750 (˚C), by the 50 (m<sup>2</sup>/g) anatase TiO<sub>2</sub>.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x10.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x11.png"/></fig><fig id ="fig3_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x12.png"/></fig><fig id ="fig3_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x13.png"/></fig></fig-group><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> TEM images of the intermediate synthesized by applying (A) 30 (m<sup>2</sup>/g); (B) 50 (m<sup>2</sup>/g) anatase TiO<sub>2</sub> after pre- sintering at 500 (˚C).</title></caption><fig id ="fig4_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x14.png"/></fig><fig id ="fig4_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x15.png"/></fig></fig-group><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> TEM images of the synthesized Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> which is (A) 700 (˚C), by the 30 (m<sup>2</sup>/g); (B) 700 (˚C), by the 50 (m<sup>2</sup>/g); (C) 750 (˚C), by the 30 (m<sup>2</sup>/g), (D); 750 (˚C), by the 50 (m<sup>2</sup>/g) anatase TiO<sub>2</sub>.</title></caption><fig id ="fig5_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x16.png"/></fig><fig id ="fig5_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x17.png"/></fig><fig id ="fig5_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x18.png"/></fig><fig id ="fig5_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1740232x19.png"/></fig></fig-group><p>plays a role of the mold in the spinel structure. These may show that the mobility of titanium ions is improved to close to the (002) Li<sub>2</sub>TiO<sub>3</sub> and the (111) Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>We attempted the single phase Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> synthesis with the higher specific surface area by using CH<sub>3</sub>COOLi∙2H<sub>2</sub>O as a Li source that was melted with low temperature at about 300˚C, and 30 or 50 m<sup>2</sup>/g anatase TiO<sub>2</sub> as a Ti source. The synthesis method obtained Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> by the sintering at 700˚C or 750˚C via Li<sub>2</sub>TiO<sub>3</sub> as the intermediate in pre-sintering at 500˚C. Then, the single phase Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> was obtained with 12 m<sup>2</sup>/g specific surface area and the higher crystallization at 750˚C. The mechanism may give a suggestion as the improvement of mobility for the titanium ions.</p></sec><sec id="s5"><title>Cite this paper</title><p>ToshihitoOhtake,Ken-ichiroIijima, (2015) Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> Synthesis with High Specific Surface Area and Single Phase. Journal of Materials Science and Chemical Engineering,03,68-73. doi: 10.4236/msce.2015.39009</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.59887-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Tsutomu, O., Atsushi, U. and Norihiro, Y. (2005) Zero-Strain Insertion Material Insertion Material of Li[Lil/3Ti5/3]O4 for Rechargeable Lithium Cells. Journal of the Electrochemical Society, 142, 1431-1435.</mixed-citation></ref><ref id="scirp.59887-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Masataka, W. (2001) Recent Developments in Lithium Ion Batteries. 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