<?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.2014.212003</article-id><article-id pub-id-type="publisher-id">MSCE-52340</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>
 
 
  Enhanced High-Temperature Cycling Stability of LiMn&lt;SUB&gt;2&lt;/SUB&gt;O&lt;SUB&gt;4&lt;/SUB&gt; by LiCoO&lt;SUB&gt;2&lt;/SUB&gt; Coating as Cathode Material for Lithium Ion Batteries
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ing</surname><given-names>Yan</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>Haohan</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yuelei</surname><given-names>Wang</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>Xinxin</surname><given-names>Zhao</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>Yiming</surname><given-names>Mi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Baojia</surname><given-names>Xia</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai, China</addr-line></aff><aff id="aff1"><addr-line>College of Chemistry and Chemical Engineering, Shanghai University of Engineering Science, Shanghai, China</addr-line></aff><aff id="aff2"><addr-line>Shanghai Nanotechnology Promotion Center, Shanghai, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>biluo1873@163.com(YM)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>12</month><year>2014</year></pub-date><volume>02</volume><issue>12</issue><fpage>12</fpage><lpage>18</lpage><history><date date-type="received"><day>27</day>	<month>November</month>	<year>2014</year></date><date date-type="rev-recd"><day>10</day>	<month>December</month>	<year>2014</year>	</date><date date-type="accepted"><day>17</day>	<month>December</month>	<year>2014</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>
 
 
  LiCoO
  <sub>2</sub> surface layer is proposed and prepared through sol-gel method. The physical and electrochemical performances of pristine LiMn
  <sub>2</sub>
  O
  <sub>4</sub>
   and LiCoO
  <sub>2</sub>
  -coated LiMn
  <sub>2</sub>
  O
  <sub>4</sub>
   cathode materials were investigated by X-ray diffraction, scanning electron microscopy, transmission electron microscopy, electrochemical measurements respectively. Comparing with the pristine LiMn
  <sub>2</sub>
  O
  <sub>4</sub>
  , the LiCoO
  <sub>2</sub>
  - coated LiMn
  <sub>2</sub>
  O
  <sub>4</sub>
   phase significantly improved cycling stability, especially at 55&#176;C. Additionally, the thermal safety of LiMn2O
  <sub>4</sub>
   is greatly enhanced after being coated by LiCoO
  <sub>2</sub>
  . ICP-AES measurement, structural analysis, and impedance experiments indicate that the improved electrochemical property of LiCoO
  <sub>2</sub>
  -coated LiMn
  <sub>2</sub>
  O
  <sub>4</sub>
   should be attributed to the alleviated dissolution loss of manganese, strengthened structural stability.
 
</p></abstract><kwd-group><kwd>LiMn&lt;SUB&gt;2&lt;/SUB&gt;O&lt;SUB&gt;4&lt;/SUB&gt;</kwd><kwd> Sol-Gel Method</kwd><kwd> Surface Coating</kwd><kwd> Electrochemical Performance</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Lithium ion battery (LIB) has become the most widely used power supply for electronics. Safer electrode material has been pursued by researchers for years [<xref ref-type="bibr" rid="scirp.52340-ref1">1</xref>] . Spinel lithium manganese oxide (LiMn<sub>2</sub>O<sub>4</sub>), with the advantages of abundant, nontoxic, and inexpensive, is a promising cathode material for power lithium ion battery mainly [<xref ref-type="bibr" rid="scirp.52340-ref2">2</xref>] . Especially, the good stability may ensure its large-scale usage in the batteries for electric vehicle or energy storage [<xref ref-type="bibr" rid="scirp.52340-ref3">3</xref>] . However, LiMn<sub>2</sub>O<sub>4</sub> shows obvious capacity fade when high-temperature working condition is applied (50˚C - 60˚C) [<xref ref-type="bibr" rid="scirp.52340-ref4">4</xref>] . The cause for the capacity degradation of LiMn<sub>2</sub>O<sub>4</sub> is Jahn-Teller distortion and accepted as electrolyte decomposition, Mn<sup>2+</sup> ions dissolution [<xref ref-type="bibr" rid="scirp.52340-ref5">5</xref>] , oxygen deficiency [<xref ref-type="bibr" rid="scirp.52340-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.52340-ref7">7</xref>] . In order to solve this problem, earlier studies have been focused on a chemical modification of LiMn<sub>2</sub>O<sub>4</sub> by a partial substitution of Mn with some metal ions to obtain LiM<sub>x</sub>Mn<sub>2−x</sub>O<sub>4</sub> (M = Co, Mg, Cr, Ni, Fe, Al, Ti and Zn) [<xref ref-type="bibr" rid="scirp.52340-ref8">8</xref>] - [<xref ref-type="bibr" rid="scirp.52340-ref12">12</xref>] . Another effective way is surface coating on LiMn<sub>2</sub>O<sub>4</sub> by oxide with high thermal and structural stability. ZrO<sub>2</sub>, SiO<sub>2</sub>, Al<sub>2</sub>O<sub>3</sub> and MgO [<xref ref-type="bibr" rid="scirp.52340-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.52340-ref16">16</xref>] have been used to coat LiMn<sub>2</sub>O<sub>4</sub> by some chemical processes. LiCoO<sub>2</sub> coating may suppress the dissolution of Mn and with de-intercalation and intercalation of Li ions, which will enhance the capacity of LiMn<sub>2</sub>O<sub>4</sub>. Therefore, it is expected that the LiMn<sub>2</sub>O<sub>4</sub> by coating LiCoO<sub>2</sub> will show an excellent cycle performance at high-temperature. In this study, the effect of LiCoO<sub>2</sub> layer on the morphology and electrochemical performances of LiMn<sub>2</sub>O<sub>4</sub> cathode materials were examined in detail.</p></sec><sec id="s2"><title>2. Experimental</title><p>LiMn<sub>2</sub>O<sub>4</sub> powder was purchased from Hebei Strong-Power Li-ion Battery Technology Co. Ltd. (D98, China). LiCH<sub>3</sub>COO∙2H<sub>2</sub>O (1.03 g), Co (CH<sub>3</sub>COO)<sub>2</sub>∙4H<sub>2</sub>O (2.53 g) with a stoichiometric ratio (1:1) were dissolved in distilled water. An aqueous solution of ethylene glycol and citric acid (1:4) as a chelating agent was added to the mixtures. pH value at 7.0 - 7.5 was achieved by Ammonium hydroxide. Then slowly add the LiMn<sub>2</sub>O<sub>4</sub> powders (50 g) to the sol and vigorously stirred at 85˚C for 5 h. As the evaporation of water proceeding, the sol was turned into a viscous transparent gel. After drying and sieving, the powder was sintering in air at 350˚C for 3 h and 650˚C for 3 h to obtain LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>. For a comparison, pristine LiMn<sub>2</sub>O<sub>4</sub> was also heat-treated in the same condition.</p><sec id="s2_1"><title>2.1. Structure and morphology characterization</title><p>X-ray diffraction patterns were recorded on a DX-2700 diffract meter (Siemens D-5000, Mac Science MXP 18) equipped with Cu Kα radiation of λ = 0.154145 nm. The diffraction patterns were recorded between scattering angles of 15˚ and 80˚ at a step of 4˚/min. The morphology was studied by a scanning electron microscopy (S4700, Hitachi) and transmission electron microscope (JEOL-1200EX). After cycling, the batteries were disassembled in glove box and the electrodes and membrane were washed by EC/DMC for several times. The cathode was used to examine the changes in structure by XRD and the obtained solution was diluted to suitable concentration to detect the content of Mn element. Inductively coupled plasma atomic emission spectrometry analysis was conducted on IRIS Intrepid П XSP inductively coupled plasma emission spectrometer (THERMO).</p></sec><sec id="s2_2"><title>2.2. Electrochemical and thermal characteristics</title><p>To obtain working electrode, 85 wt% active materials, 6 wt% polyvinylidene fluoride and 9 wt% acetylene black were homogeneously mixed in NMP. Then the resulting slurry was spread on an Al foil and thoroughly dried. The electrodes were punched in the form of 14 mm diameter disks, and the typical active material mass loading was about 6 mg/cm<sup>2</sup>. The electrolyte was 1 M LiPF<sub>6</sub> dissolved in a mixture of ethylene carbonate and dimethylene carbonate with the volume ratio of 1:1. The anode of the battery is Li electrode. The assembly process was conducted in an argon-filled glove-box with the content of H<sub>2</sub>O and O<sub>2</sub> less than 1 ppm.</p><p>Before electrochemical tests, the batteries were aged for 24 h to ensure good soakage. The cells were charged and discharged on a battery tester (CT-3008W, NEWARE) between 3.3 and 4.35 V at the rate of 2C at elevated temperatures (55˚C &#177; 2˚C) in dry oven (A201113, Shanghai).</p></sec></sec><sec id="s3"><title>3. Results and discussion</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows the XRD patterns. The peaks of both samples could be indexed to a cubic spinel structure with the space group Fd3m. There is no substantial difference between XRD patterns for LiMn<sub>2</sub>O<sub>4</sub> and modified sample. The crystal lattice parameters were calculated by using the software of Jade, are 8.245 and 8.246 &#197; for the pristine and LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>, indicating that the bulk structure of LiMn<sub>2</sub>O<sub>4</sub> unchange after surface modification. The characteristic peaks corresponding to LiCoO<sub>2</sub> are not observed because of low content (about 2.0 wt%).</p><p>Scanning electron microscopy has been shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> which reveals the pristine and modified samples</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> X-ray diffraction patterns of (a) Pristine and (b) LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x6.png"/></fig><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> SEM figures of (a) Pristine and (b) LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x7.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x8.png"/></fig></fig-group><p>present a uniform particle distribution, ranging from 3 to 6 μm. The pristine spinel crystals are smooth with well-defined facets, as observed in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a). It can be seen that the morphology and particle diameter of the LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> powders in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b), are similar to the pristine sample. No LiCoO<sub>2</sub> agglomerations and obscured facets of spinel LiMn<sub>2</sub>O<sub>4</sub> are observed.</p><p>The further investment of the surface of LiMn<sub>2</sub>O<sub>4</sub> by transmission electron microscope is displayed in <xref ref-type="fig" rid="fig3">Figure 3</xref>. Compared to the pristine sample (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)), about 3 - 5 nm thick layer of LiCoO<sub>2</sub> is uniformly formed on the surface of the LiMn<sub>2</sub>O<sub>4</sub> (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)). The coating layer is clearly distinguishable from the crystalline LiMn<sub>2</sub>O<sub>4</sub>. This result demonstrates that sol-gel method is an effective way to coat the LiCoO<sub>2</sub> layer on the surface of LiMn<sub>2</sub>O<sub>4</sub>.</p><p>To further identify the homogeneity of coating layer, the element distribution is determined by EDS mapping, which is displayed in <xref ref-type="fig" rid="fig4">Figure 4</xref>. The dense accumulation of Mn element is attributed to the host material of LiMn<sub>2</sub>O<sub>4 </sub>and there is no significant agglomeration of Co. These results indicate that LiCoO<sub>2</sub> is homogeneously dispersed on the surface of the LiMn<sub>2</sub>O<sub>4</sub> particles.</p><p>The XPS is shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, for pristine LiMn<sub>2</sub>O<sub>4</sub> sample, there is no Co2p peaks. For LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> sample, the Co2p region shows a Co2p<sub>3/2</sub> main peak at 780.4 eV with satellite peak at 796.8 eV. It is concluded that Co<sup>3+</sup> have deposited on the surface of LiMn<sub>2</sub>O<sub>4</sub>. This result is in good agreement with the</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> TEM figures of (a) Pristine and (b) LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x10.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x9.png"/></fig></fig-group><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> EDS mappings of Co and Mn elements of modified LiMn<sub>2</sub>O<sub>4</sub> sample.</title></caption><fig id ="fig4_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x12.png"/></fig><fig id ="fig4_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x11.png"/></fig><fig id ="fig4_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x13.png"/></fig></fig-group><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The Co2p X-ray photoelectron spectra of the pristine and LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x14.png"/></fig><p>observation in TEM and EDS element mapping.</p><p>The structure of pristine LiMn<sub>2</sub>O<sub>4</sub> and LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> cathodes after cycling 100 times (55˚C) was examined. The results are given in <xref ref-type="fig" rid="fig6">Figure 6</xref>. It can be seen that, the diffraction peaks of cycled LiMn<sub>2</sub>O<sub>4</sub> cathode are widened and the peak intensity declined compared with the pristine LiMn<sub>2</sub>O<sub>4</sub> cathode. In addition, some extra peaks appear in LiMn<sub>2</sub>O<sub>4</sub> cathode XRD pattern after cycling, which should be assigned to Li<sub>2</sub>Mn<sub>2</sub>O<sub>4</sub>. Usually, tetrahedral Li<sub>2</sub>Mn<sub>2</sub>O<sub>4</sub> can be generated at the final discharge stage of LiMn<sub>2</sub>O<sub>4</sub> because of more Mn<sup>3+</sup> and more significant Jahn-Teller effect. However, for the LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> cathode, the diffraction peak width changed insignificantly before and after cycling. Comparing with cycled LiMn<sub>2</sub>O<sub>4</sub> cathode, in the XRD</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> XRD patterns of (a) Pristine, (b) LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x15.png"/></fig><p>pattern of the cycled LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>, the peak intensity declines a polarization, we still should ascribe them to the LiCoO<sub>2</sub> on the surface of LiMn<sub>2</sub>O<sub>4</sub>.</p><p>In <xref ref-type="fig" rid="fig7">Figure 7</xref>, the galvanostatic charge-discharge curves under a current rate of 2C were conducted at (a) room temperature and (b) elevated temperatures in drying oven. They shows two discharge plateaus, which should be attributed to orderly intercalating of lithium ions in the tetrahedral (8a) sites at 4.1 V and disorderly intercalating lithium ions at 3.9 V which substantially maintains the intercalation feature of LiMn<sub>2</sub>O<sub>4</sub> substrate [<xref ref-type="bibr" rid="scirp.52340-ref17">17</xref>] , indicating LiCoO<sub>2</sub> surface layer rather than Ni-doped LiMn<sub>2</sub>O<sub>4</sub> because LiMn<sub>2</sub>O<sub>4</sub> with Ni-doped spinel surface showed two ambiguously resolved discharging plateaus [<xref ref-type="bibr" rid="scirp.52340-ref18">18</xref>] . LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> shows a higher discharge capacity compares to the pristine sample. The reason of high initial discharge capacity is that LiCoO<sub>2</sub> has capacity at this voltage range.</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows the cycling performance of electrodes with and without LiCoO<sub>2</sub> coating at (a) room temperature and (b) elevated temperatures. After 100 cycles at room temperature, the capacity retention of pristine sample (94.3%) is similar to that of modified sample (94.4%), as shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>(a). However, after 100 cycles at elevated temperature, the discharge capacity of the pristine LiMn<sub>2</sub>O<sub>4</sub> drops from 115.3 to 100.6 mAh/g. In contrast, the discharge capacity of modified sample changes from 117.2 to 110.1 mAh/g. The capacity retention increases from 87.5% to 93.6% after LiCoO<sub>2</sub> coating. Compared with other coating materials such as Al<sub>2</sub>O<sub>3</sub> [<xref ref-type="bibr" rid="scirp.52340-ref19">19</xref>] , La<sub>2</sub>O<sub>3</sub> [<xref ref-type="bibr" rid="scirp.52340-ref20">20</xref>] , AlPO<sub>4</sub> [<xref ref-type="bibr" rid="scirp.52340-ref21">21</xref>] , In these paper, surface modification by sol-gel method can improve the high-tempera- ture cycling stability of LiMn<sub>2</sub>O<sub>4</sub>, because oxide layer can reduce the contact area of LiMn<sub>2</sub>O<sub>4</sub> and electrolyte. However, the covering layer is not very uniform, the highest capacity retention is about 89%, coupled with the oxide itself do not have de-intercalation and intercalation of Li ions, it will result in a decrease in initial capacity.</p><p>To further verify the effects of surface coating on manganese ions dissolution, the quality of the manganese element was directly determined by using ICP-AES. Li metal anode was washed by dilute hydrochloric acid after 100th cycle at 55˚C &#177; 2˚C. It can be seen in <xref ref-type="table" rid="table1">Table 1</xref>, the dissolved quality of Mn<sup>2+</sup> ions of the pristine and LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> electrode was 22.54 and 10.17 μg/cm<sup>2</sup>, respectively. It can be concluded that after coating by LiCoO<sub>2</sub> layer, the dissolution of the manganese ions was significantly reduced. Therefore, LiCoO<sub>2</sub>- coated LiMn<sub>2</sub>O<sub>4</sub> electrode had better cycle stability at elevated temperature. The reason is that the coating material will reduce the contact area of LiMn<sub>2</sub>O<sub>4</sub> and electrolyte, which may decrease the dissolution of Mn. The reactivity between LiCoO<sub>2</sub> and electrolyte has not yet clear, which need further research in future.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In summary, the surface of LiMn<sub>2</sub>O<sub>4</sub> sample was modified by LiCoO<sub>2</sub> using a sol-gel method. TEM and XPS results confirm the existence of LiCoO<sub>2</sub> layer. A uniform and dense layer about 3 - 5 nm was coating on the</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> The first charge-discharge curves at (a) Room temperature (25˚C &#177; 2˚C); (b) Elevated temperature (55˚C &#177; 2˚C)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x16.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Cycling behaviors at (a) Room temperature (25˚C &#177; 2˚C); (b) Elevated temperature (55˚C &#177; 2˚C)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-1740139x17.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The amount of Mn ions deposited on Li anode after 100 cycles at 55˚C &#177; 2˚C</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Samples</th><th align="center" valign="middle" >The quality of Mn ions on Li anode (μg/cm<sup>2</sup>)</th></tr></thead><tr><td align="center" valign="middle" >Pristine LiMn<sub>2</sub>O<sub>4</sub></td><td align="center" valign="middle" >22.54</td></tr><tr><td align="center" valign="middle" >LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub></td><td align="center" valign="middle" >10.17</td></tr></tbody></table></table-wrap><p>surface of pristine LiMn<sub>2</sub>O<sub>4</sub>. The LiCoO<sub>2</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> sample exhibits much better cycling stability at elevated temperature (55˚C) compared with the pristine sample. These results demonstrated that this is an effective way to improve the high-temperature cyclic performance of spinel LiMn<sub>2</sub>O<sub>4</sub>.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work was supported by National Science Foundation of China (No. 50672026). This work was also supported by Shanghai Nano Technology Promotion (No. 12ZR1448800).</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.52340-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Pitchai, R., Thavasi, V., Mhaisalkar, S.G. and Ramakrishna, S. (2011) Nanostructured Cathode Materials: A Key for Better Performance in Li-Ion Batteries. 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