<?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">JMMCE</journal-id><journal-title-group><journal-title>Journal of Minerals and Materials Characterization and Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-4077</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmmce.2014.26056</article-id><article-id pub-id-type="publisher-id">JMMCE-51161</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><subject> Engineering</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 Coating LiNi&lt;sub&gt;0.5&lt;/sub&gt;Mn&lt;sub&gt;1.5&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt;
 
</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>Wei</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></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="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</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(HL)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>03</day><month>11</month><year>2014</year></pub-date><volume>02</volume><issue>06</issue><fpage>545</fpage><lpage>553</lpage><history><date date-type="received"><day>25</day>	<month>August</month>	<year>2014</year></date><date date-type="rev-recd"><day>17</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>28</day>	<month>October</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>
 
 
  To enhance the electrochemical performances of LiMn
  <sub>2</sub>O
  <sub>4</sub> at elevated temperature (55&#176;C), we proposed a sol-gel method to synthesize LiNi
  <sub>0.5</sub>Mn
  <sub>1.5</sub>O
  <sub>4</sub> modified LiMn
  <sub>2</sub>O
  <sub>4</sub>. The physical and electrochemical performances of pristine and LiNi
  <sub>0.5</sub>Mn
  <sub>1.5</sub>O
  <sub>4</sub>-coated LiMn
  <sub>2</sub>O
  <sub>4</sub> cathode materials were investigated by X-ray diffraction, scanning electron microscopy, transmission electron microscopy, X-ray photoelectron spectroscopy and electrochemical measurements, respectively. The results indicated that about 4-5 nm thick layer of LiNi
  <sub>0.5</sub>Mn
  <sub>1.5</sub>O
  <sub>4</sub> was formed on the surface of the LiMn
  <sub>2</sub>O
  <sub>4</sub> powders. The modified LiMn
  <sub>2</sub>O
  <sub>4</sub> exhibited excellent storage performance at 55&amp;degC compared to the pristine one, which was attributed to the suppression of electrolyte decomposition and the reduction of Mn dissolution.
 
</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>With the advantages of abundant, nontoxic, and inexpensive, spinel lithium manganese oxide (LiMn<sub>2</sub>O<sub>4</sub>) is a promising candidate of the layered cathode materials such as LiCoO<sub>2</sub> [<xref ref-type="bibr" rid="scirp.51161-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.51161-ref2">2</xref>] . Especially, the good stability of LiMn<sub>2</sub>O<sub>4</sub> may ensure its large-scale usage in the batteries for electric vehicle or energy storage [<xref ref-type="bibr" rid="scirp.51161-ref3">3</xref>] . However, LiMn<sub>2</sub>O<sub>4</sub> shows obvious capacity fade when cycling at high temperature [<xref ref-type="bibr" rid="scirp.51161-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51161-ref6">6</xref>] . It was reported that the capacity fading mechanism at high temperature was related to the Jahn-Teller distortion and dissolution of Mn<sup>3+</sup> ions [<xref ref-type="bibr" rid="scirp.51161-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.51161-ref8">8</xref>] . Mn dissolution is induced by HF acid, which is generated by secondary chemical reactions from temperature-enhanced electrolyte decomposition.</p><p>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.51161-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.51161-ref12">12</xref>] . These results indicated that the substitution of Mn with metal ions significantly improved the cycle performance of LiMn<sub>2</sub>O<sub>4</sub>. However, the partial substitutions decrease the capacity of LiMn<sub>2</sub>O<sub>4</sub>. 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> [<xref ref-type="bibr" rid="scirp.51161-ref13">13</xref>] , Al<sub>2</sub>O<sub>3</sub> [<xref ref-type="bibr" rid="scirp.51161-ref14">14</xref>] , SiO<sub>2</sub> [<xref ref-type="bibr" rid="scirp.51161-ref15">15</xref>] and MgO [<xref ref-type="bibr" rid="scirp.51161-ref16">16</xref>] have been used to coat LiMn<sub>2</sub>O<sub>4</sub> by some chemical processes. However, the aforementioned oxides with non-spinel structure are hard to grow on the surface of LiMn<sub>2</sub>O<sub>4</sub>. With a similar structure to LiMn<sub>2</sub>O<sub>4</sub>, LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> can grow more easily on LiMn<sub>2</sub>O<sub>4</sub> than other alien phase and form a more close-contacted protective covering layer, which may suppress the dissolution of Mn. Therefore, it is expected that the modified LiMn<sub>2</sub>O<sub>4</sub> will show an excellent cycle performance at elevated temperature. In this study, we proposed an approach to synthesize LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> on the surface of spinel LiMn<sub>2</sub>O<sub>4</sub>. The effect of LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</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 Heibei Strong-Power Li-ion Battery Tecnology Co. Ltd (D98, China). To coat LiMn<sub>2</sub>O<sub>4</sub> with LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>, LiCH<sub>3</sub>COO∙2H<sub>2</sub>O (0.558 g), Mn (CH<sub>3</sub>COO)<sub>2</sub>∙4H<sub>2</sub>O (2.011 g) and Ni (CH<sub>3</sub>COO)<sub>2</sub>∙4H<sub>2</sub>O (0.68 g) with a stoichiometric ratio (2:1:3) were dissolved in distilled water to form a clear solution. An aqueous solution of ethylene glycol and citric acid as a chelating agent was added to the mixtures. pH value at 6.5 - 7.0 was achieved by Ammonium hydroxide. Then the LiMn<sub>2</sub>O<sub>4</sub> powders (50 g) were slowly added to the sol and vigorously stirred at 85˚C for 8 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 400˚C for 10 h and 750˚C for 3 h to obtain LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</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 diffractometer (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). X-ray photoelectron spectroscopy (Kratos AXIS Ultra DLD) was employed to probe the surface for Mn Valence states. 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 electrodes, 85 wt% active materials, 9 wt% acetylene black and 6 wt% polyvinylidene fluoride were homogeneously mixed in N-methyl-pyrroline. Then the resluting slurry was spread on an aluminum 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 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). Cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS) investigations were performed on an electrochemical workstation (PGSTAT302N, Autolab) at 25˚C &#177; 2˚C. The CV curves were recorded between 3.3 and 4.35 V at a scan rate of 0.1 mV&#183;s<sup>−</sup><sup>1</sup>. The EIS measurements were performed over a frequency range from 10 kHz to 0.1 Hz.</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 of pristine and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>. 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 pristine and modified LiMn<sub>2</sub>O<sub>4</sub>. The crystal lattice parameters were calculated by using the software of Jade, are 8.245 and 8.243 &#197; for the pristine and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</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 LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> are not observed because of the low content (about 2.0 wt%).</p><p>Scanning electron microscopy reveals that the pristine and modified samples present a uniform particle distribution, ranging from 2 to 7 μm. The pristine spinel crystals are smooth with well-defined facets, as observed in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) and <xref ref-type="fig" rid="fig2">Figure 2</xref>(c). It can be seen that the morphology and particle diameter of the LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> X-ray diffraction patterns of pristine and modified 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/3-2710258x6.png"/></fig><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> SEM figures of (a), (c) pristine and (b), (d) LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>.<sub> </sub></title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x7.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x8.png"/></fig><fig id ="fig2_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x9.png"/></fig><fig id ="fig2_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x10.png"/></fig></fig-group><p>coated LiMn<sub>2</sub>O<sub>4</sub> powders in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) and <xref ref-type="fig" rid="fig2">Figure 2</xref>(d), are similar to the pristine sample. No LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> agglomerations and obscured facets of spinel LiMn<sub>2</sub>O<sub>4</sub> are observed.</p><p>The element composition is determined by EDS analysis. The element mapping of Ni and Mn is displayed in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The dense accumulation of Mn spots is attributed to the host material of LiMn<sub>2</sub>O<sub>4</sub> and there is no significant agglomeration of Ni. This indicates that LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> is homogeneously dispersed on the surface of the LiMn<sub>2</sub>O<sub>4</sub> particles.</p><p>TEM micrographs are displayed in <xref ref-type="fig" rid="fig4">Figure 4</xref>. Compared to the pristine sample (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a)), about 4 - 5 nm</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> EDS mappings of O, Mn and Ni elements of modified LiMn<sub>2</sub>O<sub>4</sub>.<sub> </sub></title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x12.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x11.png"/></fig><fig id ="fig3_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x14.png"/></fig><fig id ="fig3_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x13.png"/></fig></fig-group><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> TEM figure of pristine (a) and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> (b)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x15.png"/></fig><p>thick layer of LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> is uniformly formed on the surface of the LiMn<sub>2</sub>O<sub>4</sub> (<xref ref-type="fig" rid="fig4">Figure 4</xref>(b)). The coating layer is clearly distinguishable from the crystalline LiMn<sub>2</sub>O<sub>4</sub>. The TEM analysis demonstrates that the sol-gel method is an effective way to coat the LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> layer on the surface of LiMn<sub>2</sub>O<sub>4</sub>.</p><p>The oxidation state of manganese ions at the surface was determined from XPS data by the curve fitting of Mn 2p spectral peaks. The experimental peak shape for Mn 2p<sub>3/2</sub> was modeled by employing multiple-splitting patterns derived for Mn<sup>3+</sup> and Mn<sup>4+</sup> at binding energies of 641.6, and 642.8 eV from the standard compounds Mn<sub>2</sub>O<sub>3</sub> and MnO<sub>2</sub>. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows the fit of the models to the experimental spectra for pristine LiMn<sub>2</sub>O<sub>4</sub> and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> respectively. The surface of the pristine LiMn<sub>2</sub>O<sub>4</sub> sample consists of almost equal amounts of Mn<sup>4+</sup> and Mn<sup>3+</sup>. By contrast, LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> exhibited a Mn<sup>4+</sup>:Mn<sup>3+</sup> ratio of 59.4:40.6. The difference of Mn<sup>4+</sup>:Mn<sup>3+</sup> ratio on the surface is due to the formation of LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>, because it has higher valence state of manganese ions. This result is good agreement with the observation of HR-TEM.</p><p>As shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>, the galvanostatic charge-discharge curves under a current rate of 2C were conducted at elevated temperatures (55˚C). It 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.51161-ref17">17</xref>] , indicating LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</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. LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> shows a lower discharge capacity (104.2 mAh/g) compares to the pristine sample (106.3 mAh/g). The reason of low initial discharge capacity is that LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> shows no capacity at this voltage range due to its high discharge voltage over 4.35V [<xref ref-type="bibr" rid="scirp.51161-ref18">18</xref>] .</p><p><xref ref-type="fig" rid="fig7">Figure 7</xref> shows the cycling performance of electrodes with and without LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> coating. After 100 cycles, the discharge capacity of the pristine LiMn<sub>2</sub>O<sub>4</sub> drops from 106.3 to 89.2 mAh/g. In contrast, the discharge capacity of modified sample changes from 104.2 to 98 mAh/g. The capacity retention increases from 84.0% to 94.4% after LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> coating.</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 LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> electrode was 20.54 and 12.17 μg/cm<sup>2</sup>, respectively. It can be concluded that after coating by LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> layer, the dissolution of the manganese ions was significantly reduced. Therefore, LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> electrode had better cycle stability at elevated temperature.</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows the CV profiles of pristine and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> electrodes in the 10th and 100th cycles at the scan rate of 0.1 mV∙s<sup>−1</sup>. The CV peaks of LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated sample show two symmetrical couples of redox peaks at around 3.98 and 4.1 V respectively (<xref ref-type="fig" rid="fig8">Figure 8</xref>(b)), indicating that electrochemical insertion and extraction reactions of Li<sup>+</sup> ions are two step processes. It is in agreement with the two plateaus in <xref ref-type="fig" rid="fig6">Figure 6</xref> and demonstrates that LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> coating does not change the electrochemical reaction mechanism of LiMn<sub>2</sub>O<sub>4</sub>. After 10 cycles, two narrow and separate redox peaks appear around at 3.96 and 4.11 V, as shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>(a). However, after 100th cycles, due to the dissolution of Mn<sup>3+</sup> ions into the electrolyte</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> XPS spectra of the pristine (a) and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> (b).</title></caption><fig id ="fig5_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x16.png"/></fig><fig id ="fig5_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x17.png"/></fig></fig-group><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> The first Charge-discharge curves of LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> at elevated temperature (under 2C rate, 55˚C &#177; 2˚C)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x18.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Cycling behaviours of LiMn<sub>2</sub>O<sub>4</sub> and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> cycled (under 2C rate, 55˚C &#177; 2˚C)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x19.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The amount of Mn<sup>2+</sup> 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 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" >20.54</td></tr><tr><td align="center" valign="middle" >LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub></td><td align="center" valign="middle" >12.17</td></tr></tbody></table></table-wrap><p>(Jahn-Teller distortion), both anodic and cathodic peaks become much broader and lower in peaks current. In contrast, the oxidation and reduction peaks relate to LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> are much steadier after 100 cycles (<xref ref-type="fig" rid="fig8">Figure 8</xref>(b)), which indicated that modified LiMn<sub>2</sub>O<sub>4</sub> has better reversibility and stability than the pristine LiMn<sub>2</sub>O<sub>4</sub>.</p><p>Electrochemical impedance spectra (EIS) and equivalent circuits are shown in <xref ref-type="fig" rid="fig9">Figure 9</xref>. The measurements were carried out with fully charged state (4.35 V). An intercept in the high frequency region of the Z<sub>rel</sub>
axis indicates the ohmic resistance (Rs), the combined resistance of the electrolyte and the contacts of the cell [<xref ref-type="bibr" rid="scirp.51161-ref19">19</xref>] . The semicircle in high-middle frequency region corresponds to the charge transfer (Rct) process on the electrode interface, revealing the lithium transfer rate parameters and the capacitance of the SEI (solid eleteolyte interface) [<xref ref-type="bibr" rid="scirp.51161-ref20">20</xref>] . 
The inclined line in the lower frequency region represents the Warburg impedance (Zw), which is corresponded to the diffusion of Li<sup>+</sup> in LiMn<sub>2</sub>O<sub>4</sub> particles [<xref ref-type="bibr" rid="scirp.51161-ref21">21</xref>] . The plots are fitted and listed in <xref ref-type="table" rid="table2">Table 2</xref>. As shown in</p>
<fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Typical CV curves of 10th and 100th cycles of pristine (a), and iNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> (b). <sub> </sub></title></caption><fig id ="fig8_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x20.png"/></fig><fig id ="fig8_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2710258x21.png"/></fig></fig-group><disp-formula id="scirp.51161-formula391"><graphic  xlink:href="http://html.scirp.org/file/3-2710258x22.png"  xlink:type="simple"/></disp-formula><p><xref ref-type="fig" rid="fig9">Figure 9</xref>. EIS of pristine and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> at the end of 10th and 100th cycle. <sub> </sub></p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The AC impedance fitting data
for pristine LiMn<sub>2</sub>O<sub>4</sub> and LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub>.</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Samples</th><th align="center" valign="middle" >R<sub>s</sub>/Ω</th><th align="center" valign="middle" >R<sub>ct</sub>/Ω</th></tr>
</thead><tr><td align="center" valign="middle" >Pristine LiMn<sub>2</sub>O<sub>4</sub> at 10th fully charge state</td><td align="center" valign="middle" >2.02</td><td align="center" valign="middle" >26.82</td></tr><tr><td align="center" valign="middle" >LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> at 10th fully charged state</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >24.4</td></tr><tr><td align="center" valign="middle" >Pristine LiMn<sub>2</sub>O<sub>4</sub> at 100th fully charge state</td><td align="center" valign="middle" >3.55</td><td align="center" valign="middle" >73.8</td></tr><tr><td align="center" valign="middle" >LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> at 100th fully charged state</td><td align="center" valign="middle" >2.85</td><td align="center" valign="middle" >34.8</td></tr></tbody></table></table-wrap><p>the table, after 10 cycles, the Rs for LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> is slightly larger than the pristine sample, because that the coating layer may slightly increase the elecrolyte and contact resistance. The charge transfer resistance of both samples is approximately the similar (26.82 and 24.4 Ω∙cm<sup>2</sup>). After 100 cycles, the change in R<sub>s</sub> is negligible. However, the R<sub>ct</sub> value of the LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated electrode (34.8 Ω∙cm<sup>2</sup>) is two times smaller than that the value pristine electrode (73.8 Ω∙cm<sup>2</sup>). It attributes to the restraint of structural instability caused by the subsequent Mn dissolution and vacancies formation. This result is also in accordance with the enhanced cycling performance of LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated electrodes.</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 LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> using a sol-gel method. TEM and XPS results confirm the existence of LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> layer. A uniform and dense layer about 4 - 5 nm was coating on the surface of pristine LiMn<sub>2</sub>O<sub>4</sub>. The LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</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. The CV tests indicated that the LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> electrode has better reversibility and stability. Meanwhile, the charge transfer resistance of the LiNi<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>-coated LiMn<sub>2</sub>O<sub>4</sub> was much less than that of pristine sample after 100 cycles, which is ascribed to the better structural stability and restraint of Mn dissolution. 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.51161-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. Journal of Materials Chemistry, 21, 11040-11051.  
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