<?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.2016.79042</article-id><article-id pub-id-type="publisher-id">MSA-70287</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>
 
 
  Synthesis and Structural Characterization of Monocrystalline &lt;i&gt;α&lt;/i&gt;-V&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt; Nanowires
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>María</surname><given-names>Luisa Tafoya Ronquillo</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>Patricia</surname><given-names>Santiago Jacinto</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>Pilar</surname><given-names>Ovalle</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>Luis</surname><given-names>Rendón Vázquez</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>Elizabeth</surname><given-names>Chavira Martínez</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>Ernesto</surname><given-names>Marinero</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vicente</surname><given-names>Garibay</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff4"><addr-line>Instituto Mexicano del Petróleo IMP, México, D.F., México</addr-line></aff><aff id="aff3"><addr-line>Purdue University, Purdue Mall, West Lafayette, IN, USA</addr-line></aff><aff id="aff2"><addr-line>Instituto de Investigaciones en Materiales, UNAM, Circuito de la Investigación s/n, Ciudad Universitaria, México, D.F., México</addr-line></aff><aff id="aff1"><addr-line>Instituto de Física, UNAM, Circuito de la Investigación s/n, Ciudad Universitaria, México, D.F., México</addr-line></aff><pub-date pub-type="epub"><day>01</day><month>09</month><year>2016</year></pub-date><volume>07</volume><issue>09</issue><fpage>484</fpage><lpage>495</lpage><history><date date-type="received"><day>July</day>	<month>29,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>August</month>	<year>28,</year>	</date><date date-type="accepted"><day>September</day>	<month>1,</month>	<year>2016</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 stable one-dimensional system in an orthorhombic 
  α-V
  <sub>2</sub>O
  <sub>5</sub> nanowires monocrystalline structure was obtained by a solvothermal method from a polymorphic V
  <sub>2</sub>O
  <sub>5</sub> structure. The starting material was firstly submitted to acid hydrolysis in H
  <sub>2</sub>O
  <sub>2</sub> followed by a solvothermal treatment. The outcome of this procedure, a metastable phase of the one-dimensional system V
  <sub>10</sub>O
  <sub>24</sub>&amp;middot;12H
  <sub>2</sub>O/V
  <sub>3</sub>O
  <sub>7</sub>&amp;middot;H
  <sub>2</sub>O, was subsequently reoxidized by controlled heating in an open air system. The final product was an orange crystalline solid mainly formed by monocrystalline nanowires of 
  α-V
  <sub>2</sub>O
  <sub>5</sub> having lengths of tens of micrometers and widths of about 75 nm with a preferential [200] growth direction. It was found that the pH value of the initial solution plays an important role in the formation of the crystalline phase in the final products. Characterization was performed by X-ray diffraction (XRD), scanning electron microscopy (SEM) and high-resolution transmission electron microscopy (HRTEM). This study offers an alternate route for the synthesis of vanadium oxides and related compounds.
 
</p></abstract><kwd-group><kwd>Nanostructures</kwd><kwd> Oxides</kwd><kwd> Crystal Growth</kwd><kwd> X-Ray Diffraction</kwd><kwd> Crystal Structure</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>One-dimensional (1D) nanostructured materials, including nanotubes, nanowires, nanobelts, nanoribbons and nanorods, often exhibit specific physical and chemical properties due to their nanometer dimensions, which differ greatly from those of their bulk counterparts [<xref ref-type="bibr" rid="scirp.70287-ref1">1</xref>] . Among one-dimensional structures, the synthesis of vanadium pentoxide (V<sub>2</sub>O<sub>5</sub>) and their derivative compounds has been researched intensively due to their redox activity and layered structures [<xref ref-type="bibr" rid="scirp.70287-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.70287-ref11">11</xref>] . The layered crystal structure of V<sub>2</sub>O<sub>5</sub> allows the insertion of small ions, for example Li<sup>+</sup> and has potential applications in lithium batteries [<xref ref-type="bibr" rid="scirp.70287-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.70287-ref14">14</xref>] , electric field-effect transistors [<xref ref-type="bibr" rid="scirp.70287-ref15">15</xref>] and chemical sensors or actuators [<xref ref-type="bibr" rid="scirp.70287-ref16">16</xref>] .</p><p>Vanadium forms a variety of binary compounds with the general formula, VO<sub>2+x</sub> (−0.5 ≤ x ≤ 0.5), such as V<sub>2</sub>O<sub>3</sub>, VO<sub>2</sub>, V<sub>2</sub>O<sub>5</sub>, V<sub>3</sub>O<sub>7</sub>, V<sub>4</sub>O<sub>9</sub>, V<sub>6</sub>O<sub>13</sub> [<xref ref-type="bibr" rid="scirp.70287-ref17">17</xref>] . Among them vanadium pentoxide presents the polymorphs α-V<sub>2</sub>O<sub>5</sub> (orthorhombic) [<xref ref-type="bibr" rid="scirp.70287-ref18">18</xref>] , β-V<sub>2</sub>O<sub>5</sub> (monoclinic or tetragonal) and γ-V<sub>2</sub>O<sub>5</sub> (orthorhombic) structures [<xref ref-type="bibr" rid="scirp.70287-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.70287-ref20">20</xref>] . The polymorph α-V<sub>2</sub>O<sub>5</sub> is one of the most widely studied transition metal oxides in the V-O system, because it is the most stable phase at atmospheric pressure and room temperature. It has a band gap of ∼2.3 eV and shows a semiconductor-metal transition at about 250˚C. The α-V<sub>2</sub>O<sub>5</sub> is lightly soluble in water (0.08 g/ml, 20˚C) but extremely soluble in acids. In particular it is physically and chemically stable in hot acid solutions. By increasing pressure and temperature, it is possible to improve the contact between the phases in the orthorhombic structure formed by VO<sub>5</sub> layers forming square pyramids that share edges and corners. In addition, the interaction between these layers is based on Van der Waals chemical bonds which favour growth of the planes along the [<xref ref-type="bibr" rid="scirp.70287-ref001">001</xref>] direction [<xref ref-type="bibr" rid="scirp.70287-ref21">21</xref>] - [<xref ref-type="bibr" rid="scirp.70287-ref23">23</xref>] .</p><p>Nowadays, several research groups have reported the partial or total use of the solvothermal method of synthesis because it is an easy route to the formation of vanadium oxides with different morphologies [<xref ref-type="bibr" rid="scirp.70287-ref24">24</xref>] - [<xref ref-type="bibr" rid="scirp.70287-ref33">33</xref>] . In this work we synthesized by a solvothermal method at low temperature monocrystalline α-V<sub>2</sub>O<sub>5</sub> nanowires with preferential [<xref ref-type="bibr" rid="scirp.70287-ref200">200</xref>] growth direction. In the solvothermal synthesis the oxidation states V<sup>5+</sup>, V<sup>4+</sup> and V<sup>3+</sup> were present. The presence of V<sup>4+</sup> ions in the material, promotes the growth of V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O nanobelts in metastable phase. However the metastable phases present in the V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O template are stabilized after applying a thermal process, which encourages and promotes formation of α-V<sub>2</sub>O<sub>5</sub> nanowires in an orthorhombic phase. With the aid of XRD, SEM and HRTEM we have studied the morphological changes and structural behavior during the formation of α-V<sub>2</sub>O<sub>5</sub> nanowires. The solvothermal chemical route seems optimal, since it is suitable for the synthesis of materials that decompose at elevated temperatures, which are poorly soluble, reactive, or for species with multiple oxidation states, as in the case of α-V<sub>2</sub>O<sub>5</sub> nanowires. A benefit of this method of synthesis is that one obtains very pure products at low temperature using only V<sub>2</sub>O<sub>5</sub> as starting material and hydrogen peroxide (H<sub>2</sub>O<sub>2</sub>) as solvent-oxidant agent. Furthermore, these α-V<sub>2</sub>O<sub>5</sub> nanowires can be doped with small ions, for example Li<sup>+</sup> ions by electrochemical methods, and subsequently can be used as electrodes in rechargeable lithium-ion nanobatteries.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Synthesis of Monocrystalline α-V<sub>2</sub>O<sub>5</sub> Nanowires</title><p>The synthesis of α-V<sub>2</sub>O<sub>5</sub> nanowires was performed using a solvothermal method similar to the one reported by Guicun Li et al. [<xref ref-type="bibr" rid="scirp.70287-ref34">34</xref>] . In a typical synthesis process, 0.18 g of V<sub>2</sub>O<sub>5</sub> powders (Aldrich, 99.99%) was dispersed into 30 ml of distilled with magnetic stirring (Nuova, SP18420-26Q) to form a yellow slurry solution with pH 4 (Oakton, pH/Ion 510). Then 2.5 ml of H<sub>2</sub>O<sub>2</sub> (Aldrich, 30 wt%) were added drop wise to the slurry solution and stirred to 100 rpm for 5 min to form an orange solution where the pH dropped to 0.5. The solution was directly poured into an acid digestion vessel of 45 ml capacity with Teflon a liner (Parr instruments, 4744). The closed acid digestion vessel was introduced into a furnace (Lindberg/Blue M, BF81894C-1) and was maintained at 180˚C for 48 h. Once the thermal treatment was over, the furnace was turned off and left to cool to room temperature. Green precipitates were obtained at the bottom of the container, which was surrounded by a colorless solution (reduction from V<sup>5+</sup> to V<sup>3+</sup>). The green precipitates were collected on a paper filter, washed several times with distilled water and finally dried at room temperature for 30 h. After this, the precipitates form a film and the surface color changed from a green (V<sup>3+</sup>) to a dark-blue (V<sup>4+</sup>). The dark-blue layer that forms on the film of the green precipitates suggests that the end products of the solvotermal synthesis are in a metastable phase (this hypothesis was confirmed by XRD and HRTEM analysis). Finally at atmospheric pressure and starting from room temperature the metastable film was heated on a hot plate to 80˚C in treatments of 4 h and 12 h long. The crystallographic evolution of the α-V<sub>2</sub>O<sub>5</sub> nanowires is presented in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Starting with V<sub>2</sub>O<sub>5</sub> in an orthorhombic phase and morphologically heterogeneous, we obtained one-dimensional structures in a metastable phase after the solvothermal synthesis due to the condensation of vanadic acid via homogeneous nucleation in the redox process and ending with α-V<sub>2</sub>O<sub>5</sub> nanowires in stable orthorhombic phase formed via dehydration of the one-dimensional structures in metastable phase.</p></sec><sec id="s2_2"><title>2.2. Structural Characterization</title><p>X-ray diffraction analysis (XRD) was performed using a D8-Advanced Bruker</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Simulation CaRIne V.3.1 of the synthesis of α-V<sub>2</sub>O<sub>5</sub> nanowires</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7701863x2.png"/></fig><p>diffractometer with CuKα monochromatic radiation (λ = 1.5405 &#197;, 2θ) using a Bragg- Brentano geometry. The samples for this analysis were subjected to slight mechanical milling. The XRD was refined using the Rietveld method and the FULLPROF program. The size of the structure was determined by the Debye Scherrer method. The morph- ological characterization of the products was studied by Scanning Electron Microscopy (SEM) with a microscope JEOL model JSM 7600F equipped with tungsten filament, operating at 20 kV and a pressure of 20 Pa and using the backscattered electron signal. For SEM analysis, the samples were directly placed on a specimen carrier and without adding any conductive layer. The High-Resolution Transmission Electron Microscopy (HRTEM) was done with a TITAN 80 - 300 microscope operating in the 80 - 300 kV range and a Tecnai G2-F30 operating at 300 kV. For the HRTEM observations, mechanically milled samples were deposited on the surface of a copper grid, previously coated with carbon and fomvar films.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><p>XRD patterns and SEM images obtained from the samples show the structural and morphological changes during the synthesis of the α-V<sub>2</sub>O<sub>5</sub> nanowires. In the <xref ref-type="fig" rid="fig2">Figure 2</xref>, the SEM images correspond to each of the patterns of X-ray diffraction of the samples in different reaction times. As shown by SEM, the V<sub>2</sub>O<sub>5</sub> reagent (Aldrich) is formed by agglomerates of morphologically heterogeneous grains with sizes 62.46 nm - 816.73 nm. In this case, the reflections in the XRD pattern (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)), are indexed as V<sub>2</sub>O<sub>5</sub> in orthorhombic phase (PDF 41-1426). The precipitates dried at room temperature for 30 h obtained after solvothermal synthesis at 180˚C for 48 h, XRD patterns show that the metastable film green-blue (V<sup>3+</sup>/V<sup>4+</sup>) is a mixture of vanadium oxides in different phases (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)).</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> XRD patterns and SEM images of vanadium oxide synthesized by solvothermal method at 180˚C for 48 h. (a) V<sub>2</sub>O<sub>5</sub> reagent (Aldrich), (b) V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O in metastable phase, (c) after the thermal process for 4 h, (d) after the thermal process for 12 h</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7701863x3.png"/></fig><p>The XRD patterns refined by Rietveld (<xref ref-type="fig" rid="fig3">Figure 3</xref>), determine that the metastable film is constituted by 66% of V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O in monoclinic phase (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)) with lattice parameters a = 11.70 &#197;, b = 3.63 &#197; and c = 29.06 &#197; (PDF 25-1006). In addition this analysis shows that the other 34% present in the metastable film, corresponds to the V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O oxide in orthorhombic phase (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)) with lattice parameters a = 9.34 &#197;, b = 17.00 &#197; and c = 3.62 &#197; (PDF 28-1433). SEM images shown that the bi-com- pound template of V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O is conformed by overlapping nanobelts, growing both on the surface and in the inside of the film. These one-dimensional structures have an average width of 209.55 nm and hundreds of micrometers long.</p><p>The color of the metastable V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O film (monoclinic and orthorhombic, respectively) changes from green-blue to yellow-pale after a thermal process at 80˚C at atmospheric pressure for 4 h, which causes the oxidation of the products to V<sup>5+</sup> and the stabilization partial of the phases. The XRD pattern (<xref ref-type="fig" rid="fig2">Figure 2</xref>(c)) shows reflections corresponding to a 92.8% V<sub>2</sub>O<sub>5</sub> in orthorhombic phase (α-V<sub>2</sub>O<sub>5</sub>), with lattice parameters a = 11.51 &#197;, b = 3.56 &#197; and c = 3.22 &#197;, indexed in agreement to the PDF 41-1426. However, we see the reflections due to the remnant of the V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O in monoclinic phase (PDF 25-1006). The smaller interplanar spacing is caused by the removal of water from the interlamellar region of V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O structure. SEM images show homogeneous α-V<sub>2</sub>O<sub>5</sub> nanowires measuring in average 111.90 nm in cross section and hundreds of micrometers long. After increasing the thermal process to 12 h, the color in the metastable film change from green-blue to orange, indicating the progress of oxidation state V<sup>5+</sup> in the material. The intensity of the diffractions peaks associated α-V<sub>2</sub>O<sub>5</sub> in stable orthorhombic phase increased with 95.8% of (<xref ref-type="fig" rid="fig2">Figure 2</xref>(d)) and clearly decreased by 4.2% the reflections associated to V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O in metastable monoclinic phase. The crystal structures of the α-V<sub>2</sub>O<sub>5</sub> nanowires are similar to that of the commercial V<sub>2</sub>O<sub>5</sub> powders (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)).</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> XRD pattern refined by Rietveld of metastable phase. (a) V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O monoclinic phase; (b) V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O orthorhombic phase</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7701863x4.png"/></fig><p>A probable process for the observed evolution of morphologies and crystal structures can be understood as follows: the process begins when vanadium salts are dissolved partially in distilled water; the metal cations (V<sup>5+</sup>) are solvated by molecules of water and the proposed reaction is (Equation (1)):</p><disp-formula id="scirp.70287-formula1"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7701863x5.png"  xlink:type="simple"/></disp-formula><p>For transition metal cations, charge transfer occurs from the σ orbitals of the water molecule to the empty metal d orbitals, this causes an increase in the acidity of the water [<xref ref-type="bibr" rid="scirp.70287-ref35">35</xref>] . The molecule is dissociating by the acid hydrolysis caused by the addition of H<sub>2</sub>O<sub>2</sub>. Therefore, the degree of acid hydrolysis is controlled by pH 0.5 in the precursor phase solution (Equation (2)).</p><disp-formula id="scirp.70287-formula2"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7701863x6.png"  xlink:type="simple"/></disp-formula><p>The electron transfer increases the charge on the molecule and weakens the OH bonds [<xref ref-type="bibr" rid="scirp.70287-ref36">36</xref>] - [<xref ref-type="bibr" rid="scirp.70287-ref39">39</xref>] . Applying pressure and temperature, monoperoxo and dimer species are then progressively formed as peroxo groups are decomposed (Equation (3)).</p><disp-formula id="scirp.70287-formula3"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7701863x7.png"  xlink:type="simple"/></disp-formula><p>The system redox efficiently promotes a molecular rearrangement due to the condensation of vanadic acid via a homogeneous nucleation into the reduction of V<sup>5+</sup> ions to V<sup>3+</sup> ions, resulting in a metastable crystalline structure V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O (hydrated bariandite) in monoclinic phase with one-dimensional growth (Equation (4)).</p><disp-formula id="scirp.70287-formula4"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7701863x8.png"  xlink:type="simple"/></disp-formula><p>The partial stability of these products in metastable phase is achieved naturally when oxidized by exposure to air in the process of washing and drying (partially oxidation of V<sup>3+</sup> to V<sup>4+</sup> ions), obtaining as final products, a mixture of vanadium oxide in different phase but with an one-directional growth (Equation (5)).</p><disp-formula id="scirp.70287-formula5"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7701863x9.png"  xlink:type="simple"/></disp-formula><p>With the thermal process of 4 and 12 h the phases in the metastable products V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O are stabilized removing the un-coordinated water molecules with metal centers V-O, giving rise to structures of V<sub>2</sub>O<sub>5</sub> nanowires in stable orthorhombic phase (Equation (6)).</p><disp-formula id="scirp.70287-formula6"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7701863x10.png"  xlink:type="simple"/></disp-formula><p>The HRTEM micrographs (<xref ref-type="fig" rid="fig4">Figure 4</xref>), show the variety of one-dimensional structures forming the metastable phase V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O template. These bi-com- pound nanobelts exhibit an average width of 125 - 250 nm and in some cases are core- shell types. On the other hand it is determined that the shell is not uniform in all cases; furthermore, it varies along the same nanobelt, which clearly indicates a non- uniform oxidation.</p><p>It is determined that the shell is constituted by the V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O oxide in orthorhombic phase with families of planes {200}, {200}, {101}, {230}, {120} and interplanar distances of 0.850 nm, 0.467 nm, 0.339 nm, 0.360 nm, 0.630 nm respectively (<xref ref-type="fig" rid="fig5">Figure 5</xref>).</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> TEM images of the V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O template in metastable phase. (a) Distribution to low-magnification; (b) Metastables structures to high-magnification; (c) and (d) Bi-compound nanobelts type core-shell</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7701863x11.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> HRTEM images of V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O shell</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7701863x12.png"/></fig><p>In the same way is established that the core corresponds to V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O in monoclinic phase which exhibits the families of planes {004}, {317} and {313} with d-spacing of 0.708 nm, 0.236 nm and 0.245 nm respectively (<xref ref-type="fig" rid="fig6">Figure 6</xref>). These results are consistent with those established by the XRD patterns corresponding to the analysis in the metastable phase.</p><p>With the thermal processes of 4 and 12 h the metastable phases in the one-dimen- sional V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O template are stabilized. The crystal structure corresponds to an orthorhombic phase, obtaining α-V<sub>2</sub>O<sub>5</sub> nanowires monocrystalline that are morphologically stable at atmospheric pressure and room temperature. As result the α-V<sub>2</sub>O<sub>5</sub> nanowires are monocrystalline, they have families of planes {200}, {310}, {110}, with d-spacing of 0.576 nm, 0.340 nm and 0.261 nm, respectively (<xref ref-type="fig" rid="fig7">Figure 7</xref>).</p></sec><sec id="s4"><title>4. Conclusion</title><p>We have obtained monocrystalline nanowires of α-V<sub>2</sub>O<sub>5</sub> in orthorhombic phase by a low temperature using a solvothermal synthesis, inducing a redox process controlled in the V<sub>2</sub>O<sub>5</sub> reagent grade and morphologically heterogeneous. These one-dimensional α-V<sub>2</sub>O<sub>5</sub> structures have lengths of tens of micrometers and widths of about 75 nm, with a preferential [<xref ref-type="bibr" rid="scirp.70287-ref200">200</xref>] growth direction. Into the solvothermal synthesis, the formation of α-V<sub>2</sub>O<sub>5</sub> nanowires is promoted by a template conformed of V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> HRTEM images of V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O core</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7701863x13.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> HRTEM images of α-V<sub>2</sub>O<sub>5</sub> nanowires 12 h</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7701863x14.png"/></fig><p>nanobelts in metastable phase. In addition, formation of V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O/V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O nanobelts in metastable phase depends strongly on the reaction conditions, like pH of the phase precursor solution, temperature into the acid digestion vessel, along with the time of the solvotermal reaction. It is determined that the bi-compound system in metastable phase may present core-shell type structures with average widths 209.55 nm and hundreds of micrometers long. Furthermore, the analysis presented identified the V<sub>10</sub>O<sub>24</sub>∙12H<sub>2</sub>O in monoclinic phase as the core, and the orthorhombic phase V<sub>3</sub>O<sub>7</sub>∙H<sub>2</sub>O as the shell. A thermal process stabilized metastable phases in the products in periods of 4 and 12 h. The influence of the time in the thermal process has a direct impact on the morphologies of the monocrystalline α-V<sub>2</sub>O<sub>5</sub> nanowires, which have wide applications in lithium-ion batteries.</p></sec><sec id="s5"><title>Acknowledgements</title><p>We acknowledge the financial support CONACYT N<sup>o</sup> 311298 and PAPIIT N<sup>o</sup> IN113411. The authors are also thankful to Laboratory of Microscopy facilities of the Mexican Petroleum Institute (IMP) and Crystal Structures Refinement Laboratory (LAREC) facilities of the Institute of Physics, UNAM and particularly to M. C. Manuel Aguilar for the XRD measurements.</p></sec><sec id="s6"><title>Cite this paper</title><p>Tafoya Ronquillo, M.L., Santiago Jacinto, P., Ovalle, P., Rend&#243;n V&#225;zquez, L., Chavira Mart&#237;nez, E., Marinero, E. and Garibay, V. (2016) Synthesis and Structural Characterization of Monocrystalline α-V<sub>2</sub>O<sub>5</sub> Nanowires. Materials Sciences and Applications, 7, 484-495. http://dx.doi.org/10.4236/msa.2016.79042</p></sec></body><back><ref-list><title>References</title><ref id="scirp.70287-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Alivisatos, A.P. (1996) Semiconductor Clusters, Nanocrystals, and Quantum Dots. Science, 271, 933-937. http://dx.doi.org/10.1126/science.271.5251.933</mixed-citation></ref><ref id="scirp.70287-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Liu, J., Li, Q., Wang, T., Yu, D. and Li, Y. (2004) Metastable Vanadium Dioxide Nanobelts: Hydrothermal Synthesis, Electrical Transport, and Magnetic Properties. Angewandte Chemie International Edition in English, 43, 5048-5052. http://dx.doi.org/10.1002/anie.200460104</mixed-citation></ref><ref id="scirp.70287-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Phetmung, H., Kim, T.W., Hwang, S.J. and Choy, J.H. 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