<?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">ANP</journal-id><journal-title-group><journal-title>Advances in Nanoparticles</journal-title></journal-title-group><issn pub-type="epub">2169-0510</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/anp.2016.51013</article-id><article-id pub-id-type="publisher-id">ANP-63667</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Chemistry&amp;Materials Science</subject><subject> Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Synthesis and Characterisation of In&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt; Na-noparticles from &lt;i&gt;Astragalus gummifer&lt;/i&gt;
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>anchana</surname><given-names>Latha Chitturi</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>Aparna</surname><given-names>Yaramma</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>Ramchander</surname><given-names>Merugu</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>Ravinder</surname><given-names>Dachepalli</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>Jaipal</surname><given-names>Kandhadi</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Bio Chemistry, Mahatma Gandhi University, Nalgonda, India</addr-line></aff><aff id="aff1"><addr-line>Department of Physics, JNTUH, CEH, Kukatpally, Hyderabad, India</addr-line></aff><aff id="aff4"><addr-line>Inorganic and Physical Chemistry Division, Indian Institute of Chemical Technology, Hyderabad, India</addr-line></aff><aff id="aff3"><addr-line>Department of Physics, Osmania University, Hyderabad, India</addr-line></aff><pub-date pub-type="epub"><day>04</day><month>02</month><year>2016</year></pub-date><volume>05</volume><issue>01</issue><fpage>114</fpage><lpage>122</lpage><history><date date-type="received"><day>21</day>	<month>October</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>20</month>	<year>February</year>	</date><date date-type="accepted"><day>23</day>	<month>February</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>
 
 
  Exploitation of green chemistry approach for the synthesis of Indium Oxide nanoparticles using green synthesis has received a great attention in the field of nanotechnology. To demonstrate a biogenic method that involves the Katira gum (Astragalus gummifer) leading to the formation of different morphological In
  <sub>2</sub>O
  <sub>3</sub> using the precursor Indium (III) Acetylacetonate and TG-DTA is characterised for calcination temperature and it is found to be above 500
  ℃. Different techniques such as XRD, UV-VIS, SEM and EDAX have been used for the characterisation of In
  <sub>2</sub>O
  <sub>3</sub> nanoparticles. The average crystallite size of Indiumoxide nanoparticles is determined as 19 nm by using Scherrer’s Equation and PSA and studying optical properties.
 
</p></abstract><kwd-group><kwd>In&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt; Nanoparticles</kwd><kwd> Bio Synthesis</kwd><kwd> XRD</kwd><kwd> UV-Vis</kwd><kwd> SEM and EDAX</kwd><kwd> PSA</kwd><kwd> RAMAN FTIR and PL</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>These days nanotechnology is one of the important research fields. For several years, scientists have constantly explored different bio synthetic methods to synthesize nanoparticles. The gum mediated synthesis of nanoparticles is eco friendly, efficient and easier when compared to chemical mediated or microbe mediated synthesis. For the production of nanoparticles plant extract is an alternative method to chemical and physical methods and it eliminates the elaborate process of maintaining cell cultures.</p><p>Among the many transparent conducting oxide materials like SnO<sub>2</sub>, Indium oxide is physically stable chemically inert and hence it is superior for applications in several aspects. Usually, Indium oxide crystallizes into a cubic bixbyite structure with a melting point temperature of 1910˚C. It is highly conductive and exhibits a direct band gap between 3.55 and 3.75 eV, which is an unusual property for wide band gap material. Indium Oxide also has very interesting optical properties. It absorbs IR light waves beyond 900 nm and transmits visible light of wave length 400 to 700 nm. It has interesting properties such as high transparency to high electrical conductance, visible light and strong interaction between certain poisonous gas molecules and its surfaces [<xref ref-type="bibr" rid="scirp.63667-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.63667-ref3">3</xref>] . Indium Oxide with these properties makes an interesting material for various applications, including solar cells [<xref ref-type="bibr" rid="scirp.63667-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref2">2</xref>] , Panel Displays [<xref ref-type="bibr" rid="scirp.63667-ref4">4</xref>] , Organic Light Emitting Diodes [<xref ref-type="bibr" rid="scirp.63667-ref5">5</xref>] , Photo Catalysts [<xref ref-type="bibr" rid="scirp.63667-ref6">6</xref>] , Architectural Glasses [<xref ref-type="bibr" rid="scirp.63667-ref7">7</xref>] , Field Emission [<xref ref-type="bibr" rid="scirp.63667-ref8">8</xref>] . Moreover, Indium Oxide is an important material for Semiconductor Gas Sensors [<xref ref-type="bibr" rid="scirp.63667-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.63667-ref14">14</xref>] . Recently, investigations on preparation of Indium Oxide nano structures with various forms such as Nantubes [<xref ref-type="bibr" rid="scirp.63667-ref15">15</xref>] , Nanobelts [<xref ref-type="bibr" rid="scirp.63667-ref16">16</xref>] -[<xref ref-type="bibr" rid="scirp.63667-ref18">18</xref>] , Nanofibers [<xref ref-type="bibr" rid="scirp.63667-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref20">20</xref>] , Nanowires [<xref ref-type="bibr" rid="scirp.63667-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref21">21</xref>] -[<xref ref-type="bibr" rid="scirp.63667-ref26">26</xref>] and Nanoparticles [<xref ref-type="bibr" rid="scirp.63667-ref27">27</xref>] -[<xref ref-type="bibr" rid="scirp.63667-ref29">29</xref>] have been widely emphasised to extend their technological usages. Nanoparticulate form of Indium Oxide nanostructures has been used as a promising material for gas sensor applications. Tragacanth is a natural gum (Botanical name Astragalus gummifer) obtained from the dried sop of several species of Middle Eastern legumes of the genus Astragalus. It is tasteless, odourless and viscous and is obtained from the root of the plant and dried. The gum comes from a thorny shrub. It has been used as treatment for burns, cough, texturant additive and also as a binder to hold all the powdered herbs together.</p></sec><sec id="s2"><title>2. Experimental</title><p>For the preparation of Indium Oxide nanoparticles, the chemical materials used were Indium (III) Acetylacetonate (99.99+% purity, Sigma Aldrich) and Astragalus gummifer (Katira Gum) bought from local Unani (davaasaas) Shop. The Astragalus gummifer (0.05 gm) and Indium (III) Acetylacetonate (0.4 gm) were mixed and crushed into fine powder using mortar and pistle. The precursor was characterised by TG-DTA to determine the calcination temperature and is found to be above 450˚C (<xref ref-type="fig" rid="fig2">Figure 2</xref>). Then the precursor was calcined in box furnace at 500˚C for 2 hours in air. The yellowish nano-powder of In<sub>2</sub>O<sub>3</sub> as described in (<xref ref-type="fig" rid="fig1">Figure 1</xref>) was obtained.</p>Physical Characterization<p>The precursor was characterised by TG-DTA (HITACHI Spectrophotometer) to determine the thermal decomposition and crystallite temperature was found to be at 500˚C (<xref ref-type="fig" rid="fig2">Figure 2</xref>). The dried precursor was ground and</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Flow chart of preparation of In<sub>2</sub>O<sub>3</sub> nanoparticles</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x7.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> TG-DTA curves of thermal decompositia of In<sub>2</sub>O<sub>3</sub> precursorat a heating rate of 10˚C/min in static air</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x8.png"/></fig><p>subsequently calcined in box furnace at 500˚C for 2 hours in air. The dried precursor and calcined samples of In<sub>2</sub>O<sub>3</sub> were characterised for crystal phase identification by powder XRD using with Cuk<sub>α</sub> radiation (λ = 0.15406 nm). The optical absorption spectra were measured in the range of 200 - 800 nm using UV-Vis scanning spectrometer. Photo Luminiscence (PL) measurement was carried on a luminescence spectrometer with xenon lamp as the excitation source at 25˚C temperature. The samples were dispersed in using ethanol and the excitation wave length used in PL measurement was 353 nm.</p></sec><sec id="s3"><title>3. Results &amp; Discussion</title><sec id="s3_1"><title>3.1. TG-DTA Analysis</title><p>The TG-DTA analysis curves of as prepared In<sub>2</sub>O<sub>3</sub> precursor are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. The TG curve in <xref ref-type="fig" rid="fig2">Figure 2</xref> shows a major weight loss step from 200˚C up to about 350˚C. The major weight loss is due to the combustion of organic matter (CO and OH groups) present in the precursor and slight weight loss (combustion of remaining carbonyl group) was observed at 470˚C. On the DTA curve (<xref ref-type="fig" rid="fig2">Figure 2</xref>) a main exothermic effect was observed between 300˚C and 400˚C with maximum at about 320˚C indicating that the thermal events can be due to the burning of organic species in the precursor powders from the amorphous component.</p></sec><sec id="s3_2"><title>3.2. XRD Analysis</title><p>The formation of nano crystalline In<sub>2</sub>O<sub>3</sub> as decomposition product was confirmed by XRD pattern in <xref ref-type="fig" rid="fig3">Figure 3</xref>. All of the detectable peaks (<xref ref-type="fig" rid="fig3">Figure 3</xref>) can be indexed as the In<sub>2</sub>O<sub>3</sub> cubic structure in the Standard Data (JCPDS: 06-0416). The cubic lattice parameter “a” can be calculated from the XRD spectra is 10.222 &#197; which is close to those of lattice constants α = 0.32488 nm and C = 0.52066 nm in the Standard Data (JCPDS: 06-0416). The crystallite sizes of the powders were estimated from X-ray line broadening using Scherrer’s Equation [<xref ref-type="bibr" rid="scirp.63667-ref30">30</xref>] (i.e., D = 0.89λ/βCosθ), where λ is the wavelength of the X-ray radiation, k is a constant taken as 0.89, 2θ is the diffraction angle (30.286˚), β is the Full Width at Half Maximum (FWHM = 0.4723) and is obtained to be 19.25 nm for In<sub>2</sub>O<sub>3</sub> sample calcined at 500˚C. The particle size and lattice parameter of In<sub>2</sub>O<sub>3</sub> sample is summarised in <xref ref-type="table" rid="table1">Table 1</xref>.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> XRD pattern of nano crystalline In<sub>2</sub>O<sub>3</sub> sample calcined in air for 2 hours at 500˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x9.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> In<sub>2</sub>O<sub>3</sub> nano crystalline sample from different characterisations data</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Average Particle size (nm) from XRD</th><th align="center" valign="middle"  rowspan="2"  >Cubic lattice parameter a (nm)</th><th align="center" valign="middle"  rowspan="2"  >Morphology from SEM</th><th align="center" valign="middle"  colspan="2"   rowspan="2"  >Estimated Band gap UV PL</th><th align="center" valign="middle"  rowspan="2"  >PSA</th><th align="center" valign="middle"  colspan="2"  >EDAX</th></tr></thead><tr><td align="center" valign="middle" >Atomic %</td><td align="center" valign="middle" >Weight %</td></tr><tr><td align="center" valign="middle" >19.25 nm</td><td align="center" valign="middle" >1.0222 nm</td><td align="center" valign="middle" >Spherical</td><td align="center" valign="middle" >3.86 eV</td><td align="center" valign="middle" >3.51 eV</td><td align="center" valign="middle" >24 nm</td><td align="center" valign="middle" >O/In = 2.2</td><td align="center" valign="middle" >93</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap></sec><sec id="s3_3"><title>3.3. EDAX &amp; SEM Analysis</title><p>The SEM images in <xref ref-type="fig" rid="fig4">Figure 4</xref> showed that the In<sub>2</sub>O<sub>3</sub> nanoparticles are formed as cubic crystals. However, the particle size as well as agglomeration increased and the smaller grains coalesced to form larger size particles [<xref ref-type="bibr" rid="scirp.63667-ref31">31</xref>] . The EDAX data at 500˚C sintering temperature suggested the stoichiometry of In<sub>2</sub>O<sub>3</sub> nanoparticles with the elemental composition of oxygen and Indium and their atomic and weight percentages are given <xref ref-type="table" rid="table1">Table 1</xref>. The atomic ratio of (O/In) calculated as 2.2 indicated the stoichiometric composition of In<sub>2</sub>O<sub>3</sub> which is in good agreement with the theoretical value of 1.5.</p></sec><sec id="s3_4"><title>3.4. PSA Analysis</title><p>The average particle size of the In<sub>2</sub>O<sub>3</sub> nanoparticle from the particle size analyzer, as in <xref ref-type="fig" rid="fig5">Figure 5</xref>, was found to be 24 nm as shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p></sec><sec id="s3_5"><title>3.5. RAMAN Studies</title><p>The In<sub>2</sub>O<sub>3</sub> Raman spectrum (<xref ref-type="fig" rid="fig6">Figure 6</xref>) shows the expected vibrational modes at 109,475 cm<sup>−</sup><sup>1</sup>, which in turn is an unambiguous signature of the cubic In<sub>2</sub>O<sub>3</sub> structure [<xref ref-type="bibr" rid="scirp.63667-ref32">32</xref>] . The higher frequency (1500 cm<sup>−</sup><sup>1</sup>) is due to super position of the contribution of the In-O vibration modes with frequency 630 cm<sup>−</sup><sup>1</sup>. The intensity peaks which are known to be related to the pure In<sub>2</sub>O<sub>3</sub> vibrational modes which confirm the In<sub>2</sub>O<sub>3</sub> cubic like feature.</p></sec><sec id="s3_6"><title>3.6. FTIR Analysis</title><p>The IR spectra of In<sub>2</sub>O<sub>3</sub> indicating that the bands around 3506 cm<sup>−</sup><sup>1</sup> and 1623 cm<sup>−</sup><sup>1</sup> are attributed to the absorptions of hydroxyls from absorbed water or alcohols and those at 1416 cm<sup>−</sup><sup>1</sup> can be ascribed to the C-H vibrations of the organics in <xref ref-type="fig" rid="fig7">Figure 7</xref>. The band at 1050 cm<sup>−</sup><sup>1</sup> is due to C-O vibrations. While the absorptions around 1500 cm<sup>−</sup><sup>1</sup> are due to the In-O vibrations [<xref ref-type="bibr" rid="scirp.63667-ref33">33</xref>] . The weak absorption at 1568 cm<sup>−</sup><sup>1</sup> is due to C-O vibrations from the</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> EDAX &amp; SEM images of the nano crystalline In<sub>2</sub>O<sub>3</sub> sample</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x10.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Particle size analysis of the nano crystalline In<sub>2</sub>O<sub>3</sub> sample</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x11.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Raman Spectra of nanocrystalline In<sub>2</sub>O<sub>3</sub> sample calcined in air for 2 hours at 500˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x12.png"/></fig><p>Acetylacetone species [<xref ref-type="bibr" rid="scirp.63667-ref34">34</xref>] . The results indicate the presence of few acetyl acetone species on the surface species of the In<sub>2</sub>O<sub>3</sub> nanocrystals.</p></sec><sec id="s3_7"><title>3.7. UV-Vis Absorbance</title><p>Now let us consider the optical properties of the In<sub>2</sub>O<sub>3</sub> samples. The UV-visible absorption spectra of all the In<sub>2</sub>O<sub>3</sub> samples (<xref ref-type="fig" rid="fig8">Figure 8</xref>) exhibit a strong absorption below 450 nm (2.7 eV) with a well defined absorbance peak at around 320 nm (3.88 eV). This value is greater than that of 3.6 eV for the In<sub>2</sub>O<sub>3</sub> reported in the literature [<xref ref-type="bibr" rid="scirp.63667-ref2">2</xref>] .</p></sec><sec id="s3_8"><title>3.8. PL Spectrum</title><p><xref ref-type="fig" rid="fig9">Figure 9</xref> shows the room temperature PL spectra of the nanocrystalline In<sub>2</sub>O<sub>3</sub> samples measured using a</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> FTIR nano-crystalline In<sub>2</sub>O<sub>3</sub> sample calcined in air at 500˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x13.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Room temperature optical absorbance spectra of nano crystalline In<sub>2</sub>O<sub>3</sub> sample calcined in air for 2 hours at 500˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x14.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Room temperature photo luminescence spectra of the synthesized nano crystalline In<sub>2</sub>O<sub>3</sub> sample calcined in air for 2 hours at 500˚C</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/13-2610188x15.png"/></fig><p>Xenon laser of 270 nm as an excitation source. The spectra of all the samples mainly consist of a strong UV emission broad band having emission maximum at ~353 nm (3.51 eV). It is well known that the bulk In<sub>2</sub>O<sub>3</sub> cannot emit light at room temperature [<xref ref-type="bibr" rid="scirp.63667-ref38">38</xref>] . However PL emissions of our nano crystalline In<sub>2</sub>O<sub>3</sub> samples are possibly due to the effect of the oxygen vacancies as reported in literatures [<xref ref-type="bibr" rid="scirp.63667-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref36">36</xref>] - [<xref ref-type="bibr" rid="scirp.63667-ref38">38</xref>] . In the present work, oxygen vacancies would generally act as deep defect donors and cause the formation of new energy levels in the band gap of In<sub>2</sub>O<sub>3</sub> samples. Thus the PL emission from In<sub>2</sub>O<sub>3</sub> nanoparticles results from the radiative recombination of electron occupying oxygen vacancies with a photo excited hole which is analogous to the photo luminescence mechanism of ZnO and SnO<sub>2</sub> semi conductors [<xref ref-type="bibr" rid="scirp.63667-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.63667-ref38">38</xref>] .</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>We have synthesized nanoparticles of In<sub>2</sub>O<sub>3</sub> by a green method using Astragalus gummifer. Structural, morphological chemical composition and optical properties of the green synthesized nanoparticles were characterised. XRD, RAMAN, SEM analysis showed that the In<sub>2</sub>O<sub>3</sub> samples were cubic with particle size of 19 nm. The morphology and size of In<sub>2</sub>O<sub>3</sub> materials were affected by the calcination temperature. The prepared In<sub>2</sub>O<sub>3</sub> nanoparticles showed a strong PL emission in the UV region. The strong emissions of In<sub>2</sub>O<sub>3</sub> are attributed to the radiative recombination of electron occupying oxygen vacancies with a photo excited hole.</p></sec><sec id="s5"><title>Cite this paper</title><p>Kanchana LathaChitturi,AparnaYaramma,RamchanderMerugu,RavinderDachepalli,JaipalKandhadi, (2016) Synthesis and Characterisation of In<sub>2</sub>O<sub>3</sub> Na-noparticles from Astragalus gummifer. Advances in Nanoparticles,05,114-122. doi: 10.4236/anp.2016.51013</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.63667-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hamburg, I. and Granqvist, C.G. 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