<?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.2015.63026</article-id><article-id pub-id-type="publisher-id">MSA-54468</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>
 
 
  Effect of Composition and Morphology on Sensor Properties of Aerosol Deposited Nanostructured ZnO+In&lt;SUB&gt;2&lt;/SUB&gt; O&lt;SUB&gt;3&lt;/SUB&gt; Films
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>eonid</surname><given-names>I. Trakhtenberg</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>Seyed</surname><given-names>M. Navid Khatami</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>Genrikh</surname><given-names>N. Gerasimov</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>Olusegun</surname><given-names>J. Ilegbusi</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Semenov Institute of Chemical Physics, Russian Academy of Sciences, Moscow, Russia</addr-line></aff><aff id="aff2"><addr-line>Department of Mechanical and Aerospace Engineering, University of Central Florida,
Orlando, FL, USA</addr-line></aff><aff id="aff1"><addr-line>Moscow Institute of Physics and Technology (State University), Moscow, Russia</addr-line></aff><pub-date pub-type="epub"><day>03</day><month>03</month><year>2015</year></pub-date><volume>06</volume><issue>03</issue><fpage>220</fpage><lpage>227</lpage><history><date date-type="received"><day>11</day>	<month>February</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>3</month>	<year>March</year>	</date><date date-type="accepted"><day>9</day>	<month>March</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The structural characteristics are investigated of nanoheterogeneous films comprising ZnO, 
  In<sub>2</sub> O<sub>3</sub> and ZnO + 
  In<sub>2</sub> O<sub>3</sub> composite produced by aerosol spray pyrolysis technique (SPT). The process utilizes water solutions of zinc chloride and indium nitrate precursors. The X-ray diffraction data show that the SPT process results in polycrystalline films of hexagonal wurtzite type ZnO, and 
  In<sub>2</sub> O<sub>3</sub> crystals of cubic structure. SPT-synthesized ZnO + 
  In<sub>2</sub> O<sub>3</sub>composites contain mixtures of these crystals. The morphology of the synthesized films is studied by scanning electron microscopy as well as the dependence of morphology on the synthesis conditions, specifically the temperature of the aerosol precipitation and the concentration of the precursors in solutions. The characteristics of nucleation and growth of oxide crystals during the synthesis of ZnO + 
  In<sub>2</sub> O<sub>3</sub> composite films are also considered. The film with the composition 25 wt% ZnO + 75 wt% 
  In<sub>2</sub> O<sub>3</sub> contains a large number of small crystal aggregates of arbitrary shape with a high density of contacts between the aggregates and are characterized by a homogeneous structure with high dispersion. Such morphology has high specific surface, which favors high sensory response. In addition, in this range of aggregate composition the relationship between the particles of the catalytically active component- ZnO, cleavage of hydrogen molecule, and 
  In<sub>2</sub> O<sub>3</sub>particles with a high concentration of conduction electrons is close to optimal for the maximum sensory effect in the detection of hydrogen.
 
</p></abstract><kwd-group><kwd>Nanoheterogenous Films</kwd><kwd> Nanocomposite Films</kwd><kwd> Mixed Metal Oxide Films</kwd><kwd> Aerosol Deposition</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Metal oxide semiconductor films are widely applied in gas sensors. The properties of such sensors including sensitivity, selectivity and response time depend critically on the film microstructure [<xref ref-type="bibr" rid="scirp.54468-ref1">1</xref>] . The structure in turn is largely determined by the synthesis. Such films are usually synthesized by a variety of techniques including Spray Pyrolysis Technique (SPT) [<xref ref-type="bibr" rid="scirp.54468-ref2">2</xref>] , sol-gel technique [<xref ref-type="bibr" rid="scirp.54468-ref3">3</xref>] , and chemical vapor deposition [<xref ref-type="bibr" rid="scirp.54468-ref4">4</xref>] .</p><p>A number of studies have shown that one promising approach to improve conductometric metal oxide sensors is to utilize semiconducting nanostructured composite materials consisting of metal oxides with different electronic structure and chemical properties [<xref ref-type="bibr" rid="scirp.54468-ref5">5</xref>] -[<xref ref-type="bibr" rid="scirp.54468-ref7">7</xref>] . It has been established that using a mixture of metal oxides, the resulting composite sensor material can achieve selectivity and sensitivity for gas detection in air ambience that far exceed those achievable with the individual constituent metal oxides of the composite [<xref ref-type="bibr" rid="scirp.54468-ref8">8</xref>] -[<xref ref-type="bibr" rid="scirp.54468-ref12">12</xref>] .</p><p>Studies of sensory phenomena in metal oxide composites have shown that there are certain optimum compositions for which these effects reach maximum values [<xref ref-type="bibr" rid="scirp.54468-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.54468-ref10">10</xref>] . One of the important factors that determine the dependence of sensory phenomena in metal oxide composites on composition is the effect of composition on the morphology of the sensor film. Therefore, it is important to clarify the morphological features of the composite sensors that exhibit high sensitivity. These features depend on the nature of the components of the mixed metal oxide composite and the processing conditions.</p><p>Of particular interest are composite sensor films processed by SPT due to the inherent advantages of the technique, including ease of control, low cost, and simplicity [<xref ref-type="bibr" rid="scirp.54468-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.54468-ref14">14</xref>] . The present study focuses on SPT-synthe- sized composite films of ZnO + In<sub>2</sub>O<sub>3</sub> and comparison with similar films of ZnO and In<sub>2</sub>O<sub>3</sub>. It also relatesthe morphology of the ZnO + In<sub>2</sub>O<sub>3</sub>composite films to the sensor response.</p></sec><sec id="s2"><title>2. Experimental Setup and Procedure</title><p>Water solutions of zinc chloride and indium nitrate were used to deposit ZnO and In<sub>2</sub>O<sub>3</sub> films by SPT. The ZnO + In<sub>2</sub>O<sub>3</sub>composites were synthesized by deposition of mixed solutions of different ratios between the concentrations (C) of the zinc chloride and indium nitrate precursors. The underlying chemical reactions of the SPT deposition can be expressed thus [<xref ref-type="bibr" rid="scirp.54468-ref15">15</xref>] :</p><disp-formula id="scirp.54468-formula426"><graphic  xlink:href="http://html.scirp.org/file/2-7701539x6.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54468-formula427"><graphic  xlink:href="http://html.scirp.org/file/2-7701539x7.png"  xlink:type="simple"/></disp-formula><p>The SPT setup utilized is illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref> [<xref ref-type="bibr" rid="scirp.54468-ref16">16</xref>] . A precursor solution which contains the constituent reactant compounds is atomized in a nozzle to tiny droplets which are then sprayed onto a preheated alumina substrate. The solutions are injected through a 1 mm-diameter round spray needle and then atomized at 1 bar air pressure [<xref ref-type="bibr" rid="scirp.54468-ref17">17</xref>] . It is important that the temperature of the substrate be maintained within a range that can initiate chemical reaction in the droplet. The droplet also must still contain enough reactants in solution after reaching the surface [<xref ref-type="bibr" rid="scirp.54468-ref18">18</xref>] . A film of stable compounds subsequently forms and adheres to the substrate due to chemical reaction and thermal decomposition of the solution.</p><p>The distance between the spray nozzle and the hot surface is kept constant at 10 cm during the experiments. This distance was chosen based on the results of a previous study [<xref ref-type="bibr" rid="scirp.54468-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.54468-ref19">19</xref>] . Finally, the thin film is annealed for 30 minutes after deposition to the desired structures at 450˚C. The annealing process promotes adhesion of the film to the substrate. These conditions are kept constant for all other sets of experiments performed.</p></sec><sec id="s3"><title>3. Morphology of Aerosol Deposited Sensor Films</title><p>The XRD patterns indicate that the SPT-synthesized ZnO films exhibit a polycrystalline hexagonal wurtzite structure while In<sub>2</sub>O<sub>3</sub> films have a polycrystalline cubic structure [<xref ref-type="bibr" rid="scirp.54468-ref10">10</xref>] . The XRD data also indicate that SPT- synthesized ZnO + In<sub>2</sub>O<sub>3</sub>composites consist of mixtures of these crystal structures.</p><p>The deposited thin films were also characterized by Scanning electron microscopy (SEM). Specifically, the surface morphology was characterized using a Zeiss ULTRA-55 FEG SEM system which used Schottky field emission source and STEM detector. The ZnO films were synthesized at different temperatures. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the SEM results at 350˚C indicating that at this temperature several small spherical particles are formed and agglomerate at the surface in the shape of powders with an average size of about 50 nm.</p><p>Keeping the concentration constant and increasing the deposition temperature, the results (not shown) indicate that dense ZnO oxide film is synthesized by the aerosol deposition at 400˚C. A further increase in temperature to 450˚C increases the film uniformity, but reduces its specific surface area which can adversely affect the sensor response of the film.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows the SEM micrographs of ZnO thin films synthesized at C = 0.2 mol/lit and C = 0.3 mol/lit. The results show that the grain size of the ZnO film increases with increase in the amount of precursor dissolved in solution.</p><p>The SEM micrograph for In<sub>2</sub>O<sub>3</sub> thin films deposited on Al<sub>2</sub>O<sub>3</sub> by SPT at 400˚C and precursor concentration C = 0.3 mol/lit is presented in <xref ref-type="fig" rid="fig4">Figure 4</xref>. It is evident that the particles of both the ZnO film shown in a previous <xref ref-type="fig" rid="fig3">Figure 3</xref>(b), as well as similar particlesof the SPT-synthesized In<sub>2</sub>O<sub>3</sub> film (<xref ref-type="fig" rid="fig4">Figure 4</xref>) are not separate crystallites, but are splices or aggregates of crystallites. An analogous structure has been observed for the particles of SnO<sub>2</sub>- based nanoheterogeneous film in a previous study [<xref ref-type="bibr" rid="scirp.54468-ref20">20</xref>] .</p><p>Thus, there are interparticle contacts of two types in the synthesized films: contacts between crystallites inside crystalline aggregates and contacts between aggregates. The contacts between aggregates of crystallites largely determine the conductivity of the nanocrystalline film [<xref ref-type="bibr" rid="scirp.54468-ref20">20</xref>] .</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Schematic sketch of chemical spray pyrolysis process</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7701539x8.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> SEM micrographs of ZnO thin films synthesized by spray pyrolysis on Al<sub>2</sub>O<sub>3</sub> substrate at 350˚C and precursor solution concentration C = 0.1 mol/lit</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7701539x9.png"/></fig><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> SEM micrographs of ZnO thin films on Al<sub>2</sub>O<sub>3</sub> substrate at T = 400˚C and different concentrations of precursor: (a) C = 0.2 mol/lit and (b) C = 0.3 mol/lit.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7701539x10.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7701539x11.png"/></fig></fig-group><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> SEM micrographs of In<sub>2</sub>O<sub>3</sub> thin films on Al<sub>2</sub>O<sub>3</sub> substrate at T = 400˚C and C = 0.3 mol/lit</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7701539x12.png"/></fig><p>Our study of SPT-processed ZnO + In<sub>2</sub>O<sub>3</sub>composite oxide films has demonstrated that the morphology of the films depends strongly on the composition. <xref ref-type="fig" rid="fig5">Figure 5</xref> presents the photomicrographs of the composite films with various ZnO to In<sub>2</sub>O<sub>3</sub> ratios. The composite film 0.25ZnO + 0.75In<sub>2</sub>O<sub>3</sub> (<xref ref-type="fig" rid="fig5">Figure 5</xref>(a)) consists of elongated particles of arbitrary shape, which are aggregates that combine small crystallites of In<sub>2</sub>O<sub>3</sub> and ZnO. The composite 0.8ZnO + 0.2In<sub>2</sub>O<sub>3</sub> (<xref ref-type="fig" rid="fig5">Figure 5</xref>(b)) contains for the most part faceted particles that are large individual ZnO crystals (or splices of such crystals).In this composite, such particles of ZnO are mixed with the In<sub>2</sub>O<sub>3</sub> particles, which other studies [<xref ref-type="bibr" rid="scirp.54468-ref10">10</xref>] have shown to also increase the sensory response by about 15-20% compared to the response of pure ZnO, i.e. considerably less than in the composite of <xref ref-type="fig" rid="fig5">Figure 5</xref>(a).</p></sec><sec id="s4"><title>4. Sensor Properties of Deposited Mixed Films</title><p>As indicated above, the particles in the films considered are crystal aggregates, which in the case of the composite sensor consist of a mixture of nanocrystals of In<sub>2</sub>O<sub>3</sub> and ZnO closely interacting with each other. In order to describe the sensor phenomenon, it is necessary to first consider the concentration of conduction electrons and the sensory effect in an isolated nanocrystal line aggregate of the film.</p><p>The conductivity of the isolated composite aggregate of ZnO + In<sub>2</sub>O<sub>3</sub> is determined by the In<sub>2</sub>O<sub>3</sub>nanocrystals, since the concentration of conduction electrons in the ZnO crystals (10<sup>16</sup> - 10<sup>17</sup> cm<sup>−3</sup>) [<xref ref-type="bibr" rid="scirp.54468-ref21">21</xref>] is three to four orders of magnitude lower than in the In<sub>2</sub>O<sub>3</sub> crystals. The concentration of conduction electrons in the In<sub>2</sub>O<sub>3</sub> crystals drops sharply under the influence of atmospheric oxygen, which is chemisorbed on the surface of the crystals, capturing electrons from the conduction band of In<sub>2</sub>O<sub>3</sub> to form O<sup>−</sup> anion radicals [<xref ref-type="bibr" rid="scirp.54468-ref22">22</xref>] . Sensory response is mani-</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> SEM micrographs of ZnO + In<sub>2</sub>O<sub>3</sub> thin films on Al<sub>2</sub>O<sub>3</sub> substrate at ratios of (a) 0.25ZnO + 0.75In<sub>2</sub>O<sub>3</sub> and (b) 0.8ZnO + 0.2In<sub>2</sub>O<sub>3</sub> at T = 400˚C and total concentration of two precursors 0.1 mol/lit.</title></caption><fig id ="fig5_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7701539x13.png"/></fig><fig id ="fig5_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7701539x14.png"/></fig></fig-group><p>fested as an increase in conductivity due to the sensor reaction of the chemisorbed oxygen anions with hydrogen and the corresponding return of the electrons to the conduction band. The sensory reaction proceeds with participation of the H atoms [<xref ref-type="bibr" rid="scirp.54468-ref23">23</xref>] , formed by the catalytic dissociation of molecular hydrogen.</p><p>A characteristic of the sensor response of ZnO + In<sub>2</sub>O<sub>3</sub> aggregates to hydrogen in air is that in these composite aggregates, the In<sub>2</sub>O<sub>3</sub> nanocrystals having high concentration of the conduction electrons (about 10<sup>19</sup> - 10<sup>20</sup> cm<sup>−3</sup>) [<xref ref-type="bibr" rid="scirp.54468-ref24">24</xref>] , are in contact with the ZnOn anocrystals, which exhibit high catalytic activity in the reaction of hydrogen dissociation [<xref ref-type="bibr" rid="scirp.54468-ref25">25</xref>] . The contacts between In<sub>2</sub>O<sub>3</sub> and ZnO crystals in a composite aggregate provide particularly favorable conditions for the sensor response of the aggregate to hydrogen in air: dissociation of hydrogen proceeds at the surface of the ZnO crystals with high catalytic cactivity in this reaction while the Hatoms formed on the surface of these crystal sreact with the O<sup>−</sup> onthesurfaceofIn<sub>2</sub>O<sub>3</sub>crystals, thereby increasing the concentration of conducting electrons in the aggregate.</p><p>The effect of ZnO on sensory response reaches a maximum value at ZnO composition of about 20%, when almost all of the In<sub>2</sub>O<sub>3</sub>crystallites are in contact with the ZnO crystallites [<xref ref-type="bibr" rid="scirp.54468-ref10">10</xref>] . The 0.25ZnO + 0.75In<sub>2</sub>O<sub>3</sub> composite film (<xref ref-type="fig" rid="fig5">Figure 5</xref>(a)) has demonstrated sensor response to hydrogen in air close to the maximum, which is 1.7 times the sensor response of pure ZnO films and 4 times the sensor response of pure In<sub>2</sub>O<sub>3</sub> films [<xref ref-type="bibr" rid="scirp.54468-ref10">10</xref>] . A further increase in the composition of ZnO decreases the sensor response due to reduction of the concentration of conduction electrons in the ZnO + In<sub>2</sub>O<sub>3</sub>composite.</p><p>Under the influence of ambient hydrogen, the equilibrium concentration of conduction electrons inside the isolated ZnO + In<sub>2</sub>O<sub>3</sub> composite aggregate decreases much faster than the equilibrium concentration in the system of such units in contact. Therefore, the quasi-wire small aggregate shown in the previous <xref ref-type="fig" rid="fig5">Figure 5</xref>(a) can be considered as the basic structure and sensor unit of the film. The resistance and sensor response of the film depend on the characteristics of such units as well as on the density of contacts between the aggregates in the film [<xref ref-type="bibr" rid="scirp.54468-ref20">20</xref>] . These parameters therefore increase with decreasing size of aggregates and corresponding increase of their concentration in the film.</p><p>The crystallite sizes of In<sub>2</sub>O<sub>3</sub> and ZnO, as well as the size and shape of the aggregates formed from these crystallites are determined by the deposition of the film. It should be noted that the In<sub>2</sub>O<sub>3</sub> crystallizes in the form of cubic crystals, which can have three types of cells that differ in the mutual arrangement of the atoms and the interatomic bonds [<xref ref-type="bibr" rid="scirp.54468-ref26">26</xref>] . The complexity of the In<sub>2</sub>O<sub>3</sub> lattice influences the properties of the crystals (in particular, lattice thermal conductivity [<xref ref-type="bibr" rid="scirp.54468-ref27">27</xref>] ) and hinders the growth of crystals during the deposition of In<sub>2</sub>O<sub>3</sub> from aerosol. This explains the finding in a previous <xref ref-type="fig" rid="fig4">Figure 4</xref> that SPT-synthesized In<sub>2</sub>O<sub>3</sub> film comprises of splices of particles of arbitrary shape. In contrast, ZnO film consists of large-grained crystalline particles. It is also significant that in contrast to In<sub>2</sub>O<sub>3</sub>, ZnO crystallizes with a hexagonal structure [<xref ref-type="bibr" rid="scirp.54468-ref28">28</xref>] , such that the interaction between these oxides during the SPT-deposition of ZnO + In<sub>2</sub>O<sub>3</sub>composite film should create additional hindrance to the growth of crystals.</p><p>As a result, the rate of nucleation may be greater than the rate of crystal growth. This may cause the formation of a large number of small crystals, which combine into the aggregates. Perhaps the nature of crystallization during deposition of ZnO + In<sub>2</sub>O<sub>3</sub>composite sensor films with a high composition of In<sub>2</sub>O<sub>3</sub> is responsible for the formation of a large number of composite aggregates of small size, shown previously in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a). The shape of these aggregates indicates deformation of aggregates in the course of their formation, which may also be explained by the hindrance to the growth of crystals in the composite. As shown in the photomicrographs of the composite films with various ZnO to In<sub>2</sub>O<sub>3</sub>ratios (<xref ref-type="fig" rid="fig5">Figure 5</xref>), the composite films composed of 0.25ZnO + 0.75In<sub>2</sub>O<sub>3</sub> besides their essential sensory properties [<xref ref-type="bibr" rid="scirp.54468-ref29">29</xref>] , are characterized by a homogeneous dispersive structure with high specific surface. Thus, not only the electronic structure, but also the morphological properties of the film composition 0.25ZnO + 0.75In<sub>2</sub>O<sub>3</sub> with high density of contacts between crystal aggregates provides enhanced sensory effect in the detection of hydrogen in air ambience.</p></sec><sec id="s5"><title>5. Conclusions</title><p>Three types of films comprising ZnO, In<sub>2</sub>O<sub>3</sub> and ZnO + In<sub>2</sub>O<sub>3</sub> composite were produced by spray pyrolysis technique (SPT) using water solutions of zinc chloride and indium nitrate precursor. The polycrystalline films obtained contain hexagonal wurtzite-type ZnO crystals and cubic In<sub>2</sub>O<sub>3</sub> crystals. The study also considered the dependence of the morphology of the films on the synthesis conditions. It has been shown that increasing the deposition temperature in the range 350˚C to 450˚C results in the formation of films with more uniform particle sizes and the size of deposited particles increases with increasing concentration of precursor solution from 0.1 to 0.3 mol/liter. The particles of the film are not separate crystallites, but splices or aggregates of crystallites. The interaction between crystallites inside crystalline aggregates is stronger that the interaction between aggregates. The conductivity of the film is determined by the electron density in an aggregate and the contacts between aggregates.</p><p>The morphology of the ZnO + In<sub>2</sub>O<sub>3</sub> composite films depends strongly on the composition of the film. It is shown that the film of composition 25 wt% ZnO + 75 wt% In<sub>2</sub>O<sub>3</sub> contains a large number of small crystal aggregates of arbitrary shape and therefore has a high density of contacts between the aggregates. It should be emphasized that only the films with good homogeneous structure demonstrated high sensory properties. In this range of aggregate composition, the relationship between the particles of the catalytically active component (ZnO) that breaks hydrogen molecules and In<sub>2</sub>O<sub>3</sub> particles with a high concentration of conduction electrons is close to optimal value. Therefore, due to both morphology and electronic structure of the films of this composition, the sensor response to hydrogen in air ambience is able to reach the maximal value.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The project was supported by the National Science Foundation under grant number CMMI-1030689 and the Russian Scientific Foundation grant No. 14-19-00781.</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.54468-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kruis, F.E., Fissan, H. and Peled, A. (1998) Synthesis of Nanoparticles in the Gas Phase for Electronic, Optical and Magnetic Applications—A Review. Journal of Aerosol Science, 29, 511-535. http://dx.doi.org/10.1016/S0021-8502(97)10032-5</mixed-citation></ref><ref id="scirp.54468-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Perednis, D. and Gauckler, L.J. 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