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<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">MNSMS</journal-id>
      <journal-title-group>
        <journal-title>Modeling and Numerical Simulation of Material Science</journal-title>
      </journal-title-group>
      <issn pub-type="epub">2164-5345</issn>
      <publisher>
        <publisher-name>Scientific Research Publishing</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.4236/mnsms.2017.74004</article-id>
      <article-id pub-id-type="publisher-id">MNSMS-80922</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>


          The Influence of PbI&lt;sub&gt;2&lt;/sub&gt; on Characteristic of Organic-Inorganic Hybrid Perovskite Thin Films

        </article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" xlink:type="simple">
          <name name-style="western">
            <surname>Yuze</surname>
            <given-names>Peng</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">
            <sup>1</sup>
          </xref>
          <xref ref-type="corresp" rid="cor1">
            <sup>*</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author" xlink:type="simple">
          <name name-style="western">
            <surname>Yuxiang</surname>
            <given-names>Wu</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>Linlin</surname>
            <given-names>Tang</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>Juan</surname>
            <given-names>Li</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>Jian</surname>
            <given-names>Xu</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>Yangyang</surname>
            <given-names>Du</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>Like</surname>
            <given-names>Huang</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>Hongkun</surname>
            <given-names>Cai</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>Jian</surname>
            <given-names>Ni</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>Jianjun</surname>
            <given-names>Zhang</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">
            <sup>1</sup>
          </xref>
        </contrib>
      </contrib-group>
      <aff id="aff1">
        <addr-line>Institute of Photo-Electronics, Nankai University, The Tianjin Key Laboratory for Optical-Electronic Thin Film Devices and Tech-nology, Tianjin, China</addr-line>
      </aff>
      <author-notes>
        <corresp id="cor1">
          * E-mail:<email>253770159@qq.com(YP)</email>;
        </corresp>
      </author-notes>
      <pub-date pub-type="epub">
        <day>06</day>
        <month>12</month>
        <year>2017</year>
      </pub-date>
      <volume>07</volume>
      <issue>04</issue>
      <fpage>47</fpage>
      <lpage>57</lpage>
      <history>
        <date date-type="received">
          <day>1,</day>
          <month>October</month>
          <year>2017</year>
        </date>
        <date date-type="rev-recd">
          <day>28,</day>
          <month>October</month>
          <year>2017</year>
        </date>
        <date date-type="accepted">
          <day>31,</day>
          <month>October</month>
          <year>2017</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>


          Organic-inorganic hybrid perovskite materials have attracted significant research efforts because of their outstanding properties. Meanwhile the crystallization of organic-inorganic hybrid perovskite materials can significantly influence the films quality. Here, we research the influence of the characteristics of PbI
          <sub>2</sub>
          thin film on final perovskite films and the mechanisms of film formation based on the two-step sequential deposition method. We found that the characteristics of PbI
          <sub>2</sub>
          thin film, such as the grain size, the grain shape, the surface roughness and the film densification, have significant effects on the final perovskite films due to different film crystallization process. According to the analysis on the characteristics of the perovskite films obtained from different PbI
          <sub>2</sub>
          precursor, we suggested that the formation of perovskite film begins from the PbI
          <sub>2</sub>
          crystals expanding when they are converted to MAPbI
          <sub>3 </sub>
          perovskite by migration of MA+ cations from the grain boundaries.

        </p>
      </abstract>
      <kwd-group>
        <kwd>Perovskite</kwd>
        <kwd> Film Formation</kwd>
        <kwd> Grain Characteristics</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="s1">
      <title>1. Introduction</title>
      <p>
        Organic-inorganic hybrid perovskite materials have attracted substantial attention because of their excellent physical properties [<xref ref-type="bibr" rid="scirp.80922-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref5">5</xref>] , which enable them to be employed in solar cells and other application, such as LED. These materials show remarkable optical absorptions across a wide range of the solar spectrum, and a sharp optical band edge, which suggests low levels of disorder [<xref ref-type="bibr" rid="scirp.80922-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref7">7</xref>] . They also exhibit long charge-carrier diffusion lengths (&gt;1 mm) relative to the absorption depth of incident light (~100 nm), [<xref ref-type="bibr" rid="scirp.80922-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref9">9</xref>] meaning that almost all photoexcited species in the perovskite are able to reach the interfaces from where the charges are then transported through suitable hole- and electron-transporting layers to the electrodes. Based on these excellent properties, the power conversion efficiencies of organic-inorganic hybrid perovskite solar cells have increased from around 4% to a certified 22% in the last three years [<xref ref-type="bibr" rid="scirp.80922-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref3">3</xref>] . Now, most of the significant improvements in PCE have been a direct result of improvements in the formation of perovskite films, [<xref ref-type="bibr" rid="scirp.80922-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.80922-ref11">11</xref>] which led to a better film uniformity and crystalline quality, thus suggesting that the thin film features are of the upmost importance for achieving high performance.
      </p>
      <p>
        As we know, organic-inorganic hybrid perovskites are a family of materials that share a crystal structure with calcium titanate, that is, ABX<sub>3</sub>. These material are crystallized from organic halide and metal halide salts to form crystals in the ABX<sub>3</sub> structure, where A is the organic cation, such as methylammonium (MA = CH 3 NH 3 + ), B is the metal cation, such as lead (B = Pb<sup>2+</sup>) and X is the halide anion (X = I, Br, Cl or mixtures). As for this, there is a general schematic diagram of perovskite synthesis (<xref ref-type="fig" rid="fig1">Figure 1</xref>). And a lot of processing techniques of perovskite layers have been reported to obtain high-quality perovskite films so far, such as one-/two-step solution process, vacuum deposition, and solvent vapor/additive assisted crystal growth [<xref ref-type="bibr" rid="scirp.80922-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.80922-ref18">18</xref>] . Although these methods give some help to understand the growth mechanisms of perovskite films, however the growth mechanisms of perovskite films are not completely clear. The two-step sequential deposition method in all method for film formation is more helpful for studying the growth mechanisms of perovskite crystallites.
      </p>
      <p>
        We have found that the characteristics of PbI<sub>2</sub> layer play a significant role in the final perovskite films formation. In this paper, we research the influence of PbI<sub>2</sub> film characteristics on the final perovskite films and its mechanisms based on the two-step sequential deposition method.
      </p>
    </sec>
    <sec id="s2">
      <title>2. Experimental Section</title>
      <p>
        Many methods to fabricate organic-inorganic perovskites have emerged, each resulting in varying degrees of surface coverage [<xref ref-type="bibr" rid="scirp.80922-ref19">19</xref>] , and crystal and film quality [<xref ref-type="bibr" rid="scirp.80922-ref20">20</xref>] . Nevertheless, the two-step sequential deposition method can achieve
      </p>
      <p>
        additional control over the morphology by sequentially depositing the two precursors relative to one-step deposition [<xref ref-type="bibr" rid="scirp.80922-ref21">21</xref>] . Meanwhile the two-step sequential deposition method is more flexible to design the procession of film formation. Here, organic-inorganic perovskite films were fabricated by two-step sequential deposition methods, which is helpful to investigate the effect of PbI<sub>2</sub> layer characteristics on the perovskite films formation.
      </p> </sec>
      <sec id="s2_1">
        <title>2.1. Organic-Inorganic Perovskite Thin Films Deposition</title>
        <sec id="s2_1_1">
          <title>
            2.1.1. PbI<sub>2</sub> Layer Fabricated by Spin Coatings
          </title>
          <p>
            Here, the inorganic framework film was formed by depositing PbI<sub>2</sub> solution on the substrates. PbI<sub>2</sub> solution was prepared in DMF. The prepared PbI<sub>2</sub> solution was preheated at 110˚C on a hot plate, followed by spin coating on the substrates at 4000 rpm for 40 s, then the PbI<sub>2</sub> film was put back on the hot plate for 15 min of drying. To obtain the perovskite thin film, substrates with PbI<sub>2</sub> film were then put into a vacuum coating machine, then MAI was deposited by thermal evaporation for 30 min (<xref ref-type="fig" rid="fig2">Figure 2</xref>). After cooling down to room temperature, these perovskite thin films were annealed for 18 min at 100˚C. Then the films were rinsed with 2-propanol, and dried under a flow of clean air.
          </p>
        </sec>
        <sec id="s2_1_2">
          <title>
            2.1.2. PbI<sub>2</sub> Layer Fabricated by Thermal Evaporation
          </title>
          <p>
            This method to convert PbI<sub>2</sub> to a perovskite is aside from conversions in solution, where the substrate is exposed to the PbI<sub>2</sub> vapor. Then substrates with PbI<sub>2</sub> film were then put into a vacuum coating machine, then MAI was deposited by thermal evaporation for 30 min, sequentially (<xref ref-type="fig" rid="fig3">Figure 3</xref>). After cooling down to
          </p>
          <p>room temperature, the perovskite films were annealed for 30 min at 100˚C. Then the films are rinsed with 2-propanol, and dried under a flow of clean air.</p>
        </sec>
      </sec>
      <sec id="s2_2">
        <title>2.2. Analysis of Characteristics of the Resulted Layers</title>
        <p>
          The crystal structures of the CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> films were characterized by X-ray diffraction (XRD, Philips PANalytical X’Pert Pro) with a copper X-ray source, and the surface morphologies were observed by scanning electron microscope (SEM, Hitachi SU8010) and atomic force microscopy (AFM) (Seiko SPA-400SPM UNIT). All samples were tested in air and at room temperature.
        </p>
      </sec>
      <sec id="s3">
        <title>3. Results and Discussions</title>
        <p>
          To investigated the characteristics of PbI<sub>2</sub> layer prepared by different processes. We prepared different PbI<sub>2</sub> layers by spin coating and thermal evaporation, respectively.
        </p> </sec>
        <sec id="s3_1">
          <title>
            3.1. The Characteristics of PbI<sub>2</sub> Layer Prepared by Different Processes
          </title>
          <p>
            As our previous work described [<xref ref-type="bibr" rid="scirp.80922-ref22">22</xref>] , SEM and XRD measurements of PbI<sub>2</sub> layers fabricated by spin coating with different solution concentrations were taken. In Figures 4(f)-(j), an obvious signature peak at 12.65˚ is observed in all PbI<sub>2</sub> layers, which indicate doubtless PbI<sub>2</sub> material. Figures 4(a)-(e) show the top-view SEM images of PbI<sub>2</sub> films with the different solution concentration. It is observed that the PbI<sub>2</sub> layer has no clear morphology and fuzzy domain boundaries with low PbI<sub>2</sub> solution concentration (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a)). With the increase of PbI<sub>2</sub> solution concentration, the morphology of PbI<sub>2</sub> layer becomes
          </p>
          <p>
            gradually clear (Figures 4(a)-(e)) with pancake-shape crystalline grain, the grain size gradually increases as shown in Figures 4(a)-(e). Meanwhile, the surface roughness also gradually increases as extracted from its AFM measurements (see <xref ref-type="table" rid="table1">Table 1</xref>), which is consistent with SEM measurements (Figures 4(f)-(j)). We found the PbI<sub>2</sub> grains prepared by spin coating have fuzzy domain boundaries.
          </p>
          <p>
            Then, the characteristics of PbI<sub>2</sub> layer fabricated by thermal evaporation with different amount of PbI<sub>2</sub> were researched via the SEM images and XRD measurements in <xref ref-type="fig" rid="fig5">Figure 5</xref>. However, we found the PbI<sub>2</sub> layers by thermal evaporation appeared a completely different morphology from that by spin coating. As shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, all the PbI<sub>2</sub> layers obtained by thermal evaporation have clear surface morphology and appear rice-shaped crystalline grain. With the increase of the amount of PbI<sub>2</sub>, the surface roughness and the grain size of PbI<sub>2</sub> layers gradually increases. On the other hand, the sharp signature peak at 12.65˚ in the XRD measurements implies well crystalline degree of all PbI<sub>2</sub> layers obtained via thermal evaporation (<xref ref-type="table" rid="table2">Table 2</xref>).
          </p>
          <p>
            The SEM images and XRD measurements of twos representative PbI<sub>2</sub> layers prepared by spin coating and thermal evaporation are compared as shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>. As can be seen, there has an obvious difference between the morphology of the two types of PbI<sub>2</sub> layers. The later has a clear crystal shape and a loose structure comparing with that of the former. However the former have fuzzy domain boundaries and fewer grain boundaries than the later. From the XRD measurements in <xref ref-type="fig" rid="fig6">Figure 6</xref>(c), the sharpness of XRD peak of the PbI<sub>2</sub> layers
          </p>
          <table-wrap id="table1" >
            <label>
              <xref ref-type="table" rid="table1">Table 1</xref>
            </label>
            <caption>
              <title> Parameters derived from AFM measurements corresponding to Figures 4(a)-(e)</title>
            </caption>
          </table-wrap>
        </sec>
      </body>



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