<?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">OJCM</journal-id><journal-title-group><journal-title>Open Journal of Composite Materials</journal-title></journal-title-group><issn pub-type="epub">2164-5612</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojcm.2019.92012</article-id><article-id pub-id-type="publisher-id">OJCM-92162</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 Fabrication of Graphene and Graphene Oxide: A Review
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Adeniji</surname><given-names>Adetayo</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>Damilola</surname><given-names>Runsewe</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Chemistry and Biochemistry, Texas State University, San Marcos, TX, USA</addr-line></aff><pub-date pub-type="epub"><day>11</day><month>03</month><year>2019</year></pub-date><volume>09</volume><issue>02</issue><fpage>207</fpage><lpage>229</lpage><history><date date-type="received"><day>4,</day>	<month>April</month>	<year>2019</year></date><date date-type="rev-recd"><day>26,</day>	<month>April</month>	<year>2019</year>	</date><date date-type="accepted"><day>29,</day>	<month>April</month>	<year>2019</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 field of nanotechnology has advanced following the discovery of a two-dimensional material of sp
  <sup>2</sup>
   hybridized carbon atoms, graphene in 2004 by Geim and Novoselov. Graphene has received so much attention due to its exceptional electronic, thermal, mechanical, and optical properties in addition to its large surface area and single-atom thickness. This has led to the discovery of several techniques to obtain graphene such as chemical exfoliation, chemical vapor deposition (CVD), chemical synthesis etc. However, these techniques are majorly challenged with developing graphene with 
  fewer
   defects and in large scale
  ;
   thus, there is an increasing need to produce graphene in large quantities with high quality. Several studies have 
  been 
  carried out to find routes to producing high-quality graphene. This paper focuses majorly on the synthesis and fabrication methods of producing graphene and its derivative, graphene oxide. Characterization technique
  s
   to identify graphene such as optical microscopy, scanning electron microscopy (SEM), Raman spectroscopy, scanning probe microscopy (SPM) used to determine number of layers, quality, atomic structures, and defects in graphene is also briefly discussed. This article also covers a short description of graphene applications in transparent electrodes, composites and energy storage devices.
 
</p></abstract><kwd-group><kwd>CVD</kwd><kwd> Exfoliation</kwd><kwd> Graphene</kwd><kwd> Graphene Oxide</kwd><kwd> Synthesis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The field of nanotechnology has blossomed following several studies on carbon. Carbon exists in three-dimensional (3D) forms (regarded as allotropes) as diamond and graphite. Evidence of the 3D graphitic form of carbon dates as far back to 1500s [<xref ref-type="bibr" rid="scirp.92162-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref2">2</xref>] . This brought about its use as a writing material in the 1900s as the pencil industry was developed [<xref ref-type="bibr" rid="scirp.92162-ref3">3</xref>] . Other carbon allotropes, such as zero-dimensional (0D) fullerene [<xref ref-type="bibr" rid="scirp.92162-ref1">1</xref>] and one-dimensional (1D) carbon nanotubes [<xref ref-type="bibr" rid="scirp.92162-ref2">2</xref>] were discovered in the 1980s and 1990s (<xref ref-type="fig" rid="fig1">Figure 1</xref>). However, there remained an argument on the existence of two-dimensional (2D) allotrope of carbon until 2004, when a publication by Andre Geim and Konstantin Novoselov documented a successful isolation of a single layer of graphite (graphene) on a sticky tape by micromechanical cleavage (scotch tape method) of highly ordered pyrolytic graphite (HOPG) [<xref ref-type="bibr" rid="scirp.92162-ref4">4</xref>] .</p><p>Graphene is a two dimensional (2D) single layer structure of covalently bonded sp<sup>2</sup>-hybridized carbon atoms arranged in a hexagonal honeycomb network. It is a single-atom thick allotrope of carbon which serves as the basic structural unit for other carbon allotropic forms: 1) 0D fullerenes formed by wrapping up graphene sheet to form a sphere (Bucky ball), 2) 1D carbon nanotube (CNT) formed by rolling of a graphene sheet to form a cylindrical structure, and 3) 3D graphite formed by stacking several layers of individual graphene sheet held together by van der Waals bonds as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> [<xref ref-type="bibr" rid="scirp.92162-ref5">5</xref>] .</p><p>Single, double, and triple graphitic layers are commonly known as monolayer, bilayer, and trilayer graphene’s respectively. Graphene layers exceeding 5 and up to 30 aregenerally called multilayer graphene/thick graphene [<xref ref-type="bibr" rid="scirp.92162-ref6">6</xref>] . In graphene, the carbon-carbon bond distance is about 0.142 nm (1.42 &#197;) with the layer height (thickness) of about 0.33 nm (3.3 &#197;) (<xref ref-type="fig" rid="fig2">Figure 2</xref>) [<xref ref-type="bibr" rid="scirp.92162-ref3">3</xref>] .</p><p>Graphene shows exceptional properties including a large theoretical specific surface area (2630 m<sup>2</sup>g<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.92162-ref7">7</xref>] , high intrinsic mobility (200,000 cm<sup>2</sup>V<sup>−1</sup>s<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.92162-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref9">9</xref>] , high Young’s modulus (~1.0 TPa) [<xref ref-type="bibr" rid="scirp.92162-ref10">10</xref>] , and thermal conductivity (~5000 Wm<sup>−1</sup>K<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.92162-ref11">11</xref>] . It also has good optical transmittance (~97.7%), good electrical conductivity, and ability to withstand current density of 108 A/cm<sup>2</sup> [<xref ref-type="bibr" rid="scirp.92162-ref12">12</xref>] . Graphene is also known to be a zero-bandgap semiconductor; therefore, the band gap can be tuned through simple physicochemical processes [<xref ref-type="bibr" rid="scirp.92162-ref13">13</xref>] .</p><p>Owing to its exciting properties, study on graphene and its derivatives in the field of materials science and condensed-matter physics has generated immense attention over the past few years with various applications including membranes [<xref ref-type="bibr" rid="scirp.92162-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref15">15</xref>] , nanoelectronics [<xref ref-type="bibr" rid="scirp.92162-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref18">18</xref>] , Li-ion batteries [<xref ref-type="bibr" rid="scirp.92162-ref19">19</xref>] , electrodes [<xref ref-type="bibr" rid="scirp.92162-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref22">22</xref>] , supercapacitors [<xref ref-type="bibr" rid="scirp.92162-ref23">23</xref>] , sensors [<xref ref-type="bibr" rid="scirp.92162-ref24">24</xref>] , drug delivery [<xref ref-type="bibr" rid="scirp.92162-ref25">25</xref>] , etc.</p><p>Graphene produced through micromechanical cleavage of graphite was pure with high quality, although it was time consuming and incapable of mass scale production. Recently, several other techniques have been reported for the fabrication and synthesis of graphene, such as epitaxial growth by chemical vapor deposition on copper (Cu) substrate [<xref ref-type="bibr" rid="scirp.92162-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref27">27</xref>] , epitaxial growth by thermal deposition of Si atom from SiC surface [<xref ref-type="bibr" rid="scirp.92162-ref28">28</xref>] , colloidal suspension from graphite oxide [<xref ref-type="bibr" rid="scirp.92162-ref29">29</xref>] , and many others.</p></sec><sec id="s2"><title>2. Synthesis of Graphene</title><p>The process of fabricating or extracting graphene based on desired size and quality is regarded as synthesis of graphene. So far, numerous approaches to synthesis of graphene and graphene derivatives have been established. Mechanical cleaving (exfoliation) [<xref ref-type="bibr" rid="scirp.92162-ref4">4</xref>] , chemical synthesis [<xref ref-type="bibr" rid="scirp.92162-ref30">30</xref>] , chemical exfoliation [<xref ref-type="bibr" rid="scirp.92162-ref31">31</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref32">32</xref>] , epitaxial growth [<xref ref-type="bibr" rid="scirp.92162-ref33">33</xref>] , and thermal chemical vapor deposition (CVD) [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] methods have been extensively studied. Other methods including electrochemical exfoliation [<xref ref-type="bibr" rid="scirp.92162-ref35">35</xref>] , microwave synthesis [<xref ref-type="bibr" rid="scirp.92162-ref36">36</xref>] , and unzipping of CNT [<xref ref-type="bibr" rid="scirp.92162-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref39">39</xref>] have been reported. Generally, graphene synthesis methods for large scale production, including single layer graphene (SLG), bilayer graphene, and few layer graphene (FLG) can be broadly classified into two types: 1) top-down process, and 2) bottom-up process. The classification of each technique is shown in the flow chart in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><sec id="s2_1"><title>2.1. Top-Down Process</title><p>In the top-down process, graphene sheets are produced by exfoliation or separation of highly ordered pyrolytic graphite (HOPG) or its derivative, graphene oxide (GO).</p><sec id="s2_1_1"><title>2.1.1. Mechanical Exfoliation</title><p>Mechanical exfoliation is the first established method of extraction of graphene flakes on a substrate [<xref ref-type="bibr" rid="scirp.92162-ref4">4</xref>] . In nanotechnology, it is a top-down method of graphene synthesis, by which a stress (longitudinal or transverse) is applied to layered graphite surface using a simple adhesive tape (scotch tape) or AFM tip. Graphite structure is composed of several single-atomic layers of graphene stacked and held together by weak van der Waals forces. Between each layer is an interlayer distance of 3.3 &#197; (0.33 nm) and interbond energy of 2 eV/nm<sup>2</sup>. Single layer graphene (SLG) to few layer graphene (FLG) can be produced through mechanical cleaving by slicing down the layers from graphitic materials such as HOPG, single-crystal graphite or natural graphite [<xref ref-type="bibr" rid="scirp.92162-ref40">40</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref41">41</xref>] . This method requires an external force of about ~300 nNμm<sup>−2</sup> to separate a single graphene layer from graphite [<xref ref-type="bibr" rid="scirp.92162-ref42">42</xref>] . Mechanical exfoliation can be achieved using several agents including scotch tape [<xref ref-type="bibr" rid="scirp.92162-ref4">4</xref>] , electric field [<xref ref-type="bibr" rid="scirp.92162-ref43">43</xref>] , and ultrasonication [<xref ref-type="bibr" rid="scirp.92162-ref44">44</xref>] . Prior to the first production of a single layer graphene by Novoselov et al., Ruoff et al. [<xref ref-type="bibr" rid="scirp.92162-ref41">41</xref>] first produced thin multilayered graphite with about 200 nm thickness by mechanical exfoliation using AFM tip (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a)). <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) shows the micro-graph of fabricated thin multilayered graphite consisting of 500-600 layers of monolayer graphene.</p><p>Novoselov et al. [<xref ref-type="bibr" rid="scirp.92162-ref4">4</xref>] utilized adhesive tape to produce single graphene layer (thickness &lt; 10 nm) by exfoliation from 1 mm thick HOPG mesa. This involved compressing dry etched graphite mesa (by oxygen plasma) against a 1 mm thick wet photoresist layer over a glass substrate. Baking was done to attach the HOPG mesa to the layer of photoresist and exfoliation of the graphite flakes was achieved by using the scotch tape. Dispersed graphite flakes in acetone was transferred onto a cleaned SiO<sub>2</sub>/Si substrate. <xref ref-type="fig" rid="fig4">Figure 4</xref>(c) shows optical micro-graph of multilayer graphene flakes produced via mechanical exfoliation on top of SiO<sub>2</sub>/Si substrate while <xref ref-type="fig" rid="fig4">Figure 4</xref>(d) shows the identification of single graphene flakes with different number of layers.</p><p>The problem with the exfoliation process is scalability and reproducibility. Though it produces high quality graphene layers, there is still a need for further improvement to produce large-scale, high quality, and defect-free graphene for use in nanotechnology.</p></sec><sec id="s2_1_2"><title>2.1.2. Chemical Exfoliation</title><p>Chemical exfoliation is another route to obtaining monolayer graphene. This method involves production of suspension which changesgraphite to form graphene through the formation of graphene-intercalated compounds (GICs). This involves the introduction of alkali metals into a graphite solution to increase the interlayer spacing, thereby reducing the van der Waals forces between the layers and forming GICs which are then dispersed in a liquid medium through sonication to form single-layer graphene [<xref ref-type="bibr" rid="scirp.92162-ref45">45</xref>] . Alkali metals are the only choice of materials as they easily form GICs on reaction with graphite due to the difference in ionization potential between graphite and alkali metals. Chemical exfoliation methodology was used by Viculis et al. to obtain graphene nanoplatelets (GNP) using potassium alkali metal [<xref ref-type="bibr" rid="scirp.92162-ref46">46</xref>] . Potassium graphite (KC<sub>8</sub>) intercalated compound was formed when potassium reacted with graphite at 200˚C under inert atmosphere. Dispersion of the GIC in aqueous ethanol (CH<sub>3</sub>CH<sub>2</sub>OH) resulted in an exothermic reaction as shown in (1) and produced GNP.</p><p>KC 8 + CH 3 CH 2 OH → 8 C + KOCH 2 CH 3 + 1 2 H 2 (1)</p><p>Potassium ions dissolve into the ethanol solution forming potassium ethoxide (KOCH<sub>2</sub>CH<sub>3</sub>) and hydrogen gas is formed to aid the separation of the layers of graphene. Precaution must be taken during this reaction as alkali metals vigorously react with water and alcohol, as such there is a need for an ice bath to dissipate heat during reaction. The main advantage of alkali metals, such as potassium, is their relatively small atomic radius which is smaller than the interlayer spacing in graphite and hence fits the interlayer spacing easily as shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a).</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref>(b) shows SEM micrographs of the chemically exfoliated GNP with ~10 nm thickness and ~30 layers. Viculis et al. also carried out exfoliation via GIC formation using an alkali metal such as Cesium (Cs) and NaK<sub>2</sub> (sodium-potassium) alloy [<xref ref-type="bibr" rid="scirp.92162-ref32">32</xref>] . Work by Vall&#233;s et al. [<xref ref-type="bibr" rid="scirp.92162-ref48">48</xref>] utilized ternary potassium salt K(THF)<sub>x</sub>C<sub>24</sub> tetrahydrofuran (THF) as the alkali metal to prepare potassium-intercalated GICs which was dispersed in N-methyl pyrrolidone (NMP) to yield a stable dispersion of negatively charged SLG as shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(c).</p><p>One major challenge in this work was the reassembly of produced graphene back into graphite. Later studies have incorporated surfactants in the solvent used and utilized immiscible liquids such as heptane and water [<xref ref-type="bibr" rid="scirp.92162-ref48">48</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref49">49</xref>] . Other studies have utilized ferric chloride, supercritical carbon dioxide, and nitromethane as the intercalation chemicals [<xref ref-type="bibr" rid="scirp.92162-ref50">50</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref51">51</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref52">52</xref>] .</p><p>Graphene synthesis through chemical exfoliation is important and unique as it can produce a large amount of graphene at a low temperature. It is also scalable and can be extended to a wide range of functionalized graphene production.</p></sec><sec id="s2_1_3"><title>2.1.3. Chemical Synthesis</title><p>Chemical reduction of graphite oxide (GO) is one of the conventional ways of preparing graphene in large quantities. The three routes available for GO synthesis; the Brodie method [<xref ref-type="bibr" rid="scirp.92162-ref5">5</xref>] , Staudenmaier method [<xref ref-type="bibr" rid="scirp.92162-ref53">53</xref>] , and Hummers method [<xref ref-type="bibr" rid="scirp.92162-ref54">54</xref>] consist of oxidation of graphite through strong acids and oxidants such as concentrated sulfuric acid (H<sub>2</sub>SO<sub>4</sub>), nitric acid, and potassium permanganate. Oxidation degree can be varied by the stoichiometry, reaction conditions (pressure, temperature, etc.), and the graphite type (HOPG, pure graphite, etc.). The works of Brodie et al. [<xref ref-type="bibr" rid="scirp.92162-ref5">5</xref>] in 1859 first demonstrated the synthesis of GO by adding potassium chlorate (KClO<sub>3</sub>) to a graphite slurry in the presence of fuming nitric acid (HNO<sub>3</sub>). However, the process was time consuming, involved several steps, and hazardous. This brought about a modification to the process by Staudenmaier et al. in 1898 [<xref ref-type="bibr" rid="scirp.92162-ref53">53</xref>] with the inclusion of concentrated H<sub>2</sub>SO<sub>4</sub> to the process and resulted in the production of highly oxidized GO in a single step process. A popular method used today was developed in 1958 by Hummers et al. [<xref ref-type="bibr" rid="scirp.92162-ref54">54</xref>] . This involves the oxidation of graphite by mixing the graphite slurry in sodium nitrite (NaNO<sub>3</sub>), concentrated H<sub>2</sub>SO<sub>4</sub>, and potassium permanganate (KMnO<sub>4</sub>) without the use of HNO<sub>3</sub>. <xref ref-type="fig" rid="fig6">Figure 6</xref> shows a schematic diagram of GO synthesis from graphite method using the three methods explained.</p><p>When graphite turns to GO, the interlayer spacing is increased to between two to three times depending on the oxidation time. In the case of pristine graphite, interlayer spacing is increased from about 3.34 &#197; to 5.62 &#197; after an hour of oxidation, and then further expanded to about 7.35 &#197; upon prolonged oxidation of 24 hours [<xref ref-type="bibr" rid="scirp.92162-ref5">5</xref>] . Upon ultrasonication in a DMF/water (9:1) (dimethyl formamide), GO interlayer distance is further expanded, forming individual layer suspensions. With hydrazine hydrate treatment, GO reduces back to graphene or reduced graphene oxide (RGO). The chemical reduction process is done using dimethyl hydrazine or hydrazine in the presence of a surfactant or polymer to produce homogenous colloidal graphene suspensions [<xref ref-type="bibr" rid="scirp.92162-ref55">55</xref>] . <xref ref-type="fig" rid="fig7">Figure 7</xref> shows the process for chemical synthesis of graphene from graphite. Reduction of GO has also been performed using sodium borohydride (NaBH<sub>4</sub>) [<xref ref-type="bibr" rid="scirp.92162-ref56">56</xref>] , hydroxylamine [<xref ref-type="bibr" rid="scirp.92162-ref57">57</xref>] , hydroquinone [<xref ref-type="bibr" rid="scirp.92162-ref58">58</xref>] , ascorbic acid [<xref ref-type="bibr" rid="scirp.92162-ref59">59</xref>] , etc. as reducing agents.</p><p>The use of toxic chemicals such as HNO<sub>3</sub> and KClO<sub>3</sub> has prompted researchers to develop new methods to graphene oxide synthesis [<xref ref-type="bibr" rid="scirp.92162-ref60">60</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref61">61</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref62">62</xref>] . However, the Hummer’s method has been found to be quicker, safer, and more efficient method for graphene oxide synthesis used widely today with some modifications. Hummer’s method was modified and further improved by Marcano et al. with the use of a larger amount of KMnO<sub>4</sub>, exclusion of NaNO<sub>3</sub>, and a 9:1 reaction mixture of H<sub>2</sub>SO<sub>4</sub>/H<sub>3</sub>PO<sub>4</sub> [<xref ref-type="bibr" rid="scirp.92162-ref61">61</xref>] . Compared to the Hummer’s method, this improved method shows higher oxidation efficiency and production of better hydrophilic oxidized graphene product [<xref ref-type="bibr" rid="scirp.92162-ref61">61</xref>] .</p><p>Various reports on the production of graphene by graphene oxide reduction exists. Some of the methods involve thermal reduction [<xref ref-type="bibr" rid="scirp.92162-ref63">63</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref64">64</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref65">65</xref>] , electrochemical reduction [<xref ref-type="bibr" rid="scirp.92162-ref66">66</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref67">67</xref>] , photochemical reduction [<xref ref-type="bibr" rid="scirp.92162-ref68">68</xref>] , hydrothermal reduction [<xref ref-type="bibr" rid="scirp.92162-ref69">69</xref>] , microwave assisted reduction [<xref ref-type="bibr" rid="scirp.92162-ref70">70</xref>] , and chemical reduction using reducing agents [<xref ref-type="bibr" rid="scirp.92162-ref71">71</xref>] .</p><p>Paredes et al. [<xref ref-type="bibr" rid="scirp.92162-ref29">29</xref>] produced graphene nanosheet derived from graphene oxide using the Hummer’s method with the reduced and unreduced aqueous dispersion drop casted onto freshly cleaved HOPG substrate. It was reported that the chemically reduced graphene oxide nanosheets were hardly distinguishable from their counterparts in the topographic AFM images. However, they could be distinguished by their phase contrast with the unreduced graphene oxide showing a phase difference on the HOPG substrate while the RGO showed little phase contrast with the HOPG substrate (due to little defects). The thickness of the chemically reduced graphene oxide nanosheet was reported as ~1 nm using tapping mode AFM as shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>. It was concluded that the chemically reduced graphene oxide still contained some oxygen functional groups [<xref ref-type="bibr" rid="scirp.92162-ref29">29</xref>] .</p><p>The chemical reduction method is the most useful method as it removes most of the functional groups present in the intermediate graphene oxide with the structure of the graphene surface restored after reduction. However, the produced graphene contains some defects due to the presence of remaining oxygen functional groups (such as −OH and −COOH) that causes some disorder in the graphene electronic structure. This results in reduced electrical conductivity of produced graphene as compared to that of pristine graphene (defect-free). These remaining functional groups on graphene and RGO can be used to tune their electrical and chemical properties for different applications.</p></sec></sec><sec id="s2_2"><title>2.2. Bottom-up Process</title><p>In the bottom-up process, graphene sheets are produced by building up nanoscale material via atomic or molecular arrangement of carbon.</p><sec id="s2_2_1"><title>2.2.1. Pyrolysis of Graphene</title><p>This involves the solvothermal synthesis of graphene with the use of a solvent interacting with precursor [<xref ref-type="bibr" rid="scirp.92162-ref47">47</xref>] . This reaction is performed in a closed vessel under high pressure with a 1:1 molar ratio of ethanol and sodium. Using sonication, graphene sheets can be smoothly detached by pyrolysis of sodium ethoxide. The produced graphene sheets were determined to have dimensions up to 10 μm. Using Raman spectroscopy and transmission electron microscopy (TEM), the graphene sheets were characterized to determine the crystalline structure, number of layers, band structure, and the graphitic nature [<xref ref-type="bibr" rid="scirp.92162-ref73">73</xref>] . Raman spectra showed a broad D-band (defect) and G-band with the intensity ratio of ~1.16 (I<sub>G</sub>/I<sub>D</sub>), representative of single layer defective graphene. Though this process was less expensive, easy, and required low temperature, the presence of many defects reduced the graphene quality. This method of graphene production has not been widely explored.</p></sec><sec id="s2_2_2"><title>2.2.2. Epitaxial Growth of Graphene on SiC Surface</title><p>Epitaxial thermal synthesis of graphene on the surface of single-crystalline silicon carbide (SiC) is one of the well-known synthesis techniques. The term “epitaxy” is a method that allows the deposition of a single-crystalline film (epitaxial film) on a single-crystal substrate. When an epitaxial film is of the same material as the substrate, it is known as homoepitaxial layer, and if the epitaxial film and the substrate have different material, then an heteroepitaxial film is formed. Epitaxial growth on SiC forms an heteroepitaxial layer of single-layer graphite or graphene. In 1975, Bommel et al. [<xref ref-type="bibr" rid="scirp.92162-ref74">74</xref>] first reported heat treatment between 1000˚C and 1500˚C under ultrahigh pressure produced graphite on both polar planes of SiC. Synthesis by de Heer et al. in 2004 [<xref ref-type="bibr" rid="scirp.92162-ref75">75</xref>] produced ultrathin (few layers between 1 to 3 monoatomic graphene layers) graphitic layers on Si-terminated (0001) face of single-crystal 6H-SiC. Using the same thermal decomposition method, they fabricated 1 to 2 layers of epitaxial graphene on the (0001) face of 6H-SiC [<xref ref-type="bibr" rid="scirp.92162-ref76">76</xref>] . Synthesized epitaxial graphene on SiC although had high quality, they could not be transferred to other substrates.</p><p>In 2012, Juang et al. [<xref ref-type="bibr" rid="scirp.92162-ref77">77</xref>] reported a breakthrough with the growth of epitaxial graphene on SiC substrate coated with Ni catalyst thin film. This produced graphene which was easily transferable to other substrate for versatile applications [<xref ref-type="bibr" rid="scirp.92162-ref77">77</xref>] . Epitaxial growth of graphene on SiC is very promising due to its scalability, best electronic properties, and especially due to its high-quality graphene.</p></sec><sec id="s2_2_3"><title>2.2.3. Chemical Vapor Deposition (CVD)</title><p>Thermal chemical vapor deposition process involves exposure of a substrate to thermally decomposed precursors in gaseous state resulting in the deposition of the product onto the surface of the substrate at a high temperature. In many cases, deposition at high temperature is not desired, plasma-assisted reaction and deposition have been utilized to reduce the temperature. This process will be explained later in this paper. Depending on the quality, type of precursor, desired thickness of product, and structure, several types of CVD processes can be utilized including thermal, plasma enhanced (PECVD), reactive, hot wall, cold wall, etc. In the hot wall process, the walls of the reactor are kept relatively constant all around the reactor while in the cold wall process, the walls never get heated. Thermal CVD and PECVD are the most commonly used types of chemical vapor deposition to produce graphene. <xref ref-type="fig" rid="fig9">Figure 9</xref> demonstrates the schematic of a thermal and plasma-enhanced CVD process.</p><p>1) Thermal chemical vapor deposition of graphene</p><p>This process of graphene production involves flowing of precursor gases such as methane, hydrogen and argon in certain ratios into a quartz tube containing a substrate such as Cu at high temperatures in a furnace (<xref ref-type="fig" rid="fig9">Figure 9</xref>(a)). Over time, there is a deposition of graphene comprising of either single layer, bilayer or multilayer depending on preset conditions such as gas flow rate, reaction time, pressure, and temperature. Deposition of high-quality graphene using CVD process is usually done on various transition-metal substrate (their surface acts as catalyst) such as Ni [<xref ref-type="bibr" rid="scirp.92162-ref78">78</xref>] , Pd [<xref ref-type="bibr" rid="scirp.92162-ref73">73</xref>] , Ru [<xref ref-type="bibr" rid="scirp.92162-ref79">79</xref>] , Ir [<xref ref-type="bibr" rid="scirp.92162-ref80">80</xref>] , and Cu [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] with different hydrocarbons such as methane, benzene, acetylene, and ethylene [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] . On exposure of the transition-metal to hydrocarbon gas at high temperature, there is carbon saturation on the substrate and a thin film of carbon is formed on cooling.</p><p>In 1966 [<xref ref-type="bibr" rid="scirp.92162-ref81">81</xref>] , Ni was exposed to methane at a temperature of 900˚C to form thin graphite. Formation of FLG was observed on the evaporation of carbon from a graphite rod in 1971 [<xref ref-type="bibr" rid="scirp.92162-ref82">82</xref>] . In 1975, Lang et al. [<xref ref-type="bibr" rid="scirp.92162-ref42">42</xref>] demonstrated the deposition of monolayer graphitic structure on Pt using ethylene for the first time. Eizenberg et al. [<xref ref-type="bibr" rid="scirp.92162-ref83">83</xref>] later reported the formation of graphitic layer on Ni (111) over a long reaction time. There was over two decades interval in single graphitic layer deposition research due to inadequacy in finding applications of thin graphite films. However, the discovery of graphene in 2004 [<xref ref-type="bibr" rid="scirp.92162-ref4">4</xref>] with potential application in graphene-based electronics, there arose wide interest in this material.</p><p>In 2006, the first attempt at synthesis of graphene on Ni foil via CVD method was found using camphor (terpenoid, a white transparent solid of chemical formula C<sub>10</sub>H<sub>16</sub>O) as the precursor [<xref ref-type="bibr" rid="scirp.92162-ref84">84</xref>] . When viewed with the TEM, the product was found to have a hexagonal planar few-layer graphite-like structure consisting of almost ~35 layers of stacked SLG with interlayer spacing of 0.34 nm. However, the first evidence of large-scale monolayer graphene using CVD growth was discovered by Obraztsov et al. [<xref ref-type="bibr" rid="scirp.92162-ref85">85</xref>] in 2007. The growth was achieved using precursors of methane and hydrogen under direct current (DC) discharge of ~0.5 Acm<sup>−2</sup>. The as-deposited graphene structure shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows the anomalous surface ridges which can be described as graphene folding lines [<xref ref-type="bibr" rid="scirp.92162-ref85">85</xref>] . The ridge formation in the graphene was due to the thermal expansion coefficient difference between graphene and Ni. Raman spectroscopy and scanning tunneling microscopy (STM) confirmed the presence of about ~1 - 2 nm thick FLG [<xref ref-type="bibr" rid="scirp.92162-ref85">85</xref>] .</p><p>Successively, other reports have demonstrated synthesis of single-to few-layer graphene on Ni substrate. In 2009, Reina et al. [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] utilized e-beam evaporated Ni on SiO<sub>2</sub>/Si substrate to grow graphene using diluted hydrocarbon gas. About 1 - 10 layers of graphene were observed using high resolution transmission electron microscopy (HRTEM) as shown in Figures 11(a)-(c). Raman spectroscopy was used to confirm the number of layers by the intensity ratio of the G’(2D) to G bands. The Raman signature were found around ~1342 cm<sup>−1</sup>, ~1581 cm<sup>−1</sup>, and ~2677 cm<sup>−1</sup> corresponding to the D, G, and G’(2D) bands of produced graphene respectively as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>1(b) [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] .</p><p>Graphene growth on Cu substrate displays another method towards scalability of graphene growth with increased single layer coverage [<xref ref-type="bibr" rid="scirp.92162-ref86">86</xref>] . Li et al. in 2009 demonstrated large-scale graphene synthesis on copper foils by thermal CVD of methane at 1000˚C [<xref ref-type="bibr" rid="scirp.92162-ref86">86</xref>] . The deposition of carbon on copper was described as a high-temperature surface catalyzed process due to the limited solubility of carbon in copper [<xref ref-type="bibr" rid="scirp.92162-ref86">86</xref>] . Additionally, graphene growth on Cu occurs by segregation of supersaturated carbon and adsorbed carbon on copper surface during the rapid cooling process in CVD copper [<xref ref-type="bibr" rid="scirp.92162-ref86">86</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref87">87</xref>] . Following growth of graphene on Cu foil, grown graphene was transferred onto another surface through copper etching yielding several chemically unaffected layers of graphene confirmed by Raman spectroscopy and HRTEM [<xref ref-type="bibr" rid="scirp.92162-ref86">86</xref>] .</p><p>Similarly, Lee et al. [<xref ref-type="bibr" rid="scirp.92162-ref87">87</xref>] developed optimized condition for synthesis of graphene produced by CVD process on Cu foil. It was observed that high pressure, low hydrogen to methane ratio, with reduced growth time produced graphene layers with improved quality [<xref ref-type="bibr" rid="scirp.92162-ref87">87</xref>] . As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>2, there was formation of large Cu grains due to Cu grain coalescence during pre-annealing step, formation of copper grain boundary (Cu GB) separating the regions of small and big grains, and the presence of graphene folding lines like those obtained by Obraztsov et al. [<xref ref-type="bibr" rid="scirp.92162-ref85">85</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref87">87</xref>] .</p><p>Furthermore, grown graphene was transferred to a 290 nm-thick SiO<sub>2</sub>/Si substrate. The produced graphene on Cu substrate was first coated with polymethyl methacrylate (PMMA) on the graphene side to provide strength and serve as protection to avoid graphene damage during the transfer process. In order to etch away the Cu foil, the PMMA/graphene/Cu structure was placed in Fe(NO<sub>3</sub>)<sub>3</sub> solution (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(b)) with the PMMA side facing up. PMMA/graphene heterostructure was removed from the solution (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(c)) and rinsed severally in deionized (DI) water to remove residual Cu etchant solution (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(d)). The SiO<sub>2</sub>/Si substrate was dipped in DI water (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(e)) and the PMMA/graphene structure. Through van der Waals forces, the graphene surface adhered to the SiO<sub>2</sub>/Si substrate and the PMMA support was rinsed with solvents (acetone and isopropyl alcohol) (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(f)). The transferred graphene was distinguishable by the difference in color and contrast compared to the SiO<sub>2</sub>/Si substrate as observed by the naked eye (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(g)) [<xref ref-type="bibr" rid="scirp.92162-ref87">87</xref>] . Transferred graphene displaced some wrinkles introduced during the transfer process as evidenced by scanning electron microscopy [<xref ref-type="bibr" rid="scirp.92162-ref87">87</xref>] .</p><p>Numerous reports have shown graphene synthesis on other metal thin films and metal foils [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] . However, graphene growth by CVD method has been mostly done on Cu [<xref ref-type="bibr" rid="scirp.92162-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] and Ni substrates [<xref ref-type="bibr" rid="scirp.92162-ref34">34</xref>] . The problem of producing graphene on Ni substrate included the time consuming non-self-limiting growth, and the production of large number of wrinkles and folds. Copper substrates have demonstrated more favorable CVD growth of graphene [<xref ref-type="bibr" rid="scirp.92162-ref86">86</xref>] .</p><p>2) Plasma-Enhanced Chemical Vapor Deposition</p><p>This process of graphene production involves chemical reactions of reacting gases inside a vacuum chamber in the presence of plasma resulting in deposits of thin film on the surface of the substrate (<xref ref-type="fig" rid="fig9">Figure 9</xref>(b)), thus, the name, plasma-enhanced chemical vapor deposition (PECVD). Sources of plasma in PECVD can include radio frequency (RF), microwave, and inductive coupling (electrical currents produced by electromagnetic induction). PECVD process of graphene synthesis is performed at a relatively lower temperature and shorter deposition time than other CVD techniques and as such is more feasible for large scale industrial applications. By controlling the process parameters, catalyst-free growth can be achieved [<xref ref-type="bibr" rid="scirp.92162-ref88">88</xref>] . RF plasma-enhanced chemical vapor deposition has been achieved using substrates such as Ti, SiO<sub>2</sub>, Si, Al<sub>2</sub>O<sub>3</sub>, Mo, Hf, Zr, Nb, Cr, W, Ta, and 304 stainless steel [<xref ref-type="bibr" rid="scirp.92162-ref5">5</xref>] . This method reduces energy consumption and prevents the formation of unwanted products or amorphous carbon [<xref ref-type="bibr" rid="scirp.92162-ref89">89</xref>] .</p><p>Thin graphitic layer was first synthesized using PECVD by Obraztsov et al. [<xref ref-type="bibr" rid="scirp.92162-ref90">90</xref>] through DC discharge CVD of a methane and hydrogen mixture. Nanocrystalline graphite growth was observed on silicon wafer, Ni, Mo, and Ni substrates. A thick layer of graphene was produced by this process [<xref ref-type="bibr" rid="scirp.92162-ref90">90</xref>] . Wang et al. [<xref ref-type="bibr" rid="scirp.92162-ref91">91</xref>] deposited graphene on different substrates using PECVD method with RF power of 900 W while varying methane concentration at different temperatures. Increase in graphene growth rate with increase in temperature and methane concentration was observed [<xref ref-type="bibr" rid="scirp.92162-ref91">91</xref>] . Other studies on graphene synthesis using PECVD were done, such as atmospheric pressure process [<xref ref-type="bibr" rid="scirp.92162-ref92">92</xref>] , microwave plasma [<xref ref-type="bibr" rid="scirp.92162-ref93">93</xref>] , nitrogen-doped graphene/CNT hybrid structure [<xref ref-type="bibr" rid="scirp.92162-ref94">94</xref>] , and many others. PECVD method has been confirmed to produce high-crystalline graphene with high-purity; however, extensive research is ongoing in the production of uniform large-scale and single layer graphene through this technique.</p></sec><sec id="s2_2_4"><title>2.2.4. Other Methods</title><p>Several other ways to produce graphene exists including: arc discharge of graphite [<xref ref-type="bibr" rid="scirp.92162-ref23">23</xref>] , electron beam irradiation of PMMA nanofibers [<xref ref-type="bibr" rid="scirp.92162-ref95">95</xref>] , and conversion of nanodiamond [<xref ref-type="bibr" rid="scirp.92162-ref96">96</xref>] . Graphene can be synthesized by unzipping of multi-walled carbon nanotubes (MWCNTs) using highly oxidative KMnO<sub>2</sub> and concentrated H<sub>2</sub>SO<sub>4</sub> [<xref ref-type="bibr" rid="scirp.92162-ref38">38</xref>] , laser irradiation [<xref ref-type="bibr" rid="scirp.92162-ref38">38</xref>] , Li in liquid ammonia [<xref ref-type="bibr" rid="scirp.92162-ref10">10</xref>] , and plasma etching [<xref ref-type="bibr" rid="scirp.92162-ref39">39</xref>] to open up the carbon nanotubes for graphene nanoribbons (GNR) production. Arc discharge methods are also commonly used to synthesis boron- and nitrogen-doped graphene [<xref ref-type="bibr" rid="scirp.92162-ref97">97</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref98">98</xref>] . Arc discharge between carbon electrodes and pyridine or ammonia in the presence of nitrogen has yielded nitrogen-doped graphene sheets [<xref ref-type="bibr" rid="scirp.92162-ref97">97</xref>] . Boron-doped graphene sheet have been synthesized in the presence of hydrogen-diborane vapor mixture or boron-stuffed graphite electrodes [<xref ref-type="bibr" rid="scirp.92162-ref98">98</xref>] .</p></sec></sec></sec><sec id="s3"><title>3. Characterization of Graphene</title><p>Several microscopic and spectroscopic techniques are used to characterize graphene to determine the morphology, structure, quality, presence of defects, and number of layers. The most commonly used characterization techniques are optical microscopy, scanning probe microscopy (SPM), scanning electron microscopy (SEM), high resolution transmission electron microscopy (HRTEM), and Raman spectroscopy.</p><sec id="s3_1"><title>3.1. Optical Microscopy</title><p>Optical microscopy technique is an easy, straightforward, and effective method for non-destructive characterization of graphene. It is primarily used to determine the number of layers in graphene by using the contrast difference between graphene layers and the substrate. Size and shape of the graphene structure is also obtained from this technique. <xref ref-type="fig" rid="fig1">Figure 1</xref>4(a) shows the optical micrograph with different graphene layers of graphene on SiO<sub>2</sub>/Si substrate [<xref ref-type="bibr" rid="scirp.92162-ref99">99</xref>] .</p></sec><sec id="s3_2"><title>3.2. Scanning Probe Microscopy</title><p>Scanning probe microscopy (SPM) is a popular technique used to characterize the topography of nanomaterials such as graphene by scanning the sample with a probe. Two SPM commonly used techniques for graphene characterization are atomic force microscopy (AFM) and scanning tunneling microscopy (STM). In the AFM mode, scanning is done in either the contact or noncontact tapping mode of the probe tip with the deflection of the cantilever probe based on the topography of the graphene structure to form 2D and 3D images. <xref ref-type="fig" rid="fig1">Figure 1</xref>4(b) shows the AFM image of mechanically exfoliated graphene flake with atomic-level thickness [<xref ref-type="bibr" rid="scirp.92162-ref100">100</xref>] . STM utilizes tunneling current between the SPM probe and graphene to form similar pattern of the topography of the sample. <xref ref-type="fig" rid="fig1">Figure 1</xref>4(c) shows high contrast atomic resolution of obtained using STM for graphene hexagonal structure [<xref ref-type="bibr" rid="scirp.92162-ref101">101</xref>] .</p></sec><sec id="s3_3"><title>3.3. Scanning Electron Microscopy</title><p>Scanning electron microscopy (SEM) technique is used to determine surface morphology and number of layers of graphene. This is achieved through focusing a beam of energetic electrons on the sample. Like optical microscopy, there is a contrast difference between graphene layers and the substrate. <xref ref-type="fig" rid="fig1">Figure 1</xref>4(d) shows a micrograph from SEM for mechanical exfoliated graphene layers [<xref ref-type="bibr" rid="scirp.92162-ref102">102</xref>] .</p></sec><sec id="s3_4"><title>3.4. High Resolution Transmission Electron Microscopy (HRTEM)</title><p>HRTEM is a very powerful characterization technique for graphene’s structural characterizations. Its mode of operation is very similar to the SEM, but in this, the electron beam transmitted through the ultrathin sample. Atomic resolution images can be obtained using the HRTEM. <xref ref-type="fig" rid="fig1">Figure 1</xref>4(e) shows the atomic arrangement of graphene structure and interfaces using HRTEM [<xref ref-type="bibr" rid="scirp.92162-ref103">103</xref>] .</p></sec><sec id="s3_5"><title>3.5. Raman Spectroscopy</title><p>Raman spectroscopy is one of the most important technique used today for graphene characterization. It is a nondestructive technique which reveals bonding information. It displays this information as unique fingerprints of graphene in Raman spectra. Information relation to the graphene quality, number of graphene layers, induced strain, presence of defects, and the lattice mismatch can be determined by this technique. Raman spectra of monolayer graphene displays characteristics D-band, G-band, and 2D band at its respective positions of ~1350 cm<sup>−1</sup>, ~1580 cm<sup>−1</sup>, and ~2690 cm<sup>−1</sup> respectively [<xref ref-type="bibr" rid="scirp.92162-ref5">5</xref>] . <xref ref-type="fig" rid="fig1">Figure 1</xref>4(f) shows the Raman spectra of different layers of graphene on SiO<sub>2</sub>/Si substrate using a laser power of ~532 nm [<xref ref-type="bibr" rid="scirp.92162-ref104">104</xref>] .</p><p>Several other characterization techniques for graphene exist, the mostly used methods have been discussed in this paper.</p></sec></sec><sec id="s4"><title>4. Application</title><p>Since the ground-breaking discovery of the wonder material, graphene, there has been numerous outstanding roles of the material in this century. There are so many areas of application of the novel material. Recent progress in green technology has emerged from the exceptional mechanical, electronics, magnetic, optical, and surface area of functionalized graphene bringing about commercialization and innovative solutions to existing problems such as electronic and photonic applications for ultrahigh-frequency graphene-based devices, anode for li-ion battery [<xref ref-type="bibr" rid="scirp.92162-ref19">19</xref>] , sensors [<xref ref-type="bibr" rid="scirp.92162-ref24">24</xref>] , nanosized graphene in physics and materials science [<xref ref-type="bibr" rid="scirp.92162-ref21">21</xref>] , supercapacitors [<xref ref-type="bibr" rid="scirp.92162-ref23">23</xref>] , in ceramics [<xref ref-type="bibr" rid="scirp.92162-ref105">105</xref>] , membranes [<xref ref-type="bibr" rid="scirp.92162-ref14">14</xref>] , lightweight gas tanks, solar cells, flexible electronics, composite materials, and so many others [<xref ref-type="bibr" rid="scirp.92162-ref105">105</xref>] . Vast areas of research and development continue to open in the area of graphene applications to numerous fields including medicine, electronics, and energy [<xref ref-type="bibr" rid="scirp.92162-ref106">106</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref107">107</xref>] [<xref ref-type="bibr" rid="scirp.92162-ref108">108</xref>] .</p></sec><sec id="s5"><title>5. Conclusion</title><p>Discovery of the novel 2D material has revolutionized the nanoelectronics industry by providing an alternative to silicon, which has been used for decades. This contribution has also expanded to bio-medicine, nanorobotics, and energy. However, the issue yet to be resolved is scaling up production of graphene with high quality and uniformity. This is the goal to overcome in the years to come.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Adetayo, A. and Runsewe, D. (2019) Synthesis and Fabrication of Graphene and Graphene Oxide: A Review. Open Journal of Composite Materials, 9, 207-229. https://doi.org/10.4236/ojcm.2019.92012</p></sec></body><back><ref-list><title>References</title><ref id="scirp.92162-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kroto, H.W., Heath, J.R., O’Brien, S.C., Curl, R.F. and Smalley, R.E. (1985) C60: Buckminsterfullerene. Nature, 318, 162-163. https://doi.org/10.1038/318162a0</mixed-citation></ref><ref id="scirp.92162-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Iijima, S. (1991) Helical Microtubules of Graphitic Carbon. Nature, 354, 56-58.  
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