<?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">Soft</journal-id><journal-title-group><journal-title>Soft</journal-title></journal-title-group><issn pub-type="epub">2327-0799</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/soft.2017.51001</article-id><article-id pub-id-type="publisher-id">Soft-73905</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><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Carbon Material with Fibonacci Parastichy Structure
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Aohan</surname><given-names>Wang</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>Hiromasa</surname><given-names>Goto</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Division of Materials Science, Faculty of Pure and Applied Science, University of Tsukuba, Tsukuba, Japan</addr-line></aff><pub-date pub-type="epub"><day>04</day><month>02</month><year>2017</year></pub-date><volume>05</volume><issue>01</issue><fpage>1</fpage><lpage>8</lpage><history><date date-type="received"><day>December</day>	<month>14,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>February</month>	<year>1,</year>	</date><date date-type="accepted"><day>February</day>	<month>4,</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>
 
 
  The curd of &lt;i&gt;Romanesco broccoli&lt;/i&gt; was carbonized at 900&amp;deg;C under argon atmosphere in a gold furnace chamber. The carbonization afforded a carbon material with a fine logarithmic spiral on the surface, resembling the Fibonacci parastichy structure of the &lt;i&gt;Romanesco broccoli&lt;/i&gt; flower bud. The carbonized “flower bud” structure was observed under scanning electron microscopy. Infrared absorption spectra and X-ray photoelectron spectroscopy measurements confirmed the chemical structure and component of the carbon material.
 
</p></abstract><kwd-group><kwd>&lt;i&gt;Romanesco broccoli&lt;/i&gt;</kwd><kwd> Fibonacci Parastichy Structure</kwd><kwd> Three-Dimensional Carbon Material</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Carbon materials have had increasing attention due to their remarkable properties like conductivity and chemical stability. The morphology of the carbon materials at macro-scale provides for diversity of application, such as active carbon with a large amount of pores as a catalyst, carbon fiber for high-strength structural material.</p><p>Instead of bottom-up fabrication, carbonization of the organic compound containing large amounts of light elements, performed at high temperature in inert gas atmosphere, should afford a macro-scale carbon material with shape and fine structures preserved. Carbons with micro- or nano-sized structure resembling the starting material were obtained via the carbonization of natural plants [<xref ref-type="bibr" rid="scirp.73905-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.73905-ref2">2</xref>] , DNA [<xref ref-type="bibr" rid="scirp.73905-ref3">3</xref>] , and artificially synthesized organic compounds [<xref ref-type="bibr" rid="scirp.73905-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.73905-ref5">5</xref>] . This method is a facile and cost-effective way to apply carbons at industrial levels while conserving energy and preserving the environment. However, shape- conserving carbonization has been focused on the nano- or micro-scale in one- dimensional or two-dimensional materials. From the aspects of application and scientific interest, it is necessary to examine properties of three-dimensional samples.</p><p>3D printing technology accelerates the demand of 3D structural carbon-pre- serving method. This bottom-up method satisfies the demand to manufacture three-dimensional products with complex structure. Applications of 3D printing technology vary from functional materials [<xref ref-type="bibr" rid="scirp.73905-ref6">6</xref>] , medical devices [<xref ref-type="bibr" rid="scirp.73905-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.73905-ref8">8</xref>] to the aerospace industry. Simultaneously, “ink” material for 3D printing technology expands the possibilities of material properties. As an example, Paul Gatenholm, et al., developed a novel bioink composed of a nano-fibrillated cellulose dispersion [<xref ref-type="bibr" rid="scirp.73905-ref9">9</xref>] . Since one of the most remarkable selling points of 3D printing is the convenience of unrestricted design [<xref ref-type="bibr" rid="scirp.73905-ref10">10</xref>] , printing could provide excellent starting points for well-tailored carbon materials.</p><p>In this research, we chose the Fibonacci parastichy structure, a complex structure with aesthetic and scientific value, as an example for shape-retained carbonization. This structure is found in nature plant and animals, such as the curd of Romanesco broccoli [<xref ref-type="bibr" rid="scirp.73905-ref11">11</xref>] , seed heads of sunflowers [<xref ref-type="bibr" rid="scirp.73905-ref12">12</xref>] , and the shell of the chambered nautilus. Also, synthesized Ag-SiO<sub>2</sub> core-shell nano-particles with Fibonacci parastichy surface structures with self-similarity were reported recently [<xref ref-type="bibr" rid="scirp.73905-ref13">13</xref>] .</p><p>In this report, Romanesco broccoli flower buds and stems were observed by microscope to study the Fibonacci parastichy structure. Then, the raw flower curd was carbonized at 900˚C in the presence of argon. The flower bud consists of a large amount of cellulose and moisture. Carbonization created asynthesized carbon material with self-similar structure. Infrared absorption spectroscopy and x-ray photoelectron spectroscopy (XPS) were utilized to determine structure.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Observation</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref>(a) is an image of Romanesco broccoli curd before carbonization (<xref ref-type="fig" rid="fig1">Figure 1</xref>(a)). This structure is formed with many similar parts like a spiral tree consisting of much smaller ones. The underlying parts with no spiral components are observed under scanning electron microscopy (SEM) (<xref ref-type="fig" rid="fig1">Figure 1</xref>(b)). The small components of different sizes pack closely together. <xref ref-type="fig" rid="fig1">Figure 1</xref>(c) shows the cross section of the inside of the flower bud, where the middle part mostly consists of uniform cells (<xref ref-type="fig" rid="fig1">Figure 1</xref>(c)). It is worth noting that the Fibonacci parastichy structure was not only observed on the surface of the flower bud, but also in the fibro-vascular bundles adhered to the epidermis, as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>(d). In <xref ref-type="fig" rid="fig1">Figure 1</xref>(d), five parallel fibro-vascular bundles can be found, labelled numbers 1 to 5, from left to right, respectively (<xref ref-type="fig" rid="fig1">Figure 1</xref>(d)). The distances between each adjacent fibro-vascular bundle were measured with a ruler, with results in <xref ref-type="table" rid="table1">Table 1</xref>. The calculated results do not follow the strict definition of the</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> (a) Image of the Fibonacci parastichy structure of a Romanesco broccoli flower bud. (b) magnification (&#215;370) of a Romanesco broccoli flower bud observed under the scanning electron microscope; (c) Cross section image of a cluster of Romanesco broccoli curd; (d) Image of fibrovascular bundles adhering on the Romanesco broccoli stem epidermis</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2780013x2.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Calculated distance between adjacent fibrovascular bundles of Romanesco broccoli stem epidermis</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Bundle number</th><th align="center" valign="middle" >Distance<sup>a</sup> (mm)</th><th align="center" valign="middle" >Distance between two bundles (mm)<sup> b</sup></th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle"  rowspan="5"  >2 
<table cellpadding="0" cellspacing="0" width="100%"> 
 <tbody> 
  <tr> 
   <td> 2.8 </td> 
  </tr> 
 </tbody> 
</table> 
<table cellpadding="0" cellspacing="0" width="100%"> 
 <tbody> 
  <tr> 
   <td> 3.2 </td> 
  </tr> 
 </tbody> 
</table> 
<table cellpadding="0" cellspacing="0" width="100%"> 
 <tbody> 
  <tr> 
   <td> 5 </td> 
  </tr> 
 </tbody> 
</table></td><td align="center" valign="middle" >2.8</td><td align="center" valign="middle" >3.2</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >2.8</td></tr><tr><td align="center" valign="middle" >3.2</td></tr><tr><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2.0</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4.8</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >8.0</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >13.0</td></tr></tbody></table></table-wrap><p><sup>a</sup>Distance from bundle 1. <sup>b</sup>Increment length.</p><p>Fibonacci sequence, 0, 1, 1, 2, 3, 5, 8,…, However, the difference might be related to the growth direction of the plants that effect the surface of the morphology of the flower bud.</p></sec><sec id="s2_2"><title>2.2. Carbonization</title><p>A cluster of flower buds was carefully snipped off and washed with distilled water to remove the impurities on the surface. The sample was put in a quartz boat and set in a gold furnace chamber. Carbonization was performed by increasing the temperature from room temperature to 900˚C in argon flow with flow rate of 200 mL/min for 1 h. The obtained carbon is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> (Figures 2(a)- (e)).</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Surface Observation</title><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the images of the carbonized Romanesco broccoli flower bud captured from different angles. The material turns to black color during carbo-</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Image of the carbonized Romanesco broccoli flower bud taken for different angles</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2780013x3.png"/></fig><p>nization. The shape of the whole cluster, and the Fibonacci parastichy structure on the surface, are well retained after carbonization (Figures 2(a)-(e)). The smaller clusters attached on the surface also show Fibonacci parastichy structure. The three-dimensional system was well preserved.</p><p>It is noteworthy that the Fibonacci parastichy structure was also found at micro-scale. <xref ref-type="fig" rid="fig3">Figure 3</xref> shows the images observed under SEM (Figures 3(a)-(d)). The scale of the smallest three-dimensional Fibonacci parastichy structure on the surface of a Romanesco broccoli flower curd ranges around 50 μm (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)). In <xref ref-type="fig" rid="fig3">Figure 3</xref>(c), small sphere-like particles were found on top of a cluster (<xref ref-type="fig" rid="fig3">Figure 3</xref>(c)). The small pieces show volumetric shrinkage, with spiral lines comprised of cubic-like particles found on the apex of the curd (<xref ref-type="fig" rid="fig3">Figure 3</xref>(d)). <xref ref-type="fig" rid="fig4">Figure 4</xref> is a SEM image of the shoot apical meristem in the developmental stage of the carbonized Romanesco broccoli. This image resembles the SEM graphof raw Romanesco very well (<xref ref-type="fig" rid="fig4">Figure 4</xref>) [<xref ref-type="bibr" rid="scirp.73905-ref11">11</xref>] . These results strongly suggest that a three-dimensional Fibonacci parastichy structure in microscale was achieved by carbonization.</p></sec><sec id="s3_2"><title>3.2. Infrared Absorption</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the IR absorption spectrum of the carbonized Romanesco broccoli. An intense absorption band at 1051 cm<sup>−1</sup> is due to C-O-C stretching of cellulose backbones. An absorption band at 2940 cm<sup>−1</sup> is due to stretching vibration of CH and CH<sub>2</sub>. The peak around 1600 cm<sup>−1</sup> implies the formation of carbon.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Scanning electron microscopy images of the carbonized Romanesco broccoli flower bud. (a) &#215;16; (b) &#215;50; (c) &#215;200; (d) &#215;100</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2780013x4.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> SEM image of a carbonized shoot apical meristem of Romanesco broccoli</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2780013x5.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> IR spectrum of the carbonized Romanesco broccoli</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2780013x6.png"/></fig></sec><sec id="s3_3"><title>3.3. X-Ray Photoelectron Spectroscopy</title><p>XPS measurement was performed on the carbonized sample. Carbonization process leaves a material consisting mainly of carbon (285 eV) and oxygen (531 eV) (<xref ref-type="fig" rid="fig6">Figure 6</xref>(a)). In addition, this measurement also identifies trace elements, such as potassium, calcium, phosphorus, aluminium, and iron (<xref ref-type="fig" rid="fig6">Figure 6</xref>(b)). These previously absorbed elements remain after carbonization.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>Carbonization of a cluster of Romanesco broccoli was performed. The three- dimensional Fibonacci parastichy structure in micro-scale was successfully achieved by carbonization. This is the first report about a carbon material showing Fibonacci parastichy structure. This research suggests that complex structure composed of cellulose can remain the 3D structure in macro scale. This study can open a new avenue to create tailored carbon materials.</p>Techniques<p>IR absorption spectra were obtained with a JASCO FT-IR 550 spectrometer. Carbonization was carried out with the Electric Gold Furnace instrument, MIT Lincoln-Lab., equipped with an Ishikawa temperature controller. SEM observations were carried out with JSM-7000F, NIMS, Japan. XPS analysis was performed with a JPS-9010TR (JEOL).</p><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> XPS spectrum of the carbonized Romanesco broccoli.</title></caption><fig id ="fig6_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2780013x7.png"/></fig><fig id ="fig6_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2780013x8.png"/></fig></fig-group></sec><sec id="s5"><title>Acknowledgements</title><p>We are thankful to Research Facility Center for Science and Technology, Open Facility Network Office for XPS measurement. This work was partially supported by NIMS microstructural characterization platform as a program of the “Nanotechnology Platform” of the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan.</p></sec><sec id="s6"><title>Cite this paper</title><p>Wang, A. and Goto, H. (2017) Carbon Material with Fibo- nacci Parastichy Structure. Soft, 5, 1-8. https://doi.org/10.4236/soft.2017.51001</p></sec></body><back><ref-list><title>References</title><ref id="scirp.73905-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Liang, Y., Wu, D. and Fu, R. (2013) Carbon Microfibers with Hierarchical Porous Structure from Electrospun Fiber-Like Natural Biopolymer. Scientific Report, 3, Article ID: 1119. https://doi.org/10.1038/srep01119</mixed-citation></ref><ref id="scirp.73905-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Li, Y., Zhang, Q., Zhang, J., Jin, L., Zhao, X. and Xu, T. 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