<?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">OPJ</journal-id><journal-title-group><journal-title>Optics and Photonics Journal</journal-title></journal-title-group><issn pub-type="epub">2160-8881</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/opj.2015.57021</article-id><article-id pub-id-type="publisher-id">OPJ-58304</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>
 
 
  Imaging and Therapeutic Applications of Optical and Thermal Response of SPION-Based Third Generation Plasmonic Nanodendrimers
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>aryam</surname><given-names>Tajabadi</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>Mohammad</surname><given-names>E. Khosroshahi</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Shahin</surname><given-names>Bonakdar</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Pasteur Institute of Iran, National Cell Bank of Iran, Tehran, Iran</addr-line></aff><aff id="aff2"><addr-line>Center for Advanced Diffusion-Wave Technologies (CADIFT), Department of Mechanical and Industrial 
Engineering, University of Toronto, Toronto, Canada</addr-line></aff><aff id="aff1"><addr-line>Laser and Nanobiophotonics Laboratory, Biomaterial Group, Faculty of Biomedical Engineering, Amirkabir University of Technology, Tehran, Iran</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>khosrom@mie.utoronto.ca(MEK)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>07</month><year>2015</year></pub-date><volume>05</volume><issue>07</issue><fpage>212</fpage><lpage>226</lpage><history><date date-type="received"><day>4</day>	<month>June</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>24</month>	<year>July</year>	</date><date date-type="accepted"><day>27</day>	<month>July</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>
 
 
  In this study, 9 nm superparamagnetic iron oxide nanoparticles (SPION) were functionalized by polyamidoamine (PAMAM) dendrimer. Using tetracholoroauric acid (HAuCl
  <sub>4</sub>), magnetodendrimer (MD) samples were conjugated by gold nanoparticles (Au-NPs). Two different reducing agents, 
  i.e. sodium borohydride and hydrazine sulfate, and pre-synthesized 10-nm Au-NP were used to evaluate the efficiency of conjugation method. The samples were characterized using X-ray diffractometry (XRD), transmission electron microscopy (TEM), Fourier transform infrared (FTIR) spectroscopy, UV-visible spectroscopy and fluorescence spectroscopy. The results confirmed that Au- NPs produced by sodium borohydrate and the pre-synthesized 10-nm Au-NPs were capped by MDs whereas the Au-NP prepared by hydrazine sulfate as a reducing agent was entrapped by MDs. Optical properties of the MDs were studied by laser-induced fluorescence spectroscopy (LIF) within a wide range of visible spectrum. Also, based on the thermal analysis, all synthesized nanostructures exhibited a temperature increase using 488 nm and 514 nm wavelengths of a tunable argon laser. The new iron oxide-dendrimer-Au NPs synthesized by sodium borohydrate (IDA- NaBH
  <sub>4</sub>) produced the highest temperature increase at 488 nm whereas the other nanostructures particularly pure Au-NPs produced more heating effect at 514 nm. These findings suggest the potential application of these nanocomposites in the field of bioimaging, targeted drug delivery and controlled hyperthermia.
 
</p></abstract><kwd-group><kwd>SPIONs</kwd><kwd> PAMAM Dendrimer</kwd><kwd> Gold Nanoparticles</kwd><kwd> Fluorescence</kwd><kwd> Bioimaging</kwd><kwd> Therapy</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Recently a variety nanomaterials including magnetite superparamagnetic iron oxide nanoparticles (SPION) and nobel metal nanoparticles such as gold have been the focus of many research fields particularly in medicine and biomedical engineering which has shown a promising advancement [<xref ref-type="bibr" rid="scirp.58304-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref3">3</xref>] . Plasmonic nanoparticles exhibit unique optical properties with major advantages due to the photophysical properties: strong localized surface plasmon resonance (LSPR), surface-enhanced scattering, non-linear optical properties, tunable resonance across the Vis-NIR due to adjustable nanoparticle size and shape, biocompatibility due to their inert surface, nontoxicity, surface conjugation chemistry, i.e., they can be linked to specific ligands for tumor targeting, imaging and therapies, lack of photobleaching or blinking as with quantum dots, and very low oxidation [<xref ref-type="bibr" rid="scirp.58304-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref9">9</xref>] . Not only can gold nanoparticles (Au-NPs) operate as an optical signal transfer in plasmonic devices but also they can be used as a useful platform for analytic-receptor interaction [<xref ref-type="bibr" rid="scirp.58304-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref10">10</xref>] . Au-NPs need surface treatment with different molecules to precisely perform desirable applications. There are some evidence of Au-NPs modification with silica, liposome and linear polymers [<xref ref-type="bibr" rid="scirp.58304-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref12">12</xref>] .</p><p>Researchers explicitly assert that poly(amidoamine) (PAMAM) dendrimers can act as a template or stabilizer for preparation of inorganic nanocomposites. The resultant nanocomposites have much applicable potential such as gen vector, catalysis, resonance imaging agents and nanocapsules [<xref ref-type="bibr" rid="scirp.58304-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref14">14</xref>] . Since dendrimers have unique chemical structures, molecular weight and molecular size which can provide special type of functionality, they receive privileged attention in developing fields of materials science [<xref ref-type="bibr" rid="scirp.58304-ref15">15</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref18">18</xref>] . Considering large number of terminal groups on the exterior of the molecule and interior voids, dendrimers introduce as an attractive platform for metal ion celates [<xref ref-type="bibr" rid="scirp.58304-ref19">19</xref>] . Indeed, dendrimer-entraped inorganic nanoparticles (DENP) include a nanostructure where one or more inorganic nanoparticles with the diameter of less than 5 nm are entrapped within an individual dendrimer molecule. In the case of dendrimer-stabilized inorganic nanoparticles (DSNP), one inorganic nanoparticle which usually has the diameter larger than 5 nm is stabilized by multiple dendrimer molecules [<xref ref-type="bibr" rid="scirp.58304-ref20">20</xref>] . Evaluation of formation of both DENP and DSNP in the presence of amine-terminated PAMAM dendrimers with and without addition of reducing agents has been the subject of several studies over the past few years [<xref ref-type="bibr" rid="scirp.58304-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref21">21</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref23">23</xref>] . Most of chemical methods of Au-NP preparation include nucleation and then growth of gold clusters by reduction of a gold salt (20). The bond is formed between gold nanoparticles and dendrimers as a result of interaction between coordinating groups such as ?OH, ?NH<sub>2</sub>, or ?COOH and gold ions [<xref ref-type="bibr" rid="scirp.58304-ref24">24</xref>] .</p><p>The contemporary issues in cancer treatment are production of effective nanoprobes for tumor targeting and selective therapy [<xref ref-type="bibr" rid="scirp.58304-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref25">25</xref>] . A fine magnetite nanoparticles with simple production method, nearly uniform size distribution and high magnetization saturation were prepared in our previous study [<xref ref-type="bibr" rid="scirp.58304-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref25">25</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref27">27</xref>] , the optimal magnetite nanoparticles were chosen, coated with third generation PAMAM dendrimer and finally functionalized with Au-NP via different preparation methods. The main intention of the paper was to synthesize third generation dendrimers conjugated with Au-NPs using three methods of sodium borohydrate, hydrazine sulfate as the reducing agents and pre-synthesized Au-NP, and compare their fluorescent and optothermal properties with dendrimers for the purpose of biomedical application.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Materials</title><p>Iron chlorides (III) (FeCl<sub>3</sub>.6H<sub>2</sub>O), Iron Sulfate (FeSO<sub>4</sub>∙7H<sub>2</sub>O), and Ethanol (C<sub>2</sub>H<sub>5</sub>OH) were purchased from Merck Company. Ammonium Hydroxide (NH<sub>4</sub>OH), Methyl Acrylate (CH<sub>2</sub> = C(CH<sub>3</sub>)COOCH<sub>3</sub>), Ethylenediamine (C<sub>2</sub>H<sub>4</sub>(NH<sub>2</sub>)<sub>2</sub>), Soduiom Borohydrate (NaBH<sub>4</sub>), Hydrazine sulfate (H<sub>6</sub>N<sub>2</sub>O<sub>4</sub>S), Gold colloid solution (10 nm), and tetracholoroauric acid (HAuCl<sub>4</sub>) were obtained from Sigma Aldrich.</p></sec><sec id="s2_2"><title>2.2. Formation of Gold and Magnetodendrimer</title><p>Dendrimer grafted magentite nanoparticles (magnetodendrimers-MDs) were synthesized based on our previous published report [<xref ref-type="bibr" rid="scirp.58304-ref28">28</xref>] . The gold coated MDs were synthesized using the three aforementioned procedures to achieve the following objectives: i) to have efficient method of loading Au-NP, ii) to improve the fluorescence properties of material, and iii) to find the optimal optothermal properties.</p><p>a―Using sodium borohydrate (IDA-NaBH<sub>4</sub>): A solution of tetracholoroauric acid (HAuCl<sub>4</sub>) (5 mM) was prepared and added to the suspension of third generation magnetodendrimer (1% w/v) with the same volume under N<sub>2</sub> atmosphere. In order to produce the complex between Au (III) and amide or amine group of dendrimer, the resulting mixture was vigorously stirred for one hour at darkness. After that, 5 mL of aqueous sodium borohydrate solution (0.1 M) was added drop wise to the reaction mixture. The following reactions lead to reducing Au (III) to zero charge Au (0) nanoparticles. The reaction was continued under a vigorous stirring for 2 hours at 25˚C. The obtained nanoparticles are referred as IDA-NaBH<sub>4</sub>. These particles were rinsed with ethanol five times using magnetic separation. The same procedure was repeated with the tenfold concentration of HAuCl<sub>4</sub> and to evaluate the completion of the reactions, a UV-vis analysis was performed at 0, 15, 30, 45, 60, 90, and 120 minutes after addition of reducing agent. The product is referred as (IDA-10).</p><p>b―Using hydrazine sulfate (IDA-Hydr.): The stable gold nanoparticles were produced by adding hydrazine sulfate (H<sub>6</sub>N<sub>2</sub>O<sub>4</sub>S) aqueous solution (25 mM) to the solution of magnetodendrime-HAuCl<sub>4 </sub>complex and stirring for 2 hours. The particles were rinsed with ethanol five times as before and the sample was named IDA-Hydr.</p><p>c―Using gold nanoparticles (IDA-NP): Au-NPs (purchased from sigma Aldrich) were directly added to magnetodenrimer suspension under N<sub>2</sub> atmosphere. The mixture was stirred for an hour to complete the reaction and then particles rinsed five times with ethanol.</p></sec><sec id="s2_3"><title>2.3. Characterization</title><p>Crystalline phase of nanoparticles was confirmed using X-ray diffraction with radiation of Cu Kα (XRD, λ = 0.15406 nm, FK60-40 X-ray diffractometer). The presence of PAMAM, gold formation on the surface of magnetite nanoparticles was proved by Fourier transform infrared (FTIR) spectroscopy (BOMEM, Canada). Particle size and morphology of nanocomposites were determined by transmission electron microscopy (TEM, Philips CM-200-FEG microscope, 120 kV). The amount of Au-NP attached to the magnetodendrimer was estimated using wavelength-dispersive X-ray spectroscopy (SEM?WDX, XL30, Philips, USA). The UV-vis spectra of nanoparticles were recorded using spectrophotometer (UV-2600, Shimadzu, Japan).</p></sec><sec id="s2_4"><title>2.4. Experimental Setup</title><p>The evaluation of fluorescence emission of ID (G3), IDA-10, IDA-Hydr, and IDA-NP nanoparticles at different excitation wavelengths was performed using an ion argon laser Melles Griot-35MAP431) at 25˚C. The fluorescence signals were detected by a 600 &#181;m core diameter optical fiber (LIBS-600-6-SR, Ocean Optics) connected to spectrometer (UV-Vis USB 4000, Ocean Optics), see <xref ref-type="fig" rid="fig1">Figure 1</xref>. In our case, the excitation wavelengths were 454, 457, 465, 472, 477, 488, 496, 502 and 514 nm. After obtaining the spectra of samples, they were smoothed by Gaussian model using Findgraph software.</p><p>The next set up was to evaluate the efficiency of these nanoparticles in coloring the polymeric substrate, using two kinds of natural polymers, i.e., cotton and collagen. After the injection of nanoparticle solution to these substrates, fluorescence microscopy (Zeiss Axioshop-Germany) was used to study the materials colouring.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. UV-Vis Evaluation</title><p>The concept of dendrimer nanocomposites is based on immobilization of pre-organized metallic ions [<xref ref-type="bibr" rid="scirp.58304-ref29">29</xref>] . With respect to this concept, a dendrimer acts as a template or reactor to pre-organization of ions and small molecules [<xref ref-type="bibr" rid="scirp.58304-ref30">30</xref>] . The full generation of dendrimeric nanoparticles is electron donor in aqueous medium and form a cation. In such cases, atoms and molecules could attach to internal space or external surface of dendrimer [<xref ref-type="bibr" rid="scirp.58304-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref31">31</xref>] . This pre-organization can lead to attachment of precursor-dendrimer, which is a dynamic equilibrium between template and reactants. The dynamic equilibrium causes a homogeneous distribution of ions and molecules. At</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Experimental setup of laser-induced fluorescence spectroscopy for IDA nanocomposites</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x6.png"/></fig><p>the second stage, a series of reactions lead to production of resultant hybrid materials. At this stage, mostly a reducing agent is added to precursor-dendrimer complex and the complex loses HCl moieties and Au-NPs are stabilized in the dendrimer structure [<xref ref-type="bibr" rid="scirp.58304-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref33">33</xref>] . There are three different types of hybrid materials; i.e. internal, external and mixed type.</p><p>In this work, in order to evaluate the formation of Au-NPs during the synthesis reaction, sampling was done at different reaction times and the UV-vis spectra of these samples were recorded. <xref ref-type="fig" rid="fig2">Figure 2</xref> indicates that all samples have a unique absorption peak in the range of 520 - 540 nm [<xref ref-type="bibr" rid="scirp.58304-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref34">34</xref>] , which reveals the formation of Au- NPs. Plasmonic peak around 520 nm corresponds to the collective oscillation of gold free electrons [<xref ref-type="bibr" rid="scirp.58304-ref35">35</xref>] . During the synthesis reaction, the intensity of plasmon resonance peak was increased over time and the peak shifted toward higher wavelengths with respect to increase in particle size.</p><p>At synthesis condition of dendrimer-gold nanocomposite and in the presence of HAuCl<sub>4</sub> molecules, amine group loses electrons and electrostatically interacts with AuCl<sub>4</sub><sup>−</sup> ions. In UV-vis spectrum of the condition prior to addition of reducing agent, an absorption peak was observed around 280 nm which is the characteristic peak of bound formation between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x7.png" xlink:type="simple"/></inline-formula> and dendrimer [<xref ref-type="bibr" rid="scirp.58304-ref36">36</xref>] . After addition of reducing agent, a broad peak around 520 nm was seen. This plasmonic peak is related to the collective oscillation of electrons [<xref ref-type="bibr" rid="scirp.58304-ref35">35</xref>] . Other researches indicate that peaks at 280 and 320 nm represent the aggregation of Au-NPs [<xref ref-type="bibr" rid="scirp.58304-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref38">38</xref>] . It should be mentioned that location and shape of surface plasmon resonance is strongly dependent on the particle size of material [<xref ref-type="bibr" rid="scirp.58304-ref39">39</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref40">40</xref>] and the particle aggregation results in reduction of gold plasmon band intensity [<xref ref-type="bibr" rid="scirp.58304-ref38">38</xref>] . As it is seen in <xref ref-type="fig" rid="fig3">Figure 3</xref>, the peak ratio of 520 nm to 280 nm increases over the time which indicates the formation of Au-NPs. However, this ratio shows a reducing trend after 90 minutes which can be an indication of probability of aggregation and cluster formation of Au-NPs. No significant peak corresponding to Au NPs was observed in the UV-vis spectra shown in <xref ref-type="fig" rid="fig4">Figure 4</xref> after purification of resultant material which may suggest that the final structure contains discrete gold nanoparticles (i.e. trapped) in a dendrimer substrate. This phenomenon was previously reported by [<xref ref-type="bibr" rid="scirp.58304-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref41">41</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref42">42</xref>] .</p></sec><sec id="s3_2"><title>3.2. TEM Analysis</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> indicates that the nanocomposites synthesized using NaBH<sub>4</sub> are larger than those synthesized using hydrazine sulfate. Based on these results and other researcher suggestions, on the presence of NaBH<sub>4</sub>, the ions interact with surface amine group of magnetodendrimer [<xref ref-type="bibr" rid="scirp.58304-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref40">40</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref43">43</xref>] and forms larger particles in the expense of smaller particles [<xref ref-type="bibr" rid="scirp.58304-ref35">35</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref40">40</xref>] . When hydrazine sulfate was used as a reducing agent, the homogeneous distribution and smaller particles were obtained which could be explained as an entrapment and formation of Au-NPs on the cavity of magnetodendrimer [<xref ref-type="bibr" rid="scirp.58304-ref43">43</xref>] .</p></sec><sec id="s3_3"><title>3.3. XRD Analysis</title><p>In order to evaluate the presence of Au-NP in the final structure, XRD analysis was done (<xref ref-type="fig" rid="fig6">Figure 6</xref>). The XRD</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> UV-vis spectra of dendrimer-gold complex during the synthesis</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x8.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Change of intensity ratio of 520 nm to 280 nm peaks during synthesis of magnetodendimer―gold nanocomposite</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x9.png"/></fig><p>patterns contain diffraction peaks at 2θ equal to 38, 44.3, 64.5 and 77.9 which represent (111), (200), (220) and (311) crystallographic plane respectively which prove the FCC structure of gold (JCPDS No.00-04-0784) [<xref ref-type="bibr" rid="scirp.58304-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref44">44</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref46">46</xref>] . The broadening of the most intense peak of these nanoparticles demonstrates that the small size Au-NPs could be calculated by using the Scherrer equation (Equation (1)) [<xref ref-type="bibr" rid="scirp.58304-ref47">47</xref>] . The calculation shows that the average particle size of Au-NPs obtained using NaBH<sub>4</sub> reducing agent is about 4 orders larger than those formed by hydrazine sulfate.</p><disp-formula id="scirp.58304-formula585"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x10.png"  xlink:type="simple"/></disp-formula><p>where, D, λ and β represent the mean diameter of particles, the wavelength of incident X-ray, and the full width at half height (FWHM) respectively and constant K is equal to 0.9.</p></sec><sec id="s3_4"><title>3.4. FTIR and WDX Evaluation</title><p>FTIR analysis was used to prove the attachment of Au-NPs to magnetodendrimer shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. In the dendrimer-modified iron oxide nanoparticle (ID), the amide bands at 1570 and 1630 cm<sup>−1</sup> represent the characteristics of PAMAM dendrimer. Esumi et al. believe that the interactions of Au-NPs with amine terminated den-</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> UV-vis spectra of magnetodendimer―gold nanocomposite a) IDA, b) IDA 10, c) IDA NP, d) IDA Hydr</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x11.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> TEM image of a) IDA-10; b) IDA- Hydr and c) IDA-NP</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x12.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> XRD pattern of a) SPION; b) ID; c) IDA-NaBH<sub>4</sub>; d) IDA-Hydr; e) IDA-NP (<sup>*</sup>represents magnetite phase and ■ indicates gold phase)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x13.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> FTIR Spectra of a) G 3; b) IDA-NaBH<sub>4</sub>; c) IDA-10; d) IDA-Hydr; e) IDA-NP</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x14.png"/></fig><p>drimers are stronger than carboxyl terminated dendrimers as the FTIR bands of dendrimer are shifted while the half generations do not show any changes [<xref ref-type="bibr" rid="scirp.58304-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref48">48</xref>] . Furthermore, according to [<xref ref-type="bibr" rid="scirp.58304-ref34">34</xref>] the FTIR and UV-vis evaluations of dendrimer depend on the size and their generations, at lower generations’ external type and at higher generations a mixed type could be observed.</p><p>Type I amide band (wave number of 1630 cm<sup>−1</sup>) is generally related to C=O stretching vibration (70% - 85%) and directly appertain to combination and structure of polymer backbone. Type II amide band (wave number 1570 cm<sup>−1</sup>) represents the N-H bending vibration (20%) [<xref ref-type="bibr" rid="scirp.58304-ref49">49</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref52">52</xref>] . As shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>, FTIR spectra regarding IDA complex samples do not contain the band at 1570 cm<sup>−1</sup> and the band 1630 cm<sup>−1</sup> remain without any changes. This shows that the Au-NPs interact with N-H groups of MD structure whereas the polymer backbone relatively retains its original structure. In this figure, the peaks at 581 and 629 cm<sup>−1</sup> represent the iron oxide phase at all synthesized structures. In order to quantitatively appraise attachment of Au-NPs to MD, WDX (Wavelength-dispersive X-ray spectroscopy) analysis was performed. The analysis confirms the presence of gold phase in the prepared nanoparticles (<xref ref-type="fig" rid="fig8">Figure 8</xref>) [<xref ref-type="bibr" rid="scirp.58304-ref46">46</xref>] and <xref ref-type="fig" rid="fig9">Figure 9</xref> shows the efficiency of synthesis in terms</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> WDX images of a) IDA-NaBH<sub>4</sub>; b) IDA-10; c) IDA-Hydr; d) IDA- NP nanoparticles at three different levels of synthesized nanoparticles (L), Fe element (M), and Au element (R) respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x15.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Relative Counts of Fe/Au for different synthesized nanoparticles</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x16.png"/></fig><p>of relative counts of Fe: Au where hydrazine sulfate reducing agent has shown to produce the best nanoparticles compared to other synthesis methods.</p></sec><sec id="s3_5"><title>3.5. Laser-Induced Fluorescence Spectroscopy</title><p>One of the early works regarding the fluorescence of PAMAM dendrimer was reported by Klajnart et al. [<xref ref-type="bibr" rid="scirp.58304-ref53">53</xref>] . It has been shown that after addition of HAuCL<sub>4</sub>, the fluorescence intensity is red shifted towards the longer wavelength [<xref ref-type="bibr" rid="scirp.58304-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref36">36</xref>] . After adding the reducing agent, the peaks are changed considerably which shows the close attachment of Au-NPs to the dendrimers. The shift of fluorescence spectra could be explained by strong interaction between gold crystals and amine groups of dendrimer [<xref ref-type="bibr" rid="scirp.58304-ref35">35</xref>] . Optical properties of Au-NPs are highly sensitive to their particle size and have an effective influence on the fluorescence spectra of dendrimer [<xref ref-type="bibr" rid="scirp.58304-ref39">39</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref40">40</xref>] . This is because of the internal interaction between flexible structure of dendrimer and rigid structure of entrapped Au-NPs, whereas the larger particles damp the fluorescence of dendrimers. These phenomena could be explained in terms of fluorescence resonance energy transfer (FRET) [<xref ref-type="bibr" rid="scirp.58304-ref40">40</xref>] . In this study, IDA-Hydr nanocomposites strongly changed the initial fluorescent spectra of MD, i.e. the shape and location of peaks were sharply changed. In most cases, the fluorescence spectra of IDA-Hydr are stronger than others with highest signals at about 525 nm and 550 nm respectively. One reason for this is more likely due to their smaller size which helps them to be entrapped easily by dendrimers and hence intensify the fluorescence signals, see <xref ref-type="fig" rid="fig1">Figure 1</xref>0.</p><p>Considering the chemical structures of collagen and cotton, there is a possibility of hydrogen interaction between the hydroxyl group of the substrate and amine group of dendrimer nanocomposites which produces a new fluorescent moieties with a time dependent behaviour. The longer the time, the more fluorescent moieties is produced hence, more intense fluorescence image could be obtained. <xref ref-type="fig" rid="fig1">Figure 1</xref>1 and <xref ref-type="fig" rid="fig1">Figure 1</xref>2 represent the fluorescence image of nanoparticles with different formulation in close contact with collagen and cotton, respectively.</p></sec><sec id="s3_6"><title>3.6. Thermal Response of Synthesized Nanoparticles</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref>3 shows the thermal response of different synthesized nanocomposites at 488 nm (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(a)) and</p><fig-group id="fig10"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Fluorescence of emission wavelengths (a) and the relative intensities (b) of G3, IDA-NP, IDA-10, IDA-Hydr, IDA-NaBH<sub>4</sub> at different excitation wavelengths.</title></caption><fig id ="fig10_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x17.png"/></fig><fig id ="fig10_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x18.png"/></fig></fig-group><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Fluorescence image of a) G3; b) IDA-NaBH<sub>4</sub>; c) IDA-10; d) IDA- Hydr; and e) IDA-NP nanoparticles on the collagen substrate</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x19.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Fluorescence image of a) G3; b) IDA-NaBH<sub>4</sub>; c) IDA-10; d) IDA- Hydr; and e) IDA-NP nanoparticles on the cotton substrate</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x20.png"/></fig><p>514 nm (<xref ref-type="fig" rid="fig1">Figure 1</xref>3(b)) for 5 minutes. Clearly, the highest temperature rise was produced by IDA-NaBH4 at 488 nm and pure Au-NPs at 514 nm due to its proximity to gold surface plasmon resonance (SPR) peak absorption at about 530 nm. It has been reported hat photon excitation of metallic nanostructures leads to production of hot</p><fig-group id="fig13"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> The effect of laser irradiation at two different wavelengths of a) 488 nm and b) 514 nm on thermal behaviour of different synthesized nanoparticles.</title></caption><fig id ="fig13_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x21.png"/></fig><fig id ="fig13_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1190427x22.png"/></fig></fig-group><p>electron cloud which cools down in about 1 ps as a result of heat transfer within the nanoparticle lattice which is then followed by phonon-phonon interactions in 100 ps where the metallic lattice transfers the heat to its surrounding medium and cools down [<xref ref-type="bibr" rid="scirp.58304-ref54">54</xref>] -[<xref ref-type="bibr" rid="scirp.58304-ref59">59</xref>] . The phenomena of energy absorption and increasing the temperature are well known in SPR frequencies where these rapid changes of temperature lead to variety of applications of nanocomposites.</p><p>The temperature distribution around optically-stimulated plasmonic nanoparticles can be described by the following equation [<xref ref-type="bibr" rid="scirp.58304-ref60">60</xref>] :</p><disp-formula id="scirp.58304-formula586"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x23.png"  xlink:type="simple"/></disp-formula><p>where T is the local temperature, and ρ, c, and K represent density, specific heat capacity, and thermal conductivity of material, respectively. Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x24.png" xlink:type="simple"/></inline-formula> is the average heat power dissipated inside the NP and the heat power is given by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x25.png" xlink:type="simple"/></inline-formula>. V<sub>NP</sub> indicated using Equation 3:</p><disp-formula id="scirp.58304-formula587"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x26.png"  xlink:type="simple"/></disp-formula><p>where C is the speed of light, e<sub>Au</sub> and e<sub>w</sub> are the permittivity of gold and water, respectively. This definition obtained from the original formula [<xref ref-type="bibr" rid="scirp.58304-ref61">61</xref>] :</p><disp-formula id="scirp.58304-formula588"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x27.png"  xlink:type="simple"/></disp-formula><p>s<sub>abs</sub> is the optical absorption cross section of the gold nanoparticles and I is the intensity of incoming light.</p><disp-formula id="scirp.58304-formula589"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x28.png"  xlink:type="simple"/></disp-formula><p>And</p><disp-formula id="scirp.58304-formula590"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x29.png"  xlink:type="simple"/></disp-formula><p>After a transient evolution, materials reach steady state temperature profile under CW illumination. Dimensional analysis of the two diffusion equations demonstrates two time scale of the system:</p><disp-formula id="scirp.58304-formula591"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x30.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.58304-formula592"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x31.png"  xlink:type="simple"/></disp-formula><p>where k = K/ρc is thermal diffusivity (m<sup>2</sup>∙s<sup>−1</sup>), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x32.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x33.png" xlink:type="simple"/></inline-formula> represent the characteristic times associated with the evolution of the temperature profile in the surrounding water and inside Au-NP, respectively. Thermalization inside the nanoparticle happens much faster than the water, as k<sub>Au</sub> is far greater than k<sub>w</sub>. Hence, the best consideration of reaching comprehensive temperature profile of the total system is directed by the time scale <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1190427x34.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.58304-ref61">61</xref>] .</p><p>In the final steady state regime, Equation (2) reduces to:</p><disp-formula id="scirp.58304-formula593"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x35.png"  xlink:type="simple"/></disp-formula><p>This equation is formally equivalent to Poisson’s equation and produces a profile of temperature increase ΔT given by a Coulomb potential outside the particle [<xref ref-type="bibr" rid="scirp.58304-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref58">58</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref62">62</xref>] .</p><disp-formula id="scirp.58304-formula594"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x36.png"  xlink:type="simple"/></disp-formula><p>Substituting the Equation (3) in Equation (10), it gives the temperature increase at the surface of nanoparticle (i.e. r = R),</p><disp-formula id="scirp.58304-formula595"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1190427x37.png"  xlink:type="simple"/></disp-formula><p>here R represents the nanoparticle’s radius and I is the intensity of incident beam. Equation (11) shows that temperature of the system containing plasmonic nanoparticles is proportional to the square of the nanoparticle radius, i.e. ΔT &#181; R<sup>2</sup>. As the TEM results show, the use of sodium borohydrate as a reducing agent produced clusters of Au-NPs which consists a greater particle size than the other formulation. Based on above analysis we expect to obtain a higher temperature in IDA-NaBH<sub>4</sub> shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>3. Also this figure indicates that IDA-Hydr formulation leads to the least significant changes in temperature which could be described by its smaller particles size compare to other gold containing formulations. Furthermore, it was shown that temperature of NP changes with regard to their exciting wavelengths and hence the maximum spectral position of the plasmonic band [<xref ref-type="bibr" rid="scirp.58304-ref49">49</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref58">58</xref>] [<xref ref-type="bibr" rid="scirp.58304-ref60">60</xref>] i.e., the temperature drastically decreases at both lower and higher wavelengths. As IDA nanoparticles contain clusters, their plasmonic peak may be obtained at 320 nm. The thermal analysis indicates that at shorter exciting wavelengths, these nanocomposites produce more heat than the longer wavelengths and on the other hand longer wavelengths cause more temperature increase in the case of pure Au-NPs. This lies on the fact that the shorter exciting wavelength (488 nm) is closer to the plasmonic band of the Au-NPs than 514 nm.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>Gold-magneto dendrimer nanocomposites were prepared using two different reducing agents and pre-synthe- sized Au-NP. To the best of our knowledge, there was no evidence of the in-situ monitoring of the Au-NP formation which was done in this study. WDX, XRD, and FTIR analysis of the nanocomposites indicated the simultaneous presence of magnetite and gold phase in the materials. Also, the WDX and TEM results suggest that the use of hydrazine sulfate as a reducing agent can both produce a uniform structure and load higher degree of Au-NPs in the materials. LIF spectroscopy and fluorescent microscopy results confirmed that synthesized metal/dendrimer nanocomposites could fluorescently dye biopolymers such as cotton and collagen. The interaction of 488 nm and 514 nm wavelengths with the all three nanocomposite media resulted in temperature increase with IDA-NaBH<sub>4</sub> and IDA-Hydr showing the highest and the lowest temperature at 488 nm respectively. At 514 nm, however, pure-Au NP synthesized by hydrazine sulfate exhibited the highest heating effect which was closer to its maximum absorption peak of plasmonic band. Considering the outcomes of these experiments, we suggest that these novel nanocomposites can be employed as biomarker and therapeutic agents based on their magnetic, fluorescence and SPR-based optothermal properties.</p></sec><sec id="s5"><title>Cite this paper</title><p>MaryamTajabadi,Mohammad E.Khosroshahi,ShahinBonakdar, (2015) Imaging and Therapeutic Applications of Optical and Thermal Response of SPION-Based Third Generation Plasmonic Nanodendrimers. Optics and Photonics Journal,05,212-226. doi: 10.4236/opj.2015.57021</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.58304-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Pankhurst, Q., Connolly, J., Jones, S. and Dobson, J. 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