<?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">AJAC</journal-id><journal-title-group><journal-title>American Journal of Analytical Chemistry</journal-title></journal-title-group><issn pub-type="epub">2156-8251</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajac.2012.38069</article-id><article-id pub-id-type="publisher-id">AJAC-21907</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>
 
 
  Interaction of N-(2-Methyl Thio Phenyl)-2-Hydroxy-1-Naphthaldimine with Tin Dioxide Nanoparticles: A Spectroscopic Approach
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uvetha</surname><given-names>Rani Jayaprakash</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ramakrishnan</surname><given-names>Veerabahu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Laser Studies, School of Physics, Madurai Kamaraj University, Madurai – 625 021, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>nsuvetha@yahoo.co.in(URJ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>22</day><month>08</month><year>2012</year></pub-date><volume>03</volume><issue>08</issue><fpage>518</fpage><lpage>523</lpage><history><date date-type="received"><day>May</day>	<month>16,</month>	<year>2012</year></date><date date-type="rev-recd"><day>June</day>	<month>17,</month>	<year>2012</year>	</date><date date-type="accepted"><day>June</day>	<month>28,</month>	<year>2012</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 interaction of N-(2-methyl thiophenyl)-2-hydroxy-1-naphthaldimine (NMTHN) with tin dioxide nanoparticles (SnO
  <sub>2</sub> NPs) has been investigated by spectroscopic tools such as absorption and fluorescence spectroscopy. Absorption spectroscopy reveals the formation of ground state complex. Fluorescence spectroscopy has been used to study the signatures of fluorescence quenching. SnO
  <sub>2</sub> NPs are found to quench the intrinsic fluorescence of NMTHN via static and dynamic quenching. The deviation from linearity in the Stern-Volmer plot has been observed.
 
</p></abstract><kwd-group><kwd>N-(2-Methyl Thiophenyl)-2-Hydroxy 1-Naphthaldimine; Tindioxide Nanoparticles; Optical Absorption; Fluorescence Quenching</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Owing to their potential application in solar energy conversion, semiconductor nanoparticles have been extensively studied from both experimental and theoretical viewpoints [1-4]. Variety of techniques including spectroscopy, microscopy and X-ray techniques has been used to characterize the properties of nanoparticles. Most of the studies have been focused on their equilibrium properties such as absorption and emission, particle shape, surface structure, inter particle interaction, self assembly, and formation of superlattices [<xref ref-type="bibr" rid="scirp.21907-ref5">5</xref>]. Tindioxide (SnO<sub>2</sub>) is a n-type metal oxide semiconductor with the wide bandgap of 3.6 eV. Because of its remarkable electrical, optical and electrochemical properties, SnO<sub>2</sub> serves a wide range of applications in solar cells, catalytic supporting materials, transparent electrodes and solid state chemistry [<xref ref-type="bibr" rid="scirp.21907-ref6">6</xref>]. The higher electron mobility (~100 - 200 cm<sup>2</sup>&#183;v<sup>–</sup><sup>1</sup>&#183;s<sup>–</sup><sup>1</sup>) of SnO<sub>2</sub> NPs proposes a faster diffusion of photo induced electrons in SnO<sub>2</sub> and its larger band gap would be creating fewer oxidation holes in the valence band. Thus low sensitivity of SnO<sub>2</sub> to UV degradation facilitates the long-term stability of dye senstitized solar cells. The low isoelectric point (at pH 4 - 5) of SnO<sub>2</sub> leads to less absorption of the dye with acidic carboxyl groups [7,8]. The ability of organic dyes to sensitize large band gap semiconductor materials has been used for the design of light energy conversion devices [<xref ref-type="bibr" rid="scirp.21907-ref9">9</xref>]. Schiff bases play an important part in the development of co-ordination chemistry. The common structural feature of these compounds is the azomethine group with a general formula RHC=N-R’, where R and R’ are alkyl, aryl, cyclo alkyl or heterocyclic group which may be variously substituted. They are easily prepared in general by the condensation reaction of primary amines with carbonyl compounds [<xref ref-type="bibr" rid="scirp.21907-ref10">10</xref>]. In the field of co-ordination chemistry, Schiff bases from 2-hydroxy 1-napthaldehyde have been used as chelating ligands. N-H…O (keto form) and N…H-O (enol form) are the two types of intra molecular hydrogen bonds in Schiff bases. Both types of hydrogen bonds were found in the aldimine compounds derived from 2-hydroxy 1-Naphthaldehyde [<xref ref-type="bibr" rid="scirp.21907-ref11">11</xref>]. The existence of tautomerism between these two types of bonds created a great interest in 2-hydorxy Schiff base ligands. The ortho hydroxyl naphthalidene anilines show two bands above 400 nm in the visible region which are assigned to the keto form. In naphthaldimines both forms keto/enolimino are possible and O-H…N or N-H…O intra molecular hydrogen bonds can occur [<xref ref-type="bibr" rid="scirp.21907-ref12">12</xref>]. If combined with chelating activities, Schiff base may become a promising dye sensitizer in molecular photovoltaic cells [<xref ref-type="bibr" rid="scirp.21907-ref13">13</xref>].</p><p>Semiconducting oxides such as TiO<sub>2</sub> and SnO<sub>2</sub> directly interact with the excited dye molecules thus inducing heterogeneous electron transfer at the semiconductor/dye interface. This interesting property of sensitizing dyes is useful in the design of photochemical solar cells.</p><p>A process which decreases the fluorescence intensity of a given substance is known as quenching. It may also result from a photo-induced electron transfer process between the excited dye and the nanoparticles. Our group has studied spectral investigation of NMTHN by silver nanoparticle using fluorescence quenching [<xref ref-type="bibr" rid="scirp.21907-ref14">14</xref>]. Although there are many studies on the photochemical and fluorescence behavior of organic dyes on SnO<sub>2</sub> thin film, there is none for SnO<sub>2 </sub>NPs on the fluorescence quenching of Schiff base in methanol medium [15-18]. In the present study, using optical absorption and fluorescence emission techniques the effect of SnO<sub>2 </sub>NPs on NMTHN has been investigated.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Materials</title><p>All chemicals that are used in this work were obtained from Merck with 99.9% purity and also used without further purification. The procedure of synthesis of NMTHN (<xref ref-type="fig" rid="fig1">Figure 1</xref>) is described as follows [<xref ref-type="bibr" rid="scirp.21907-ref14">14</xref>].</p><p>2-hydroxy 1-napthldehyde (1.72 g, 10 mmol) was dissolved in alcohol and treated with an alcoholic solution of 2-(methylthio) aniline (1.39 g, 10 mmol). The content of the above solution was kept at room temperature over night. The formation of Schiff base took place slowly with good yield. The pure brownish yellow crystals of the Schiff base was filtered, washed with alcohol and dried.</p><p>SnO<sub>2</sub> nanoparticles used in this study were synthesized as follows: Solution of SnCl<sub>2</sub>&#183;5H<sub>2</sub>O (4.5126 g) of 0.1 M was prepared in the de-ionized water (200 ml) to get a mixed aqueous solution. To this mixed aqueous solution, ammonia solution was added into drop wise under vigorous stirring to get the pH value of the solution in the range of 8 - 9. Now, the precipitate had been formed at the bottom of the glass beaker. For about 2 hours the precipitate was kept at room temperature for ageing and then washed with deionized water. The washing was repeated for a number of 5 - 6 times. The resulting precipitate was heated at 80˚C for about 5 hours. The dried precipitate was kept at 105˚C for 4 hours, and it was loaded into the alumina crucible. Then for about</p><p>5 hours in air it was annealed in a muffle furnace at 600˚C to enhance the crystallinity of SnO<sub>2</sub> NPs and the product appeared as white in color after the heat treatment. The particle size of the resultant product was found as 160 nm using micro Raman spectroscopic technique [<xref ref-type="bibr" rid="scirp.21907-ref19">19</xref>].</p></sec><sec id="s2_2"><title>2.2. Apparatus</title><p>At room temperature using 1cm path length rectangular quartz cell by means of UV-Vis absorption spectrophotometer (Shimadzu UV 2450) and Spectrofluorophotometer (Shimadzu RC 5301-PC), steady state optical absorption and fluorescence emission spectra of the samples were recorded. While the concentration of SnO<sub>2</sub> NPs ranged from 0.5 to 0.9 mM, the concentration of NMTHN in methanol was 0.01 mM throughout the experiment and was precisely maintained the same in all samples. The optical absorption and fluorescent measurements have been repeated for five times for each set of samples. It was noticed that the data are reproducible with an accuracy of &#177;0.1 nm. And hence, there is a good reliability of the data.</p></sec></sec><sec id="s3"><title>3. Results</title><sec id="s3_1"><title>3.1. Absorption Spectroscopy</title><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the UV-Vis absorption spectrum of NMTHN in methanol. The absorption maximum occurs at 441 nm. The entire spectrum undergoes a hyper chromic effect with a little spectral shift (<xref ref-type="fig" rid="fig3">Figure 3</xref>), with each addition of SnO<sub>2</sub> NPs concentration.</p></sec></sec></body><back><ref-list><title>References</title><ref id="scirp.21907-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">R. S. Ningthoujam and S. K. Kulshreshtha, “Nanocrystalline SnO2 from Thermal Decomposition of Tin Citrate Crystal: Luminescence and Raman Studies,” Materials Research Bulletin, Vol. 44, No. 1, 2009, pp. 57-62. 
doi:10.1016/j.materresbull.2008.04.004 </mixed-citation></ref><ref id="scirp.21907-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">S. G. Ansari, P. Boroojerdian, S. R. Sainker, R. N. Karekar, R. C. Aiyer and S. K. Kulkarni, “Grain Size Effects on H2 Gas Sensitivity of Thick Film Resistor Using SnO2 Nanoparticles,” Thin Solid Films, Vol. 295, No. 1-2, 1997, pp. 271-276. doi:10.1016/S0040-6090(96)09152-3</mixed-citation></ref><ref id="scirp.21907-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">X. Peng, M. C. Schlamp, A. V. Kadavanich and A. P. Alivisatos, “Epitaxial Growth of Highly Luminescent CdSe/CdS Core/Shell Nanocrystals with Photostability and Electron Accessibility,” Journal of the American Chemical Society, Vol. 119, No. 30, 1997, pp. 7019-7029.  
doi:10.1021/ja970754m</mixed-citation></ref><ref id="scirp.21907-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">W.-Y. Chung, D.-D. Lee and B.-K. Sohn, “Effects of Added TiO2 on the Characteristics of SnO2 Based Thick Film Gas Sensors,” Thin Solid Films, Vol. 221, No. 1-2, 1992, pp. 304-310. doi:10.1016/0040-6090(92)90832-V</mixed-citation></ref><ref id="scirp.21907-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">J. Z. Zhang, “Intefacial Charge Carrier Dynamics of Colloidal Semiconductor Nanoparticles,” Journal of Phy- sical Chemistry B, Vol. 104, No. 31, 2000, pp. 7239- 7253. doi:10.1021/jp000594s</mixed-citation></ref><ref id="scirp.21907-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">S. Ferrere, A. Zaban, and B. A. Gregg, “Dye Sensitization of Nanocrystalline Tin Oxide by Perylene Derivatives,” Journal of Physical Chemistry B, Vol. 101, No. 23, 1997, pp. 4490-4493. doi:10.1021/jp970683d</mixed-citation></ref><ref id="scirp.21907-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">J. F. Qian, P. Liu, Y. Xiao, Y. Jiang, Y. L. Cao, X. P. Ai and H. X. Yang, “TiO2 Coated Multilayered SnO2 Hollow Microspheres for Dye-Sensitized Solar Cells,” Advanced Materials, Vol. 21, No. 36, 2009, pp. 3663-3667.</mixed-citation></ref><ref id="scirp.21907-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">S. Gubbala, V. Chakrapani, V. Kumar and M. K. Sunkara, “Band Edge Engineered Hybrid Structures for Dye-Sensitized Solar Cells Based on SnO2 Nanowires,” Ad-vanced Functional Materials, Vol. 18, No. 16, 2008, pp. 2411- 2418. doi:10.1002/adfm.200800099</mixed-citation></ref><ref id="scirp.21907-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">S. Das and P. V. Kamat, “Can H-Aggregates Serve as Light Harvesting Antennae? Triplet-Triplet Energy Transfer between Excited Aggregates and Monomer Thionine in Aerosol-OT Solutions,” Journal of Physical Chemistry B, Vol. 103, No. 1, 1999, pp. 209-215.  
doi:10.1021/jp983816j</mixed-citation></ref><ref id="scirp.21907-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">A. Blagus, D. Cincic, T. Friscic, B. Kaitner and V. Stili-novic, “Schiff Bases Derived from Hydroxyaryl Alde-hydes: Molecular and Crystal Structure, Tautomerism, Quinoid Effect, Coordination Compounds,” Macedonian Journal of Chemistry and Chemical Engineering, Vol. 29, No. 2, 2010, pp. 117-138. </mixed-citation></ref><ref id="scirp.21907-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">H. Unver and T. Nuri Durlu, “Crystal Structure and Conformational Analysis of 1-[N-2-Bromophenyl Naphthal- dimine,” Journal of Molecular Structure, Vol. 655, No. 3, 2003, pp. 369-374. doi:10.1016/S0022-2860(03)00277-1</mixed-citation></ref><ref id="scirp.21907-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">A. M. Asiri and K. O. Badahdah, “Synthesis of Some New Anils: Part 1. Reaction of 2-Hydroxy-Benzaldehyde and 2-Hydroxy Naphthaldehyde with 2-Aminopyridene and 2-Aminopyrazine,” Molecules, Vol. 12, 2007, pp. 1796-1804. </mixed-citation></ref><ref id="scirp.21907-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">H. Dincalp, S. Yavuz, O. Hakli, C. Zafer, C. Ozsoy, I. Durucasu and SiddikIcli, “Optical and Photovoltaic Properties of Salicylaldimine Based Azo Ligands,” Journal of photochemistry and Photobiology A: Chemistry, Vol. 210, No. 1, 2010, pp. 8-16.  
doi:10.1016/j.jphotochem.2009.12.012</mixed-citation></ref><ref id="scirp.21907-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">P. Manikandan and V. Ramakrishnan, “Spectral Investigations on N-(2-Methyl Thiophenyl) 2-Hydroxy-1-Na- phthaldimine by Silver Nano-particles: Quenching,” Journal of Fluorescence, Vol. 21, No. 2, 2011, pp. 693-699. 
doi:10.1007/s10895-010-0757-3</mixed-citation></ref><ref id="scirp.21907-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">I. Bedja, S. Hotchandani and P. V. Kamat, “Preparation and Photochemical Characteri-zation of Thin SnO2 Nanocrystalline Semiconductor Films and Their Sensitization with Bis(2,2’-bipyridine) (2,2’-bipyridine-4,4’-dicar-boxylic acid) Ruthenium (II) Com-plex,” Journal of Physical Chemistry, Vol. 98, 1994, pp. 4133-4140.  
doi:10.1021/j100066a037</mixed-citation></ref><ref id="scirp.21907-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">H. J. Snaith and C. Ducati, “SnO2 Based Dye Sensitized Hybrid Solar Cells Exhibiting near Unity Absorbed Photon to Electron Conversion Efficiency,” Nanoletters, Vol. 10, No. 4, 2010, pp. 1259-1265. 
doi:10.1021/nl903809r</mixed-citation></ref><ref id="scirp.21907-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">D. Liu, R. W. Fessenden, G. L. Hug and P. V. Kamat, “Dye Capped Semiconductor Nanoclusters. Role of Back Electron Transfer in the Photosen-sitization of SnO2 Nano- crystallites with Cresyl Violet Aggre-gates,” Journal of Physical Chemistry B, Vol. 101, No. 14, 1997, pp. 2583- 2590. doi:10.1021/jp962695p</mixed-citation></ref><ref id="scirp.21907-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">C. Nasr, D. Liu, S. Hotchandani and P. V. Kamat, “Dye Capped Semiconductor Nanoclusters. Excited State and Photosensitization Aspects of Rhodamine 6G H-Aggre- gates Bound to SiO2 and SnO2 Colloids,” Journal of Physical Chemistry, Vol. 100, No. 26, 1996, pp. 11054- 11061. doi:10.1021/jp9537724</mixed-citation></ref><ref id="scirp.21907-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">P. Sangeetha, V. Sasirekha and V. Ramakrishnan, “Micro Raman Investigation of Tin Dioxide Nanostructured Material Based on Annealing Effect,” Journal of Raman Spectroscopy, Vol. 42, No. 8, 2011, pp. 1634-1639. </mixed-citation></ref><ref id="scirp.21907-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">S. Barazzouk, H. Lee, S. Hotchandani and P. V. Kamat, “Photosensitization Aspects of Pinacyanol H-Aggregates. Charge Injection from Singlet and Triplet Excited States into SnO2 Nanocrystallites,” Journal of Physical Chemistry B, Vol. 104, No. 15, 2000, pp. 3616-3623.  
doi:10.1021/jp994311b</mixed-citation></ref><ref id="scirp.21907-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">I.-Y. S. Lee and H. Suzuki, “Quenching Dynamics Promoted by Silver Nanoparticles,” Journal of Photochemistry and Photobiology A: Chemistry, Vol. 195, No. 2-3, 2008, pp. 254-260.  
doi:10.1016/j.jphotochem.2007.10.009</mixed-citation></ref><ref id="scirp.21907-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">B. Chakraborty and S. Basu, “Interaction of BSA with Proflavin: A Spectroscopic Approach,” Journal of Luminescence, Vol. 129, No. 1, 2009, pp. 34-39.  
doi.10.1016/j.jlumin.2008.07.012</mixed-citation></ref><ref id="scirp.21907-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">J. R. Lakowicz, “Principles of Fluorescence Spectroscopy,” 3rd Edition, Springer Science, New York, 2010.</mixed-citation></ref><ref id="scirp.21907-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">H. M. Suresh Kumar, R. S. Kunabenchi, J. S. Biradar, N. N. Math, J. S. Kadadevarmath and S. R. Inamdar, “Analysis of Fluorescence Quenching of New Indole Derivative by Aniline Using Stern-Volmer Plots,” Journal of Luminescence, Vol. 116, No. 1-2, 2006, pp. 35-42.  
doi.10.1016/j.jlumin.2005.02.012</mixed-citation></ref><ref id="scirp.21907-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">A. J. Cox, A. J. DeWeerd and J. Linden, “An Experiment to Measure Mie and Rayleigh Total Scattering cross Sections,” American Journal of Physics, Vol. 70, No. 6, 2002, pp. 620-625. doi:10.1119/1.1466815</mixed-citation></ref></ref-list></back></article>