<?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">MSA</journal-id><journal-title-group><journal-title>Materials Sciences and Applications</journal-title></journal-title-group><issn pub-type="epub">2153-117X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msa.2018.911065</article-id><article-id pub-id-type="publisher-id">MSA-88184</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>
 
 
  Optimization of 6,13Bis(triisopropylsilylethynyl)pentacene (TIPS-Pentacene) Organic Field Effect Transistor: Annealing Temperature and Solvent Effects
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Diallo</surname><given-names>Abdoul Kadri</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>Diallo</surname><given-names>Abdou Karim</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>Mané</surname><given-names>Seck</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kobor</surname><given-names>Diouma</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>Pasquinelli</surname><given-names>Marcel</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Gaston Berger University, Department of Applied Physics, Saint Louis, Senegal</addr-line></aff><aff id="aff3"><addr-line>OPTO-PV Group/Institut Matériaux Microélectronique Nanosciences de Provence (IM2NP), Marseille, France</addr-line></aff><aff id="aff1"><addr-line>Laboratoire de Chimie et de Physique des Matériaux (LCPM), Assane Seck University, Ziguinchor, Senegal</addr-line></aff><pub-date pub-type="epub"><day>10</day><month>10</month><year>2018</year></pub-date><volume>09</volume><issue>11</issue><fpage>900</fpage><lpage>912</lpage><history><date date-type="received"><day>28,</day>	<month>August</month>	<year>2018</year></date><date date-type="rev-recd"><day>27,</day>	<month>October</month>	<year>2018</year>	</date><date date-type="accepted"><day>30,</day>	<month>October</month>	<year>2018</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 contribution, we report on the effect of solvents with different boiling points and annealing temperature on the performance of TIPS-pentacene transistors. Several solvents have been used for TIPS-pentacene thin film processing: toluene, chlorobenzene and tetrahy-drofuran. To study the influence of solvent and temperature; the electrical parameters of TIPS-pentacene field effect transistor were measured. The highest values of mobilities were 7.1 
  &#215; 10<sup>-3</sup> cm
  <sup>2</sup>
  &#183;V
  <sup>-1</sup>
  &#183;s
  <sup>-1</sup>, 
  4.5 &#215; 10
  <sup>-3 </sup>cm
  <sup>2</sup>&#183;V
  <sup>-1</sup>&#183;s
  <sup>-1</sup> and 1.43 
  &#215; 10<sup>-3</sup> cm
  <sup>2</sup>&#183;V
  <sup>-1</sup>&#183;s
  <sup>-1</sup> respectively for TIPS-pentacene field effect transistor using chlorobenzene, toluene and tetrahydrofuran and annealed respectively at 120
  &#176;C, 150
  &#176;C and 120
  &#176;C. We have correlated these electrical performances with AFM images in order to point out the role of morphological properties. It is found that the grain size, and roughness highly affect the electrical parameters.
 
</p></abstract><kwd-group><kwd>Tips-Pentacene</kwd><kwd> Transistor</kwd><kwd> Solvent</kwd><kwd> Annealing Temperature</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Organic field-effect transistors (OFETs) have gained recently a lot of attraction in organic electronics. Since they achieve a good performance comparable to amorphous silicon (a-Si-H), organic transistors play a key role in next generation of electronic devices. Organic materials such as polymers and small molecules have potential advantages as active layers in the field-effect transistors (FETs) due to processable solution that allows them low-cost, large area and compatibility with flexible substrates [<xref ref-type="bibr" rid="scirp.88184-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref3">3</xref>] . Recently, many efforts have been done to making crystalline organic semiconducting thin films from solution for the use of organic field-effect transistor [<xref ref-type="bibr" rid="scirp.88184-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref5">5</xref>] . Small molecule like 6,13-Bis(triisopropylsilyl)pentacene (TIPS-Pentacene) has gained a lot of consideration due to its environmental stability [<xref ref-type="bibr" rid="scirp.88184-ref6">6</xref>] , its solubility in organic solvents [<xref ref-type="bibr" rid="scirp.88184-ref3">3</xref>] and its high field effect mobility higher than 1 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup> [<xref ref-type="bibr" rid="scirp.88184-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref8">8</xref>] . Solution-processed organic semiconductor active layers are highly interesting mostly in low-coast manufacturing approaches are needed. Hence several works have been done on TIPS-pentacene as active layer of electronics devices. Several studies were achieving to improve the performance of TIPS-pentacene organic field-effect transistors [<xref ref-type="bibr" rid="scirp.88184-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref12">12</xref>] . From those researches, one can identify the influence of process parameters in the performances of organic transistors. Even spin coating [<xref ref-type="bibr" rid="scirp.88184-ref13">13</xref>] , dip coating [<xref ref-type="bibr" rid="scirp.88184-ref14">14</xref>] and Ink-jet printing [<xref ref-type="bibr" rid="scirp.88184-ref15">15</xref>] are currently the most widely used solution processing method in organic electronics, many other technics have been used to improve the crystalline film growth [<xref ref-type="bibr" rid="scirp.88184-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref16">16</xref>] . Previous studies show that charge transport properties of organic semiconductor are widely dependent on their crystal structure and morphology [<xref ref-type="bibr" rid="scirp.88184-ref17">17</xref>] - [<xref ref-type="bibr" rid="scirp.88184-ref24">24</xref>] . In solution process, most of organic semiconductors require dissolution in organic solvent. Consequently, various works have done to explore the effect of annealing temperature [<xref ref-type="bibr" rid="scirp.88184-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref29">29</xref>] and solvent influence on the thin film morphology and crystallinity [<xref ref-type="bibr" rid="scirp.88184-ref30">30</xref>] - [<xref ref-type="bibr" rid="scirp.88184-ref35">35</xref>] . It is well known that processing conditions impacted the electrical performances and especially when solvents and temperature are involved.</p><p>In this paper we study the influence of solvent and annealing temperature in TIPS-pentacene organic transistor. For that purpose three different solvents, chlorobenzene (CB), toluene and tetrahydrofuran (THF), have been used to dissolve the organic material. The temperature for post fabrication annealing was also chosen from non-annealing (as-prepared) to temperature above the boiling point of all solvents. In order to understand the electrical parameters change, we have correlated the electrical performances to thin film morphology by using atomic force microscopic (AFM) It turns out that the highest value of mobility was obtained with Toluene and chlorobenzene solvents at T = 150˚C and 120˚C respectively.</p></sec><sec id="s2"><title>2. Experimental</title><p>We used a prefabricated bottom-gate/bottom-contact (BG-BC) structure (as seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>) from Fraunhofer IPMS. N-doped silicon (doping at wafer surface n~3.10<sup>17</sup> cm<sup>−3</sup>) are used as gate electrode with 230 nm of SiO<sub>2</sub> (thermal oxidation) as dielectric. 30 nm Au with 10 nm high work function adhesion layer</p><p>(ITO) was deposited on wafer for source and drain contacts. All characterized OFETs present a channel length (L) of 20 &#181;m and a width (W) of 10 mm. The devices fabrications begun by the classic steps of cleaning of substrates: sonication in detergent (15 min), acetone (15 min) and isopropyl alcohol (15 min) and deionized water. The substrates were then dried in a UV-Ozone for 15 min to remove organic residuals.</p><p>The organic material 6,13 bis(triisopropylsilylethynyl)-pentacene (TIPS-pen-tacene) was purchased from OSSILA. Three solutions for different solvents were prepared. 15 mg of TIPS-pentacene was dissolved in 1 ml of each solvent (CB, toluene and THF). Each solution was stirring for 24 h at 40˚C to dissolve completely the organic material. The hexamethyldisilazane (HMDS) treatment is performed first to ensure a uniform adhesion of the film and solution dewetting on the substrate. 70 &#181;l of TIPS-pentacene solution is deposited on Si/SiO<sub>2</sub> substrate by spin coating to form thin film in two steps: the first one at 2000 rpm for 120 s and the second one at (2500 rpm for 60 s). And then samples are annealed for 10 min before characterization. The chosen annealing temperature was 50˚C, 80˚C, 100˚C, 120˚C and 150˚C, although we only showed the electrical characteristics of transistor devices for three different temperatures. The thickness of each TIPS-pentacene film was determined by a surface profiler BRUKER DektakXT. Optical proprieties are investigated by using a UV-visible spectrophotometer Perkin Elmer (150 mm InGaAs sphere). The morphology of thin film deposited on SiO<sub>2</sub> was studied by using an XE-100 Atomic Force Microscopic (AFM)electrical characterization was performed by using KEITHLEY 4200-SCS semiconductor characterization system in a glovebox with controlled atmosphere.</p><p>The mobility &#181; was extracted from the saturation region of the transfer curves with the equation:</p><p>I D , s a t = W 2 L μ C i ( V G − V T h ) 2 (1)</p><p>where I D , s a t is drain current in the saturation regime, W/L is the width to length ratio, C<sub>i</sub> is the capacitance per unit area, V<sub>G</sub> the gate voltage and V T h the threshold voltage.</p></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Effect of Solvent and Temperature on Optical Properties</title><p>Optical experiment provides a good way to examine the properties of semiconductors. Measuring the absorption for various wavelength gives information about the band gap of the material, which is important for understanding the optical (electrical) properties of the semiconductors. Measurement are performed at room temperature on 60.5 nm, 88.56 nm and 250.0 nm of TIPS-pentacene film respectively from toluene, chlorobenzene (CB) and tetrahydrofuran (THF) as solvent.</p><p>Figures 2(a)-(c) show the absorption spectra of TIPS-pentacene thin film respectively for toluene, CB and THF as solvents.</p><p>The absorption curves shows that the absorption rate is higher in TIPS-pentacene thin film cast from tetrahydrofuran film (<xref ref-type="fig" rid="fig2">Figure 2</xref>(c)) than TIPS-pentacene film from toluene and chlorobenzene as solvent.</p><p>The absorptions spectra show intense peaks in redshift between 660 nm and 680 nm. These peaks are attributed to electronic transition between the HOMO and the LUMO states and correspond to optical band gap wavelength [<xref ref-type="bibr" rid="scirp.88184-ref36">36</xref>] . From the <xref ref-type="fig" rid="fig2">Figure 2</xref>, there is no shift in the absorption spectra. It is just observed a small enhancement of the absorption rate in the case of toluene as solvent before and after thermal annealing. The increase in the absorption could be recognized as a better molecular organization in the annealed samples [<xref ref-type="bibr" rid="scirp.88184-ref28">28</xref>] which is confirmed by our AFM images of thin films from the three solvents.</p><p><xref ref-type="table" rid="table1">Table 1</xref> shows the optical band gap values of TIPS-pentacene for different annealing temperatures and for the three using solvents. By estimating the wavelength at the absorption edge in the absorption spectra, it is possible to calculate the optical band gap of TIPS-pentacene.</p><p>Optical band gap energy is obtained from the wavelength of the most intense peak by using Planck’s equation:</p><p>E g = 1240 λ ( n m ) (2)</p><p>where λ correspond to the threshold absorption wavelength in the spectra and E<sub>g</sub> the optical band gap.</p><p>Vibronic bands in absorption spectra of TIPS-pentacene films show the influence of solvent, with relative intensities of the bands varied depending on the film thickness and the surface of the film. For example, films deposited with toluene as solvent, the absorption increase by increasing the annealing temperature, which correlates the absorption and the morphology. TIPS-pentacene films cast from toluene as solvent are better organized when the temperature increase. In contrast, the influence of temperature in THF as solvent in TIPS-pentacene thin films absorption is more visible compare to other solvents. Indeed one can see that the film’s absorption increase as well as the temperature increases. These results suggest that the absorption depends only on film structure and</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Optical band gap of TIPS-pentacene thin film obtained from different temperatures and solvent</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Solvents T (˚C)</th><th align="center" valign="middle" >Toluene</th><th align="center" valign="middle" >CB</th><th align="center" valign="middle" >THF</th></tr></thead><tr><td align="center" valign="middle" >Eg (eV)</td><td align="center" valign="middle" >Eg (eV)</td><td align="center" valign="middle" >Eg (eV)</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >1.68</td><td align="center" valign="middle" >1.69</td><td align="center" valign="middle" >1.67</td></tr><tr><td align="center" valign="middle" >80</td><td align="center" valign="middle" >1.67</td><td align="center" valign="middle" >1.67</td><td align="center" valign="middle" >1.68</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.69</td><td align="center" valign="middle" >1.70</td><td align="center" valign="middle" >1.67</td></tr><tr><td align="center" valign="middle" >120</td><td align="center" valign="middle" >1.72</td><td align="center" valign="middle" >1.72</td><td align="center" valign="middle" >1.69</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >1.68</td><td align="center" valign="middle" >1.72</td><td align="center" valign="middle" >1.67</td></tr></tbody></table></table-wrap><p>morphology in samples using toluene as solvent while in THF solvent, the annealing influence may be considered. This study shows that all values of the optical band gap are close to 1.6 eV or 1.81 eV [<xref ref-type="bibr" rid="scirp.88184-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref39">39</xref>] and less than that (1.91 eV) given by Saeed et al. [<xref ref-type="bibr" rid="scirp.88184-ref40">40</xref>] .</p></sec><sec id="s3_2"><title>3.2. Influence of Solvent and Annealing in Morphology and Electrical Performance</title><p>The AFM results of the non-annealed and annealed samples have been investigated to obtain a better insight into the topographical changes as a result of the thermal annealing treatment and solvent effect. The AFM images of the TIPS-pentacene thin film deposited by toluene, chlorobenzene and tetrahydrofuran are respectively shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. It shows 1 &#181;m &#215; 1 &#181;m AFM topographic images of the TIPS-pentacene thin films before and after post fabrication thermal annealing at 120˚C and 150˚C.</p><p>From the AFM images of Figures 3(a)-(c), it is clearly observed the effect of postfabrication thermal treatment. The grain size in toluene’s case increases with temperature: 72 nm for non-annealed 70 nm for heated at 120˚C and 151 nm for annealed at 150˚C. The grain size of TIPS-pentacene in CB is 191 nm, 61 nm and 96 nm for as-prepared, 120˚C and 150˚C. And for THF, the grain sizes are 29.9 nm, 49 nm, and 82 nm respectively for non-annealed, 120˚C and 150˚C. The non-annealed film exhibits many small projections and has a grain size of less than 30 nm (<xref ref-type="fig" rid="fig3">Figure 3</xref>(c): non-annealed). The largest of crystal grain suggesting that during thermal annealing, some adjacent TIPS-pentacene grains in the non-annealed or annealed at 120˚C film join together via a recrystallization process. Several works show postfabrication thermal annealing influence in grain size that could improve electrical performance [<xref ref-type="bibr" rid="scirp.88184-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref41">41</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref42">42</xref>] . The roughness (RMS) of spin-coated film from toluene decreased when increasing postfabrication annealing temperature. <xref ref-type="fig" rid="fig4">Figure 4</xref> shows the output and transfer characteristics of a Bottom-Gate/Bottom-Contact (BG/BC) TIPS-pentacene FETs cast respectively from toluene, chlorobenzene and tetrahydrofuran as solvent. The organic transistors operate in the accumulation mode since the gate electrode is biased negatively with respect to the grounded source electrode. Drain current (I<sub>D</sub>) is almost linear with drain voltage at low V<sub>D</sub>, whereas it tends to</p><p>saturate at higher drain voltage due to the pinch off of the accumulation layer. For all electrical output characteristics (<xref ref-type="fig" rid="fig4">Figure 4</xref>) we clearly observed a linear and saturation regime confirming a field effect behaviour despite the contact resistance effect appears at the origin when temperature increases.</p><p>In the case of toluene as solvent, the field effect mobility was 1.2 &#215; 10 − 3 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup>, 1.5 &#215; 10 − 3 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup> and 4.5 &#215; 10 − 3 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup> respectively for no-annealed and for thermal annealed at 120˚C and 150˚C. The saturation mobilities were 2.1 &#215; 10 − 5 cm<sup>2</sup>∙V<sup>−1</sup>.s<sup>−1</sup>, 7.1 &#215; 10 − 3 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup>, 1.34 &#215; 10 − 4 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup> and 1.41 &#215; 10 − 4 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup>, 1.43 &#215; 10 − 3 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup>, 5.13 &#215; 10 − 4 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup> respectively for CB and THF at non-annealed, 120˚C and 150˚C. The slight increase of the mobility could be explained by thermal organisation of film morphology after annealing. The field-effect mobility increases with decreasing the surface roughness (RMS 16.65 nm at 150˚C for toluene, 27.51 nm at 120˚C for CB and 37.08 nm at 120˚C for THF) (<xref ref-type="table" rid="table2">Table 2</xref>).</p><p>From this table one could observe the evolution of the surface roughness with grain size depending on the annealing temperature. From <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(c), one could observe the instability of device performance with decreasing of drain current when the annealing temperature is above 120˚C. As it is shown by Kim et al. [<xref ref-type="bibr" rid="scirp.88184-ref30">30</xref>] this instability is induced by solvent impurities. The presence of impurities or additional ions at the semiconductor/dielectric interface might induce positive threshold voltage shift observed in devices with CB and THF. This phenomenon is commonly observed in solution processed p-type OFETs in which absorbed water molecules could influence the charge transport. The TIPS-pentacene devices using toluene present negative threshold voltage. At high temperature-temperature above the boiling point of those solvents―the polar atom of the solvent could be ionised and affect the interface of conduction channel. The drain current decrease could also be explained by the contact resistance effect appearing at the origin of the characteristic. The solvent could also influence the field-effect mobility. Kim et al. [<xref ref-type="bibr" rid="scirp.88184-ref32">32</xref>] showed that the field-effect mobility increases when the solvent polarity is increased. Many studies showed</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Electrical parameters of OFETs and film morphological properties</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Solvents</th><th align="center" valign="middle" >Temperature</th><th align="center" valign="middle" >&#181; (10<sup>−3</sup> cm<sup>2</sup>∙V<sup>−</sup><sup>1</sup>∙s<sup>−</sup><sup>1</sup>)</th><th align="center" valign="middle" >V<sub>Th</sub> (V)</th><th align="center" valign="middle" >I<sub>on</sub>/I<sub>off</sub></th><th align="center" valign="middle" >RMS (nm)</th><th align="center" valign="middle" >Grain size (nm)</th></tr></thead><tr><td align="center" valign="middle"  rowspan="3"  >Toluene</td><td align="center" valign="middle" >Non-annealed</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >−2.5</td><td align="center" valign="middle" >8∙10<sup>3</sup></td><td align="center" valign="middle" >20.41</td><td align="center" valign="middle" >72</td></tr><tr><td align="center" valign="middle" >120˚C</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >−6.2</td><td align="center" valign="middle" >10<sup>3</sup></td><td align="center" valign="middle" >22.4</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >150˚C</td><td align="center" valign="middle" >4.5</td><td align="center" valign="middle" >−4.3</td><td align="center" valign="middle" >7∙10<sup>2</sup></td><td align="center" valign="middle" >16.65</td><td align="center" valign="middle" >151</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >CB</td><td align="center" valign="middle" >Non-annealed</td><td align="center" valign="middle" >0.021</td><td align="center" valign="middle" >6.8</td><td align="center" valign="middle" >10<sup>4</sup></td><td align="center" valign="middle" >57.79</td><td align="center" valign="middle" >191</td></tr><tr><td align="center" valign="middle" >120˚C</td><td align="center" valign="middle" >7.1</td><td align="center" valign="middle" >−2.4</td><td align="center" valign="middle" >10<sup>3</sup></td><td align="center" valign="middle" >27.51</td><td align="center" valign="middle" >61</td></tr><tr><td align="center" valign="middle" >150˚C</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >−2.5</td><td align="center" valign="middle" >18.7</td><td align="center" valign="middle" >34.01</td><td align="center" valign="middle" >96</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >THF</td><td align="center" valign="middle" >Non-annealed</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >6.1</td><td align="center" valign="middle" >2.2∙10<sup>3</sup></td><td align="center" valign="middle" >13.67</td><td align="center" valign="middle" >29.9</td></tr><tr><td align="center" valign="middle" >120˚C</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.2∙10<sup>3</sup></td><td align="center" valign="middle" >37.08</td><td align="center" valign="middle" >49</td></tr><tr><td align="center" valign="middle" >150˚C</td><td align="center" valign="middle" >0.51</td><td align="center" valign="middle" >2.2</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >63.07</td><td align="center" valign="middle" >82</td></tr></tbody></table></table-wrap><p>how annealing could affect the morphology of film by creating cracks when solvent is removed consequently the charge carries transport is affected [<xref ref-type="bibr" rid="scirp.88184-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.88184-ref43">43</xref>] . With a boiling point of 66˚C for THF, film obtained from THF used as solvent is rough and disorganized with small grain size. This behavior could be attributed to a rapid solidification of the deposited film. In contrast to high boiling point solvent, the material crystallizes better when increasing temperature with well-ordered film. Toluene and chlorobenzene have respectively 111˚C and 132˚C as boiling point. So the film has sufficient time to be well organized. This could explain the highest value 7.1 &#215; 10 − 3 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup> obtained for OFETs fabricated from chlorobenzene annealed at 120˚C and 4.5 &#215; 10 − 3 cm<sup>2</sup>∙V<sup>−1</sup>∙s<sup>−1</sup> at 150˚C for the toluene using as solvents.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>In summary, we report solvent and temperature effects on performance of TIPS-pentacene usingtoluene, chlorobenzene and tetrahydrofuran with different boiling points. The optical band gap of TIPS-pentacene is not affected by the annealing temperature and solvent. In contrast the electrical parameters are highly affected by the solvent and annealing temperature. We found that increasing annealing temperature led to increase the field effect mobility. This observation suggests a crystalline structure organisation in TIPS-pentacene semiconductor depending on temperature and used solvent. The processing conditions being highly crucial for device performance, it is well desired in these conditions to take into account solvent and temperature annealing in solution-processed organic transistor. This study confirms and points out the role of slow evaporation rate in solvent and annealing temperature which are of outmost prominence to improve molecular organisation and promote charge transport in organic semiconductor. Transistor devices using Toluene and chlorobenzene as solvents exhibited better performances.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Kadri, D.A., Karim, D.A., Seck, M., Diouma, K. and Marcel, P. (2018) Optimization of 6,13Bis(triisopropylsilylethynyl)pentacene (TIPS-Pentacene) Organic Field Effect Transistor: Annealing Temperature andSolvent Effects. Materials Sciences and Applications, 9, 900-912. https://doi.org/10.4236/msa.2018.911065</p></sec></body><back><ref-list><title>References</title><ref id="scirp.88184-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Feng, L., Tang, W., Zhao, J., Cui, Q., Jiang, C. and Guo, X. (2014) All-Solution-Processed Low-Voltage Organic Thin-Film Transistor Inverter on Plastic Substrate. 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