Poster Session, Thursday, June 17Humidity Sens<strong>in</strong>g Properties of Copper Phthalocyan<strong>in</strong>e (CuPc) Th<strong>in</strong> FilmsTheme F686 - N1123Özgen SÖKE 1 , Salih OKUR 1 , Nesli T. YAĞMURCUKARDEŞ 11 Izmir Institute of Technology, Faculty of Science, Department of Physics, Gulbahce Koyu Kampusu, 35430, Urla, Izmir, TurkeyAbstract—This study focuses on the humidity adsorption and desorption k<strong>in</strong>etics of copper phthalocyan<strong>in</strong>e (CuPc) nanoparticle th<strong>in</strong> filmprepared by drop cast method, were <strong>in</strong>vestigated by quartz crystal microbalance (QCM) technique. Reproducible experimental results show thatCuPc th<strong>in</strong> films have a great potential for humidity sens<strong>in</strong>g applications at room temperature.Phthalocyan<strong>in</strong>e (Pc) are the subject of a great deal withwide-rang<strong>in</strong>g applications. Copper phthalocyan<strong>in</strong>e (CuPc)th<strong>in</strong> films have potential applications as surfaceconductivity-based gas sensors, solar cells, dyes, field-effecttransistors , and organic light emitt<strong>in</strong>g diodes (OLEDs). Thehumidity adsorption and desorption studies of CuPc is veryimportant for many humidity and gas sens<strong>in</strong>g deviceapplications. In Fig.1 molecular structure of copperphthalocyan<strong>in</strong>e (CuPc) is shown. [1]- [6]F/Hz50-5-10-15-20-25(a)11%22%11%43%22%53%43%53%75%84% 75%84%94% 94%97%-300 1000 2000 3000 4000 5000 6000 7000Time(sec)- F (Hz)100101y = 0.45016 * e^(0.042563x) R= 0.99637y = 1.1664 * e^(0.033464x) R= 0.99547downwardupward0,10 20 40 60 80 100Relative humidity %(RH%)Fig.2 (a and b) The frequency response of Copper phthalocyan<strong>in</strong>e (CuPc)th<strong>in</strong> films covered QCM adsorption–desorption process at fixed po<strong>in</strong>trelative humidity conditions between 11% and 97% RH.(b)Fig.1 Structure of Copper Phthalocyan<strong>in</strong>e (CuPc)50%11 RH%11 RHQuartz crystal microbalance (QCM) is a technique that wasused to analyze the change <strong>in</strong> the resonant frequency. Thisresonant frequency is sensitive to mass changes of thecrystal. In our study, we used QCM with the model ofCHI400A Series from CH, after exposure of the crystalmass load<strong>in</strong>g of water molecules at different humidityenvironments e.g. at 11%, 22%, 43%, 55%, 75%, 84%,94%, 97% relative humidity (RH). [1]- [6]The mass change (Δm) from the measured frequency change(Δf) is calculat<strong>in</strong>g to use Saurbey Equation ;22 f0mf A (1)where f 0 is the resonant frequency of the QCM crystal, ρ isthe density of the crystal, μ is the shear modulus of quartzand A is the area of the gold disk on the crystal.CuPc molecules (99% Purity) were solved <strong>in</strong> toluene with1mg/ml concentration and 5μl of solution were coated ontosurface of QCM by drop-cast<strong>in</strong>g method. After evaporationof toluene, thicknesses of CuPc film was measured as300nm with Dektak 150 profilometer of Veeco.Fig.2 (a) shows the frequency response of copperphthalocyan<strong>in</strong>e (CuPc) film when the relative humidity<strong>in</strong>creased and decreased between 11% and 97% RH for anequal time(400sec) <strong>in</strong>tervals and (b) show how the quartzcrystal microbalance (QCM) frequency changes with<strong>in</strong>creas<strong>in</strong>g and decreas<strong>in</strong>g RH values.F/Hz-5-10-15-20-2522%43%53%75%84%94%97%-300 200 400 600 800 1000120014001600Time(sec)Fig.3 Comparison of frequency shifts between 11% and 97% RH.Fig.3 shows the comparison of QCM frequency shifts for11%, 22%, 43%, 55%, 75%, 84%, 94%, 97% RH values.Our QCM and electrical measurements results show thathumidity sens<strong>in</strong>g properties of Copper Phthalocyan<strong>in</strong>e(CuPc) is very sensitive to humidty changes and reversibleadsorption/desorption behavior which is an <strong>in</strong>dicative of agood humidity sensor even at room temprature.*Correspond<strong>in</strong>g author: salihokur@iyte.edu.tr[1] S. Okur, M. Kus, F. Özel, V. Aybek, M. Yilmaz, Talanta, 81;1-2; 2010;248.[2] F.Young, M. Shte<strong>in</strong>, S.R. Forrest, Nature Mater.4,37,(2005)[3] Caronna, T.; Colleoni, C.; Dotti, S.; Fontana, F.; Rosace, G.J.Photochem. Photobiol., A, 184, 135 (2006)[4] Z. Bao, A. J. Lov<strong>in</strong>ger, and A. Dodabaladur, Appl. Phys. Lett. 69, 3066(1996).[5]Yamashita M, Inui F, Irokawa K, Mor<strong>in</strong>aga A, Tako T, Mito A,ApplSurf Sci, 130, 883 (1998).[6] A. Schmidt, L.K. Chau, A. Back, N.R. Armstrong, C.C. Leznoff, B.P.Lewer (Eds.), Phthalocyan<strong>in</strong>es, Properties and Applications, New York:VCH, 1996. M6th Nanoscience and Nanotechnology Conference, zmir, 2010 697
Poster Session, Thursday, June 17Humidity Sens<strong>in</strong>g Investigation of ZnO Nanostructures Us<strong>in</strong>g QCM TechniqueNurdan Asar 1 , Nesli Tekguzel Yagmurcukardes 2 , Ayse Erol 1 , Salih Okur 2 , M. Cet<strong>in</strong> Arikan 11 Istanbul University Faculty of Science Physics Department 34134 Vezneciler, Istanbul, Turkey2 Izmir Institute of Technology 35430 Urla, Izmir, TurkeyTheme F686 - N1123Abstract: ZnO nanostructures were synthesized via chemical sol-gel method <strong>in</strong> two different morphologies. Their humidity sens<strong>in</strong>g properties were <strong>in</strong>vestigated byus<strong>in</strong>g Quartz Crystal Microbalance (QCM) technique. It was found that the frequency shift of the ZnO nanostructures coated on QCM <strong>in</strong>creases with <strong>in</strong>creas<strong>in</strong>g relativehumidity between 33-77 % at room temperature. The results show that humidity sens<strong>in</strong>g properties are strongly dependent on morphology of the nanostructures.ZnO is one of the most important promis<strong>in</strong>g metal oxidesemiconductors for gas/vapour/humidity sens<strong>in</strong>g applications and haspronounced sensitivity to gases such as NH 3 , NO 2 , CO, H 2 , ethanoland humidity [1-4]. It has been observed that ZnO nanostructuressynthesized <strong>in</strong> different morphologies compared with its th<strong>in</strong> film orbulk counterparts have much more sensitivity due to their highsurface to volume ratio and more chemically active centers [5].In this study we synthesized ZnO nanostructures by us<strong>in</strong>g chemicalsol-gel method. Crystal structure and morphology of ZnOnanostructures synthesized <strong>in</strong> different experimental conditions werecharacterized by X-Ray Diffraction (XRD) and Scann<strong>in</strong>g ElectronMicroscopy (SEM).(a)(a)Samples S2 and S3 were synthesized with different molarities of Zn +2and OH - solutions. Samples dried <strong>in</strong> ambient air for 24 hours. As seenfrom the Figures 1 (a) and (b), the morphology of S2 is nanoparticlewhile the morphology of S3 is nanowire and both structures havediameter as ~ 20 nm. XRD patterns showed that both samples arecrystallized <strong>in</strong> hexagonal wurtzite structure.Humidity sens<strong>in</strong>g <strong>in</strong>vestigations of ZnO nanostructures werecarried out us<strong>in</strong>g Quartz Crystal Microbalance (QCM) technique.Samples dispersed <strong>in</strong> ethanol were dropped on quartz crystal andexposed to various saturated salt solutions. The frequency responsesof the ZnO nanostructure sensors to relative humidity chang<strong>in</strong>gbetween 33-77% RH were measured at room temperature. Relativehumidity was recorded by commercial sensor simultaneously.(b)Figure 2: Frequency responses of S2 and S3 sensors under 33 – 77% relative humidityexposure at room temperature.(c)(d)Figure 2 shows response and recovery curves of the sensors. When%RH was decreased from 77 to 33%, frequencies of the sensors werebackshifted to their <strong>in</strong>itial values. In comparison with nanowires,nanoparticles showed larger frequency shift.The experimental results demonstrated that ZnO nanoparticles aremore sensitive to humidity changes compared to nanowires due tohav<strong>in</strong>g high surface to volume ratio and much more chemically activecenters.This work was supported by Scientific Research ProjectsCoord<strong>in</strong>ation Unit of Istanbul University. Project number 4907.Figure 1: (a-b) SEM images and (c-d) XRD patterns of samples S2 and S3, respectively.[1] Hongsith N., Choopun S., Mangkorntong P.,Mangkorntong N., 2005. CMU. J.Special issue on nanotechnology. vol. 4 No. 1: 15-20.[2] Sadek A. Z., Choopun S., Wlodarski W., Ippolito S. J., Kalantar Zadeh K., 2007.IEEE Sensors Journal. Vol. 7, No. 6.[3] Krishnakumar T., Jayaprakash R., P<strong>in</strong>na N., Donato N., Bonavita A., Micali G. andNeri G., 2009. Sensors & Actuators: B. 143, 198.[4] Qi Q., Zhang T., Yu Q., Wang R., Zeng Y., Liu L., Yang H., 2008. Sensors andActuators B: Chemical. 638-643.[5] Hongsith N., Viriyaworasakul C., Mangkorntong P. , Mangkorntong N. , ChoopunS., 2008 Ceramics International 34: 823–826.6th Nanoscience and Nanotechnology Conference, zmir, 2010 698
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