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ICMCTF 2012! - CD-Lab Application Oriented Coating Development

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spectrophotometer, respectively. Moreover, to analyze the device<br />

characteristics of the SZO:B TFTs, the output and transfer current-voltage<br />

characteristics were measured using a semiconductor parameter analyzer<br />

(4200-SCS, Keithley).<br />

CP-9 Investigation on High-Performance Aluminum Zinc Tin Oxide<br />

Thin Film Transistors, L.F. Teng, P.T. Liu (ptliu@mail.nctu.edu.tw), C.S.<br />

Fuh, National Chiao Tung University, Taiwan, Z.Z. Li, Ming-Hsin<br />

University of Science and Technology,Taiwan<br />

In recent years, amorphous oxide semiconductors (AOSs) are attracted<br />

much attention due to high mobility, low temperature deposition, suitable<br />

for flexible display, transmission, and good uniformity. The thin film<br />

transistors with a-AZTO thin film as the active layer perform higher<br />

mobility and better reliability than conventional hydrogenated amorphous<br />

silicon TFT (a-Si: H TFT). In addition, the uniformity of a-AZTO TFT is<br />

also superior to Low Temperature Polycrystalline Silicon TFT (LTPS TFT).<br />

Therefore, the a-AZTO TFT s have the potential to replace a-Si: H TFTs<br />

and LTPS TFTs for Active Matrix Organic Light Emitting Display<br />

(AMOLED). In this study, we used rf sputter, which is compatible with<br />

industry application and integration, deposit a-AZTO active layer and then<br />

modulated the different processing oxygen flux, and discussed electrical<br />

and optical properties of the device impact.<br />

CP-10 A Magnetization Study of Cobalt Oxide Films Deposited at<br />

Different Temperatures by Pulsed Injection MOCVD Using a β-<br />

Diketonate Complex of Cobalt as the Precursor, L. Apatiga<br />

(apatiga@unam.mx), J. Espindola, N. Mendez, Universidad Nacional<br />

Autónoma de México - Centro de Fisica Aplicada y Tecnología Avanzada,<br />

Mexico<br />

The magnetic response of cobalt oxide films was studied using a vibrating<br />

sample magnetometer system. A strong magnetic susceptibility, which<br />

corresponds to antiferromagnetic spin alignments typical of films with low<br />

chemical inhomogeneities was found. The films were deposited by pulsed<br />

injection MOCVD using a β-diketonate complex of cobalt mixed in a<br />

toluene solution as the precursor, at different temperatures ranging from 650<br />

to 800 °C on silicon substrates (Si (100)). According to the x- ray studies,<br />

the Co3O2 phase was homogeneously deposited along the entire substrate. In<br />

addition, the SEM observations show, together with the FT Raman studies,<br />

a high crystallinity, characteristic of the CVD metallic oxide structures.<br />

CP-11 Investigating the Illuminated Hot-Carrier Effect under DC and<br />

AC operations for InGaZnO Thin-Film Transistors, T.Y. Hsieh, T.C.<br />

Chang (tcchang@mail.phys.nsysu.edu.tw), T.C. Chen, M.Y. Tsai, Y.T. Chen,<br />

National Sun Yat-Sen University, Taiwan, F.Y. Jian, National Chiao Tung<br />

University, Taiwan<br />

This paper investigates the effect of DC and AC hot-carrier stress under<br />

light illumination for amorphous InGaZnO thin-film transistors (TFTs).<br />

Drain current-gate voltage (ID-VG) as well as capacitance-voltage (C-V)<br />

measurements are utilized to analyze the degradation mechanism.<br />

Illuminated DC hot-carrier stress leads to not only a negative parallel shift<br />

but also a C-V curve distortion at the off-state. This can be attributed to the<br />

asymmetric hole-trapping effect induced barrier-lowering near the drain<br />

side. To further verify the origin of the degradation behavior, AC bias with<br />

identical stress voltage is instead imposed on either gate terminal or drain<br />

terminal. It is deduced that hole-trapping phenomenon near the drain is<br />

dominated by the voltage across gate and drain, and is responsible for the<br />

degradation mechanism under illuminated hot-carrier stress.<br />

CP-12 High Supercapacitive Performance of Sol-Gel ZnO-Added<br />

Manganese Oxide <strong>Coating</strong>s, C.-Y. Chen (chencyi@fcu.edu.tw), C.-Y.<br />

Chiang, Feng Chia University, Taiwan, S.-J. Shih, National Taiwan<br />

University of Science and Technology, Taiwan, C.Y. Tsay, C.K. Lin, Feng<br />

Chia University, Taiwan<br />

In the present study, ZnO-added manganese (Mn) oxide coating were<br />

prepared as a function of ZnO addition (≤ 40 at.%) by sol-gel process. After<br />

post heat treatment at 300 °C, the influences of ZnO addition on the<br />

microstructural characteristics and pseudocapacitive performance of the<br />

Mn-oxide films were investigated. The structural analyses identified the solgel<br />

ZnO-added Mn-oxide powder as a tetragonal Mn3O4 phase with a<br />

nanocrystalline structure. The formation of spinel ZnxMn3-xO4 occurred<br />

when ZnO addition was ≥ 20 at.%. The crystallite size of Mn-oxide powder<br />

increased when a small amount of ZnO was added, then decreased with<br />

increased the ZnO content. The cyclic voltammetry (CV) data showed that<br />

the specific capacitance (SC) of the Mn-oxide film in 1 M Na2SO4<br />

electrolyte can be increased from 236 F/g to 301 F/g at 25 mV/s by adding<br />

with 10 at.% ZnO. The formation of spinel phase tended to inhibit the SC<br />

value of the films. After activation of the Mn-oxide film, however, a<br />

relatively high cycling efficiency of > 85% was obtained for all the<br />

compositions after 1200 CV cycles.<br />

Thursday Afternoon Poster Sessions 106<br />

CP-13 Characterization of dye sensitized solar cells with growth of<br />

ZnO passivating layer by Electron-beam evaporation, S.W. Rhee, K.H.<br />

Kim, H.W. Choi (chw@kyungwon.ac.kr), Kyungwon University, Republic<br />

of Korea<br />

Dye-sensitized solar cells have been studied intensively since the discovery<br />

of DSSCs in 1991, has paved the way to cell efficiency as high as 11%,<br />

allowing to foresee the possibility of obtaining cost efficient cells.[1] In this<br />

study, ZnO thin film have been growth on FTO glass which used for dye<br />

sensitized solar cells(DSSC) by electron-beam evaporation. While a great<br />

number of various deposition techniques were reported for Zinc<br />

Oxide(ZnO) thin films, e.g. R.F and D.C. sputtering, pulsed laser<br />

deposition, metal organic chemical vapor deposition, and others. most of the<br />

ZnO active layers in TFT have been deposited by physical vapor deposition<br />

methods.<br />

Electron was caused in N-719 and get through photoelectron (TiO2) and<br />

TCO. Electron loss occurs at each interface. Specially, TiO2 electrode on<br />

FTO. Fig.1 show the various components of a DSSC. It is also shows the<br />

process flow of occurred electron in dye, and electron recombination in<br />

TiO2 to FTO interface. One of the reason deposition ZnO passivating layer<br />

can prevent recombination effectively. In addition the interfacial contact<br />

properties between the semiconductor metal oxide layer and the transparent<br />

conducting oxide (TCO) have been considered to play a significant role in<br />

the enhancement of the photovoltaic performance of DSSCs. In theory, ZnO<br />

has wide band gap (larger than 3eV) also excellent electron collecting<br />

capability and mobility[2]. ZnO passivating layer at room temperature and<br />

the chamber pressure was kept below 5 10 6 torr at different atmosphere O2<br />

gas flow. Electron-beam voltage was 8kv. The crystal structure and<br />

morphology were observed by X-ray diffraction (XRD) and scanning<br />

electron microscopy (SEM), The transmittance of the film was examined<br />

using a UV-spectrometer. The conversion efficiency of the DSSC fabricated<br />

was measured using I-V solar stimulator.<br />

CP-15 Preparation of ZnyCd1-yS thin film by chemical bath deposition<br />

and application for dye-sensitized solar cell, C.C. Chang, Institute of<br />

Physics, Academia Sinica, Nankang, Taiwan, C.S. Hsu, Feng Chia<br />

University, Taiwan, C.H. Hsu, M.K. Wu, Institute of Physics, Academia<br />

Sinica, Nankang, Taiwan, C.C. Chan (ccchan@fcu.edu.tw), Feng Chia<br />

University, Taiwan<br />

In the present study, ZnyCd1-yS thin film was coated on the ITO glass with<br />

chemical bath deposition method, using zinc acetate and cadmium acetate<br />

as precursors. Dye-sensitized solar cell was prepared from the ZnyCd1-yS<br />

/ITO glass with Anthocyanin, which was extracted from the grape skin, as a<br />

dye. Pt-sputtered ITO glass was used as the counter electrode. The<br />

influences of zinc/cadmium ratio and reaction time on the performance of<br />

the prepared dye-sensitized solar cell were discussed. FESEM was used to<br />

characterize the surface microstructure and sectional thickness of the<br />

ZnyCd1-yS film . The absorption spectra of the ZnyCd1-yS film and<br />

Anthocyanin dye were recorded using UV-VIS spectrophotometer . The<br />

characteristic of the Anthocyanin dye was also analyzed by FTIR<br />

spectrophotometer. Photocurrent-voltage (I-V) measurements were<br />

performed using an electrochemical analyzer. According to the UV-VIS<br />

results, Anthocyanin dye has a significant absorption band within the<br />

wavelength of 400~700nm, which can enhance the visible light absorption<br />

of the ZnyCd1-yS film. The results that the dye-sensitized solar cell prepared<br />

from the Zn0.2Cd0.8S film exhibited the best performance. The open-circuit<br />

voltage, short-circuit current, and photo-to-electron power conversion<br />

efficiency are 0.695V, 1.408mA, and 4.07%, respectively.<br />

CP-16 Effect of Thermal Treatment on Physical and Electrical<br />

Properties of porogen-containing and porogen-free ultralow-k plasmaenhanced<br />

chemical vapor deposition dielectrics, W.Y. Chung, National<br />

Chi-Nan University, Taiwan, Y.M. Chang, J.I.M. Leu, National Chiao Tung<br />

University, Taiwan, T.J. Chiu, Y.L. Cheng (yjcheng@ncnu.edu.tw),<br />

National Chi-Nan University, Taiwan<br />

The effect of the thermal annealing on the physical and electrical properties<br />

of porogen-containing and porogen-free ultralow-k dielectrics prepared by<br />

plasma-enhanced chemical vapor deposition (PECVD) was investigated.<br />

The porogen-free ultralow-k dielectric is obtained by using UV curing<br />

process to remove the organic sacrificial phase and generate open porosity.<br />

The results are also compared with the PECVD porogen-containing low-k<br />

films without UV curing process and PECVD low-k dielectrics without<br />

containing organic sacrificial phase. All low-k films in this study are totally<br />

deteriorated after >800 o C thermal annealing. As the annealing temperature<br />

below 700 o C, low-k dielectrics without containing organic sacrificial phase<br />

remain stable. The microstructure of the ultralow-k dielectrics changes with<br />

the thermal annealing. However, two kinds of ultralow-k dielectrics after the<br />

thermal annealing show the different physical and electrical characteristics.<br />

The porogen-containing low-k films without UV curing can produce more<br />

pore after the thermal annealing, resulting in the worse electrical<br />

performance as compared to the porogen-free ultralow-k dielectrics.

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