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ICMCTF 2012! - CD-Lab Application Oriented Coating Development

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dominates the characteristics of a-Si:H TFTs. The behavior of electrical<br />

characteristics with mechanical strain can be explained by trap state<br />

redistribution of the bandgap. The disordered bonds may generate a<br />

redistribution of trap states, resulting in unstable electrical characteristics<br />

such as threshold voltage, subthreshold swing, and mobility of carriers.<br />

During mechanical strain the deep states are redistributed in a Gaussian<br />

distribution, and are dissimilar to ordinary acceptor-like deep states which<br />

manifest with exponential distributions. Electronic states near the Fermi<br />

level act as recombination centers for photogenerated carries, and it may<br />

valuable for illumination of the transistors. We conclude that the gap state<br />

density of an a-Si:H layer under mechanical strain is fundamental to the<br />

reliability and development of flexible electronics.<br />

CP-25 Effects of RF power on the properties of Si thin films deposited<br />

by an ICP CVD system with internal antennas, J.H. Hsieh<br />

(jhhsieh@mail.mcut.edu.tw), YAN-LIANG. Lai, Ming Chi University of<br />

Technology, Taiwan, Yuichi. Setsuhara, Osaka University, Japan<br />

The plasma of an ICP-CVD system attached with four internal antennas was<br />

used to deposit doped and un-doped Si thin films. Hydrogenated<br />

microcrystalline silicon (μc-Si:H) films were prepared under various RF<br />

power, while the flow ratio of SiH4/H2 was fixed at 1/4. During deposition,<br />

an OES (optical emission spectrometer) and a plasma probe were used to<br />

characterize the conditions of plasma. The crystalllinity and opto-electrical<br />

properties of the Si:H films were investigated using Raman scattering<br />

spectroscopy, XRD, Hall effect measurement system, and UV-Vis<br />

photometer. It is found that the crystallinity of μc-Si:H film was<br />

significantly affected by plasma density which was increased with the<br />

increase of the power. This could be caused by the increase of I*SiH3/IHa. It is<br />

also found the plasma potential would decrease with the increase of power,<br />

while the plasma density would increase with the increase of power. The<br />

carrier density, mobility, and photoconductivity were found related to the<br />

plasma potential and density which might affect defect density in the films.<br />

CP-27 The different radio-frequency powers on characteristics of<br />

boron-doped amorphous carbon films prepared by reactive radiofrequency<br />

chemical vapor deposition, T.S. Chen, S.E. Chiou, S.T. Shiue<br />

(stshiue@dragon.nchu.edu.tw), National Chung Hsing University, Taiwan<br />

Boron-doped amorphous carbon (a-C:B) films were deposited on n-type<br />

silicon (n-Si) wafers using reactive radio-frequency (RF) chemical vapor<br />

deposition. A boron target was used as the dopant source, and a mixture of<br />

pure methane (CH4) and argon (Ar) gases with flow rates of 2 and 10 sccm,<br />

respectively, was selected as the precursor gas. Five kinds of a-C:B films<br />

were prepared with RF powers of 100, 200, 300, 400, and 500 W. The<br />

substrate temperature and working pressure were set at 298 K and 6 Pa,<br />

respectively. The thicknesses of a-C:B films were measured using field<br />

emission scanning electron microscopy (FESEM). Alternatively, the<br />

characteristics of a-C:B films were analyzed by X-ray photoelectron<br />

spectrometer (XPS) and Raman scattering spectra (RSS). After the a-C:B/n-<br />

Si junction was sputtered with gold (Au) and aluminum (Al) electrodes, the<br />

current-voltage (I-V) and capacitance-voltage (C-V) characteristics of Au/a-<br />

C:B/n-Si/Al heterojunction devices were measured.<br />

FESEM results show that all the thicknesses of a-C:B films are about 100<br />

nm. XPS analyzed results reveal that the boron atoms are successfully<br />

doped into amorphous carbon films, and the boron content increases from<br />

0.02 to 28.87 at.% as the RF power increases from 100 to 500 W. The RSS<br />

data of a-C:B films indicate that the ratio of the integrated intensity of the D<br />

band to that of the G band (ID/IG) increases with increasing the RF power<br />

from 100 to 300 W, but decreases with increasing the RF power from 300 to<br />

500 W. It implies that the a-C:B film prepared with the RF power of 300 W<br />

has a relatively higher graphitization degree. Our analyzed results also show<br />

that all the I-V characteristics of Au/a-C:B/n-Si/Al heterojunction devices<br />

exhibit the rectifying behavior. When the a-C:B film was prepared with the<br />

RF power of 300 W, the Au/a-C:B/n-Si/Al heterojunction device displays<br />

the best rectifying I-V characteristics, and its ideality factor is about 1.40.<br />

The C-V measurement under the frequency of 1 kHz shows that as the a-<br />

C:B film was prepared by the RF power of 300 W, the built-in voltage of<br />

the Au/a-C:B/n-Si/Al device is about 0.2 V.<br />

CP-28 InN/GaN Quantum Well Heterostructures: Structural<br />

Characteristics and Strain Induced Modifications of the Electronic<br />

Properties, -. Kioseoglou, Kalesaki, Aristoteles University of Thessaloniki,<br />

Greece, Komninou, Aristotleles University of Thessaloniki, Greece,<br />

Karakostas (karakost@auth.gr), Aristoteles University of Thessaloniki,<br />

Greece<br />

An important step towards optimization of InN/GaN based devices is the<br />

identification of the structural characteristics of the corresponding interfaces<br />

since the favourable bonding configurations determine the materials<br />

polarity and consequently the direction of spontaneous polarization. We<br />

have addressed this issue through empirical potential calculations on<br />

Thursday Afternoon Poster Sessions 108<br />

InN/GaN interfaces comprising misfit dislocations [1]. An appropriately<br />

parameterized Tersoff interatomic potential [2] was implemented and<br />

energetic calculations were performed on interfaces of III- and N- polarity,<br />

lying at the single- or double bonds and having a wurtzite or zinc blende<br />

stacking sequence in accordance with high resolution transmission electron<br />

microscopy observations. Based on these results III-polarity interfaces,<br />

cutting single bonds are energetically favourable.<br />

In our present study, additional calculations are performed on subcritical<br />

thickness InN/GaN QWs, which exhibit lower dislocation densities as well<br />

as reduced InN decomposition and are currently implemented in the<br />

fabrication of near-UV light emitting diodes [3,4]. Ab initio calculations are<br />

performed under modified pseudopotentials, accurately reproducing the InN<br />

and GaN band gap values, on supercells comprising 1 monolayer (ML)<br />

thick InN elastically strained in 5 nm thick GaN barriers having a wurtzite<br />

or zinc blende stacking at the interface. The former is found to be<br />

energetically favourable. Subsequent calculations on supercells comprising<br />

1 ML thick InN in 8 and 11 nm thick GaN barriers as well as 3 ML InN in<br />

11 nm thick GaN having a wurtzite stacking, depicted a variation in III-N<br />

bond lengths. This variation become more significant as the barrier<br />

thickness decreases or the QW thickness increases. Hence the strain and<br />

consequently piezoelectric polarization are modified. The latter is attested<br />

by density of states calculations, which show a vast decrease of the band<br />

gap when 5 nm thick barriers are considered, while a significant decrease is<br />

also recorded at the 3 ML InN / 11 nm GaN barrier heterostructure in<br />

comparison with the 1 ML InN supercell. Our results scrutinize recent<br />

experimental observations [3,4] and could prove beneficial for tailoring the<br />

optoelectronic properties of InN/GaN QWs.<br />

[1] J. Kioseoglou et al., J. Mater. Sci. 43, 3982 (2008)<br />

[2] J. Kioseoglou et al., Phys. Stat. Sol. (b) 245, 1118 (2008)<br />

[3] E. Dimakis et al., Phys. Stat. Sol. (a) 205, 1070 (2008)<br />

[4] A. Yoshikawa et al., J. Vac. Sci. Technol. B 26, 1071 (2008)<br />

[5] Work supported by EC under the 7 th European Framework Project<br />

DOTSENSE (Grant No.<br />

STREP 224212)<br />

CP-29 Optical properties of AlN:Ag and Al-Si-N:Ag nanostructured<br />

films and the effect of thermal annealing, A. Siozios, E. Lidorikis, P.<br />

Patsalas (ppats@cc.uoi.gr), University of Ioannina, Greece<br />

Aluminum Nitride (AlN) is a wide bandgap semiconductor that has been<br />

studied extensively because of its remarkable optical, mechanical, physical<br />

and chemical properties that make it suitable for a variety of applications<br />

such as optoelectronic devices, protective coatings, wave-guides, etc. The<br />

incorporation of Ag into an AlN matrix can provide additional functionality<br />

through the localized surface plasmon resonance (LSPR): a collective<br />

oscillation of conduction electrons, fueled by light illumination at the proper<br />

frequency. In this work we investigate under which circumstances LSPR is<br />

manifested. In particular, we have grown nanostructured films consisting of<br />

an AlN matrix and Ag inclusions in the form of nanospheres, nanosheets<br />

and atomic dispersions, by sputtering and pulsed laser deposition (PLD).<br />

The refractive index of the matrix was varying by controlling the matrix<br />

microstructure and density (amorphous or wurtzite AlN, a-AlN and w-AlN,<br />

respectively) and the optical absorption in the visible range was controlled<br />

by the incorporation of Si in to the AlN matrix. The refractive index of the<br />

films is correlated with the films’ density measured by X-Ray Reflectivity<br />

(XRR). The optical properties of the films were studied using Optical<br />

Reflectivity Spectroscopy (ORS) in vertical incidence in the 1.5-5.25 eV<br />

spectral range. The spectroscopic data are critically compared to Finite<br />

Difference Time Domain (FDTD) calculations of the optical response. The<br />

effect of the thermal annealing to the plasmonic behavior of the AlN:Ag<br />

and Al-Si-N:Ag has been studied systematically by repeating the ORS<br />

measurement after annealing in inert Ar atmospheres cycles at various<br />

temperatures as high as 800 o C.<br />

CP-30 Investigation of photoluminescent characteristics and optical<br />

properties of thin film zinc silicate doped with manganese, K.H. Yoon,<br />

J.H. Kim (joohan@cbnu.ac.kr), Chungbuk National University, Republic<br />

of Korea<br />

The photoluminescent characteristics and optical properties of manganesedoped<br />

zinc silicate (Zn2SiO4:Mn) thin films were investigated. The<br />

Zn2SiO4:Mn films were deposited by radio frequency magnetron sputtering,<br />

followed by post-deposition annealing at temperatures of 600 – 1200 °C.<br />

The Zn2SiO4:Mn films exhibited a pronounced optical absorption edge in<br />

the near ultraviolet wavelength region and a high optical transparency in the<br />

visible spectral range. The maximum transmittance reached 0.922 at 597<br />

nm, which was very close to the transmittance of the fused quartz substrate<br />

alone. The refractive index of the Zn2SiO4:Mn films showed normal<br />

dispersion behavior. X-ray diffraction and atomic force microscopy<br />

measurements revealed that the as-deposited Zn2SiO4:Mn films had an

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