• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.30 no.5
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• pp.294-300
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• 2017

$TeO_x$ thin films were deposited at various $O_2$/Ar gas-flow ratios by a reactive RFmagneton sputtering technique from $TeO_2$ and Te targets. X-ray diffraction (XRD) results revealed that the $TeO_x$ thin films were amorphous. The structure and chemical composition of the $TeO_x$ thin films were investigated by fourier transform infrared spectroscopy (FT-IR) and X-ray photoelectron spectroscopy (XPS). The optical characteristics of the $TeO_x$ thin films were investigated by an Ellipsometer and a UV-VIS-NIR spectrophotometer. According to the $O_2$/Ar gas-flow ratios, the atomic composition ratio of $TeO_x$ thin films was divided into two regions(x=1-2, 2-3). Different optical characteristics were shown in each region. With an increasing $O_2$/Ar gas-flow ratio, the refractive index of the $TeO_x$ thin films decreased and the optical bandgap of the films increased.

• The Transactions of The Korean Institute of Electrical Engineers
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• v.67 no.10
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• pp.1370-1374
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• 2018

A heterojunction $SnS_2/p-Si$ photodetector was fabricated by RF magnetron sputtering system. $SnS_2$ was formed with 2-inch $SnS_2$ target. Al was applied as the front and the back metal contacts. Rapid thermal process was conducted at $500^{\circ}C$ to enhance the contact quality. 2D material such as $SnS_2$, MoS2 is very attractive in various fields such as field effect transistors (FET), photovoltaic fields such as photovoltaic devices, optical sensors and gas sensors. 2D material can play a significant role in the development of high performance sensors, especially due to the advantages of large surface area, nanoscale thickness and easy surface treatment. Especially, $SnS_2$ has a indirect bandgap in the single and bulk states and its value is 2 eV-2.6 eV which is considerably larger than that of the other 2D material. The large bandgap of $SnS_2$ offers the advantage for the large on-off current ratio and low leakage current. The $SnS_2/p-Si$ photodetector clearly shows the current rectification when the thickness of $SnS_2$ is 80 nm compared to when it is 135 nm. The highest photocurrent is $19.73{\mu}A$ at the wavelength of 740 nm with $SnS_2$ thickness of 80 nm. The combination of 2D materials with Si may enhance the Si photoelectric device performance with controlling the thickness of 2D layer.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.27 no.11
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• pp.760-765
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• 2014

MgZnO has attracted a lot of attention for flexible device. In the flexible substrate, the crystal structure of the thin films as well as the surface morphology is not good. Therefore, in this study, we studied on the effects of the oxygen pressure on the structure and crystallinity of $Mg_{0.3}Zn_{0.7}O$ thin films deposited on PES substrate by using pulsed laser deposition. We used X-ray diffraction and atomic force microscopy in order to observe the structural characteristics of $Mg_{0.3}Zn_{0.7}O$ thin films. The crystallinity of $Mg_{0.3}Zn_{0.7}O$ thin films with increasing temperature was improved, Grain size and RMS of the films were increased. UV-visible spectrophotometer was used to get the band gap energy and transmittance. $Mg_{0.3}Zn_{0.7}O$ thin films showed high transmittance over 90% in the visible region. As increased working pressure from 30 mTorr to 200 mTorr, the bandgap energy of $Mg_{0.3}Zn_{0.7}O$ thin film were decreased from 3.59 eV to 3.50 eV.

• Korean Chemical Engineering Research
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• v.58 no.3
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• pp.486-492
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• 2020

The method for preparing a perovskite-type bismuth ferrite (BFO) photocatalyst which reacts to visible LED light and the characteristics of visible light photocatalysis were investigated. BFO was prepared according to the sol-gel method. The prepared BFO consisted mainly of BiFeO₃ structure and formed a nano-sized crystal including Bi₂₄Fe₂O₃₉ structure. The BFO nano crystallines were identified from the UV-visible diffuse reflectance spectra to absorb UV and visible light up to about 600 nm. The bandgap of the BFO determined from the diffuse reflectance spectrum was about 2.2 eV. Formaldehyde was decomposed by the photoreaction of BFO photocatalysts with the visible light LED lamps with wavelengths of 585 nm and 613 nm. The narrow bandgap of BFO led to elicit BFO photocatalytic activity in visible LED light.

• Journal of the Institute of Electronics Engineers of Korea TC
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• v.45 no.1
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• pp.115-119
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• 2008

In this paper, the linearity of Doherty power amplifier has been improved by applying a new Photonic Bandgap(PBG) structure on the output of amplifier. The reposed spiral PBG structure is a two-dimensional(2-D) periodic lattice patterned on a dielectric slab that does not require nonplanar fabrication process. This structure has more broad stopband and high suppression performance than the conventional three cell PBG. Also, It has a sharp skirt property. We obtained the 3rd-order intermodulation distortion(IMD3) of -33dBc for CDMA applications with that of maintaining the constant power added efficiency(PAE), the IMD3 performance is improved as much as -8 dB compared with a Doherty power amplifier without PBG structure. Moreover, the physical length of PBG is shortened, therefore the whole amplifier circuit size is considerably reduced.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.35D no.6
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• pp.79-91
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• 1998

Design principles for high-brightness ligh-temitting diodes have been derived by using escape cone concepts. Based on the design principles, some important high-brightness LED structures developed thus far have been reviewed and, in addition, their external coupling efficiencies have also been estimated. In AlGaAs or InGaAIP LEDs, in which photon absorption in the ohmic electrodes is known to be serious, photon shielding by the electrodes is minimized by using window layer (WL) as well as transparent substrate (TS) leading to significantly improved light-emitting efficiency. However, in InGaN LEDs emitting blue to green lights, the photon absorption in ohmic contact to wide bandgap GaN may be negligible and therefore, photon shielding by the electrodes would not lead to as significant problems as in conventional In AIGaAs or InGaAIP LEDs.

• Journal of the Institute of Electronics Engineers of Korea TC
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• v.38 no.12
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• pp.39-48
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• 2001

We have studied the design of the photonic bandgap (PBG) structure on the microstrip line that can effectively control the fractional bandwidth of the passband formed in the stopband by adding the stub in the cell of the microstrip PBG structure. As the length of the stub increases, the cutoff frequency and the center frequency of the stopband are decreased, while the bandwidth of the stopband is increased. We have also found that the fractional bandwidth of the passband formed in stopband by the introduction of defect decreases as the stub length is increased. These results mean that adding the stub in the normal PBG structure is an effective way to control the fractional bandwidth. As an application example, we have implemented a microwave duplexer using the proposed structure.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.320-320
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• 2014

Amorphous silicon alloy (a-Si) solar cells and modules have been receiving a great deal of attention as a low-cost alternate energy source for large-scale terrestrial applications. Key to the achievement of high-efficiency solar cells using the multi-junction approach is the development of high quality, low band-gap materials which can capture the low-energy photons of the solar spectrum. Several cell designs have been reported in the past where grading or buffer layers have been incorporated at the junction interface to reduce carrier recombination near the junction. We have investigated profiling the composition of the a-SiGe alloy throughout the bulk of the intrinsic material so as to have a built-in electrical field in a substantial portion of the intrinsic material. As a result, the band gap mismatch between a-Si:H and $a-Si_{1-x}Ge_x:H$ creates a barrier for carrier transport. Previous reports have proposed a graded band gap structure in the absorber layer not only effectively increases the short wavelength absorption near the p/i interface, but also enhances the hole transport near the i-n interface. Here, we modulated the GeH4 flow rate to control the band gap to be graded from 1.75 eV (a-Si:H) to 1.55 eV ($a-Si_{1-x}Ge_x:H$). The band structure in the absorber layer thus became like a U-shape in which the lowest band gap was located in the middle of the i-layer. Incorporation of this structure in the middle and top cell of the triple-cell configuration is expected to increase the conversion efficiency further.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.457-457
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• 2014

오존발생방법은 다양한 방식으로 구현이 가능하나 대용량 장치를 만들기 위해서는 DBD (Dielectric barrier discharge) 구조의 형태의 가지고 있다. 이러한, DBD는 반도체의 MOS (Metal On Semiconductor)의 반대 구조를 가진 SOM (Semiconductor On Metal)의 형태를 가지고 있으며 대부분이 Oxidation 산화물을 가지고 구현한다. 오존발생기는 반도체 공정, 환경 및 정화 등 다양한 분야에 사용이 되고 있는 상황으로 성능개선을 위한 연구가 필요한 상황이다. 대표적으로 사용되는 물질인 $SiO_2$를 가지고 있는 상황이며 Silicon은 에너지 Bandgap이 1.1 eV로 금속위에 증착되어 통상적으로 사용되는 문턱전압은 0.7 V에 해당이 된다. 현재 점차적으로 연구가 진행되고 있는 $Al_2O_3$는 8.8 eV의 bandgap을 가지고 있으며 유전 상수가 9로 $SiO_2$인 3.9보다 높은 유전률 특징을 가지고 있다. 따라서, 본 연구는 오존 발생장치에 사용되는 방전관을 기존의 $SiO_2$에서 $Al_2O_3$ 방식으로 대체하므로써 실제적인 유전율의 값의 차이와 오존 발생시 오존변화율 증대에 관하여 연구하였다. $SiO_2$ 방전관은 Fe 메탈위에 약 3 mm정도의 두께를 binding시켜 N4L사의 PSM1700 모델 LCR meter를 사용하여 1.3 kHz시 7.2 pF의 유전율 확인 할 수 있으며 동일한 조건의 금속 메탈위에 $Al_2O_3$를 binding 시켜 측정한 결과 1.07 kHz시 10.7 pF의 유전율을 가지게 되어 40% 이상 높은 유전율을 가지게 되는 것을 확인 할 수 있다. 오존발생을 위하여 가변 주파수형 트랜스 드라이버를 통한 공진 주파수를 생성하여 방전 증폭을 위한 Amplifier를 통하여 변환률을 높이는 방식을 적용하여 MIDAC사의 I1801모델 적외선 분광기(FT-IR)를 통한 오존발생량을 측정하여 기존의 $SiO_2$의 방전관은 시간당 54 g의 오존 발생률 가지게 된다. $Al_2O_3$는 시간당 70 g 정도의 오존 발생률 가지므로 기존의 $SiO_2$ 보다 발생률 높은 것을 확인 할 수 있다.

• Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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• 2012.10a
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• pp.221-224
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• 2012

This paper presents a CMOS interface circuit for MEMS acceleration sensor. It consists of a capacitance to voltage converter(CVC), a second-order switched-capacitor (SC) integrator and comparator. A bandgap reference(BGR) has been designed to supply a stable bias to the circuit and a ${\Sigma}{\Delta}$ Modulator with chopper - stabilization(CHS) has also been designed for more suppression of the low frequency noise and offset. As a result, the output of this ${\Sigma}{\Delta}$ Modulator increases about 10% duty cycle when the input voltage amplitude increases 100mV and the sensitivity is x, y-axis 0.45v/g, z-axis 0.28V/g. This work is designed and implemented in a 0.35um CMOS technology with a supply voltage of 3.3V and a sampling frequency of 3MHz sampling frequency. The size of the designed chip including PADs is $0.96mm{\times}0.85mm$.