• Journal of the Institute of Electronics Engineers of Korea SD
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• v.38 no.10
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• pp.671-677
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• 2001

A RuO$_2$ Schottky photo-detector was designed and fabricated with GaN layers on the sapphire substrate. For good absorption of UV light, an epitaxial structure with undoped GaN(0.5 ${\mu}{\textrm}{m}$)/n￣-GaN(0.1${\mu}{\textrm}{m}$)/n＋-GaN(1.5${\mu}{\textrm}{m}$) was grown by MOCVD. The structure had the carrier concentrations of 3.8$\times$10$^{18}$ cm￣$^3$, the mobility of 283$\textrm{cm}^2$/V.s. After ECR etching process for mesa structure with the diameter of about 500${\mu}{\textrm}{m}$, Al ohmic contact was formed on GaN layer. After proper passivation between the contacts with Si$_3$/N$_4$, was formed on undoped GaN layer. The fabricated Schottky diode had a specific contact resistance of 1.15$\times$10$^{-5}$ ［$\Omega$.$\textrm{cm}^2$］. It has a low leakage current of 305 pA at -5 V, which was attributed by stable characteristics of RuO$_2$ Schottky contact. In optical measurement, it showed the high UV to visible extinction ratio of 10$^{5}$ and very high responsivity of 0.23 A/W at the wavelength of 365nm.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.45 no.5
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• pp.12-18
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• 2008

Ag paste was employed for source and drain electrode of OTFTs and for the data metal lines of OTFT-OLED array on PC(polycarbonate) substrate. We tested two kinds of Ag-pastes such as pastes for 325 mesh and 500 mesh screen mask to examine the pattern ability and electrical performance for OTFTs. The minimum feature size was 60 ${\mu}m$ for 325 mesh screen mask and 40 ${\mu}m$ for 500 mesh screen mask. The conductivity was 60 $m{\Omega}/\square$ for 325 mesh and 133.1 $m{\Omega}/\square$ for 500 mesh. For the OTFT performance the mobility was 0.35 $cm^2/V{\cdot}sec$ and 0.12 $cm^2/V{\cdot}sec$, threshold voltage was -4.7 V and 0.9 V, respectively, and on/off current ratio was ${\sim}10^5$, for both screen masks. We applied the 500 mash Ag paste to OTFT-OLED array because of its good patterning property. The pixel was composed of two OTFTs and one capacitor and one OLED in the area of $2mm{\times}2mm$. The panel successfully worked in active mode operation even though there were a few bad pixels.

• The Korean Journal of Pesticide Science
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• v.16 no.3
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• pp.195-201
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• 2012

We tested for pesticide residues in 124 samples of 22 different items of imported fruits circulated in Gyeonggido. Total 218 pesticides were analyzed by multi-residue method using gas chromatography/nitrogen phosphorus detector-electron capture detector (GC/NPD-ECD), time of flight/mass spectrometer (TOF/MS), ultra performance liquid chromatography/photo diode array (UPLC/PDA), high performance liquid chromatography/fluorescence detector (HPLC/FLD) and mass spectrometer (LC/MS/MS). The pesticides were detected in 18 fruits samples, ranging 0.003~0.3 mg/kg and no samples had violative residue. The separation test to 14 sample pesticides detected was conducted to monitor the current status of pesticide residues according to the partial characteristic. The pesticides were detected in 14 peels ranging 0.03~1.5 mg/kg and 2 fleshes in less than detection limits. These results indicate that imported fruits are safe when the human takes normally but even the small amount of pesticides is harmful when the human takes it in a prolonged period. Therefore, the pesticide residual amounts of imported friuts should be constantly monitored for food safety.

• Journal of the Korean Electrochemical Society
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• v.2 no.1
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• pp.17-22
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• 1999

Since the use of porous silicon for microsensors and microactuators is in the euly stage of study, only several application devices, such as light-emitting diodes and chemical sensors have so far been demonstrated. In this paper we present an overview of the present status of porous silicon sensors and actuators research with special emphasis on the applications of chemical sensors and optical devices. The capacitive type porous silicon humidity sensors had a nonlinear capacitance-humidity characteristic and a good sensitivity at higher humidity above $40\%RH$. The porous silicon $n^+-p-n^+$ device showed a sharp increase in current when exposed to an ethanol vapor. The $p^+-PSi-n^+$ diode fabricated on porous silicon diaphragm exhibited an optical switching characteristic, opening up its utility as an optical sensor or switch. The photoluminescence (PL) spectrum, taken from porous silicon under 365 nm excitation, had a broad emission, peaked at -610 nm. The electroluminescence(EL) from ITO/PSi/In LED had a broader spectrum with a blue shifted peak at around 535nm than that of the PL.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.44 no.9
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• pp.71-80
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• 2007

This paper presents a new push-push VCO technique that extracts a second harmonic output signal from a capacitive commonnode in a negativegm oscillator topology. The generation of the $2^{nd}$ harmonics is accounted for by the nonlinear current-voltage characteristic of the emitter-base junction diode causing; 1) significant voltage clipping and 2) different rising and falling time during the switching operation of core transistors. Comparative investigations show the technique is more power efficient in the high-frequency region that a conventional push-push technique using an emitter common node. Prototype 12GHz and 17GHz MMIC VCO were realized in GaInP/GaAs HBT technology. They have shown nominal output power of -4.3dBm and -5dBm, phase noise of -108 dBc/Hz and -110.4 dBc/Hz at 1MHz offset, respectively. The phase noise results are also equivalent to a VCO figure-of-merit of -175.8 dBc/Hz and -184.3 dBc/Hz, while dissipate 25.68mW(10.7mA/2.4V) and 13.14mW(4.38mA/3.0V), respectively.

• Clean Technology
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• v.18 no.4
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• pp.366-372
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• 2012

Three acrylic copolymers containing tris(8-hydroxyquinoline) aluminum (AlQ3) pendant group (25 wt%), acrylateco-HEMA-$AlQ_3$ (25 wt%), were successfully synthesized by free radical polymerization from acrylates [methyl methacrylate (MMA), acrylonitrile (AN) or 2-hydroxyethyl methacrylate (HEMA)] with HEMA functionalized with AlQ3 pendant groups (HEMA-p-$AlQ_3$). The glass transition temperatures ($T_g$) of MMA-co-HEMA-p-$AlQ_3$ (copolymer 1), AN-co-HEMA-p-$AlQ_3$ (copolymer 2) and HEMA-co-HEMA-p-$AlQ_3$ (copolymer 3) were found to be 158, 150 and $126^{\circ}C$, respectively. They have good thermal stability: a very desirable feature for the stability of OLEDs. Their solubility, thermal properties, UV-visible absorption and photoluminescence behaviors were investigated. They were found to be soluble in various organic solvents such as tetrahydrofuran (THF), dimethylformamide (DMF), toluene and chloroform. It was also found that the UV-visible absorption and photoluminescence behaviors of these copolymers were similar to those of pristine $AlQ_3$. Green organic light-emitting diodes (OLEDs) have also been fabricated using these copolymers as light emission/electron transport components obtained easily by spin coating, and their current density voltage (J-V) curves were compared. The OLED device of the copolymer 3 had the lowest turn-on voltage of about 2 V compared to other copolymer types devices.

• Korean Journal of Materials Research
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• v.3 no.2
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• pp.121-130
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• 1993

The GaP crystals were grown by synthesis solute diffusion method and its properties were investigated. High quality single crystals were obtained by pull-down the crystal growing ampoule with velocity of 1.75mm/day. Etch pits density along vertical direction of ingot was increased from 3.8 ${\times}{10^4}$c$m^{-2}$ of the first freeze to 2.3 ${\times}{10^5}$c$m^2$ of the last freeze part. The carrier concentration and mobilities at room temperature were measured to 197.49cc$m^2$/V.sec and 6.75 ${\times}{10^{15}}$c$m^{-3]$, respectively. The temperature dependence of optical energy gap was empirically fitted to $E_g$(T)=[2.3383-(6.082${\times}{10^{-4}}$)$T^2$/(373. 096+TJeV. Photoluminescence spectra measured at low temperature were consist with sharp line-spectra near band-gap energy due to bound-exciton and phonon participation in band edge recombination process. Zn-diffusion depth in GaP was increased with square root of diffusion time and temperature dependence of diffusion coefficient was D(Tl = 3.2 ${\times}{10^3}$exp( - 3.486/$k_{\theta}$T)c$m^2$/sec. Electroluminescence spectra of p-n GaP homojunction diode are consisted with emission at 630nm due to recombination of donor in Zn-O complex center with shallow acceptors and near band edge emission at 550nm. Photon emission at current injection level of lower than 100m A was due to the band-filling mechanism.

• Journal of the Korean Society for Nondestructive Testing
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• v.27 no.4
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• pp.299-304
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• 2007

There are to be some cracks on the material degradation part or the stress concentration parts of the main members, which carry on over-loads, of structures. Because these cracks can be used to evaluate the structural health status, it is important to monitor the crack growth for maintaining the structural safety. In this study, the fiber Bragg grating sensor with a drop ball was developed as a sensor for crack growth detection of an existing crack. The crack growth detection sensor was constructed with three parts: a probe part, a wavelength controling light source and receiver part, and an impact part. The probe part was just formed with a fiber Bragg grating optical fiber The wavelength controling light source part was composed of a current supplying circuit, a DFB laser diode, and a TEC controling circuit for wavelength control. Also, the impact part was just implemented by dropping a steel ball. The performance of this sensor was confirmed by the experiments of the crack detection with an aluminum plate having one existing crack. According to these experiments, the difference of the sensor signal outputs was correlated with the crack length. So, it was confirmed that this sensor could be applied to monitor the crack growth.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.08a
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• pp.125-126
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• 2010

플라즈마 아킹은 PECVD, 플라즈마 식각 그리고 토카막과 같은 플라즈마를 이용하는 여러 공정과 연구 분야에서 문제점을 야기시켜왔다. 하지만, 이에 대한 연구는 아킹 현상의 불규칙성과 과도적인 행동으로 인해 미비한 상태이다. 특히, RF 방전에서의 아킹 연구는 DC 방전에서의 아킹 연구에 비해 많이 부족한 것이 현실이다. 플라즈마 아킹은 집단전자방출(collective electron emission)에 의한 스파크 방전(spark discharge)현상이다. 집단전자방출은 전계방출(field emission)이나 플라즈마와 쉬스를 두고 인접한 표면위에서의 유전분극(dielec emission)에 의해 발생한다. 이렇게 방출된 집단 전자들은 쉬스에서 가속되어 에너지를 얻게 되고 원자와의 충돌로 전자 아발란체를 일으킨다. 이렇게 배가된 전자들은 아킹 스트리머(arcing streamer)를 형성하게 되고 아킹 발생 시 높은 전류와 공정 실패의 원인이 된다. 우리는 $30cm{\times}20cm$ 크기의 사각 전극을 위 아래로 가진 챔버에서 Ar 가스를 RF(13.56 MHz)파워를 이용해 방전시켰다. 방전 전압과 전류는 파워 전극 압단에서 High voltage probe (Tektronix P6015A)와 Current probe (TCPA300 + TCP312)를 이용해 측정했다. 플라즈마 아킹시 변하는 플라즈마 플로팅 포텐셜은 챔버 중앙에 위치한 랑뮈프 프로브에 의해 측정되고 챔버 옆의 뷰포트 앞에 위치한 PM-tube를 이용해 아킹시 변하는 광량을 측정한다. RF 방전에서의 플라즈마 아킹은 아킹시 플로팅 포텐셜의 변화에 의해 크게 세부분으로 나눌 수 있다. 아킹 발생과 동시에 급격히 감소하는 감소부분 (약 2us) 그리고 감소한 포텐셜이 유지되는 유지부분 (약 0~10ms) 그리고 감소했던 포텐셜이 서서히 원래 상태로 회복되는 회복부분(약 100 us)이다. 아킹 초기시 방출된 집단 전자들과 원자들간의 충돌에 의해 형성된 아킹 스트리머는 플라즈마 전체를 단락시키게 되고 이로 인해 플로팅 포텐셜은 급격히 감소하게 된다. 이렇게 감소한 플로팅 포텐셜은 아킹 스트리머가 유지되는 한 계속 감소한 상태를 유지하게 된다. 그리고 플라즈마를 섭동했던 아킹 스트리머가 중단되면 플라즈마는 섭동전의 원래 상태로 돌아가려 하기 때문에 플로팅 포텐셜은 서서히 증가하면서 원래 상태로 회복된다. 플라즈마 아킹 발생시 생성되는 아킹 스트리머는 순간적으로 많은 전자들을 국소적으로 생성하게 되고 이 전자들에 의해 광량이 순간적으로 증가하게 된다. PM-tube (750.4 nm)에 의해 측정된 아킹시 광량은 정상방전 상태의 두배 가량이 된다. 그리고 이 순간적으로 증가된 광량은 시간이 지남에 따라 감소하게 되고 정상방전 일때의 광량이 된다. 광량이 증가한 후 정상방전 상태의 광량에 이르는 부분은 플로팅 포텐셜이 감소한 상태에서 유지되는 부분과 일치하고 이는 플로팅 포텐셜의 유지부분동안 아킹 스트리머가 발생하고 있다는 간접적인 증거가 된다. 그리고 정상 방전 상태 일때의 광량이 되면 아킹 스트리머가 중단되었다는 것이므로 그 시점부터 플로팅 포텐셜은 정산 방전상태 일 때의 포텐셜로 복구되기 시작한다. 이처럼 PM-tube를 이용한 아킹 광량 측정은 아킹 스트리머를 간접적으로 측정하게 하고 아킹 스트리머를 이용해 아킹시의 플로팅 포텐셜의 변화를 설명하게 해 준다. 응용적인 측면에서 아킹 광량 측정을 이용한 아킹 판독은 방전 전류와 방전 전압과 같은 전기적 신호를 이용한 아킹 판독에 비해 여러가지 장점을 가진다. 우선, 전기적 신호를 이용한 아킹 판독처럼 매칭 회로나 플라즈마를 섭동시키지 않는다. 그리고 원하는 부분의 아킹만을 판독하는 것도 가능하며 photo-diode를 이용할 경우 전기적 신호를 이용하는 것에 비해 경제적으로 유리하다.

• Journal of the Korea Institute of Information and Communication Engineering
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• v.11 no.10
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• pp.1899-1909
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• 2007

A cross-coupled charge pump with internal pumping capacitor, witch is advantages from a point of minimizing TFT-LCD driver IC module, is newly proposed in this paper. By using a NMOS and a PMOS diode connected to boosting node from VIN node, the pumping node is precharged to the same value each pumping node at start pumping operation. Since the lust-stage charge pump is designed differently from the other stage pumps, a back current of pumped charge from charge pumping node to input stage is prevented. As a pumping clock driver is located the font side of pumping capacitor, the driving capacity is improved by reducing a voltage drop of the pumping clock line from parasitic resistor. Finally, a layout area is decreased more compared with conventional cross-coupled charge pump by using a stack-MIM capacitors. A proposed charge pump for TFT-LCD driver IC is designed with $0.13{\mu}m$ triple-well DDI process, fabricated, and tested.