• 천문학회보
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• 제40권1호
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• pp.68.2-69
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• 2015

We present [Fe II] $1.644{\mu}m$ features around ultracompact H II regions (UCHIIs) found on a quest for the "footprint" outflow features of UCHIIs -the features produced by outflowing materials ejected during an earlier, active accretion phase of massive young stellar objects (MYSOs). We surveyed 237 UCHIIs in the first Galactic quadrant, employing the CORNISH UCHII catalog and UWIFE data, which is an imaging survey in [Fe II] $1.644{\mu}m$ performed with UKIRT-WFCAM under ~0.''8 seeing conditions. The [Fe II] features were found around five UCHIIs. We interpret the [Fe II] features to be shock-excited by outflows from YSOs and estimate the outflow mass-loss rates from the [Fe II] flux which are ${\sim}1{\times}10^{-6}-4{\times}10^{-5}M{\odot}yr^{-1}$. We propose that the [Fe II] features might be the "footprint" outflow features, but more studies are required to clarify whether or not this is the case. This is based on the morphological relation between the [Fe II] and 5 GHz radio features, the outflow mass-loss rate, the travel time of the [Fe II] features, and the existence of several YSO candidates near the UCHIIs.

• 한국전자파학회논문지
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• 제23권3호
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• pp.314-319
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• 2012

본 논문에서는 MICS(Medical Implant Communication Service, 402~405 MHz)와 ISM(The Industrial, Scientific and Medical, 2.40~2.48 GHz) 대역에서 동작하는 인체 통신 중계용 안테나를 제안하고, 인체의 영향을 고려한 안테나 성능에 대한 분석을 하였다. 제안된 안테나는 loop 안테나와 영차 공진 안테나로 구성되어 있다. Loop 안테나는 ISM 대역에서 동작하며, MICS 대역에서의 동작은 loop 안테나와 영차 공진기의 용량성 결합에 의해 요구 성능을 만족할 수 있도록 구현하였다. 근거리장에 인체가 존재할 때 인체가 안테나에 미치는 영향을 분석하기 위하여 인체 팬텀을 이용하여 시뮬레이션과 측정을 하였다. 시뮬레이션 및 측정 결과, 제안된 안테나는 MICS와 ISM 대역에서 대역폭을 만족하였고, 측정된 이득값은 MICS 대역에서 -28.53 dBi, ISM 대역에서 3.85 dBi였다. 또한, 설계된 안테나의 이중 대역 특성은 인체 내 외부 간의 통신 중계 용도로 적절하다고 사료된다.

• ETRI Journal
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• 제42권4호
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• pp.491-504
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• 2020

We present AB9, a neural processor for inference acceleration. AB9 consists of a systolic tensor core (STC) neural network accelerator designed to accelerate artificial intelligence applications by exploiting the data reuse and parallelism characteristics inherent in neural networks while providing fast access to large on-chip memory. Complementing the hardware is an intuitive and user-friendly development environment that includes a simulator and an implementation flow that provides a high degree of programmability with a short development time. Along with a 40-TFLOP STC that includes 32k arithmetic units and over 36 MB of on-chip SRAM, our baseline implementation of AB9 consists of a 1-GHz quad-core setup with other various industry-standard peripheral intellectual properties. The acceleration performance and power efficiency were evaluated using YOLOv2, and the results show that AB9 has superior performance and power efficiency to that of a general-purpose graphics processing unit implementation. AB9 has been taped out in the TSMC 28-nm process with a chip size of 17 × 23 ㎟. Delivery is expected later this year.

• JSTS:Journal of Semiconductor Technology and Science
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• 제4권3호
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• pp.189-195
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• 2004

A 10 Gb/s limiting amplifier IC with the emitter area of $1.5{\times}10{\mu}m^2$ for optical transmission system was designed and fabricated with a AIGaAs/GaAs HBTs technology. In this stud)', we evaluated fine pitch bump using WL-CSP (Wafer Level-Chip Scale Packaging) instead of conventional wire bonding for interconnection. For this we developed WL-CSP process and formed fine pitch solder bump with the $40{\mu}m$ diameter and $100{\mu}m$ pitch on bonding pad. To study the effect of WL-CSP, electrical performance was measured and analyzed in wafer and package module using WL-CSP. In a package module, clear and wide eye diagram openings were observed and the riselfall times were about 100ps, and the output" oltage swing was limited to $600mV_{p-p}$ with input voltage ranging from 50 to 500m V. The Small signal gains in wafer and package module were 15.56dB and 14.99dB respectively. It was found that the difference of small signal gain in wafer and package module was less then 0.57dB up to 10GHz and the characteristics of return loss was improved by 5dB in package module. This is due to the short interconnection length by WL-CSP. So, WL-CSP process can be used for millimeter wave GaAs MMIC with the fine pitch pad.

• Journal of electromagnetic engineering and science
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• 제18권1호
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• pp.63-69
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• 2018

This work demonstrates attenuation effects of plasma on waves propagating in the 26.5-40 GHz range. The effect is investigated via experiments measuring the transmission between two Ka-band horn antennas set 30 cm apart. A dielectric-barrier-discharge (DBD) plasma generator with a size of $200mm{\times}100mm{\times}70mm$ and consisting of 20 layers of electrodes is placed between the two antennas. The DBD generator is placed in a $400mm{\times}300mm{\times}400mm$ acrylic chamber so that the experiments can be performed for plasma generated under various conditions of gas and pressure, for instance, in air, Ar, and He environments at 0.001, 0.05, and 1 atm of pressure. Attenuation is calculated by the difference in the transmission level, with and without plasma, which is generated with a bias voltage of 20 kV in the 0.1-1.4 kHz range. Results show that the attenuation varies from 0.05 dB/m to 9.0 dB/m depending on the environment. Noble gas environments show higher levels of attenuation than air, and He is lossier than Ar. In all gas environments, attenuation increases as pressure increases. Finally, electromagnetic models of plasmas generated in various conditions are provided.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2003년도 추계학술대회 논문집 전기물성,응용부문
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• pp.98-100
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• 2003

The microwave dielectric properties and microstructure of the $0.7Mg_4Ta_2O_9-0.3CaTiO_3$ ceramics were investigated. All sample of the $0.7Mg_4Ta_2O_9-0.3CaTiO_3$ ceramics were prepared by conventional mixed oxide method. The sintering temperature was $1375^{\circ}C{\sim}1450^{\circ}C$. The structural properties of the $0.7Mg_4Ta_2O_9-0.3CaTiO_3$ ceramics were investigated by X-ray diffractormeter. According to the X-ray diffraction patterns of the $0.7Mg_4Ta_2O_9-0.3CaTiO_3$ ceramics, the major phase of the hexagonal $Mg_4Ta_2O_9$ were presented. In the case of the $0.7Mg_4Ta_2O_9-0.3CaTiO_3$ ceramics sintered at $1425^{\circ}C$, density, dielectric constant, quality factor were $5.799g/cm^2$, 23.26, 40,054 GHz, respectively.

• 한국자기학회지
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• 제17권2호
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• pp.55-59
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• 2007

본 논문에서는 Co를 주성분으로 하는 아몰퍼스 자성 와이어를 동축케이블의 신호선으로 하는 자계센서를 제작하여 외부자계에 대한 특성을 측정하였다. 측정된 임피던스의 주파수의존성에는 전송선로의 공진특성이 반영되었으며 인가자계가 없을 때, 1/4 파장에 해당하는 주파수가 250 MHz에서 나타났다. 측정 주파수대역에서는 표피효과에 의한 저항성분이 임피던스를 거의 결정하였으며 또한 외부자계가 $0\;Oe{\sim}1\;Oe$ 사이에서 임피던스는 자성 아몰퍼스와이어의 투자율의 변화에 의해 크게 변화하였다. 0.1 Oe 부근에서 150 MHz의 ${\Delta}Z/{\Delta}H$가 $300{\Omega}/Oe$이라는 매우 큰 값이 얻어져 Co를 주성분으로 하는 자성와이어를 동축케이블형 자계센서로 사용하는 경우 센서로서 매우 유용함을 알 수 있었다.

• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2002년도 Proceedings
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• pp.471-473
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• 2002

Public concerns associated with the electromagnetic field (EMF) exposures from mobile phones on human body are increased. Although studies on the effects of the EMF exposures on human have been carried out for a long time, it is not proved yet whether the EMF effect is harmful or not. Based on the scientific results by experts, EMF exposure limits have been regulated as a precautionary approach on the assumption that the EMF effect may be harmful. It is well known that absorbed EMF can be transformed into heat within biological tissues and that thermal effects are related with the specific absorption rate (SAR) distribution. However, the relative magnitude and distribution of the energies are not well defined. Although there is comprehensive information of the thermal effects, most of them come from animal and in vitro studies. Considerable efforts have been made to analyze the EMF absorption model while the actual temperature in the human body has been rarely measured. Temperature changes on the face of a healthy male volunteer were studied. A digital mobile phone of 1.8GHz was used. A digital infrared imaging system (IRIS-5000, Medicore, Seoul, Korea) was applied to take infrared pictures of the face every minute while the volunteer talked over the mobile phone for 20 minutes. The specification of the imaging system was as follows: Temperature resolution = 0.1$^{\circ}C$; Range of temperature measurement = 17～40$^{\circ}C$; Pixel size = 0.9mm ${\times}$ 0.9mm; Frame time = 2.6s; Active temperature of detector = 77$^{\circ}$K. The result showed that temperature of the ear region was increased during the phone call and the region of the temperature increase on the face was expanded as the phone call time increased. Further study is necessary to investigate the temperature rise analytically and quantitatively.

• 대한전자공학회논문지TC
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• 제39권11호
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• pp.34-39
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• 2002

본 논문에서는 마이크로스트립 전송선로의 유전체 기판(substrate) 내에 삽입된 EGP(Elevated Ground Plane)와 비아를 이용하는 소형의 새로운 포토닉 밴드갭(PBG：Photonic Bandgap) 구조를 제안였하고, 세라믹 기판에 적용된 최적구조를 설계하였다. 해석 결과, 제안된 새로운 PBG 구조는 기존의 평면 PBG 구조에 비해서 크기가 52.5 % 축소되었고 대역폭은 45 % 증가하였다. 그리고 접지면 식각 다층 PBG 구조에 비해서는 크기가 32 % 감소하였고 첨예도(sharpness)가 향상되었으며 차단주파수 이상에서 40 GHz까지 전력손실이 8 dB 이상 개선되었다. 따라서 본 논문에서 제안된 PBG 구조는 대역 저지 또는 저역통과 여파기로 사용할 수 있으며, 이러한 여파기 특성은 경박 단소화된 마이크로파 대역 집적회로나 모듈 개발에 효과적으로 활용될 수 있으리라 기대된다.

• 한국전자파학회논문지
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• 제11권6호
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• pp.876-885
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• 2000

추가적인 DC 측정이나 반복 계산법 또는 최적화 방법에 의존하지 않고도, 정상적인 바이어스(Normal activebias) 조건에서 측정하 S-파라미터로부터 MESFET과 HEMT의 외부 기생 저항을 간단히 구할 수 있는 방법이 제시되었다. 이를 위해서 zero 바이어스 조건에서 측정한 Z-파라미터로부터 Rs와 Rd의 차이를 구할수 있다는 사실이 이용된다. 측정한 S-파라미터로부터 외부 기생 인덕터와 캐패시터의 효과를 제거하면, 내부 소자와 외부 기생 저항을 포함한 새로운 소자를 정의할 수 있다. 내부 소자의 Y-파라미터인 Yint,11과 Yint,12의 실수부 값이 이론적으로 0이라는 사실을 이용하여 S-, Y-, Z-파라미터 행렬간의 상화관계를 이용하여 기생 저항 값을 쉽게계산할수 있다. 제시된 방법으로 기생 저항들을 구하고, 이 결과를 이용하여 내부 소자 등가회로를 구한 후에 40GHz까지 S-파라미터를 계산한 결과, 측정된 S-파라미터와 잘 일치하였다.