• Proceedings of the KIEE Conference
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• 1993.11a
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• pp.243-245
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• 1993

The negative curvature effect on the breakdown voltage of p-n junction, which may realize 1-D breakdown voltage due to the lower peak electric field at the junction, is proposed and verified by the fabrication of lateral diode on Silicon-on-Insulator (SOI) together with MEDICI simulation. The experimental and simulation results show good agreements with the theoretical expectation. The proposed method is effectively applicable to the lateral, especially on SOI, power devices.

• Journal of the Korean Institute of Telematics and Electronics A
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• v.32A no.1
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• pp.111-118
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• 1995

The three-dimentional effects on the breakdown voltage of non-reachthrough planar junctions which have the finite lateral radius of window curvature are analytically investigated. The critical electric fields at breakdown and the breakdown voltages are expressed successfully in a form which is normalized to the parallel plane case. The analytical results are in excellent agreement with the published results of experiment and the quasi-three-dimensional device simulation by MEDICI for non-reachthrough plane junctions having different background doping and junction depth. The results may be applicable to the estimations of breakdown voltages in many practical power devices.

• ETRI Journal
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• v.20 no.1
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• pp.37-45
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• 1998

Reduced surface field lateral double-diffused MOS transistor for the driving circuits of plasma display panel and field emission display in the 120V region have been integrated for the first time into a low-voltage $1.2{\mu}m$ analog CMOS process using p-type bulk silicon. This method of integration provides an excellent way of achieving both high power and low voltage functions on the same chip; it reduces the number of mask layers double-diffused MOS transistor with a drift length of $6.0{\mu}m$ and a breakdown voltage greater than 150V was self-isolated to the low voltage CMOS ICs. The measured specific on-resistance of the lateral double-diffused MOS in $4.8m{\Omega}{\cdot}cm^2$ at a gate voltage of 5V.

• Proceedings of the KSME Conference
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• 2001.11a
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• pp.544-549
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• 2001

The effect of power supply voltage on the performance limits in a laboratory Magneto-rheological fluid based device was identified by experiments. It suggests that the frequency range of motion for control be limited by the voltage attenuation due to the coil inductance and the maximum power supply voltage set for practical use of MRF devices. In this work, the magnetic and electrical characteristics of MRF device are investigated and a design procedure is formulated to achieve the desired performance for a given power supply.

• Proceedings of the IEEK Conference
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• 1999.06a
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• pp.918-921
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• 1999

The breakdown voltage in fully depleted SOI N-MOSFET’s have been studied over a wide range of film thicknesses, channel doping, and channel lengths. An asynmmetric Source/Drain SOI technology is proposed, which having the advantages of Normal LDD SOI(Silicon-On-Insulator) for breakdown voltage and gives a high drivability of LDD SOI without sacrificings hot carrier immunity The two-dimensional simulations have been used to investigate the breakdown behavior in these device. It is found that the breakdown voltage(BVds) is almost same with high current drivability as that in Normal LDD SOI device structure.

• Korean Journal of Optics and Photonics
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• v.5 no.2
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• pp.340-346
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• 1994

2.5Gbps 광통신시스템용 수광소자로서 charge plate층을 갖는 링구조의 separate absorption grading multiplication avalanche photodiode를 제작하고 그 특성을 조사 분석하였다. Avalanche Photodiode의 제작은 Metal-Organic Chemical Vapor Deposition 과 Liquid Phase Epitaxy법을 이용한 에피성장과 Br:Methanol을 이용한 채널식각 방법을 사용하였고, passivation과 평탄화는 photosensitive polyimide를 이용하였다. 제작된 ADP는 10nA 이하의 작은 누설전류를 나타내었고, -38~39 V의 항복전압을 나타내었다. 제작된 ADP를 GaAs FET hybrid 전치증폭기와 결합하여 2.5Gbps 속도에서 $2^{23}-1$의 길이를 갖는 입력 광신호에 대해 $ 10^{-10}$ Bit Error Rate에서 -31.0dBm의 수신감도를 얻었다.

• Proceedings of the KIEE Conference
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• 1996.07c
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• pp.1612-1614
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• 1996

Analytical expression for the breakdown voltage of the Schottky diode with double epitaxial layer has been obtained. Analytical results agree reasonably with the numerical simulations using MEDICI. It is expected that our results can be used for the optimum design of power MOSFET as well as the Schottky diodes with double epitaxial layer.

• Proceedings of the KIEE Conference
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• 1996.07c
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• pp.1431-1433
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• 1996

Effective ionization coefficients for (100), (110) and (111) oriented gallium arsenide are extracted from the ionization coefficients far electrons and holes. Analytical formulas for the breakdown voltage of the GaAs Schottky rectifiers are derived by employing the ionization coefficients. The breakdown voltages obtained from our analytical model agree fairly well with the numerical results as well as the experimental ones reported in the range of $10^{14}\;cm^{-3}$ - $5{\times}10^{17}\;cm^{-3}$ doping concentrations.

• Proceedings of the KIEE Conference
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• 2015.07a
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• pp.1124-1125
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• 2015

밴드-갭이 큰 반도체는 실리콘에 비하여 다양한 전기 물성 장점을 가져 고주파수 증폭 소자나 차세대 전력 반도체 소자로 각광을 받고 있다. 다양한 와이드 밴드-갭 반도체 중 AlGaN/GaN 이종접합 반도체는 채널의 높은 전도성과 높은 임계 전계로 인하여 우수한 전기적 특성을 가진다. 최근 발전된 수치해석 시뮬레이션을 이용하여 AlGaN/GaN 고전자 이동도 트랜지스터 (high-electron-mobility transistor, HEMT)의 설계연구를 진행하였다. AlGaN 장벽층의 두께가 증가할수록 채널의 전자 면 농도가 증가하도록 설계하였다. 또한 게이트 필드 플레이트 설계를 통하여 AlGaN/GaN HEMT의 역방향 전계 피크를 1개에서 2개로 증가시켜 항복전압을 368 V에서 최대 822 V로 개선하였다. 수렴문제를 개선한 수치해석 시뮬레이션은 RF power AlGaN/GaN HEMT의 설계에 유용하다.

• The Transactions of the Korean Institute of Electrical Engineers C
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• v.48 no.4
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• pp.226-231
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• 1999

Temperature dependence of effective ionization coefficients in GaAs is formulated as a single polynomial function of temperature, which allows analytical expressions for breakdown voltage of GaAs $p^+n$ junctions as a function of temperature. At 300 K, extracted effective ionization coefficient of GaAs $p^+n$ junction especially agrees well with the published result of <111> oriented GaAs. The analytic results agree with the simulation as well as the experimental ones reported within 10% in error for the doping concentrations in the range of $10_{14}cm_{-3}~10_{17}cm_{-3}$ at 100 K, 300 K and 500 K.