• 반도체디스플레이기술학회지
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• 제18권4호
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• pp.138-142
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• 2019

As the NAND flash memory goes to 3D vertical Silicon-Oxide-Nitride-Oxide-Silicon (SONOS) structure, the lateral charge migration can be critical in the reliability performance. Even more, with miniaturization of flash memory cell device, just a little movement of trapped charge can cause reliability problems. In this paper, we propose a method of predicting the trapped charge profile in the retention mode. Charge diffusivity in the charge trapping layer (Si₃N₄) was extracted experimentally, and the effect on the trapped charge profile was demonstrated by the simulation and experiment.

• 한국결정성장학회지
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• 제28권4호
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• pp.141-147
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• 2018

태양광 에너지는 깨끗하며 무한한 재생에너지의 한가지로 많은 관심을 받아왔다. 태양광 에너지는 다결정 실리콘 웨이퍼 혹은 단결정 실리콘 웨이퍼로 구성된 솔라셀에 의해서 전기에너지로 전환된다. 제조원가를 낮추기 위하여 한 개의 석영 도가니에 폴리실리콘의 충진 크기를 증가시키는 연구가 많이 개발되어 왔다. 충진 크기를 증가시키면, 쵸크랄스키 공정장비의 온도제어가 강한 멜트 대류 때문에 힘들어진다. 본 연구에서는 20 inch와 24 inch 석영도가니와 90 Kg, 120 Kg, 150 Kg, 200 Kg, 250 Kg의 다양한 폴리실리콘 충진 크기에서 시뮬레이션을 통해 장비 온도 프로파일을 얻었으며, 실제값과 비교하고 분석하였다. 시뮬레이션 온도 프로파일과 실제 온도프로파일이 잘 일치하였으며, 이로써 충진 사이즈가 증가할 경우, 실제온도 프로파일 최적화를 위해 시뮬레이션을 사용할 수 있게 되었다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.897-900
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• 2001

Space charge distributions in silane crosslinked polyethylene (SXLPE)/ crosslinked polyethylene (XLPE) laminates was investigated using a pulsed electroacoustic (PEA) method. XLPE shows heterocharge while SXLPE shows homocharge. Positive charge is accumulated at the interface of SXLPE/XLPE laminate when applied electric field is more than 20 kV/mm. The charge profile at various temperatures was also acquired using temperature-controllable PEA system. Although applied electric field is only 8.6 kV/mm, positive interfacial charge starts to appear near 50$^{\circ}C$.

• 한국전기전자재료학회논문지
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• 제15권2호
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• pp.127-132
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• 2002

Space charge distributions and behaviors in silane crosslinked polyethylene(SXLPE)/ crosslinked polyethylene(XLPE) laminates were investigated using a pulsed electroacoustic (PEA) method. In case of monolayer, XLPE shows heterocharge while SXLPE shows homocharge. It was observed that charges were accumulated at the interface of SXLPE/XLPE laminate when applied electric field was more than 20kV/mm. The charge profile at various temperatures was also acquired using temperature-controllable PEA system. Although applied electric field is only 8.6 kV.mm, positive interfacial charge starts to appear near 50$^{\circ}C$. It was found that the interfacial charge behavior of SXLPE/XLPE laminate under low voltage at high temperature is corresponding to that under high voltage at room temperature.

• Korea-Australia Rheology Journal
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• 제15권2호
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• pp.83-90
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• 2003

In cases of the microfluidic channel, the electrokinetic influence on the transport behavior can be found. The externally applied body force originated from the electrostatic interaction between the nonlinear Poisson-Boltzmann field and the flow-induced electrical field is applied in the equation of motion. The electrostatic potential profile is computed a priori by applying the finite difference scheme, and an analytical solution to the Navier-Stokes equation of motion for slit-like microchannel is obtained via the Green's function. An explicit analytical expression for the induced electrokinetic potential is derived as functions of relevant physicochemical parameters. The effects of the electric double layer, the zeta potential of the solid surface, and the charge condition of the channel wall on the velocity profile as well as the electroviscous behavior are examined. With increases in either electric double layer or zeta potential, the average fluid velocity in the channel of same charge is entirely reduced, whereas the electroviscous effect becomes stronger. We observed an opposite behavior in the channel of opposite charge, where the attractive electrostatic interactions are presented.

• Transactions on Electrical and Electronic Materials
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• 제5권4호
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• pp.148-152
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• 2004

The direct lateral profile and retention characteristics of locally trapped-charges in the nitride layer of the two-bit polysilicon-oxide-nitride-oxide-silicon (SONOS) memory are investigated by using the charge pumping method. After charges injection at the drain junction region, the lateral diffusion of trapped charges as a function of retention time is directly shown by the results of the local threshold voltage and the trapped-charges quantities.

• 전기학회논문지
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• 제58권11호
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• pp.2229-2235
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• 2009

In this paper, each specimen blended at weight proportions of 80% HDPE to 20% EVA, 70% HDPE to 30% EVA, 60% HDPE to 40% EVA, and 50% HDPE to 50% EVA was manufactured respectively. The insulation performances of the proposed insulator were compared with conventional XLPE, main insulating material of CV cable on the basis of the investigation results of DC insulation performances. From the space charge density, electric field and potential profiles with raising DC voltage and time variation in HE82, distortion of electric field distribution was improved. As EVA mixed into the bulks acts as nucleation in crystallization process of HDPE, the size of spherulites became decreased and finally formed continuous network structure. Ultimately, it resulted from extinction of space charge in the interfacial region of spherulites.

• ETRI Journal
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• 제9권1호
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• pp.97-103
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• 1987

짧은 채널($L<1\mum$) MOSFET의 전기적 변수, 특히 문턱전압(threshold voltage)을 최적화시키기 위하여 분석적 문턱전압 모델을 개발하였다. 채널 영역에서의 붕소profile은 계단 (step) profile로 근사시켜 표면전하층과 기판전하층으로 구성하였다. 최대공핍층내에 있는 두 전하층의 각각에 대하여 기하학적으로 근사시킨 전하분배(charge sharing)모델을 적용하고 이차원적 분석을 이용하여 짧은 채널 효과를 계산하였다. 본 모델을 실험치와 비교하고 이온주입 공정의 최적조건을 이끌어내는 데 필요한 변수에 대하여 논의하였다.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 춘계학술대회논문집D
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• pp.286-291
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• 2001

This paper describes an optimal scheduling for ice slurry systems for energy cost saving. The optimization technique applied in the study is the dynamic programming method, for which the state variable is the storage in the ice storage tank and the control variable is the state of chiller's on-off switching. Though the costs during charge period is included in optimization by taking the average cost of ice per hour for slurry making, the time horizon for the simulation is limited building cooling period because accurate charge rate from the ice maker into the ice storage tank cannot be estimated during the charge period. In the operating simulation after optimizing procedure, energy consumption and operating cost for the optimal control are calculated and compared with them for a conventional control with one case of cooling load profile.

• 한국지능시스템학회논문지
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• 제20권2호
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• pp.214-219
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• 2010

본 논문은 리튬폴리머 배터리의 잔존충전용량 추정을 위한 비선형 퍼지 $H_{\infty}$ 필터의 설계 방법을 제시한다. 배터리 셀의 동적방정식을 T-S 퍼지시스템으로 모델하고 선형행렬 부등식의 해를 이용하여 퍼지필터를 설계한다. 제시한 퍼지 $H_{\infty}$ 필터의 성능을 입증하기 위하여 UDDS 전류 프로파일을 사용한 실험 데이터를 이용하여 모의실험을 수행하였다.