Changhwan Shin
성균관대학교 전기컴퓨터공학과 · 공학
Changhwan Shin 교수의 연구실은 나노전자소자 및 에너지 저장 소자의 핵심 기반 기술을 연구하고 있습니다. 특히, 고성능 트랜지스터 설계(예: 트리게이트 MOSFET, FD-SOI, 음성용량 FET)와 랜덤 도핑 불확실성, 임계전압 변동성 등의 미세공정 문제를 원자구조 수준의 3D 시뮬레이션과 실험을 융합하여 해결하고자 합니다. 또한, 초용량 축전기, 이브리데이트(ReSe₂) 기반 near-IR 광검출기, 허프리티컬렉터 기반 메모리 소자 등 차세대 에너지 및 전자 소자에 응용 가능한 신소재와 신기법을 개발하고 있습니다.
표시된 성과는 수집된 데이터 기준으로 산출되며, 일부 차이가 있을 수 있습니다.
A study of random-dopant-fluctuation (RDF) effects on the trigate bulk MOSFET versus the planar bulk MOSFET is performed via atomistic 3D device simulation for devices with a 20 nm gate length. For identical nominal body and source/drain doping profiles and layout width, the trigate bulk MOSFET shows less threshold voltage (V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">th</sub> ) lowering and variation. RDF effects are found to be caused primari
Supercapacitors have shown great potential as a possible solution to the increasing global demand for next-generation energy storage systems. Charge repositioning is based on physical or chemical mechanisms. There are three types of supercapacitors-the electrochemical double layer, the pseudocapacitor, and a hybrid of both. Each type is further subdivided according to the material used. Herein, a detailed overview of the working mechanism as well as a new method for capacitance enhancement are p
A negative capacitance field‐effect transistor (FET) with sub‐60 mV/decade subthreshold slope (SS) at different temperatures (i.e. 14.8 mV/decade at 300 K, 15.7 mV/decade at 360 K and 24.3 mV/decade at 400 K) is experimentally demonstrated. A detailed account of the fabrication process of a negative capacitor is first introduced, followed by the measurement setup for the negative capacitance FET. The impact of temperature on negative capacitance FETs is investigated: (i) the equation for the int
The performance and threshold voltage variability of fully depleted silicon-on-insulator (FD-SOI) MOSFETs are compared against those of conventional bulk MOSFETs via 3-D device simulation with atomistic doping profiles. Compact (analytical) modeling is then used to estimate six-transistor SRAM cell performance metrics (i.e., read and write margins, and read current) at the 22 nm CMOS technology node. The dependences of these metrics on cell ratio, pull-up ratio, and operating voltage are analyze
In this study, a near-infrared photodetector featuring a high photoresponsivity and a short photoresponse time is demonstrated, which is fabricated on rhenium diselenide (ReSe<sub>2</sub>) with a relatively narrow bandgap (0.9-1.0 eV) compared to conventional transition-metal dichalcogenides (TMDs). The excellent photo and temporal responses, which generally show a trade-off relation, are achieved simultaneously by applying a p-doping technique based on hydrochloric acid (HCl) to a selected ReSe
The endurance characteristic of Zr-doped HfO<sub>2</sub> (HZO)-based metal-ferroelectric-metal (MFM) capacitors fabricated under various deposition/annealing temperatures in the atomic layer deposition (ALD) process was investigated. The chamber temperature in the ALD process was set to 120 °C, 200 °C, or 250 °C, and the annealing temperature was set to 400 °C, 500 °C, 600 °C, or 700 °C. For the given annealing temperature of 700 °C, the remnant polarization (2P<sub>r</sub>) was 17.21 µC/cm<sup>
Feedback field-effect transistors (FBFETs) are devices based on a positive feedback loop in which the electrons and holes in the channel region act on the energy states of the potential barrier and wall. Owing to the positive feedback phenomenon, FBFETs have an excellent subthreshold swing (~0 mV/decade at 300 K), a high on-/off current ratio (~1010), and a clear saturation region. The power consumption of both the turn-on state and turn-off state is significantly low until operation commences.
The performance and threshold voltage variability of quasi-planar bulk MOSFETs are compared against those of conventional bulk MOSFETs, via three-dimensional (3-D) device simulations with gate line-edge roughness and atomistic doping profiles, at 25 nm gate length. The nominal performance of sixtransistor (6-T) SRAM cells is studied via 3-D simulation of full cell structures. Compact (analytical) modeling is used to estimate SRAM cell yields. As compared to conventional bulk CMOS technology, qua