Earticle

본 논문에서는 대칭형 이중 게이트 MOSFET의 회로해석에 대한 등가모델을 제시하고자 해석적 모델을 연구하였다. 본 연구의 해석적 모델에 사용된 방법은 2차원 포아송 방정식의 해를 가정하여 표면 전위 관계식을 유도하여 실리콘 몸체 내의 전위분포를 풀어 드레인 전압 변화에 대한 문턱전압 관계식을 도출하였다. 단채널 및 장채널 실리콘 채널에서 모두 해석이 가능한 해석적 모델을 적용 가능하도록 하기 위해 MOSFET의 채널 길이에 따른 제한된 지수함수를 적용함으로써 수백 나노미터까지 해석이 가능한 대칭형 이중 게이트 MOSFET 해석적 모델을 연구하였다.

In this thesis, in order to a equivalent circuit-analytical study for a symmetric double gate type MOSFET, we slove analytically the 2D Poisson's equation in a a silicon body. To solve the threshold voltage in a symmetric double gate type MOSFET from the derived expression for the surface potential which the two-dimensional potential distribution of a symmetric double gate type MOSFET is assumed approximately. This thesis can use short and long channel in a silicon body we introduce a new the threshold voltage model in a symmetric double gate type MOSFET and measure it the distance about the range of channel length up to 0.1 [㎛].

Silicon nanowire (SiNW) silicon-oxide-nitride-oxide-silicon (SONOS) flash memory devices were fabricated and their electrical characteristics were analyzed. Compared to planar SONOS devices, these SiNW SONOS devices have good program/erase (P/E) characteristics and a large threshold voltage ($V_T$) shift of 2.5 V in 1ms using a gate pulse of +14 V. The devices also show excellent immunity to short channel effects (SCEs) due to enhanced gate controllability, which becomes more apparent as the nanowire width decreases. This is attributed to the fully depleted mode operation as the nanowire becomes narrower. 3D TCAD simulations of both devices show that the electric field of the junction area is significantly reduced in the SiNW structure.

This paper presents the improvement of the boron penetration and the reverse short channel effect (RSCE) in the 130nm W/WNx/Poly-Si dual gate PMOSFET for a high performance embedded DRAM. In order to suppress the boron penetration, we studied a range in the process heat budget. It has shown that the process heat budget reduction results in suppression of the boron penetration. To suppress the RSCE, we experimented with the halo (large tilt implantation of the same type of impurities as those in the device well) implant condition near the source/drain. It has shown that the low angle of the halo implant results in the suppression of the RSCE. The experiment was supported from two-dimensional(2-D) simulation, TSUPREM4 and MEDICI.

In this paper, we present a compact model of gate-voltage-dependent quantum effects in short-channel surrounding-gate (SG) metal-oxide-semiconductor field-effect transistors (MOSFETs). We based the model on a two-dimensional (2-D) analytical solution of Poisson's equation using cylindrical coordinates. We used the model to investigate the electrostatic potential and current sensitivities of various gate lengths ($L_g$) and radii (R). Schr$\ddot{o}$dinger's equation was solved analytically for a one-dimensional (1-D) quantum well to include quantum effects in the model. The model takes into account quantum effects in the inversion region of the SG MOSFET using a triangular well. We show that the new model is in excellent agreement with the device simulation results in all regions of operation.

Density gradient method is used to analyze the quantum effect in MOSFET, Quantization effect in the poly gate leads to a negative threshold voltage shift, which is opposed to the positive shift caused by quantization effect in the channel. Quantization effects in the poly gate are investigated using the density gradient method, and the impact on the short channel effect of double gate device is more significant.

Spacer 유무와 핀 폭, 채널길이에 따른 n채널 MuGFET의 단채널 및 열화 특성을 비교 분석 하였다. 사용된 소자는 핀 수가 10인 Tri-Gate이며 Spacer 유무에 따른 핀 폭이 55nm, 70nm인 4종류이다. 측정한 소자 특성은 DIBL, subthreshold swing, 문턱전압 변화 (이하 단채널 현상)과 소자열화이다. 측정 결과, 단채널 현상은 spacer가 있는 것이 감소하였고, hot carrier degradation은 spacer가 있고 핀 폭이 작은 것이 소자열화가 적었다. 따라서, spacer가 있는 LDD(Lightly Doped Drain) 구조이며 핀 폭이 작은 설계방식이 단채널 현상 및 열화특성에 더욱 바람직하다.

The device performance of n-channel MuGFET with different fin width, existence of spacer and channel length has been characterized. Tri-Gate structure(fin number=10) has been used. There are four kinds of Tri-Gate with fin width=55nm with spacer, fin width=70nm with spacer, fin width=55nm without spacer, fin width=70nm without spacer. DIBL, subthreshold swing, Vt roll-off, (above Short Channel Effect)and hot carrier stress degradation have been measured. From the experiment results, short Channel Effect with spacer was decreased, hot carrier degradation with spacer and narrow fin width was decreased. Therefore, layout of LDD structure with spacer and narrow fin width is desirable in short channel effect and hot carrier degradation.

본 연구에서는 시뮬레이션을 통해 채널 폭과 채널 도핑 형태에 따른 수직형 나노와이어 GAA MOSFET의 특성을 비교, 분석하였다. 첫 번째로, 드레인의 끝부분을 20nm로 고정시키고 소스의 끝부분이 30nm, 50nm, 80nm, 110nm로 식각된 모양으로 설계한 구조의 특성을 비교, 분석하였다. 두 번째로는 드레인, 채널, 소스의 폭이 50nm로 일정한 직사각형 모양의 구조를 설계하였다. 이 구조를 기준으로 삼아 드레인의 끝부분이 20nm가 되도록 식각된 사다리꼴 모양과 반대로 소스의 끝부분이 20nm가 되도록 식각된 역 사다리꼴 모양의 구조를 설계하여 위 세 구조의 특성을 비교, 분석하였다. 마지막으로는 폭 50nm의 직사각형 구조의 채널을 다섯 구간으로 나누어 도핑 형태를 다양하게 변화시킨 것의 특성을 비교, 분석하였다. 첫 번째 시뮬레이션에서는 채널 폭이 가장 작을 때, 두 번째 시뮬레이션에서는 사다리꼴 모양의 구조일 때, 세 번째 시뮬레이션에서는 채널의 중앙 부분이 높게 도핑 되었을 때 가장 좋은 특성을 보였다.

In this work, we have analyzed the characteristics of vertical nanowire GAA MOSFET according to channel width and the type of channel doping through the simulation. First, we compared and analyzed the characteristics of designed structures which have tilted shapes that ends of drains are fixed as 20nm and ends of sources are 30nm, 50nm, 80nm and 110nm. Second, we designed the rectangular structure which has uniform width of drain, channel and source as 50nm. We used it as a standard and designed trapezoidal structure which is tilted so that the end of drain became 20nm and reverse trapezoidal structure which is tilted so that the end of source became 20nm. We compared and analyzed the characteristic of above three structures. For the last, we used the rectangular structure, divided its channel as five parts and changed the type of the five parts of doping concentration variously. In the first simulation, when the channel width is the shortest, in the second, when the structure is trapezoid, in the third, when the center of channel is high doped show the best characteristics.