全耗尽异质栅单Halo SOI MOSFET二维模型

为了抑制深亚微米SOI MOSFET的短沟道效应,并提高电流驱动能力,提出了异质栅单Halo SOI MOSFET器件结构,其栅极由具有不同功函数的两种材料拼接而成,并在沟道源端一侧引入Halo技术.采用分区的抛物线电势近似法和通用边界条件求解二维Poisson方程,为新结构器件建立了全耗尽条件下的表面势及阈值电压二维解析模型.对新结构器件与常规SOI MOSFET性能进行了对比研究.结果表明,新结构器件能有效抑制阈值电压漂移、热载流子效应和漏致势垒降低效应,并显著提高载流子通过沟道的输运速度.解析模型与器件数值模拟软件MEDICI所得结果高度吻合.     

隐埋层中二维效应对全耗尽SOI非对称HALO结构阈值电压的影响

在非对称HALO结构的全耗尽SOI二维阈值电压解析模型的基础上,对阈值电压受隐埋层中二维效应的影响进行了讨论.通过与一维模型的比较,说明在深亚微米SOI MOSFET器件中隐埋层的二维效应会导致器件提前出现短沟道效应.新模型结果与二维数值模拟软件MEDICI吻合较好.     

隐埋层中二维效应对全耗尽SOI非对称HALO结构阈值电压的影响

在非对称HALO结构的全耗尽SOI二维阈值电压解析模型的基础上,对阈值电压受隐埋层中二维效应的影响进行了讨论.通过与一维模型的比较,说明在深亚微米SOI MOSFET器件中隐埋层的二维效应会导致器件提前出现短沟道效应.新模型结果与二维数值模拟软件MEDICI吻合较好.     

全耗尽SOIMOSFET辐照导致的阈值电压漂移模型

报道了全耗尽SOI MOSFET器件阈值电压漂移与辐照剂量和辐照剂量率之间的解析关系.模型计算结果与实验吻合较好.该模型物理意义明确,参数提取方便,适合于低辐照总剂量条件下的加固SOI器件与电路的模拟.讨论了抑制阈值电压漂移的方法.结果表明,对于全耗尽SOI加固工艺,辐照导致的埋氧层(BOX)氧化物电荷对前栅的耦合是影响前栅阈值电压漂移的主要因素,但减薄埋氧层厚度并不能明显提高SOI MOSFET的抗辐照性能.     

对异型硅岛实现的厚膜全耗尽SOIMOSFET的模拟研究

本文提出了用异型硅岛实现的厚膜全耗尽(FD)SOI MOSFET的新结构,并分析了其性能与结构参数的关系.通过在厚膜SOI MOSFET靠近背栅的界面形成一个相反掺杂的硅岛,从而使得厚膜SOI MOSFET变成全耗尽器件.二维模拟显示,通过对异型硅岛的宽度、厚度、掺杂浓度以及在沟道中位置的分析与设计,厚膜SOI MOSFET不仅实现了全耗尽,从而克服了其固有的Kink效应,而且驱动电流也大大增加,器件速度明显提高,同时短沟性能也得到改善.模拟结果证明:优化的异型硅岛应该位于硅膜的底部中央处,整个宽度约为沟道长度的五分之三,厚度大约等于硅膜厚度的一半,掺杂浓度只要高出硅膜的掺杂浓度即可.重要的是,异型硅岛的设计允许其厚度、宽度、掺杂浓度以及位置的较大波动.可以看出,异型硅岛实现的厚膜全耗尽 SOI MOSFET 为厚膜SOI器件提供了一个更广阔的设计空间.     

0.15μm薄膜全耗尽MOS／SOI器件的设计和研制

利用自己开发的二维数值深亚微米SOI器件模拟软件,较为详细地分析了沟道长度小于o.2μm的 SOI器件的阈值电压特性、穿通和击穿特性、亚阈值特性以及直流稳态特性等.通过这些模拟和分析计算,给出了沟道长度为0.18、0.15和0.1μm的薄膜全耗尽 SOI／MOS器件的设计方案,并根据该设计方案成功地研制出了性能良好的沟道长度为0.15μm的凹陷沟道 SOI器件.沟道长度为0.15μm薄膜全耗尽凹陷沟道SOI器件的亚阈值斜率为87mV/dec,击穿电压为1.6V,阈值电压为0.42V,电源电压为1.5V时的驱动电流为1.85mA,泄漏电流为0.5pA/μm沟道宽度.     

半导体与微电子技术

本会议录收集了会上发表的72篇论文,内容涉及蓝宝石上硅 CMOS 有源像素传感器,全耗尽 SOI 器件用4管 Schmitt 触发器,系统级芯片设计 SOI MOS-FET 分析,SOI 浮体存储器,应变硅技术β比率电路技术,SOI 碳纳米管场效应晶体管,MOSFET,超薄应变SOI CMOS 短沟道效应和阈值电压控制,纳米级应变硅生长对绝缘体上 SiGe 电子迁移率的影响,未来微处理机 FinFET 技术。     

簿全耗尽SOI膜N沟道MOSFET强反型电流模型

本文在仔细分析薄膜SOI器件特点及其特殊物理效应的基础上,发展了电路模拟所需要的N沟道薄全耗尽SOI膜MOSFET强反型电流模型.模拟计算和实际SOI器件测试结果之间的对比证实,在合理提取器件参数的情况下,该模型公式可较好地描述薄膜SOI器件的电流特性.     

异质栅非对称Halo SOI MOSFET

为了抑制异质栅SOI MOSFET的漏致势垒降低效应,在沟道源端一侧引入了高掺杂Halo结构.通过求解二维电势Poisson方程,为新结构器件建立了全耗尽条件下表面势和阈值电压解析模型,并对其性能改进情况进行了研究.结果表明,新结构器件比传统的异质栅SOI MOSFETs能更有效地抑制漏致势垒降低效应,并进一步提高载流子输运效率.新结构器件的漏致势垒降低效应随着Halo区掺杂浓度的增加而减弱,但随Halo区长度非单调变化.解析模型与数值模拟软件MEDICI所得结果高度吻合.     

异质栅非对称Halo SOI MOSFET

为了抑制异质栅SOI MOSFET的漏致势垒降低效应，在沟道源端一侧引入了高掺杂Halo结构．通过求解二维电势Poisson方程，为新结构器件建立了全耗尽条件下表面势和阈值电压解析模型，并对其性能改进情况进行了研究．结果表明，新结构器件比传统的异质栅SOI MOSFETs能更有效地抑制漏致势垒降低效应，并进一步提高载流子输运效率．新结构器件的漏致势垒降低效应随着Halo区掺杂浓度的增加而减弱，但随Halo区长度非单调变化．解析模型与数值模拟软件MEDICI所得结果高度吻合．     

全耗尽SOI MOSFETs阈值电压解析模型

提出了一种新的全耗尽SOI MOSFETs阈值电压二维解析模型.通过求解二维泊松方程得到器件有源层的二维电势分布函数,氧化层-硅界面处的电势最小值用于监测SOI MOSFETs的阈值电压.通过对不同栅长、栅氧厚度、硅膜厚度和沟道掺杂浓度的SOI MOSFETs的MEDICI模拟结果的比较,验证了该模型,并取得了很好的一致性.     

Suppression of short channel effects by full inversion in deep sub-micron gate SOI MOSFETs

Classical modeling of fully inverted SOI MOSFET (FI MOSFET) has been performed. In FI MOSFETs, the top Si layer is thinner than the thickness of the inversion layer at the conducting state and so the depleted region in the top Si layer is completely eliminated. It was found that the gate electric field induces carriers in the channel more effectively in FI MOSFET than in the fully depleted SOI MOSFETs (FD MOSFET), so that the short channel effects can be suppressed significantly.     

On the high-temperature subthreshold slope of thin-film SOI MOSFETs

This paper addresses the validity of the classical expression for the subthreshold swing (S) in SOI metal-oxide semiconductor field effect transistors (MOSFETs) at high temperature. Using numerical simulation, it is shown that two effects invalidate the classical expression of S at high temperature. Firstly, the depletion approximation becomes invalid and intrinsic free carriers must be taken into account to determine the effective body capacitance. Secondly, the charge-sheet model for the inversion layer becomes inaccurate due to a lowering of the electric field at the surface and a broadening of the inversion layer thickness in weak inversion. These effects must be taken into account to predict accurately the high-temperature subthreshold characteristics of both partially depleted and fully depleted SOI MOSFETs     

Threshold-Voltage Control of AC Performance Degradation-Free FD SOI MOSFET With Extremely Thin BOX Using Variable Body-Factor Scheme

The bias scheme of the variable body-factor fully depleted (FD) silicon-on-insulator (SOI) MOSFET, which has been previously proposed, is reexamined. Using a new scheme, the inversion and accumulation on the substrate in the active state can be avoided, and thus, ac performance in the active state is not degraded even with extremely thin buried-oxide (BOX), owing to the depletion of the substrate. Moreover, subthreshold leakage can be sufficiently suppressed in the standby state, owing to extremely thin BOX. This scheme provides threshold-voltage adjustability for the suppression of interdie and within-die variation in the active state. This device scheme is also applicable to multichannel FD SOI MOSFETs including FinFETs with a low-aspect-ratio fin, where the back-bias scheme can be applied     

Scaling fully depleted SOI CMOS

Quasi-two-dimensional (2-D) device analyses, 2-D numerical device simulations, and circuit simulations of nanoscale conventional, single-gate fully depleted (FD) silicon-on-insulator (SOI) CMOS are done to examine the scalability and performance potential of the technology. The quasi-2-D analyses, which can apply to double-gate devices as well, also provide a simple expression to estimate the effective channel length (L/sub eff/) of FD/SOI MOSFETs. The insightful results show that threshold-voltage control via channel doping and polysilicon gates is not a viable option for extremely scaled FD/SOI CMOS, and hence that undoped channels and metal gate(s) with tuned work function(s) must be employed. Quantitative as well as qualitative insights gained on the short-channel effects reveal the need for ultrathin films (t/sub Si/ < 10 nm) for L/sub eff/ < 50 nm. However, the implied manufacturing burden, compounded by effects of carrier-energy quantization for ultrathin t/sub Si/, forces a pragmatic limit on t/sub Si/ of about 5 nm, which in turn limits the scalability to L/sub eff/ = 25-30 nm. Unloaded CMOS-inverter ring-oscillator simulations, done with our process/physics-based compact model (UFDG) in SPICE3, show very good performance for L/sub eff/ = 35 nm, and suggest viable technology designs for low-power as well as high-performance applications. These simulations also reveal that moderate variations in t/sub Si/ can be tolerated, and that the energy quantization significantly influences the scaled-technology performance and hence must be properly accounted for in optimal FD/SOI MOSFET design.     

SOIMOSFET因辐照引起的部分耗尽与全耗尽过渡区的漂移

首次报道了辐照所引起的 SOI/ MOS器件 PD (部分耗尽 )与 FD (全耗尽 )过渡区的漂移 .基于含总剂量辐照效应的 SOI MOSFET统一模型 ,模拟了 FD与 PD过渡区随辐照剂量的漂移 .讨论了辐照引起 FD与 PD器件转化的原因 ,进一步分析了 FD与 PD器件的辐照效应     

Threshold voltage and C-V characteristics of SOIMOSFET's related to Si film thickness variation on SIMOX wafers

C-V characteristics of fully depleted SOI MOSFETs have been studied using a technique for measuring silicon-film thickness using a MOSFET. The technique is based on C-V measurements between the gate and source/drain at two different back-gate voltages, and only a large-area transistor is required. Using this technique, SOI film thickness mapping was made on a finished SIMOX wafer and a thickness variation of ±150 Å was found. This thickness variation causes as much as a 100-mV variation in the device threshold voltage. The silicon-film thickness variation and threshold-voltage variation across a wafer shows a linear correlation dependence for a fully depleted device. C-V measurements of the back-gate device yield the buried-oxide thickness and parasitic capacitances. The effects of GIDL (gate-induced drain leakage) current on C-V characteristics are also discussed     

Complimentary single-electron/hole action of nanoscale SOI CMOS transistors

We propose a new device structure for room-temperature single-electron/hole transistors based on nanosize narrow-width fully depleted silicon-on-insulator (SOI) CMOS transistors. The floating body of SOI MOSFETs can become a Coulomb island, whose single charging energy is more than 30 meV, as the gate length and width of MOSFETs is less than 10 nm. As SOI MOSFETs are biased at accumulation, single-electron, or hole tunnels, are sent, one by one, from the source to the floating body and then to the drain via Zener tunneling process. N-channel SOI MOSFETs can have the functions of single-electron transistors (n-SETs) while p-channel MOSFETs can have the functions of single-hole transistors (p-SETs). SOI MOSFETs still behave as typical MOSFETs when biased at inversion. There is a gate voltage margin of 0.9 V to separate Coulomb blockade oscillations from CMOS normal operation.     

On the gate capacitance limits of nanoscale DG and FD SOI MOSFETs

An analytical total gate capacitance C/sub G/ model for symmetric double-gate (DG) and fully depleted silicon-on-insulator (FD/SOI) MOSFETs of arbitrary Si film is developed and demonstrated. The model accounts for the effects of carrier-energy quantization and inversion-layer screening and is verified via self-consistent numerical solutions of the Poisson and Schro/spl uml/dinger equations. Results provide good physical insight regarding C/sub G/ degradation due to quantization and screening governed by device structure and/or transverse electric field for nanoscale DG and FD/SOI MOSFETs. Two limits of C/sub G/ at ON-state are then derived when the silicon film t/sub Si/ approaches zero and infinity. The effect of inversion-layer screening on C/sub G/, which is significant for ultrathin Si-film DG MOSFETs, is quantitatively defined for the first time. The insightful results show that the two-dimensional screening length for DG MOSFETs is independent of the doping density and much shorter than the bulk Debye length as a result of strong structural confinement.     

Short-channel effects in SOI MOSFETs

Short-channel effects in thin-film silicon-on-insulator (SOI) MOSFETs are shown to be unique because of dependences on film thickness and body and back-gate (substrate) biases. These dependences enable control of threshold-voltage reduction, channel-charge enhancement due to a drain bias, carrier velocity saturation, channel-length modulation and its effect on output conductance, as well as device degradation due to hot carriers in short-channel SOI MOSFETs. A short-channel effect exclusive to SOI MOSFETs, back-surface charge modulation, is described. Because of the short-channel effects, the use of SOI MOSFETs in VLSI circuits provides the designer with additional flexibility as compared to bulk-MOSFET design. Various design tradeoffs are discussed