FinFET静电可靠性及新型Fix-base SOI FinFET研究

在鳍型场效应晶体管(SOI FinFET)相关静电防护技术研究基础上,提出了一种新型的体区接触固定型绝缘体上硅鳍型场效应晶体管泄放钳位装置(Fix-base SOI FinFET Clamp)。该新型结构的器件解决了基区接触浮空在静电防护设计时引起的一系列问题,而且对正常的FinFET工艺具有良好的兼容性。通过计算机辅助工艺设计(TCAD)仿真论证了Fix-base SOI FinFET Clamp具有明显效果,详细阐述和讨论了SOI FinFET和Fix-base SOI FinFET Clamp工作状态下的电流和热分布。     

BJMOSFET温度特性分析及计算机模拟

对兼有双极型和场效应型两种器件特点的双极MOS场效应晶体管(BJMOSFET)的电流和阈值电压的温度特性进行了详细分析．推导出它们随温度变化率的解析表达式。建立BJMOSFET的直流小信号模拟分析等效电路和频率特性模拟分析等效电路,采用通用电路仿真软件PSpice9,对BJMOSFET的输出特性、瞬态特性和幅频特性随温度的变化进行了计算机模拟,得到了随温度变化的特性曲线,并且理论分析与计算机模拟取得了一致的结果。相对传统MOSFET,证明了BJMOSFET具有较好的温度特性。     

SOI横向双晶体管结构研究

本文首先概括地介绍了体硅、SOI纵向双极晶体管和横向双极晶体管的各自特点，并简要地阐述了SOI横向双极晶体管的发展；其次，对各种SOI横向双极晶体管的结构与性能进行了分析研究；最后，我们认为SOI横向双极晶体管是一种比较理想的双极器件，不失为SOI／BiCMOS的理想选择。     

基于UTB-SOI技术的双辅助触发SCR ESD防护器件研究

为了提高FDSOI ESD防护器件的二次击穿电流,基于UTB-SOI技术,提出了一种SOI gg-NMOS和寄生体硅PNP晶体管双辅助触发SCR器件。通过gg-NMOS源区的电子注入和寄生PNP晶体管的开启,共同辅助触发主泄放路径SCR,快速泄放ESD电流。TCAD仿真结果表明,新结构能够泄放较高的二次击穿电流,具有可调节的触发电压。     

新型半导体器件—联栅晶体管（GAT）

联栅晶体管（ＧＡＴ）是一种介于双极型晶体管和结型场效应晶体管之间的电流控制型电力电子器件。本文介绍了ＧＡＴ的结构、特点及其应用。     

超深亚微米SOI总剂量效应泄漏电流模型

总剂量辐射效应会导致绝缘体上硅金属氧化物半导体场效应晶体管(SOI MOSFET)器件的阈值电压漂移、泄漏电流增大等退化特性。浅沟槽隔离(STI)漏电是器件退化的主要因素,会形成漏极到源极的寄生晶体管。针对130 nm部分耗尽(PD) SOI NMOSFET器件的总剂量辐射退化特性,建立了一个包含总剂量辐射效应的通用模拟电路仿真器(SPICE)模型。在BSIM SOI标准工艺集约模型的基础上,增加了STI寄生晶体管泄漏电流模型,并考虑了辐射陷阱电荷引起寄生晶体管的等效栅宽和栅氧厚度的变化。通过与不同漏压下、不同宽长比的器件退化特性的实验结果对比,该模型能够准确反映器件辐射前后的漏电流特性变化,为器件的抗辐射设计提供参考依据。     

双极双栅MOS晶体管静态特性解析模型的模拟与分析

提出了一种应用于VHF和UHF的新型功率电子器件－双极双栅MOS晶体管（BDGMOSFET）,该结构是在单栅MOSFET一侧引入双极型压控晶体管（BJMOSFET）,使之在正向工作时具有MOSFET和BJT的工作特性,通态电较小,同时,减少了寄生双极晶体管效应,改善了频率特性。文章对其静态特性的解析模型进行了详细研究,在该模型基础上运用通用电路模拟软件PSPICE的多瞬态分析法模拟了BDEMOSFET的直流特性,结果表明,在同等条件下,BDGMOSFET的电流密度比双栅MOSFET提高大约30％。     

DSOI总剂量效应模型及背偏调控模型

总剂量辐射效应会导致绝缘体上硅金属氧化物半导体场效应晶体管(DSOI MOSFET)器件的阈值电压漂移、泄漏电流增大等退化特性。由于背栅端口的存在,SOI器件存在新的总剂量效应加固途径,对于全耗尽SOI器件,利用正背栅耦合效应,可通过施加背栅偏置电压补偿辐照导致的器件参数退化。本文研究了总剂量辐照对双埋氧层绝缘体上硅金属氧化物半导体场效应晶体管(DSOI MOSFET)总剂量损伤规律及背栅偏置调控规律,分析了辐射导致晶体管电参数退化机理,建立了DSOI晶体管总剂量效应模拟电路仿真器(SPICE)模型。模型仿真晶体管阈值电压与实测结果≤6 mV,同时根据总剂量效应模型给出了相应的背栅偏置补偿模型,通过晶体管背偏调控总剂量效应SPICE模型仿真输出的补偿电压与试验测试结果对比,N型金属氧化物半导体场效应晶体管(NMOSFET)的背偏调控模型误差为9.65%,P型金属氧化物半导体场效应晶体管(PMOSFET)为5.24%,该模型可以准确反映DSOI器件辐照前后阈值特性变化,为器件的背栅加固提供参考依据。     

SOI LIGBT抗闩锁效应的研究与进展

概述了绝缘层上硅横向绝缘栅双极晶体管(SOI LIGBT)抗闩锁结构的改进历程,介绍了从早期改进的p阱深p+欧姆接触SOI LIGBT结构到后来的中间阴极SOI LIGBT、埋栅SOILIGBT、双沟道SOI LIGBT、槽栅阳极短路射频SOI LIGBT等改进结构;阐述了一些结构在抗闩锁方面的改善情况,总结指出抑制闩锁效应发生的根本出发点是通过降低p基区电阻的阻值或减小流过p基区电阻的电流来削弱或者切断寄生双极晶体管之间的正反馈耦合。     

低温大注入多晶硅发射极硅双极晶体管电流增益的定量模拟

已有的理论和实验都已证明，多晶硅发射极硅双极晶体管适合于低温工作，但至今为止，其完整的大注入时电流增益的理论分析还不成熟，特别是进行定量的计算。本文定量地模拟了低温７７Ｋ和常温３００Ｋ下多晶硅发射极硅双极晶体管电流增益与集电极电流密度的关系，并且分析了低温和常温下决定该晶体管电流增益大注入效应的主要物理效应。     

Numerical Simulation of BJMOSFET on Current-Voltage Characteristics

A new power MOSFET Structure with a pn junction--Bipolar Junction MOSFET (BJMOSFET) has been proposed. The device has the advantages of both BJT and FET. The numerical model of the I-V characteristics of BJMOSFET has been obtained on the basis of both numerical and analytical methods. With the software package of Mathematic, we firstly calculate the gain factor, and then simulate the voltage tranmission, voltage output and voltage transfer's characteristic graphs of the BJMOSFET. The simulation result indicates that BJMOSFET has the current density, which is about 25% larger than the power MOSFET, under the same operating conditions and with the same structure parameters, except that the threshold voltage increase a little.     

Modeling for floating body effects in fully depleted SOI MOSFETs

A model based on SOI MOSFET and BJT device theories is developed to describe the current kink and breakdown phenomena in thin-film SOI MOSFET drain-source current-voltage characteristics operated in strong inversion. The modulation of MOSFET current by raised floating body potential is discussed to provide an insight for understanding the suppression of current kink in fully depleted thin-film SOI devices. The proposed analytical model successfully simulates the drain current-voltage characteristics of thin-film SOI n-MOSFETs fabricated on SIMOX wafers     

Analysis and control of floating-body bipolar effects in fullydepleted submicrometer SOI MOSFET's

Floating-body effects triggered by impact ionization in fully depleted submicrometer silicon-on-insulator (SOI) MOSFETs are analyzed based on two-dimensional device simulations. The parasitic bipolar junction transistor (BJT) effects are emphasized, but the kink effect and its disappearance in the fully depleted device are first explained physically to provide a basis for the BJT analysis. The results of simulations of the BJT-induced breakdown and latch phenomena are given, and parametric dependences are examined to give physical insight for optimal design. The analysis further relates the DC breakdown and latch mechanisms in the fully depleted submicrometer SOI MOSFET to actual BJT-related problems in an operating SOI CMOS circuit. A comprehensive understanding of the floating-body effects is attained, and a device design to control them utilizing a lightly doped source (LDS) is suggested and shown to be feasible     

Computer-aided performance assessment of fully depleted SOI CMOSVLSI circuits

A physical model for the fully depleted submicrometer SOI MOSFET is described and used to assess the performance of SOI CMOS VLSI digital circuits. The computer-aided analysis is focused on both problematic and beneficial effects of the parasitic bipolar junction transistor (BJT) in the floating-body device. The study shows that the bipolar problems overwhelm the benefits, and hence must be alleviated by controlling the activation of the BJT via device design tradeoffs. A feasible approach to the needed design optimization is demonstrated by veritable device/circuit simulations, which also predict significant speed superiority of SOI over bulk-silicon CMOS circuits in scaled, submicrometer technologies     

High-gain lateral bipolar action in a MOSFET structure

A hybrid-mode device based on a standard submicrometer CMOS technology is presented. The device is essentially a MOSFET in which the gate and the well are internally connected to form the base of a lateral bipolar junction transistor (BJT). At low collector current levels, lateral bipolar action with a current gain higher than 1000 is achieved. No additional processing steps are needed to obtain the BJT when the MOSFET is properly designed. n-p-n BJTs with a 0.25-μm base width have been successfully fabricated in a p-well 0.25-μm bulk n-MOSFET process. The electrical characteristics of the n-MOSFET and the lateral n-p-n BJT at room and liquid nitrogen temperatures are reported     

Study on the device characteristics of a quasi-SOI power MOSFETfabricated by reversed silicon wafer direct bonding

The device characteristics of a quasi-SOI power MOSFET were investigated to obtain its optimum device structure. The oxide at the original bottom surface of the bulk power MOSFET of the quasi-SOI power MOSFET formed by reversed silicon wafer direct bonding acts as the buried oxide of the conventional SOI power MOSFET. The short channel effect of the quasi-SOI power MOSFET was larger than that in the conventional SOI power MOSFET. It was suppressed by increasing the width of the oxide in the body region, and the parasitic bipolar effect was suppressed by decreasing it. We also propose a new device structure which can suppress the short channel effect and parasitic bipolar effect of a quasi-SOI power MOSFET based on the results of these experiments     

Characterization of double gate MOSFETs fabricated by a simple method on a recrystallized silicon film

A simple process to fabricate double gate SOI MOSFET is proposed. The new device structure utilizes the bulk diffusion layer as the bottom gate. The active silicon film is formed by recrystallized amorphous silicon film using metal-induced-lateral-crystallization (MILC). While the active silicon film is not truly single crystal, the material and device characteristics show that the film is equivalent to single crystal SOI film with high defect density, like SOI wafers produced in early days. The fabricated double gate MOSFETs are characterized, which demonstrate excellent device characteristics with higher current drive and stronger immunity to short channel effects compared to the single gate devices.     

以Si3N4为埋层的SOI结构制备与器件模拟

为了减少经典SOI器件的自加热效应,首次成功地用外延方法制备以Si3N4薄膜为埋层的新结构SOSN,用HRTEM和SRP表征了SOI的新结构.实验结果显示,Si3N4层为非晶状态,新结构的SOSN具有良好的结构和电学性能.对传统SOI和新结构SOI的MOSFETs输出电流的输出特性和温度分布用TCAD仿真软件进行了模拟.模拟结果表明,新结构SOSN的MOSFET器件沟道温度和NDR效益都得到很大的降低,表明SOSN能够有效地克服自加热效应和提高MOSFET漏电流.     

Low-voltage transient bipolar effect induced by dynamicfloating-body charging in scaled PD/SOI MOSFETs

An increased significance of the parasitic bipolar transistor (BJT) in scaled floating-body partially depleted SOI MOSFETs under transient conditions is described. The transient parasitic BJT effect is analyzed using both simulations and high-speed pulse measurements of pass transistors in a sub-0.25 μm SOI technology. The transient BJT current can be significant even at low drain-source voltages, well below the device breakdown voltage, and does not scale with technology. Our analysis shows that it can be problematic in digital circuit operation, possibly causing write disturbs in SRAMs and decreased retention times for DRAMs. Proper device/circuit design, suggested by our analysis, can however control the problems     

A physical model of floating body thin film silicon-on-insulatornMOSFET with parasitic bipolar transistor

An analytical model for SOI nMOSFET with a floating body is developed to describe the I_ds-V_ds characteristics. Considering all current components in MOSFET as well as parasitic BJT, this study evaluates body potential, investigates the correlations among many device parameters, and characterizes the various phenomena in floating body: threshold voltage reduction, kink effect, output conductance increment, and breakdown voltage reduction. This study also provides a good physical insight on the role of the parasitic current components in the overall device operation. Our model explains the dependence of the channel length on the I_ds-V_ds characteristics with parasitic BJT current gain. Results obtained from this model are in good agreement with the experimental I_ds-V _ds curves for various bias and geometry conditions