应变SiGe沟道PMOSFET亚阈值特性模拟

通过简化的模型,对应变SiGe沟道PMOSFET及Si PMOSFET的亚阈值特性作出了简单的理论分析,然后用二维模拟器Medici进行了模拟和对比;研究了截止电流和亚阈值斜率随SiGe PMOSFET垂直结构参数的变化关系。模拟结果同理论分析符合一致,表明应变SiGe沟道PMOSFET的亚阈值特性比Si PMOSFET更差,并且对垂直结构参数敏感,在器件设计时值得关注。     

一种适合制作CMOS的SiGePMOSFET

在通常适合于制作埋沟 Si Ge NMOSFET的 Si/弛豫 Si Ge/应变 Si/弛豫 Si Ge缓冲层 /渐变 Ge组分层的结构上 ,制作成功了 Si Ge PMOSFET.这种 Si Ge PMOSFET将更容易与 Si Ge NMOSFET集成 ,用于实现 Si Ge CMOS.实验测得这种结构的 Si Ge PMOSFET在栅压为 3.5 V时最大饱和跨导比用作对照的 Si PMOS提高约 2倍 ,而与常规的应变 Si Ge沟道的器件相当     

深亚微米应变SiGe沟PMOSFET特性模拟

为研究深亚微米尺度下应变 Si Ge沟改进 PMOSFET器件性能的有效性 ,运用二维数值模拟程序MEDICI模拟和分析了 0 .1 8μm有效沟长 Si Ge PMOS及 Si PMOS器件特性。Si Ge PMOS垂直方向采用 Si/Si Ge/Si结构 ,横向结构同常规 PMOS,N+ -poly栅结合 P型δ掺杂层获得了合理阈值电压及空穴局域化。研究表明 ,经适当设计的 Si Ge PMOS比对应 Si PMOS的 IDmax、gm、f T均提高 1 0 0 %以上 ,表明深亚微米尺度 Si Ge沟PMOSFET具有很大的性能提高潜力     

一种适合制作CMOS的SiGe PMOSFET

在通常适合于制作埋沟SiGe NMOSFET的Si/弛豫SiGe/应变Si/弛豫SiGe缓冲层/渐变Ge组分层的结构上,制作成功了SiGe PMOSFET.这种SiGe PMOSFET将更容易与SiGe NMOSFET集成,用于实现SiGe CMOS.实验测得这种结构的SiGe PMOSFET在栅压为3.5V时最大饱和跨导比用作对照的Si PMOS提高约2倍,而与常规的应变SiGe沟道的器件相当.     

双应变SiGe/Si异质结CMOS的设计及其电学特性的Medici模拟

本文提出一种沟道长度为0.125 μm的异质结CMOS(HCMOS)器件结构.在该结构中,压应变的SiGe与张应变的Si分别作为异质结PMOS(HPMOS)与异质结NMOS(HNMOS)的沟道材料,且HPMOS与HNMOS为垂直层叠结构;为了精确地模拟该器件的电学特性,修正了应变SiGe与应变Si的空穴与电子的迁移率模型;利用Medici软件对该器件的直流与交流特性,以及输入输出特性进行了模拟与分析.模拟结果表明,相对于体Si CMOS器件,该器件具有更好的电学特性,正确的逻辑功能,且具有更短的延迟时间,同时,采用垂直层叠的结构此类器件还可节省约50%的版图面积,有利于电路的进一步集成.     

考虑库仑散射屏蔽效应的Si_(1-x)Ge_x pMOSFET低场空穴迁移率模型

在考虑应变对SiGe合金能带结构参数影响的基础上,建立了一个半经验的Si1-xGexpMOSFET反型沟道空穴迁移率模型。该模型重点讨论了反型电荷对离化杂质散射的屏蔽作用,由此对等效体晶格散射迁移率进行了修正。并且详细讨论了等效体晶格散射迁移率随掺杂浓度Nd和组分x的变化。利用该模型,对影响空穴迁移率的主要因素进行了分析讨论。通过模拟得出,增加组分x可以显著提高等效体晶格散射迁移率,从而可以提高PMOSFET的空穴迁移率。     

考虑源漏串联电阻时6H-SiC PMOSFET解析模型

在考虑源漏串联电阻的基础上,建立了一组适用于Si C PMOSFET的解析模型.计算结果与实验结果符合得很好     

绝缘层上Si/应变Si1-xGex/Si异质结p-MOSFET电学特性二维数值分析

对绝缘层上Si/应变Si1-xGex/Si异质结p-MOSFET电学特性进行二维数值分析,研究了该器件的阈值电压特性、转移特性、输出特性.模拟结果表明,随着应变Si1-xGex沟道层中的Ge组分增大,器件的阈值电压向正方向偏移,转移特性增强;当偏置条件一定时,漏源电流的增长幅度随着Ge组分的增大而减小;器件的输出特性呈现出较为明显的扭结现象.     

应变Si1-xGex沟道PMOSFET空穴局域化研究

为充分利用应变 Si Ge材料相对于 Si较高的空穴迁移率 ,研究了 Si/Si Ge/Si PMOSFET中垂直结构和参数同沟道开启及空穴分布之间的依赖关系。在理论分析的基础上 ,以数值模拟为手段 ,研究了栅氧化层厚度、Si帽层厚度、Si Ge层 Ge组分及厚度、缓冲层厚度及衬底掺杂浓度对阈值电压、交越电压和空穴分布的影响与作用 ,特别强调了 δ掺杂的意义。模拟和分析表明 ,栅氧化层厚度、Si帽层厚度、Si Ge层 Ge组分、衬底掺杂浓度及 δ掺杂剂量是决定空穴分布的主要因素 ,而 Si Ge层厚度、缓冲层厚度和隔离层厚度对空穴分布并不敏感。最后总结了沟道反型及空穴分布随垂直结构及参数变化的一般规律 ,为优化器件设计提供了参考。     

基于应变Si/SiGe的CMOS电特性模拟研究

提出了一种应变Si/SiGe异质结CMOS结构,采用张应变Si作n-MOSFET沟道,压应变SiGe作p-MOSFET沟道,n-MOSFET与p-MOSFET采用垂直层叠结构,二者共用一个多晶SiGe栅电极.分析了该结构的电学特性与器件的几何结构参数和材料物理参数的关系,而且还给出了这种器件结构作为反相器的一个应用,模拟了其传输特性.结果表明所设计的垂直层叠共栅结构应变Si/SiGe HCMOS结构合理、器件性能提高.     

应变SiGe沟道PMOSFET阈值电压模型

首先建立了应变SiGe沟道PMOSFET的一维阈值电压模型,在此基础上,通过考虑沟道横向电场的影响,将其扩展到适用于短沟道的准二维阈值电压模型,与二维数值模拟结果呈现出好的符合。利用此模型,模拟分析了各结构参数对器件阈值电压的影响,并简要讨论了无Sicap层器件的阈值电压。     

Fabrication of strained Si channel PMOSFET on thin relaxed Si1−xGex virtual substrate

A novel MBE-grown method using low-temperature Si technology is introduced into the fabrication of strained Si channel PMOSFETs. The thickness of relaxed Si_1−xGe_x epitaxy layer on bulk silicon is reduced to approximate 400 nm (x=0.2). The Ge fraction and relaxation of Si_1−xGe_x film are confirmed by DCXRD (double crystal X-ray diffraction) and the DC characteristics of strined Si channel PMOSFET measured by HP 4155B indicate that hole mobility μ_p has an maximum enhancement of 25% compared to similarly processed bulk Si PMOSFET.     

High-mobility strained-Si PMOSFET's

Operation and fabrication of a new high channel mobility strained-Si PMOSFET are presented. The growth of high-quality strained Si layer on completely relaxed, step-graded, SiGe buffer layer is demonstrated by gas source MBE. The strained-Si layer is characterized by double crystal X-ray diffraction, photoluminescence, and transmission electron microscopy. The operation of a PMOSFET is shown by device simulation and experiment. The high-mobility strained-Si PMOSFET is fabricated on strained-Si, which is grown epitaxially on a completely relaxed step-graded Si_0.82Ge_0.18 buffer layer on Si(100) substrate. At high vertical fields (high |V_g|), the channel mobility of the strained-Si device is found to be 40% and 200% higher at 300 K and 77 K, respectively, compared to those of the bulk Si device. In the case of the strained-Si device, degradation of channel mobility due to Si/SiO₂ interface scattering is found to be more pronounced compared to that of the bulk Si device. Carrier confinement at the type-II strained-Si/SiGe-buffer interface is clearly demonstrated from device transconductance and C-V measurements at 300 K and 77 K     

Simulation and comparison of MOS inversion layer quantum mechanics effects in SiGe PMOSFET and Si PMOSFET

By employing the semiconductor device 2D simulator Medici, the inversion layer quantum mechanics effects (QME) in the strained SiGe-channel PMOSFET are studied. The influences of the inversion layer QME on the channel hole sheet density, the surface potential, the electric field and the threshold voltage in strained SiGe PMOS and Si PMOS are simulated and compared. It is theoretically predicted and validated by the numeric simulation results that QME lead to much difference in device performance between SiGe PMOS and Si PMOS. This study shows that SiGe PMOS suffers less disadvantageous influence when compared with Si PMOS, in ultra-deep submicron dimension, where QME are becoming increasingly more important.     

Si/SiGe PMOSFET USING P^＋ IMPLANTATION TECHNOLOGY

Si/SiGe P-channel Metal-Oxide-Semiconductor Field Effect Transistor （PMOSFET） using P^＋ （phosphor ion） implantation technology is successfully fabricated. P^＋ implantation into SiGe virtual substrate induces a narrow defect region slightly below the SiGe/Si interface, which gives rise to strongly enhanced strain relaxation of SiGe virtual substrate. X-Ray Diffraction （XRD） tests show that the degree of relaxation of SiGe layer is 96% while 85% before implantation. After annealed, the sample appeared free of Threading Dislocation densities （TDs） within the SiGe layer to the limit of Transmission Electron Microscopy （TEM） analysis. Atomic Force Microscope （AFM） test of strained Si channel surface shows that Root Mean Square （RMS） is 1.1nm. The Direct Current （DC） characters measured by HP 4155B indicate that the maximum saturated transconductance is twice bigger than that of bulk Si PMOSFET.     

基于SiGe虚拟衬底的低场迁移率提升140%的应变Si沟道NMOS器件 Cui Wei(崔伟)1,2,Tang Zhaohuan(唐昭焕)2, Tan Kaizhou(谭开洲)2, Zhang Jing(张静)2,

本文研究了一种应变SiGe沟道的NMOS器件,通过调整硅帽层、SiGe缓冲层,沟道掺杂和Ge组分变化,并采用变能量硼注入形成P阱的方式,成功完成了应变NMOS器件的制作。测试结果表明应变的NMOS器件在低场(Vgs=3.5V, Vds=0.5V)条件下,迁移率极值提升了140%,而PMOS器件性能保持不变。文中对硅基应变增强机理进行了分析。并利用此NMOS器件研制了一款CMOS倒向器,倒向器特性良好, 没有漏电,高低电平转换正常。     

调制掺杂层在SiGe PMOSFET中的应用

在普通Si器件性能模拟的基础上，详细研完了长沟应变SiGe器件的模拟，并进一步探讨了调制掺杂层的引入对器件性能(主要是跨导)的影响。在器件模拟过程中，采用隐含的SiGe材料和Si材料模型会得到与实际情况差别较大的结果。根据前人的材料研完工作，引入了插值所得的近似因子，以修正Silvaco中隐含的SiGe能带模型和迁移率参数。然后，依据修正后的模型对SiGe PMOS进行了更为精确的二维模拟，并验证了调制掺杂层的作用。     

Simple structured PMOSFET fabricated using molecular layer doping

The application of molecular layer doping (MLD) to the formation of shallow source and drain regions of a PMOSFET is discussed. The MLD process consists of three steps. First, the natural oxide on the Si surface is removed by thermal cleaning to expose an active Si surface. Second, a boron adsorbed layer is formed on the Si surface. Third, boron atoms undergo solid-phase diffusion from the adsorbed layer into the bulk. The electrical characteristics of the PMOSFET in the short-channel region are superior to those of devices fabricated by conventional techniques