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1.
SOI反偏肖特基势垒动态阈值MOS特性   总被引:1,自引:0,他引:1  
将Ti硅化物-p型体区形成的反偏肖特基势垒结构引入绝缘体上硅动态阈值晶体管.传统栅体直接连接DTMOS,为了避免体源二极管的正向开启,工作电压应当低于0.7V.而采用反偏肖特基势垒结构,DTMOS的工作电压可以拓展到0.7V以上.实验结果显示,室温下采用反偏肖特基势垒SOI DTMOS结构,阈值电压可以动态减小200mV.反偏肖特基势垒SOI DTMOS结构相比于传统模式,显示出优秀的亚阈值特性和电流驱动能力.另外,对浮体SOI器件、传统模式SOI器件和反偏肖特基势垒SOI DTMOS的关态击穿特性进行了比较.  相似文献   

2.
毕津顺  海潮和 《半导体学报》2006,27(9):1526-1530
将Ti硅化物-p型体区形成的反偏肖特基势垒结构引入绝缘体上硅动态阈值晶体管.传统栅体直接连接DTMOS,为了避免体源二极管的正向开启,工作电压应当低于0.7V.而采用反偏肖特基势垒结构,DTMOS的工作电压可以拓展到0.7V以上.实验结果显示,室温下采用反偏肖特基势垒SOI DTMOS结构,阈值电压可以动态减小200mV.反偏肖特基势垒SOI DTMOS结构相比于传统模式,显示出优秀的亚阈值特性和电流驱动能力.另外,对浮体SOI器件、传统模式SOI器件和反偏肖特基势垒SOI DTMOS的关态击穿特性进行了比较.  相似文献   

3.
提出了一种基于部分耗尽绝缘体上硅的体源连接环形栅nMOS器件,并讨论了相应的工艺技术和工作机理。采用体源连接环形栅器件结构,有效地抑制了浮体环形栅器件中存在的浮体效应和寄生双极晶体管效应,使器件性能得到很大的提高。消除了浮体环形栅器件的反常亚阈值斜率和Kink效应,DIBL从120.7mV/V降低到3.45mV/V,关态击穿电压从4.8V提高到12.1V。最后指出,体源连接环形栅器件非常适合于抗辐照加固等应用领域。  相似文献   

4.
连军  海潮和 《半导体学报》2005,26(4):672-676
采用新的工艺技术,成功研制了具有抬高源漏结构的薄膜全耗尽SOI CMOS器件.详细阐述了其中的关键工艺技术.器件具有接近理想的亚阈值特性,nMOSFETs和pMOSFETs的亚阈值斜率分别为65和69mV/dec.采用抬高源漏结构的1.2μm nMOSFETs的饱和电流提高了32%,pMOSFETs的饱和电流提高了24%.在3V工作电压下101级环形振荡器电路的单级门延迟为75ps.  相似文献   

5.
在国内首次将等效氧化层厚度为1.7nm的N/O叠层栅介质技术与W/TiN金属栅电极技术结合起来,用于栅长为亚100nm的金属栅CMOS器件的制备.为抑制短沟道效应并提高器件驱动能力,采用的关键技术主要包括:1.7nm N/O叠层栅介质,非CMP平坦化技术,T型难熔W/TiN金属叠层栅电极,新型重离子超陡倒掺杂沟道剖面技术以及双侧墙技术.成功地制备了具有良好的短沟道效应抑制能力和驱动能力的栅长为95nm的金属栅CMOS器件.在VDS=±1.5V,VGS=±1.8V下,nMOS和pMOS的饱和驱动电流分别为679和-327μA/μm.nMOS的亚阈值斜率,DIBL因子以及阈值电压分别为84.46mV/dec,34.76mV/V和0.26V.pMOS的亚阈值斜率,DIBL因子以及阈值电压分别为107.4mV/dec,54.46mV/V和0.27V.结果表明,这种结合技术可以完全消除B穿透现象和多晶硅耗尽效应,有效地降低栅隧穿漏电并提高器件可靠性.  相似文献   

6.
在国内首次将等效氧化层厚度为1.7nm的N/O叠层栅介质技术与W/TiN金属栅电极技术结合起来,用于栅长为亚100nm的金属栅CMOS器件的制备.为抑制短沟道效应并提高器件驱动能力,采用的关键技术主要包括:1.7nm N/O叠层栅介质,非CMP平坦化技术,T型难熔W/TiN金属叠层栅电极,新型重离子超陡倒掺杂沟道剖面技术以及双侧墙技术.成功地制备了具有良好的短沟道效应抑制能力和驱动能力的栅长为95nm的金属栅CMOS器件.在VDS=±1.5V,VGS=±1.8V下,nMOS和pMOS的饱和驱动电流分别为679和-327μA/μm.nMOS的亚阈值斜率,DIBL因子以及阈值电压分别为84.46mV/dec,34.76mV/V和0.26V.pMOS的亚阈值斜率,DIBL因子以及阈值电压分别为107.4mV/dec,54.46mV/V和0.27V.结果表明,这种结合技术可以完全消除B穿透现象和多晶硅耗尽效应,有效地降低栅隧穿漏电并提高器件可靠性.  相似文献   

7.
制造了栅长0.1μm,栅氧厚度5.6nm,栅槽180nm的SOI槽栅pMOSFET.给出了器件的转移特性和输出特性.在Vds=-1.5V时,其饱和漏电流为380μA,关态泄漏电流为1.9nA;在Vds=-0.1V下的亚阈值斜率为115mV/dec,DIBL因子为70.7mV/V.实验结果表明,0.1μm SOI槽栅pMOSFET比同尺寸体硅槽栅pMOSFET拥有更好的电流驱动能力和亚阈值特性.  相似文献   

8.
制造了栅长0.1μm,栅氧厚度5.6nm,栅槽180nm的SOI槽栅pMOSFET.给出了器件的转移特性和输出特性.在Vds=-1.5V时,其饱和漏电流为380μA,关态泄漏电流为1.9nA;在Vds=-0.1V下的亚阈值斜率为115mV/dec,DIBL因子为70.7mV/V.实验结果表明,0.1μm SOI槽栅pMOSFET比同尺寸体硅槽栅pMOSFET拥有更好的电流驱动能力和亚阈值特性.  相似文献   

9.
研究了一种采用非对称结构和注Ge的部分耗尽0.8μm SOI nMOSFET的浮体效应,实验结果表明这种结构能够提高漏端击穿电压约1V,减轻反常亚阈值斜率和kink现象.浮体效应的减少是由于源区的浅结和注Ge 引入的晶体缺陷减少了寄生的横向npn晶体管的电流增益.  相似文献   

10.
采用非对称结构和注Ge的部分耗尽SOI nMOSFET的浮体效应   总被引:3,自引:3,他引:0  
研究了一种采用非对称结构和注Ge的部分耗尽0.8μm SOI nMOSFET的浮体效应,实验结果表明这种结构能够提高漏端击穿电压约1V,减轻反常亚阈值斜率和kink现象.浮体效应的减少是由于源区的浅结和注Ge 引入的晶体缺陷减少了寄生的横向npn晶体管的电流增益.  相似文献   

11.
AC floating body effects in PD SOI nMOSFETs operated at high temperature are investigated. Both source/body and drain/body junction diode characteristics are greatly influenced by temperature, significantly impacting the ac kink effect as well its low-frequency (LF) noise characteristics. This is especially true for the pre-dc kink operation at high temperature. The increase of junction thermal generation current becomes an important body charging source and induces the LF Lorentzian-like excess noise  相似文献   

12.
分别采用不同的背栅沟道注入剂量制成了部分耗尽绝缘体上硅浮体和H型栅体接触n型沟道器件.对这些器件的关态击穿特性进行了研究.当背栅沟道注入剂量从1.0×1013增加到1.3×1013cm-2,浮体n型沟道器件关态击穿电压由5.2升高到6.7V,而H型栅体接触n型沟道器件关态击穿电压从11.9降低到9V.通过测量寄生双极晶体管静态增益和漏体pn结击穿电压,对部分耗尽绝缘体上硅浮体和H型栅体接触n型沟道器件的击穿特性进行了定性解释和分析.  相似文献   

13.
分别采用不同的背栅沟道注入剂量制成了部分耗尽绝缘体上硅浮体和H型栅体接触n型沟道器件.对这些器件的关态击穿特性进行了研究.当背栅沟道注入剂量从1.0×1013增加到1.3×1013cm-2,浮体n型沟道器件关态击穿电压由5.2升高到6.7V,而H型栅体接触n型沟道器件关态击穿电压从11.9降低到9V.通过测量寄生双极晶体管静态增益和漏体pn结击穿电压,对部分耗尽绝缘体上硅浮体和H型栅体接触n型沟道器件的击穿特性进行了定性解释和分析.  相似文献   

14.
Haond  M. Colinge  J.P. 《Electronics letters》1989,25(24):1640-1641
The reduction of drain breakdown voltage in SOI nMOSFETs with floating substrate is related to the presence of a parasitic n-p-n bipolar structure, the base of which is the floating body of the device. reduction of breakdown voltage (compared to the case where a body contact is used) is shown to be dependent on both channel length and minority carrier lifetime in the SOI material. Conversely, it is shown that mere measurement of MOSFET breakdown voltages can be used to extract the minority carrier lifetime in the SOI material.<>  相似文献   

15.
The thickness effects of a high-tensile-stress contact etch stop layer (HS CESL) and the impact of layout geometry (length of diffusion (LOD) and gate width) on the mobility enhancement of lang100rang/(100) 90-nm silicon-on-insulator (SOI) n-channel MOSFETs (nMOSFETs) were studied in detail. Additionally, the low-frequency characteristics were inspected using low-frequency noise investigation for floating body (FB)-SOI nMOSFETs. Experimental results show that a device with a 1100-Aring HS CESL has worse characteristics and hot-carrier-induced degradations than a device with a 700-Aring; HS CESL due to larger stress-induced defects. The lower plateau of the Lorentzian noise spectrum that was observed from the input-referred voltage noise Svg implies a higher leakage current for devices with a 1100-Aring HS CESL. On the other hand, it was found that devices with narrow gate widths have higher driving capacity for a larger fringing electric field and higher compressive stress in the direction perpendicular to the channel. Because of the more serious impact of compressive stress in a direction parallel to the channel, a device with shorter LOD experiences more serious performance degradation  相似文献   

16.
A thorough investigation of hot carrier effects is made in mesa-isolated SOI nMOSFETs operating in the Bi-MOS mode (abbreviated as Bi-nMOSFETs). As a result of its unique hybrid operation mechanism, significant reduction of hot carrier induced maximum transconductance degradation and threshold voltage shift in the Bi-nMOSFET is observed in comparison with that in the conventional SOI nMOSFETs. Device lifetime of SOI Bi-nMOSFETs and conventional SOI nMOSFETs was roughly estimated for comparison. In view of the analysis of the degradation mechanism, the devices were stressed under different conditions. The post-stress body current and stress body current in Bi-nMOSFETs as a function of the stress time and stress drain voltage were evaluated as further proofs of the aging reasons. The hot electron injection is found to be the dominant degradation process in the SOI Bi-nMOSFETs. Compared with SOI nMOSFETs, SOI Bi-nMOSFETs show better immunity to the parasitic bipolar transistor action due to the body contact. In addition, the positive body bias can result in lowered hot hole injection into the gate oxide due to the provision of the generated hole leakage path, and thus decreased interface traps  相似文献   

17.
A novel CMOS-compatible thin film SOI LDMOS with a novel body contact structure is proposed. It has a Si window and a P-body extended to the substrate through the Si window, thus, the P-body touches the PC region to form the body contact. Compared with the conventional floating body SOI LDMOS(FB SOI LDMOS) structure, the new structure increases the off-state BV by 54%, decreases the specific on resistance by 20%, improves the output characteristics significantly, and suppresses the self-heating effect. Furthermore, the advantages of the low leakage current and low output capacitance of SOI devices do not degrade.  相似文献   

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