复合栅控二极管新技术提取热载流子诱生的NMOS/SOI器件界面陷阱的横向分布

提出了用复合栅控二极管新技术提取MOS/SOI器件界面陷阱沿沟道横向分布的原理,给出了具体的测试步骤和方法.在此基础上,对具有体接触的NMOS/SOI器件进行了具体的测试和分析,给出了不同的累积应力时间下的界面陷阱沿沟道方向的横向分布.结果表明:随累积应力时间的增加,不仅漏端边界的界面陷阱峰值上升,而且沿沟道方向,界面陷阱从漏端不断向源端增生.     

DCIV技术表征MOS/SOI界面陷阱能级密度分布

基于直流电流电压(DCIV)理论和界面陷阱能级U型对称分布模型,可以获取硅界面陷阱在禁带中的分布,即利用沟道界面陷阱引起的界面复合电流与不同源/漏-体正偏电压(Vpn)的函数关系,求出对应每个Vpn的有效界面陷阱面密度(Neff),通过Neff函数与求出的每个Neff值作最小二乘拟合,将拟合参数代入界面陷阱能级密度(DIT)函数式,作出DIT的本征分布图.分别对部分耗尽的nMOS/SOI和pMOS/SOI器件进行测试,得到了预期的界面复合电流曲线,并给出了器件界面陷阱能级密度的U型分布图.结果表明,两种器件在禁带中央附近的陷阱能级密度量级均为109 cm-2·eV-1,而远离禁带中央的陷阱能级密度量级为1011 cm-2·eV-1.     

热载流子诱生MOSFET/SOI界面陷阱的正向栅控二极管技术表征

本文完成了热载流子诱生MOSFET/SOI界面陷阱正向栅控二极管技术表征的实验研究 .正向栅控二极管技术简单、准确 ,可以直接测得热载流子诱生的平均界面陷阱密度 ,从而表征器件的抗热载流子特性 .实验结果表明 :通过体接触方式测得的MOSFET/SOI栅控二极管R G电流峰可以直接给出诱生的界面陷阱密度 .抽取出来的热载流子诱生界面陷阱密度与累积应力时间呈幂指数关系 ,指数因子约为 0 787     

热载流子诱生MOSFET／SOI界面陷阱的正向机控二极管技术表征

本文完成了热载流子诱生MOSFET/SOI界面陷阱正向栅控二极管技术表征的实验研究。正向栅控二极管技术简单、准确，可以直接测得热载流子诱生的平均界面陷阱密度，从而表征器件的抗热载流子特性。实验结果表明：通过体接触方式测得的MOSFET/SOI栅控二级管R-G电流峰可以直接给出诱生的界面陷阱密度。抽取出来的热载流子诱生界面陷阱密度与累积应力时间呈幂指数关系，指数因子约为0.787。     

一种基于电荷泵技术的界面态横向分布测量方法

本文以电荷泵技术为测量手段，结合数值计算，提出了一种新的测量界面态横向分布的方法．与传统方法相比具有理论模型较完善、测量中不引入新的蜕变、易于实现的特点，适用于研究短沟道器件的热载流子蜕变效应．用该方法对１．２μｍＬＤＤ结构ｎ－ＭＯＳＦＥＴ进行了研究，得到了应力后漏端附近产生的界面态的横向分布以及应力后阈值电压、平带电压的变化，并能确定由于热电子注入产生的氧化层陷阱电荷的数量和位置     

一种用于提取LDD结构n-MOSFET热载流子应力下界面陷阱产生的改进方法

提出了一种新的基于电荷泵技术和直流电流法的改进方法,用于提取LDD n-MOSFET沟道区与漏区的界面陷阱产生.这种方法对于初始样品以及热载流子应力退化后的样品都适用.采用这种方法可以准确地确定界面陷阱在沟道区与漏区的产生,从而有利于更深入地研究LDD结构器件的退化机制.     

栅控二极管R-G电流法表征SOI-MOS器件埋氧层界面陷阱的敏感性分析

通过数值模拟手段,用归一化的方法研究了界面陷阱、硅膜厚度和沟道掺杂浓度对R-G电流大小的影响规律.结果表明:无论在FD还是在PD SOI MOS器件中,界面陷阱密度是决定R-G电流峰值的主要因素,硅膜厚度和沟道掺杂浓度的影响却因器件的类型而异.为了精确地用R-G电流峰值确定界面陷阱的大小,器件参数的影响也必须包括在模型之中.     

一种用于提取LDD结构n-MOSFET热载流子应力下界面陷阱产生的改进方法

提出了一种新的基于电荷泵技术和直流电流法的改进方法,用于提取LDDn MOSFET沟道区与漏区的界面陷阱产生.这种方法对于初始样品以及热载流子应力退化后的样品都适用.采用这种方法可以准确地确定界面陷阱在沟道区与漏区的产生,从而有利于更深入地研究LDD结构器件的退化机制.     

部分耗尽SOI器件背栅界面陷阱密度的提取

利用基于复合理论的直流电流电压法,提取SOI器件背栅界面陷阱密度。给出了具体的测试原理,以0.13 μm SOI工艺制造的部分耗尽NMOS和PMOS器件为测试对象,分别对两种器件的背界面复合电流进行测试。将实验得到的界面复合电流值与理论公式作最小二乘拟合,不仅可以获得背界面陷阱密度,还可以得到界面陷阱密度所在的等效能级。结果表明,采用智能剥离技术制备的SOI器件的背界面陷阱密度量级均为10¹⁰cm-2,但NMOS器件的背界面陷阱密度略大于PMOS器件,并给出了界面陷阱密度所在的等效能级。     

超薄栅MOS器件热载流子应力下SILC的产生机制

通过测量界面陷阱的产生,研究了超薄栅nMOS和pMOS器件在热载流子应力下的应力感应漏电流(SILC).在实验结果的基础上,发现对于不同器件类型(n沟和p沟)、不同沟道长度(1、0.5、0.275和0.135μm)、不同栅氧化层厚度(4和2.5nm),热载流子应力后的SILC产生和界面陷阱产生之间均存在线性关系.这些实验证据表明MOS器件减薄后,SILC的产生与界面陷阱关系非常密切.     

Extraction of the lateral distribution of interface traps in MOSFETs by a novel combined gated-diode technique

A novel combined gated-diode technique for qualitatively extracting the lateral distribution of interface traps in N-MOSFETs is presented in this paper. The key of this technique lies in the recombination–generation current peak originating from the interface trap recombination is being modulated by the drain voltage of the combined forward gated-diode architecture. The extraction principle is introduced in detail and the extraction procedure is also erected. The experimental results qualitatively show that the induced interface traps gradually decrease from the drain and source edges to the channel region while showing the highest value near both edges in N-MOSFETs.     

新的正向栅控二极管技术分离热载流子应力诱生SOI NMOSFET界面陷阱和界面电荷的研究

报道了用新的正向栅控二极管技术分离热载流子应力诱生的SOI-MOSFET界面陷阱和界面电荷的理论和实验研究.理论分析表明:由于正向栅控二极管界面态R-G电流峰的特征,该峰的幅度正比于热载流子应力诱生的界面陷阱的大小,而该峰的位置的移动正比于热载流子应力诱生的界面电荷密度. 实验结果表明:前沟道的热载流子应力在前栅界面不仅诱生相当数量的界面陷阱,同样产生出很大的界面电荷.对于逐渐上升的累积应力时间,抽取出来的诱生界面陷阱和界面电荷密度呈相近似的幂指数方式增加,指数分别为为0.7 和0.85.     

Hot-carrier effects on gate-induced-drain-leakage (GIDL) current inthin-film SOI/NMOSFET's

The gate-induced-drain-leakage (GIDL) currents in thin-film SOI/NMOSFET's have been studied before and after front-channel hot-carrier stress. Both the normal-mode stress (with the front gate biased beyond the threshold voltage and the drain biased at a high positive voltage, while the source is grounded with the back gate) and the reverse-mode stress (with the source and drain interchanged) have been investigated. The following significant changes have been observed: i) an increase of the off-state drain GIDL current after the normal-mode stress, especially in the low gate field region, and ii) a decrease of the off-state GIDL current after the reverse-mode stress, especially in the high gate field region. These changes can be attributed to the hot-carrier induced interface traps and their effects on the parasitic bipolar transistor gain in the thin-film SOI/NMOSFET     

栅控二极管R-G电流法表征SOI-MOS器件埋氧层界面陷阱的敏感性分析

通过数值模拟手段 ,用归一化的方法研究了界面陷阱、硅膜厚度和沟道掺杂浓度对 R- G电流大小的影响规律 .结果表明 :无论在 FD还是在 PD SOI MOS器件中 ,界面陷阱密度是决定 R- G电流峰值的主要因素 ,硅膜厚度和沟道掺杂浓度的影响却因器件的类型而异 .为了精确地用 R- G电流峰值确定界面陷阱的大小 ,器件参数的影响也必须包括在模型之中     

Numerical Analysis of Characterized Back Interface Traps of SOI Devices by R-G Current

Characterized back interface traps of SOI devices by the Recombination-Generation (R-G) curren: has been analyzed numerically with an advanced semiconductor simulation tool,namely DESSiS-ISE. The basis of the principle for the R-G current's characterizing the back interface traps of SOI lateral p+p-n+ diode has been demonstrated. The dependence of R-G cur rent on interface trap characteristics has been examined, such as the state density, surface recombination velocity and the trap energy level. The R-G current proves to be an effective tool for monitoring the back interface of SOI devices.     

Numerical Analysis of Characterized Back Interface Traps of SOI Devices by R-G Current

Characterized back interface traps of SOI devices by the Recombination\|Generation (R\|G) current has been analyzed numerically with an advanced semiconductor simulation tool,namely DESSIS\|ISE.The basis of the principle for the R\|G current's characterizing the back interface traps of SOI lateral p\++p\+-n\++ diode has been demonstrated.The dependence of R\|G current on interface trap characteristics has been examined,such as the state density,surface recombination velocity and the trap energy level.The R\|G current proves to be an effective tool for monitoring the back interface of SOI devices.     

Deep submicron PDSOI thermal resistance extraction

Deep submicron partially depleted silicon on insulator (PDSOI) MOSFETs with H-gate were fabricated based on the 0.35μm SOI process developed by the Institute of Microelectronics of the Chinese Academy of Sciences. Because the self-heating effect (SHE) has a great influence on SOI, extractions of thermal resistance were done for accurate circuit simulation by using the body-source diode as a thermometer. The results show that the thermal resistance in an SOI NMOSFET is lower than that in an SOI PMOSFET; and the thermal resistance in an SOI NMOSFET with a long channel is lower than that with a short channel. This offers a great help to SHE modeling and parameter extraction.     

“Gated-diode” in SOI MOSFETs: a sensitive tool forcharacterizing the buried Si/SiO2 interface

A “gated diode” technique is described for the measurement of the interface state density of the silicon film/buried oxide interface of SOI MOSFETs. This approach becomes possible by taking advantage of the front gate, which is biased to inversion (NMOSFET) or accumulation (BC-PMOSFET) during the measurement, while scanning the back interface through depletion. Using this technique the estimated value of the buried interface state density of typical low dose SIMOX MOSFETs was slightly over 10¹¹/cm²     

FORWARD GATED—DIODE METHOD FOR EXTRACTING HOT—CARRIER—STRESS0INDUCED BACK INTERFACE TRAPS IN SOI／NMOSFETs

The forward gated-diode R-G current method for extracting the hot-carrier-stress-induced back interface traps in SOI/NMOSFET devices has been demonstrated in this letter. This easy and accurate experimental method directly gives the induced interface trap density from the measured R-G current peak of the gated-diode architecture. An expected power law relationship between the induced back interface trap density and the accumulated stress time has been obtained.     

一种抗热载流子退化效应的新型CMOS电路结构

本文在分析MOSFET衬底电流原理的基础上,提出了一种新型抗热载流子退化效应的CMOS数字电路结构.即通过在受热载流子退化效应较严重的NMOSFET漏极串联一肖特基二级管,来减小其所受电应力.经SPICE及电路可靠性模拟软件BERT2.0对倒相器的模拟结果表明:该结构使衬底电流降低约50%,器件的热载流子退化效应明显改善而不会增加电路延迟;且该电路结构中肖特基二级管可在NMOSFET漏极直接制作肖特基金半接触来方便地实现,工艺简明可行又无须增加芯片面积.