氧化物缺陷处重组的证据和新的SILC模型

D. Ielmini, A.S. Spinellii, A. Lacaita, G. Ghidini
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引用次数: 10

摘要

这项工作提出了对SILC的物理机制的实验和计算研究。在氧化厚度为6-8 nm的MOS样品上进行了载流子分离测量,突出了电子和空穴对SILC的贡献。我们用时间松弛的方法研究了这些分量之间的关系。发现在初始高场应力后不同时间测量的电子硅固相密度与空穴硅固相密度之间存在线性关系。在固定应力场下,注入电子的影响增加,也观察到同样的线性关系。通过比较n/sup +/-和p/sup +/-多晶硅器件的载流子分离数据,发现了电子和空穴ILC之间的相关性。这些实验数据表明,空穴SILC是由复合电流引起的。基于这些实验结果,我们建立了一个新的SILC模型。该模型基于陷阱辅助隧道作用,但也考虑了空穴隧道作用,并将块体氧化物中的Shockley-Hall-Read复合过程作为一种新的泄漏机制。在5.9 ~ 8.2 nm的氧化厚度范围内的模拟结果与I-V测量值和载流子分离数据非常吻合。所得到的缺陷浓度与氧化物厚度成正比,与已发表的结果一致。导致稳态泄漏的缺陷能量分布在硅导带最小值以下0.7 ~ 1.3 eV。假设电子和空穴的俘获截面分别为10/sup -13/和10/sup -16/ cm/sup 2/,与silc相关缺陷中心的供体电荷态相容。最后给出了氧化层厚度t/sub =2.8 nm时的模拟结果。体氧化物中的复合机制很好地解释了超薄氧化物中低压硅碳交换的观察结果,表明了所提出的硅碳交换模型的有效性。
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Evidence for recombination at oxide defects and new SILC model
This work presents experimental and computational investigations on the physical mechanisms of SILC. Carrier separation measurements are carried out on MOS samples with oxide thickness 6-8 nm, highlighting the electron and hole contributions to the SILC. We have investigated the relation between these components by means of time-relaxation. It is found that a linear relationship holds between electron SILC and hole SILC, measured at different times after the initial high-field stress. The same linearity has been observed for increasing fluences of injected electrons, at fixed stressing field. A correlation between electron and hole ILC is found also from a comparison between carrier separation data obtained in n/sup +/- and p/sup +/- polysilicon devices. These experimental data entails that hole SILC is due to a recombination current. As a result of these experimental findings, a new model for the SILC is developed. This model is based on trap-assisted tunneling, but also accounts for hole tunneling and includes Shockley-Hall-Read recombination process in the bulk oxide as a new leakage mechanism. Simulations in the oxide thickness range 5.9-8.2 nm show excellent agreement with I-V measurements and carrier-separation data. The resulting defect concentration scales with the oxide thickness, in agreement with published results. The energy distribution of defects responsible for the steady-state leakage is located 0.7-1.3 eV below the Si conduction-band minimum. Capture cross sections of 10/sup -13/ and 10/sup -16/ cm/sup 2/ have been assumed for electrons and holes respectively, compatible with a donor charge state of the SILC-related defect centers. Simulations are finally shown for oxide thickness t/sub 0x/=2.8 nm. The mechanism of recombination in the bulk oxide accounts very well for the observation of low-voltage SILC in ultrathin oxide, showing the effectiveness of the proposed SILC model.
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