量化Al沉积方法对Al2O3/Si界面质量的影响

I. Mack, Kawa Rosta, U. Quliyeva, J. Ott, T. Pasanen, V. Vähänissi, Zahra Sadat Jahanshah Rad, J. Lehtiö, P. Laukkanen, C. Soldano, H. Savin
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引用次数: 0

摘要

氧化物-半导体界面的质量通常直接影响器件的电学性能和性能。传统上,通过沉积金属层和测量电容电压(C-V)特性来表征金属氧化物半导体(MOS)结构的性能。然而,金属沉积过程本身可能会对氧化物和氧化物-半导体界面产生影响。通过半导体电晕表征(COCOS)和MOS C-V测量,研究了磁控溅射、电子束蒸发和热蒸发对原子层沉积(ALD) a2o3 / ssi界面的影响。后者允许表征界面也在其原始状态在金属化之前。结果表明,随着界面缺陷密度D从10 11 cm−2 eV增加到10 13 cm−2 eV,溅射对基体a2o3 / ssi界面造成了明显的损伤。有趣的是,当电荷从−2 × 10 12 cm−2变为+ 7 × 10 12 cm−2时,溅射也在界面处产生高密度的正电荷Q tot。热蒸发是一种较为温和的方法,对dit和qtot的影响不大。最后,退火修复了损伤,但也对薄膜的电荷产生了重大影响,恢复了a2o3的特征负电荷(~−4 × 1012 cm−2)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantifying the Impact of Al Deposition Method on Underlying Al2O3/Si Interface Quality
Oxide–semiconductor interface quality has often a direct impact on the electrical properties of devices and on their performance. Traditionally, the properties are characterized through metal–oxide–semiconductor (MOS) structures by depositing a metal layer and measuring the capacitance–voltage (C–V) characteristics. However, metal deposition process itself may have an impact on the oxide and the oxide–semiconductor interface. The impact of magnetron sputtering, e‐beam evaporation, and thermal evaporation on an A l 2 O 3 / S i interface is studied, where atomic layer deposited (ALD) A l 2 O 3 is used, by MOS C–V and corona oxide characterization of semiconductors (COCOS) measurements. The latter allows characterization of the interface also in its original state before metallization. The results show that sputtering induces significant damage at the underlying A l 2 O 3 / S i interface as the measured interface defect density D it increases from 10 11 to 10 13  cm−2 eV. Interestingly, sputtering also generates a high density of positive charges Q tot at the interface as the charge changes from − 2 × 10 12 to + 7 × 10 12  cm − 2 . Thermal evaporation is found to be a softer method, with modest impact on D it and Q tot . Finally, Alnealing heals the damage but has also a significant impact on the charge of the film recovering the characteristic negative charge of A l 2 O 3 (∼−4 × 1012 cm − 2 ).
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