Characteristics of In0.17Al0.83N/AlN/GaN MOSHEMTs with steeper than 60 mV/decade sub-threshold slopes in the deep sub-threshold region

Zongyang Hu, R. Jana, M. Qi, S. Ganguly, B. Song, E. Kohn, D. Jena, H. Xing
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引用次数: 8

Abstract

Realization of steep sub-threshold slope (SS) transistors requires exploiting carrier transport mechanisms such as tunneling [1], and also alternative gate barrier materials (i.e. ferroelectric materials) with internal voltage gain [2]. Theoretical studies on piezoelectric barriers indicate that it is possible to achieve internal voltage amplification and steep SS in GaN MOSHEMTs by utilizing electrostriction in conjunction with piezoelectricity in AlN and InAlN [3] [4]. Less than 60 mV/decade SS was experimentally observed in GaN MOSHEMTs with InAlN barriers, in which the steep transition was tentatively correlated with the inhomogeneous distribution of polarization in the barrier [5]. However, steep SS were only observed at drain current (Id) near nA/mm regimes, which leads to difficulties in interpretation of experiment data. Understanding of the mechanism of the steep SS in these devices is still unclear and needs more characterization and modeling. In this work we demonstrate InAlN/AlN/GaN MOSHEMTs with less than 60 mV/decade SS in deep sub-threshold regions (1E-8 A/mm and below) at room temperature (RT). Drain voltage and temperature dependent characteristics are provided with analysis for advancing our understanding of this phenomenon.
深度亚阈值区斜率大于60 mV/ 10年的In0.17Al0.83N/AlN/GaN MOSHEMTs的特性
实现陡峭亚阈值斜率(SS)晶体管需要利用载流子传输机制,如隧道[1],以及具有内部电压增益的替代栅极阻挡材料(即铁电材料)[2]。对压电势垒的理论研究表明,利用电伸缩与AlN和InAlN中的压电性相结合,可以在GaN moshemt中实现内部电压放大和陡SS[3][4]。在具有InAlN势垒的GaN MOSHEMTs中,实验观察到小于60 mV/decade的SS,其中陡峭的跃迁暂时与势垒中极化的不均匀分布有关[5]。然而,只有在nA/mm附近的漏极电流(Id)下才观察到陡峭的SS,这导致实验数据的解释困难。对这些器件中陡坡SS的机制的理解仍然不清楚,需要更多的表征和建模。在这项工作中,我们在室温(RT)下展示了深亚阈值区域(1e - 8a /mm及以下)具有小于60 mV/ 10年SS的InAlN/AlN/GaN MOSHEMTs。漏极电压和温度依赖特性提供了分析,以提高我们对这一现象的理解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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