限制双掺杂PHEMTs在亚100纳米尺度下运行的击穿机制

K. Kalna, A. Asenov
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引用次数: 0

摘要

采用蒙特卡罗模拟方法,对双δ掺杂伪晶高电子迁移率晶体管(PHEMTs)的击穿极限进行了研究。导致击穿的两种机制是通道冲击电离和从栅极穿隧。双掺杂phemt可以具有第二δ掺杂层的两种可能位置:在沟道下方或在栅和第一δ掺杂层之间。量子力学隧穿从极低的漏极电压开始,但很快饱和,对那些在原始掺杂之上放置第二掺杂层的phemt有更大的影响。冲击电离的阈值出现在较大的漏极电压下,这将保证双掺杂phemt可靠的工作电压范围。在通道下方放置第二δ掺杂层的双掺杂phemt,由于冲击电离导致通道长度的减小,其劣化速度比在原掺杂之上放置第二δ掺杂层的phemt更快。
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Breakdown mechanisms limiting the operation of double doped PHEMTs scaled into sub-100 nm dimensions
The breakdown limit of pseudomorphic high electron mobility transistors (PHEMTs) with double delta-doping structure scaled down into sub-100 nm dimensions is extensively investigated by Monte Carlo device simulations. The two mechanisms responsible for breakdown are channel impact ionization and tunnelling from the gate. The double doped PHEMTs may have two possible placements of the second delta doping layer: either below the channel or between the gate and the first delta doping layer. Quantum mechanical tunnelling starts at very low drain voltages but quickly saturates, having a greater effect on those PHEMTs with the second doping layer placed above the original doping. The threshold for impact ionization occurs at larger drain voltages which should assure the reliable operation voltage scale of double doped PHEMTs. Those double doped PHEMTs with the second delta doping layer placed below the channel deteriorate faster with the reduction of the channel length due to impact ionization than those devices with the second doping layer above the original doping.
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