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首页> 外文期刊>Journal of Computational Electronics >Improvement in electrostatic characteristics of doped TFETs by hole layer formation
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Improvement in electrostatic characteristics of doped TFETs by hole layer formation

机译:通过孔层形成改善掺杂TFET的静电特性

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We present a distinct approach to enhance the performance of physically doped tunnel field-effect transistors (TFETs) based on creation of a layer of positive charge at the semiconductor-insulator interface in the source region. Formation of such a hole layer resolves the issue related to material solubility and improves direct-current (DC) as well as high-frequency figures of merit. To implement this approach, a typical P+-I-N+-type physically doped TFET structure is considered. Furthermore, a metal electrode with workfunction of 4.53 eV is placed over the heavily doped P+ source region with a negative supply voltage. The negative voltage at the source electrode attracts holes from the source region and creates a hole layer just below the semiconductor-insulator interface. This phenomenon makes the source-channel junction abrupt and reduces the tunneling barrier width, resulting in higher tunneling generation rate of charge carriers at the source-channel junction. Thus, the proposed device shows 100-fold increased ON-state current and a threshold voltage reduction of 300 mV. Analog/radiofrequency (RF) parameters are also greatly improved compared with the conventional device. Furthermore, optimization of the spacer length (L-SG), i.e., the gap between the source and gate electrode, and application of a negative voltage (-V-SE) at the source electrode (SE), were applied to achieve the optimum performance. Moreover, device linearity was also analyzed in a comparative manner.
机译:我们基于在源极区域中的半导体-绝缘体界面处创建一层正电荷,提出了一种独特的方法来增强物理掺杂隧道场效应晶体管(TFET)的性能。这样的孔层的形成解决了与材料溶解性有关的问题,并改善了直流(DC)以及高频品质因数。为了实现这种方法,需要考虑典型的P + -I-N +型物理掺杂TFET结构。此外,将功函数为4.53 eV的金属电极置于负电源电压下的重掺杂P +源极区域上方。源电极上的负电压吸引了来自源区域的空穴,并在半导体-绝缘体界面的正下方形成了一个空穴层。这种现象使源极-沟道结突然发生并减小了隧穿势垒宽度,从而导致源极-沟道结处的载流子的隧穿产生速率更高。因此,提出的器件显示出100倍的增加的导通状态电流和300 mV的阈值电压降低。与传统设备相比,模拟/射频(RF)参数也得到了极大改善。此外,对间隔物长度(L-SG)(即源极和栅极之间的间隙)进行了优化,并在源极(SE)上施加了负电压(-V-SE),以实现最佳效果。性能。此外,还以比较的方式分析了器件的线性度。

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