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Impact of Source-to-Gate and Drain-to-Gate Overlap Lengths on Performance of Inverted Staggered a-IGZO TFTs With an Etch Stopper

机译:源代到栅极和漏极 - 栅极重叠长度对蚀刻停止器的倒置交错A-IGZO TFT性能的影响

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We report a comprehensive study on the impact of source-to-gate ( ${L}_{S}$ ) and drain-to-gate ( ${L}_{D}$ ) overlap lengths on the performance of amorphous indium–gallium–zinc–oxide (a-IGZO) thin-film transistors (TFTs) employing the inverted staggered structure with an etch stopper (ES). Although drain current ( ${I}_{D}$ ) is found to marginally decrease with increasing ${L}_{S}$ , it is found to considerably increase with ${L}_{D}$ . With the help of technology computer-aided design (TCAD) simulations, the increase in ${I}_{D}$ with ${L}_{D}$ is attributed to backchannel formation in the region beneath the drain, while the decrease in ${I}_{D}$ with increasing ${L}_{S}$ is attributed to the depletion of carriers from the backchannel in the region beneath the source. In addition, the threshold voltage ( ${V}_{TH}$ ) shifts negatively with increasing ${L}_{D}$ and drain voltage ( ${V}_{D}$ ). All these effects are more pronounced in short channel TFTs than long channel TFTs, which could be the origin of the anomalous dependence of ${V}_{TH}$ of the ES-type a-IGZO TFTs on channel length.
机译:我们举报了关于源头门的影响的全面研究(<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {l} _ {s} $ )和排水沟(<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {l} _ {d} $ )与采用蚀刻塞子(ES)的非晶铟 - 镓 - 氧化锌(A-IGZO)薄膜晶体管(TFT)的性能的重叠长度。虽然排水电流(<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {i} _ {d} $ )被发现与越来越多地减少<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {l} _ {s} $ ,发现它有很大增加<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {l} _ {d} $ 。借助技术计算机辅助设计(TCAD)模拟,增加了<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {i} _ {d} $ 和<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {l} _ {d} $ 归因于漏极下方区域的后轴承形成,同时减少<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {i} _ {d} $ 随着时间的增加<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {l} _ {s} $ 归因于来自源下方的区域中的载体的耗尽。此外,阈值电压(<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {v} _ {Th} $ )随着越来越多地转变<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {l} _ {d} $ 和漏极电压(<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {v} _ {d} $ )。所有这些效果在短频道TFT中更明显,而不是长通道TFT,这可能是异常依赖的起源<内联公式XMLNS:MML =“http://www.w3.org/1998/math/mathml”xmlns:xlink =“http://www.w3.org/1999/xlink”> $ {v} _ {Th} $ 在通道长度上的ES型A-IGZO TFT。

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