首页> 外文期刊>Electron Devices, IEEE Transactions on >High-Mobility Ge p- and n-MOSFETs With 0.7-nm EOT Using src='/images/tex/20780.gif' alt='hbox {HfO}_{2}/hbox {Al}_{2}hbox {O}_{3}/hbox {GeO}_{x}/hbox {Ge}'> Gate Stacks Fabricated by Plasma Postoxidation
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High-Mobility Ge p- and n-MOSFETs With 0.7-nm EOT Using src='/images/tex/20780.gif' alt='hbox {HfO}_{2}/hbox {Al}_{2}hbox {O}_{3}/hbox {GeO}_{x}/hbox {Ge}'> Gate Stacks Fabricated by Plasma Postoxidation

机译:使用 src =“ / images / tex / 20780.gif” alt =“ hbox {HfO} _ {2} /的具有0.7nm EOT的高迁移率Ge p和n-MOSFET hbox {Al} _ {2} hbox {O} _ {3} / hbox {GeO} _ {x} / hbox {Ge}“> 通过等离子体后氧化法制造的栅叠层

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An ultrathin equivalent oxide thickness (EOT) $hbox{HfO}_{2}/hbox{Al}_{2} hbox{O}_{3}/hbox{Ge}$ gate stack has been fabricated by combining the plasma postoxidation method with a 0.2-nm-thick $hbox{Al}_{2}hbox{O}_{3}$ layer between $hbox{HfO}_{2}$ and Ge for suppressing $hbox{HfO}_{2}{-}hbox{GeO}_{x}$ intermixing, resulting in a low-interface-state-density $(D_{rm it})$  $hbox{GeO}_{x}/hbox{Ge}$ metal–oxide–semiconductor (MOS) interface. The EOT of these gate stacks has been scaled down to 0.7–0.8 nm with maintaining the $D_{rm it}$ in $ hbox{10}^{11} hbox{cm}^{-2}cdot hbox{eV}^{-1}$ level. The p- and n-channel MOS field-effect transistors (MOSFETs) (p- and n-MOSFETs) using this gate stack have been fabricated on (100) Ge substrates and exhibit high hole and electron mobilities. It is found that the Ge p- and n-MOSFETs exhibit peak hole mobilities of 596 and 546 $hbox{cm}^{2}/hbox{V}cdot hbox{s}$ and peak electron mobilities of 754 and 689 $hbox{cm}^{2}/hbox{V}cdot hbox{s}$ at EOTs of 0.82 and 0.76 nm, respectively, which are the record-high reports so far for Ge MOSFETs in subnanometer EOT range because of the sufficiently passivated Ge MOS interfaces in present $hbox{HfO}_{2}/hbox{Al}_{2}hbox{O}_{3}/hbox{- eO}_{x}/hbox{Ge}$ gate stacks.
机译:通过结合等离子体后氧化工艺制造了超薄等效氧化物厚度(EOT)$ hbox {HfO} _ {2} / hbox {Al} _ {2} hbox {O} _ {3} / hbox {Ge} $栅叠层$ hbox {HfO} _ {2} $和Ge之间具有0.2纳米厚的$ hbox {Al} _ {2} hbox {O} _ {3} $层的方法来抑制$ hbox {HfO} _ {2 } {-} hbox {GeO} _ {x} $混合在一起,导致接口状态密度低的$(D_ {rm it})$ $ hbox {GeO} _ {x} / hbox {Ge} $金属–氧化物–半导体(MOS)接口。这些栅极堆叠的EOT已缩小至0.7–0.8 nm,同时保持$ hbox {10} ^ {11} hbox {cm} ^ {-2} cdot hbox {eV} ^中的$ D_ {rm it} $ {-1} $级。使用该栅叠层的p和n沟道MOS场效应晶体管(MOSFET)(p和n-MOSFET)已经在(100)Ge衬底上制造,并且具有很高的空穴和电子迁移率。发现Ge p-和n-MOSFET的峰值空穴迁移率分别为596和546 $ hbox {cm} ^ {2} / hbox {V} cdot hbox {s} $和峰值电子迁移率分别为754和689 $ hbox {cm} ^ {2} / hbox {V} cdot hbox {s} $的EOT分别为0.82和0.76 nm,这是迄今为止在亚纳米EOT范围内的Ge MOSFET的最高记录,因为Ge被充分钝化当前$ hbox {HfO} _ {2} / hbox {Al} _ {2} hbox {O} _ {3} / hbox {-eO} _ {x} / hbox {Ge} $门堆栈中的MOS接口。

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