首页> 外文期刊>Electron Devices, IEEE Transactions on >Germanium N and P Multifin Field-Effect Transistors With High-Performance Germanium (Ge) ${rm p}^{+}/{rm n}$ and ${rm n}^{+}/{rm p}$ Heterojunctions Formed on Si Substrate
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Germanium N and P Multifin Field-Effect Transistors With High-Performance Germanium (Ge) ${rm p}^{+}/{rm n}$ and ${rm n}^{+}/{rm p}$ Heterojunctions Formed on Si Substrate

机译:具有高性能锗(Ge)的锗N和P多鳍场效应晶体管$ {rm p} ^ {+} / {rm n} $和$ {rm n} ^ {+} / {rm p} $形成异质结在硅衬底上

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We demonstrate the characteristics of ${{rm p}}^{+}$-Ge-Si and ${{rm n}}^{+}$-Ge/p-Si heterojunction diodes formed by heteroepitaxial Ge grown on Si leading to high performance and very low leakage current. The ON/OFF current ratio of the ${rm p}^{+}$-Ge-Si and ${rm n}^{+}$-Ge/p-Si heterojunction was ${>}{10^{7}}$ and ${>}{10^{6}}$, respectively. The OFF current density was extremely low at ${<}{rm 10}~mu{rm A}/{rm cm}^{2}$ for the ${rm p}^{+}$-Ge-Si formed with different implantation energies of 10–40 KeV and ${sim}{rm 20}~mu{rm A}/{rm cm}^{2}$ for the ${rm n}^{+}$-Ge/p-Si with different implantation energies of 20–50 KeV at a reverse bias of $vert V_{rm R}vert=pm1~{rm V}$ , respectively. Both p and n-Ge channel multifin field-effect transistors (FinFETs) were formed by a mesa structure using these ${rm p}^{+}$-Ge-Si and ${rm n}^{+}$-Ge/p-Si heterojunctions. A high-$kappa$/metal gate stack was employed. The body-tied Ge multifin FinFET with a fin width $({W}_{rm Fin})$ of ${sim}{rm 40}~{rm nm}$, and the channel length $({rm L}_{rm Channel})$ was 150 nm for p-FinFET and of 110 nm for n-FinFET, exhibiting a driving current of 174 $mu{rm A}/mu{rm m}$ at $V_{rm G}=-2~{rm V}$ and 102 $mu{rm A}/mu{rm m}$ at $V_{rm G}=2~{rm V}$ , respectively. This is the first experimental demonstration of a body-tied high mobility Ge channel multifin FinFET using a top-down approach.
机译:我们展示了由生长在其上的异质外延Ge形成的$ {{rm p}} ^ {+} $-Ge / n-Si和$ {{rm n}} ^ {+} $-Ge / p-Si异质结二极管的特性Si导致高性能和极低的泄漏电流。 $ {rm p} ^ {+} $-Ge / n-Si和$ {rm n} ^ {+} $-Ge / p-Si异质结的ON / OFF电流比为$ {>} {10 ^ {7}} $和$ {>} {10 ^ {6}} $。对于$ {rm p} ^ {+} $-Ge / n-Si,关态电流密度非常低,为$ {<} {rm 10}〜mu {rm A} / {rm cm} ^ {2} $对于$ {rm n} ^ {+} $-Ge /,用10–40 KeV和$ {sim} {rm 20}〜mu {rm A} / {rm cm} ^ {2} $的不同注入能量形成p-Si分别具有20–50 KeV的不同注入能量,且反向偏压分别为$ vert V_ {rm R} vert = pm1〜{rm V} $。 p和n-Ge沟道多鳍场效应晶体管(FinFET)都是由台面结构使用$ {rm p} ^ {+} $-Ge / n-Si和$ {rm n} ^ {+} $ -Ge / p-Si异质结。采用高kappa /金属门叠层。鳍状宽度为 $({W} _ {rm Fin})$ of {{sim} {rm 40}〜{rm nm} $}的束缚式Ge多鳍FinFET,以及沟道长度$({rm L} _ {rm Channel})$对于p-FinFET为150 nm,对于n-FinFET为110 nm,驱动电流为174 $ mu {rm A} / mu {rm m}在$ V_ {rm G} =-2〜{rm V} $时的$和在$ V_ {rm G} = 2〜{rm V} $时分别为102 $ mu {rm A} / mu {rm m} $。这是使用自上而下的方法进行的束缚式高迁移率Ge沟道多鳍FinFET的首次实验演示。

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