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Properties of Unshunted and Resistively Shunted Nb/AlOx-Al/Nb Josephson Junctions With Critical Current Densities from 0.1 mA/{\mu}m^2 to 1 mA/{\mu}m^2

机译:Nh / alOx-al / Nb Josephson无阻和电阻分布的性质   临界电流密度为0.1 ma / {\ mu} m ^ 2至1的结   毫安/ {\亩}平方公尺

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摘要

We investigated current-voltage characteristics of unshunted and externallyshunted Josephson junctions (JJs) with high critical current densities, Jc, inorder to extract their basic parameters and statistical characteristics for JJmodeling in superconducting integrated circuits and to assess their potentialfor future technology nodes. Nb/AlOx-Al/Nb JJs with diameters from 0.5 {\mu}mto 6 {\mu}m were fabricated using a fully planarized process with Mo or MoNxthin-film shunt resistors with sheet resistance Rsq = 2 {\Omega}/sq and Rsq = 6{\Omega}/sq, respectively. We used our standard MIT LL process SFQ5ee tofabricate JJs with Jc = 0.1 mA/{\mu}m^2 and our new process SFQ5hs to make JJswith Jc = 0.2 mA/{\mu}m^2 and higher current densities up to about 1mA/{\mu}m^2. Using LRC resonance features on the I-V characteristics of shuntedJJs, we extract the inductance associated with molybdenum shunt resistors of1.4 pH/sq. The main part this inductance, about 1.1 pH/sq, is the inductance ofthe 40-nm Mo resistor film, while the geometrical inductance of superconductingNb wiring contributes the rest. We attribute this large inductance to kineticinductance arising from the complex conductivity of a thin normal-metal film inan electromagnetic field with angular frequency {\omega},{\sigma}({\omega})={\sigma}0/(1+i{\omega}{\tau}), where {\sigma}0 is the staticconductivity and {\tau} the electron scattering time. Using a resonance in alarge-area unshunted high-Jc junction excited by a resistively coupledsmall-area shunted JJ, we extract the Josephson plasma frequency and specificcapacitance of high-Jc junctions in 0.1 to 1 mA/{\mu}m^2 Jc range. We alsopresent data on Jc targeting and JJ critical current spreads. We discuss using0.2-mA/{\mu}m^2 JJs in VLSI Single Flux Quantum circuits and 0.5-mA/{\mu}m^2JJs in high-density integrated circuits without shunt resistors.
机译:我们研究了具有高临界电流密度Jc的未分流和外部分流的约瑟夫逊结(JJs)的电流-电压特性,以提取它们的基本参数和统计特性,用于超导集成电路中JJmodeling,并评估它们对未来技术节点的潜力。使用Mo或MoNx薄膜分流电阻器(其薄层电阻Rsq = 2 {\ Omega} / sq)使用完全平坦的工艺制造直径为0.5 {μm至6 {μm}的Nb / AlOx-Al / Nb JJ和Rsq分别为6 {\ Omega} / sq。我们使用标准的MIT LL工艺SFQ5ee来制造Jc = 0.1 mA / {\ mu} m ^ 2的JJ,并使用新工艺SFQ5hs来制造Jc = 0.2 mA / {\ mu} m ^ 2的JJ,并且电流密度高达大约1mA / {\ mu} m ^ 2。利用LRC谐振特性对并联JJ的I-V特性,我们提取了与1.4 pH / sq的钼并联电阻相关的电感。该电感的主要部分约为1.1 pH / sq,是40 nm Mo电阻膜的电感,而超导Nb布线的几何电感则贡献了其余部分。我们将大电感归因于在角频率为{\ omega},{\ sigma}({\ omega})= {\ sigma} 0 /(1+ i {\ omega} {\ tau}),其中{\ sigma} 0是静电导率,{\ tau}是电子散射时间。在电阻耦合的小面积分流JJ激发的大面积未分流高Jc结中使用共振,我们提取了约瑟夫森等离子体频率和0.1至1 mA / {\ mu} m ^ 2 Jc范围内的高Jc结的比电容。 。我们还将提供有关Jc定位和JJ临界电流点差的数据。我们讨论了在VLSI单通量量子电路中使用0.2mA / {μm^ 2JJs,在没有分流电阻器的高密度集成电路中使用0.5mA / {μm^ 2JJs。

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