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YBa2Cu3O7 grain boundary junctions and low-noise superconducting quantum interference devices patterned by a focused ion beam down to 80 nm linewidth

机译:YBa2Cu3O7晶界结和低噪声超导量子阱   由聚焦离子束图案化的干涉装置,线宽低至80nm

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摘要

YBa$_2$Cu$_3$O$_7$ 24$^\circ$ (30$^\circ$) bicrystal grain boundary junctions(GBJs), shunted with 60\,nm (20\,nm) thick Au, were fabricated by focused ionbeam milling with widths $80\,{\rm nm} \le w \le 7.8\,\mu$m. At 4.2\,K we findcritical current densities $j_c$ in the $10^5\,{\rm A/cm^2}$ range %\dkc{\#1}(without a clear dependence on $w$) and an increase in resistance timesjunction area $\rho$ with an approximate scaling $\rho\propto w^{1/2}$. For thenarrowest GBJs $j_c\rho\approx 100\,\mu$V, which is promising for therealization of sensitive nanoSQUIDs for the detection of small spin systems. Wedemonstrate that our fabrication process allows the realization of sensitivenanoscale dc SQUIDs; for a SQUID with $w\approx 100$\,nm wide GBJs we find anrms magnetic flux noise spectral density of $S_\Phi^{1/2}\approx4\,\mu\Phi_0/{\rm Hz}^{1/2}$ in the white noise limit. We also derive anexpression for the spin sensitivity $S_\mu^{1/2}$, which depends on$S_\Phi^{1/2}$, on the location and orientation of the magnetic moment of amagnetic particle to be detected by the SQUID, and on the SQUID geometry. Forthe not optimized SQUIDs presented here, we estimate$S_\mu^{1/2}=390\,\mu_B/\sqrt{\rm{Hz}}$, which could be further improved by atleast an order of magnitude.
机译:YBa $ _2 $ Cu $ _3 $ O $ _7 $ 24 $ ^ \ circ $(30 $ ^ \ circ $)双晶晶界结(GBJs)与60nm(nm)(20nm)分流了通过聚焦离子束铣削加工而成,宽度为$ 80 \,{\ rm nm} \ le w \ le 7.8 \,\ mu $ m。在4.2 \,K处,我们发现临界电流密度$ j_c $在$ 10 ^ 5 \,{\ rm A / cm ^ 2} $范围%\ dkc {\#1}(与$ w $没有明显依赖)和一个电阻乘以连接面积$ \ rho $的增加,缩放比例为\\ rho \ proto w ^ {1/2} $。对于最窄的GBJ,j_c \ rho \约100 \,\ mu $ V,这有望实现用于检测小型自旋系统的灵敏nanoSQUID。希望我们的制造工艺能够实现灵敏的纳米级直流SQUID;对于具有$ w \大约100 $ \,nm宽的GBJ的SQUID,我们发现anrms磁通量噪声频谱密度为$ S_ \ Phi ^ {1/2} \ approx4 \,\ mu \ Phi_0 / {\ rm Hz} ^ { 1/2噪声限制。我们还导出了自旋灵敏度$ S_ \ mu ^ {1/2} $的表达式,该表达式取决于要检测的非磁性粒子的磁矩的位置和方向,取决于$ S_ \ Phi ^ {1/2} $通过SQUID以及SQUID几何图形。对于此处介绍的未优化的SQUID,我们估计$ S_ \ mu ^ {1/2} = 390 \,\ mu_B / \ sqrt {\ rm {Hz}} $,可以至少提高一个数量级。

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