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在氧化镁双晶衬底上的钇钡铜氧纳米超导量子干涉器件。

YBaCuO nano superconducting quantum interference devices on MgO bicrystal substrates.

作者信息

Lin Jianxin, Müller Benedikt, Linek Julian, Karrer Max, Wenzel Malte, Martínez-Pérez Maria José, Kleiner Reinhold, Koelle Dieter

机构信息

Physikalisches Institut - Experimentalphysik II and Center for Quantum Science (CQ) in LISA+, University of Tübingen, Auf der Morgenstelle 14, 72076 Tübingen, Germany.

Instituto de Ciencia de Materiales de Aragón and Departamento de Física de la Materia Condensada, CSIC-Universidad de Zaragoza, 50009 Zaragoza, Spain and Fundacíon ARAID, Avda. de Ranillas, 50018 Zaragoza, Spain.

出版信息

Nanoscale. 2020 Mar 5;12(9):5658-5668. doi: 10.1039/c9nr10506a.

Abstract

We report on nanopatterned YBa2Cu3O7-δ (YBCO) direct current superconducting quantum interference devices (SQUIDs) based on grain boundary Josephson junctions. The nanoSQUIDs are fabricated by epitaxial growth of 120 nm-thick films of the high-transition temperature cuprate superconductor YBCO via pulsed laser deposition on MgO bicrystal substrates with 24° misorientation angle, followed by sputtering of dAu = 65 nm thick Au. Nanopatterning is performed by Ga focused ion beam (FIB) milling. The SQUID performance is comparable to devices on SrTiO3 (STO), as demonstrated by electric transport and noise measurements at 4.2 K. MgO has orders of magnitude smaller dielectric permittivity than STO; i.e., one may avoid Au as a resistively shunting layer to reduce the intrinsic thermal flux noise of the nanoSQUIDs. However, we find that the Au layer is important for avoiding degradation during FIB milling. Hence, we compare devices with different dAu produced by thinning the Au layer via Ar ion milling after FIB patterning. We find that the reduction of dAu yields an increase in junction resistance, however at the expense of a reduction of the critical current and increase in SQUID inductance. This results in an estimated thermal flux noise that is almost independent of dAu. However, for two devices on MgO with 65 nm-thick Au, we find an order of magnitude lower low-frequency excess noise as compared to nanoSQUIDs on STO or those on MgO with reduced dAu. For one of those devices we obtain with bias-reversal readout ultra-low flux noise of ∼175 nΦ0 Hz-1/2 down to ∼10 Hz.

摘要

我们报道了基于晶界约瑟夫森结的纳米图案化钇钡铜氧(YBCO)直流超导量子干涉器件(SQUID)。通过脉冲激光沉积在取向差为24°的MgO双晶衬底上外延生长120nm厚的高温转变温度铜酸盐超导体YBCO薄膜,随后溅射65nm厚的金来制备纳米SQUID。通过镓聚焦离子束(FIB)铣削进行纳米图案化。如在4.2K下的电输运和噪声测量所示,该SQUID的性能与在SrTiO3(STO)上的器件相当。MgO的介电常数比STO小几个数量级;也就是说,可以避免使用金作为电阻分流层来降低纳米SQUID的固有热通量噪声。然而,我们发现金层对于避免FIB铣削过程中的退化很重要。因此,我们比较了通过FIB图案化后用氩离子铣削减薄金层而产生的不同金厚度的器件。我们发现金厚度的减小会导致结电阻增加,但代价是临界电流降低和SQUID电感增加。这导致估计的热通量噪声几乎与金厚度无关。然而,对于两个在MgO上具有65nm厚金的器件,我们发现与在STO上的纳米SQUID或金厚度减小的MgO上的纳米SQUID相比,低频过量噪声低一个数量级。对于其中一个器件,我们通过偏置反转读出获得了低至约10Hz时约175nΦ0 Hz-1/2的超低通量噪声。

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