首页> 外文OA文献 >Exchange-bias-modulated inverse superconducting spin switch in CoO/Co/YBa_(2)Cu_(3)O_(7-δ)/La_(0.7)Ca_(0.3)MnO_(3) thin film hybrids
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Exchange-bias-modulated inverse superconducting spin switch in CoO/Co/YBa_(2)Cu_(3)O_(7-δ)/La_(0.7)Ca_(0.3)MnO_(3) thin film hybrids

机译:CoO / Co / YBa_(2)Cu_(3)O_(7-δ)/ La_(0.7)Ca_(0.3)MnO_(3)薄膜复合材料中的交换偏置调制逆超导自旋开关

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摘要

We examine the interplay between ferromagnetism and superconductivity in bilayer and trilayer heterostructures based on Co, YBa_(2)Cu_(3)O_(7-δ) (YBCO), and La_(0.7)Ca_(0.3)MnO_(3) (LCMO) thin films grown on SrTiO_(3) substrates with typical thicknesses of 10–15 nm. We have measured magnetoresistance below the resistive-superconducting onset of the YBCO. Naturally oxidized antiferromagnetic CoO top layer films give rise to pronounced exchange bias, modifying the coercive field of the Co by several hundred Oe. This allows separating effects at coercivity, such as stray fields, from those of parallel vs. antiparallel magnetic alignment between top and bottom ferromagnetic layers. In bilayers of Co/YBCO and of LCMO/YBCO, we observe a small magnetoresistance peak centered at the coercive field of the ferromagnetic layer of at most 20%, which we attribute to the effect of stray fields generated in the domain state of the ferromagnet. In the case of the CoO/Co/YBCO/LCMO/SrTiO_(3) trilayer, aside from the peaks at coercivity, we observe a well-defined plateau of the magnetoresistance extending between the coercive fields of the LCMO and Co, with a width that is modified by the exchange-biased Co layer. Reactivity between Co and YBCO at the interface gives rise to a progressive deterioration in the superconducting transition temperature. Aged samples display magnetoresistance peaks at the coercive fields of the Co and LCMO characteristic of stray fields without the magnetoresistance plateau between them.
机译:我们研究了基于Co,YBa_(2)Cu_(3)O_(7-δ)(YBCO)和La_(0.7)Ca_(0.3)MnO_(3)(LCMO)的双层和三层异质结构中铁磁与超导之间的相互作用)在SrTiO_(3)衬底上生长的薄膜,典型厚度为10–15 nm。我们已经测量了YBCO的超导超导磁阻以下的磁阻。天然氧化的反铁磁CoO顶层薄膜会产生明显的交换偏压,从而将Co的矫顽场提高了数百Oe。这允许将矫顽力(例如杂散场)与顶部和底部铁磁层之间的平行与反平行磁对准的效应分开。在Co / YBCO和LCMO / YBCO的双层结构中,我们观察到一个以铁磁层的矫顽场为中心的小磁致电阻峰,其最大强度为20%,这归因于在铁磁体的畴态中产生的杂散磁场的影响。 。在CoO / Co / YBCO / LCMO / SrTiO_(3)三层的情况下,除矫顽力峰值外,我们还观察到了在LCMO和Co的矫顽场之间扩展的磁阻稳定区,其宽度为通过交换偏置的Co层进行修改。 Co和YBCO在界面处的反应性导致超导转变温度的逐步降低。老化的样品在Co的矫顽场和杂散场的LCMO特性处显示出磁阻峰,而它们之间没有磁阻平稳。

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