首页> 外文OA文献 >Structural, magnetic and superconducting properties of pulsed-laser-deposition-grown $ m{La_{1.85}Sr_{0.15}CuO_{4}/La_{2/3}Ca_{1/3}MnO_{3}}$ superlattices on $ m{(001)}$-oriented $ m{LaSrAlO_{4}}$ substrates
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Structural, magnetic and superconducting properties of pulsed-laser-deposition-grown $ m{La_{1.85}Sr_{0.15}CuO_{4}/La_{2/3}Ca_{1/3}MnO_{3}}$ superlattices on $ m{(001)}$-oriented $ m{LaSrAlO_{4}}$ substrates

机译:结构,磁性和超导性能   脉冲激光沉积生长   $ \ rm {La_ {1.85} sr_ {0.15} CuO_ {4} / La_ {2/3} Ca_ {1/3} mnO_ {3}} $ superlattices on   $ \ rm {(001)} $ - 面向$ \ rm {LasralO_ {4}} $基板

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摘要

Epitaxial La1.85Sr0.15CuO4/La2/3Ca1/3MnO3 superlattices on (001)-orientedLaSrAlO4 substrates have been grown with pulsed laser deposition technique.Their structural, magnetic and superconducting properties have been determinedwith in-situ reflection high energy electron diffraction, x-ray diffraction,specular neutron reflectometry, scanning transmission electron microscopy,electric transport, and magnetization measurements. We find that despite thelarge mismatch between the in-plane lattice parameters of LSCO and LCMO thesesuperlattices can be grown epitaxially and with a high crystalline quality.While the first LSCO layer remains clamped to the LSAO substrate, a sizeablestrain relaxation occurs already in the first LCMO layer. The following LSCOand LCMO layers adopt a nearly balanced state in which the tensile andcompressive strain effects yield alternating in-plane lattice parameters withan almost constant average value. No major defects are observed in the LSCOlayers, while a significant number of vertical antiphase boundaries are foundin the LCMO layers. The LSCO layers remain superconducting with a relativelyhigh superconducting onset temperature of about 36 K. The macroscopicsuperconducting response is also evident in the magnetization data due to aweak diamagnetic signal below 10 K for H || ab and a sizeable paramagneticshift for H || c that can be explained in terms of a vortex-pinning-inducedflux compression. The LCMO layers maintain a strongly ferromagnetic state witha Curie temperature of about 190 K and a large low-temperature saturationmoment of about 3.5(1) muB. These results suggest that the LSCO/LCMOsuperlattices can be used to study the interaction between the antagonisticferromagnetic and superconducting orders and, in combination with previousstudies on YBCO/LCMO superlattices, may allow one to identify the relevantmechanisms.
机译:利用脉冲激光沉积技术在(001)取向的LaSrAlO4衬底上生长了外延La1.85Sr0.15CuO4 / La2 / 3Ca1 / 3MnO3超晶格,并通过原位反射高能电子衍射,x-射线衍射,镜面中子反射仪,扫描透射电子显微镜,电传输和磁化强度测量。我们发现,尽管LSCO和LCMO的面内晶格参数之间存在较大的不匹配,但这些超晶格仍可以外延生长并具有较高的结晶质量。尽管第一LSCO层仍被夹持在LSAO衬底上,但在第一LCMO中已经出现了相当大的应变松弛层。随后的LSCO和LCMO层采用接近平衡的状态,其中拉伸和压缩应变效应会产生交替的面内晶格参数,其平均值几乎恒定。在LSCO层中未观察到主要缺陷,而在LCMO层中发现了大量的垂直反相边界。 LSCO层保持超导状态,并且具有约36 K的相对较高的超导起始温度。由于H ||低于10 K,抗磁强度弱,因此宏观磁导数据在磁化数据中也很明显。 a和H的相当大的顺磁位移c可以用涡旋钉扎引起的磁通压缩来解释。 LCMO层保持强铁磁状态,居里温度约为190 K,低温饱和力矩约为3.5(1)μB。这些结果表明,LSCO / LCMO超晶格可用于研究拮抗铁磁和超导阶之间的相互作用,并结合有关YBCO / LCMO超晶格的先前研究,可能使人们识别相关机制。

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