4.6 Article

Structural, magnetic, and superconducting properties of pulsed-laser-deposition-grown La1.85Sr0.15CuO4/La2/3Ca1/3MnO3 superlattices on (001)-oriented LaSrAlO4 substrates

Journal

PHYSICAL REVIEW B
Volume 89, Issue 9, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.89.094511

Keywords

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Funding

  1. Schweizer Nationalfonds (SNF) [200020-140225, 206021-139102]
  2. National Centre of Competence in Research Materials with Novel Electronic PropertiesMaNEP
  3. US Department of Energy (DOE), Basic Energy Sciences (BES), Materials Sciences and Engineering Division
  4. ERC starting Investigator Award, [239739]
  5. European Commission [283883]
  6. Swiss National Science Foundation (SNF) [200020_140225, 206021_139102] Funding Source: Swiss National Science Foundation (SNF)
  7. European Research Council (ERC) [239739] Funding Source: European Research Council (ERC)

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Epitaxial La1.85Sr0.15CuO4/ La2/ 3Ca1/ 3MnO3 ( LSCO/ LCMO) superlattices on ( 001)-oriented LaSrAlO4 substrates have been grown with pulsed laser deposition technique. Their structural, magnetic, and superconducting properties have been determined with 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 the large mismatch between the in-plane lattice parameters of LSCO (a = 0.3779 nm) and LCMO (a = 0.387 nm) these superlattices can be grown epitaxially and with a high crystalline quality. While the first LSCO layer remains clamped to the LaSrAlO4 substrate, a sizable strain relaxation occurs already in the first LCMO layer. The following LSCO and LCMO layers adopt a nearly balanced state in which the tensile and compressive strain effects yield alternating in-plane lattice parameters with an almost constant average value. No major defects are observed in the LSCO layers, while a significant number of vertical antiphase boundaries are found in the LCMOlayers. The LSCO layers remain superconducting with a relatively high superconducting onset temperature of T onset c approximate to 36 K. The macroscopic superconducting response is also evident in the magnetization data due to a weak diamagnetic signal below 10 K for H parallel to ab and a sizable paramagnetic shift for H parallel to c that can be explained in terms of a vortex-pinning-induced flux compression. The LCMO layers maintain a strongly ferromagnetic state with a Curie temperature of T Curie approximate to 190 K and a large low-temperature saturation moment of about 3.5(1) mu(B) per Mn ion. These results suggest that the LSCO/ LCMO superlattices can be used to study the interaction between the antagonistic ferromagnetic and superconducting orders and, in combination with previous studies on YBa2Cu3O7-x/ La2/ 3Ca1/ 3MnO3 superlattices, may allow one to identify the relevant mechanisms.

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