Aviso: para depositar documentos, por favor, inicia sesión e identifícate con tu cuenta de correo institucional de la UCM con el botón MI CUENTA UCM. No emplees la opción AUTENTICACIÓN CON CONTRASEÑA
 

Structural, magnetic, and superconducting properties of pulsed-laser-deposition-grown La_1.85Sr_0.15CuO_4/La_2/3Ca_1/3MnO_3 superlattices on (001)-oriented LaSrAlO_4 substrates

Loading...
Thumbnail Image

Full text at PDC

Publication date

2014

Advisors (or tutors)

Editors

Journal Title

Journal ISSN

Volume Title

Publisher

American Physical Society
Citations
Google Scholar

Citation

S. Das, K. Sen, I. Marozau, M. A. Uribe-Laverde, N. Biskup, M. Varela, Y. Khaydukov, O. Soltwedel, T. Keller, M. Döbeli, C. W. Schneider, and C. Bernhard, Phys. Rev. B 89, 094511 (2014).

Abstract

Epitaxial La_1.85Sr_0.15CuO4/La_2/3Ca_1/3MnO_3 (LSCO/LCMO) superlattices on (001)-oriented LaSrAlO_4 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 ffraction, 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 highcrystalline 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 LCMO layers. The LSCO layers remain superconducting with a relatively high superconducting onset temperature of T onset c ≈ 36 K. The macroscopic superconducting response is also evident in the magnetization data due to a weak diamagnetic signal below 10 K for H ab and a sizable paramagnetic shift for H 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 ≈ 190 K and a large low-temperature saturation moment of about 3.5(1) μB per Mn ion. These results suggest that the LSCO/LCMO superlattices can be used to study the interaction between the antagonistic ferromagnetic and uperconducting orders and, in combination with previous studies on YBa_2Cu_3O_7−x /La_2/3Ca_1/3MnO_3 superlattices, may allow one to identify the relevant mechanisms.

Research Projects

Organizational Units

Journal Issue

Description

Keywords

Collections