Materials Map

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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Topics

Publications (1/1 displayed)

  • 2024New insights into the magnetism and magnetic structure of LuCrO<sub>3</sub> perovskite1citations

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Alonso, José Antonio
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Céspedes, Eva
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Fernández-Díaz, Maria Teresa
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Martinez, José Luis
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Zhou, Jian-Shi
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Gainza, Javier
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2024

Co-Authors (by relevance)

  • Alonso, José Antonio
  • Céspedes, Eva
  • Fernández-Díaz, Maria Teresa
  • Martinez, José Luis
  • Zhou, Jian-Shi
  • Gainza, Javier
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article

New insights into the magnetism and magnetic structure of LuCrO<sub>3</sub> perovskite

  • Alonso, José Antonio
  • Céspedes, Eva
  • Fernández-Díaz, Maria Teresa
  • Martinez, José Luis
  • Zhou, Jian-Shi
  • Muñoz, Angel
  • Gainza, Javier
Abstract

<jats:p>A polycrystalline sample LuCrO<jats:sub>3</jats:sub> has been characterized by neutron powder diffraction (NPD) and magnetization measurements. Its crystal structure has been Rietveld refined from NPD data in space group <jats:italic>Pnma</jats:italic>; this perovskite contains strongly tilted CrO<jats:sub>6</jats:sub> octahedra with extremely bent Cr—O—Cr superexchange angles of ∼142°. The NPD data show that below Néel temperature (<jats:italic>T</jats:italic><jats:sub>N</jats:sub> ≃ 131 K), the magnetic structure can be defined as an A-type antiferromagnetic arrangement of Cr<jats:sup>3+</jats:sup> magnetic moments, aligned along the <jats:italic>b</jats:italic> axis, with a canting along the <jats:italic>c</jats:italic> axis. A noticeable magnetostrictive effect is observed in the unit-cell parameters and volume upon cooling down across <jats:italic>T</jats:italic><jats:sub>N</jats:sub>. The AC magnetic susceptibility indicates the onset of magnetic ordering below 112.6 K; the magnetization isotherms below <jats:italic>T</jats:italic><jats:sub>N</jats:sub> show a nonlinear behaviour that is associated with the described canting of the Cr<jats:sup>3+</jats:sup> magnetic moments. From the Curie–Weiss law, the effective moment of the Cr<jats:sup>3+</jats:sup> sublattice is found to be μ<jats:sub>eff</jats:sub> = 3.55 μ<jats:sub>B</jats:sub> (calculated 3.7 μ<jats:sub>B</jats:sub>) while the Θ<jats:sub>CW</jats:sub> parameter yields a value of −155 K, indicating antiferromagnetic interactions. There is a conspicuous increase of <jats:italic>T</jats:italic><jats:sub>N</jats:sub> upon the application of external pressure, which must be due to shortening of the Cr—O bond length under compression that increases the orbital overlap integral.</jats:p>

Topics
  • perovskite
  • impedance spectroscopy
  • susceptibility
  • magnetization
  • space group
  • aligned