Abstract

We investigated the structural and magnetic properties of 20 nm-sized nanoparticles of the half-doped manganite Ho0.5Ca0.5MnO3 prepared by sol-gel approach. Neutron powder diffraction patterns show Pbnm orthorhombic symmetry for 10 K < T < 290 K, with lattice parameters a, b, and c in the relationship c/√2 < a < b, indicating a cooperative Jahn–Teller effect, i.e., orbital ordering OO, from below room temperature. In contrast with the bulk samples, in the interval 250 < T < 300 K, the fingerprint of charge ordering (CO) does not manifest itself in the temperature dependence of lattice parameters. However, there are signs of CO in the temperature dependence of magnetization. Accordingly, below 100 K superlattice magnetic Bragg reflections arise, which are consistent with an antiferromagnetic phase strictly related to the bulk Mn ordering of a charge exchange-type (CE-type), but characterized by an increased fraction of ferromagnetic couplings between manganese species themselves. Our results show that in this narrow band half-doped manganite, size reduction only modifies the balance between the Anderson superexchange and Zener double exchange interactions, without destabilizing an overall very robust antiferromagnetic state.

Highlights

  • IntroductionCa2+ , Sr2+ , Ba2+ , 0 ≤ x ≤ 1, have been the subject of intense research for over twenty years thanks to their rich physics

  • Published: 11 January 2022Hole-doped colossal magnetoresistive (CMR) manganites with general formulaRE1−x AEx MnO3

  • Ca2+, Sr2+, Ba2+, 0 ≤ x ≤ 1, have been the subject of intense research for over twenty years thanks to their rich physics. This emerges from an outstanding variety of interconnected structural, electronic, and magnetic phase transitions, which lead to competing ground states, either metallic ferromagnetic (FM), with predominant Zener double exchange interaction [1], or insulating antiferromagnetic (AFM), with predominant Anderson superexchange interaction [2]

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Summary

Introduction

Ca2+ , Sr2+ , Ba2+ , 0 ≤ x ≤ 1, have been the subject of intense research for over twenty years thanks to their rich physics. This emerges from an outstanding variety of interconnected structural, electronic, and magnetic phase transitions, which lead to competing ground states, either metallic ferromagnetic (FM), with predominant Zener double exchange interaction [1], or insulating antiferromagnetic (AFM), with predominant Anderson superexchange interaction [2]. The crystal structures of the undoped phases depend on the RE size, changing from orthorhombic GdFeO3 -type perovskite La to Tb), to hexagonal non-perovskite LuMnO3 -type 2(rB + rO ) expressed, with reference to the ABO3 simple perovskite chemical formula, in terms of octahedral B-site cation and oxygen radii, respectively, rB and rO , and of the radius of the A-type cation, this latter

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