Magnetocaloric effects and critical behavior of La0.65Ca0.35−xGdxMnO3 (0≤x≤0.15)

Author:

Huaijin Ma1ORCID,Xiang Jin12ORCID,Lei Gao3ORCID,Jing Zhao1ORCID,Ru Xing1ORCID,Huiqin Yun1ORCID,Jianjun Zhao1ORCID

Affiliation:

1. School of Physical Science and Technology, Baotou Teachers’ College, Key Laboratory of Magnetism and Magnetic Materials for Higher Education in Inner, Mongolia Autonomous Region, Baotou 014030, P. R. China

2. School of Physics and Electronic Information, Inner Mongolia Normal University, Hohhot 010020, P. R. China

3. National Key Laboratory of Baiyunobo Rare, Earth Resource Research and Comprehensive Utilization, Baotou Research Institute of Rare Earths, Baotou 014030, P. R. China

Abstract

In this study, we investigate the magnetocaloric effects (MCE) and critical behavior of Gd-doped La[Formula: see text]Ca[Formula: see text]GdxMnO3 ([Formula: see text]) polycrystalline materials. Our results reveal excellent MCE in the Gd-doped samples. Under a magnetic field of 7[Formula: see text]T, the full-width at half maximum ([Formula: see text] increases from 41[Formula: see text]K ([Formula: see text]) to 121[Formula: see text]K ([Formula: see text]) and 112[Formula: see text]K ([Formula: see text]). Additionally, the refrigerant capacity (RC) is enhanced by 149% and 145% at [Formula: see text] and [Formula: see text], respectively, compared to the parent phase. We propose that these improvements can be attributed to the introduction of Gd[Formula: see text] ions, which possess smaller ionic radii. This reduction in the average A-site ionic radius weakens the double exchange (DE) interactions, resulting in a more continuous phase transition within the system. Supporting this view, we observe a decrease in magnetization strength after doping, a reduction in Curie temperature ([Formula: see text] from 250[Formula: see text]K ([Formula: see text]) to 134[Formula: see text]K ([Formula: see text]) and 130[Formula: see text]K ([Formula: see text]) and a transformation from a first-order to a second-order phase transition in the doped samples. To characterize the critical behavior of the phase transition in the doped samples, we employ the K-F method. The obtained critical exponents for [Formula: see text] and [Formula: see text] are [Formula: see text], [Formula: see text], [Formula: see text] and [Formula: see text], [Formula: see text], [Formula: see text], respectively. Furthermore, the calculation of the n values suggests a transition of the phase transition in the doped samples from short-range ordering to long-range ordering.

Funder

State Key Development Program for Basic Research of China

Publisher

World Scientific Pub Co Pte Ltd

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