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    Long-period incommensurate magnetic orderings associated with the large magnetocaloric effect in GdCo2B2

    Simon Rosenqvist Larsen*, Noriki Terada†, and Hiroaki Mamiya

    Hiraku Saito and Taro Nakajima

    Shinichi Itoh

    Pascal Manuel, Dmitry Khalyavin, and Fabio Orlandi

    Hideaki Kitazawa

    • Institute for Solid State Physics, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581, Japan

    • Institute of Materials Structure Science, High Energy Accelerator Research Organization, 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan and Materials and Life Science Division, J-PARC Center, 2-4 Shirane Shirakata, Tokai-mura, Naka-gun, Ibaraki 319-1195, Japan

    • *Contact author: larsen.simon@nims.go.jp
    • †Contact author: terada.noriki@nims.go.jp

    Phys. Rev. B 113, 104411 – Published 5 March, 2026

    DOI: https://doi.org/10.1103/yyx5-3dnv

    Abstract

    GdCo2B2 is a member of the ThCr2Si2 family of compounds which exhibits good magnetocaloric properties associated with antiferromagnetic orderings in the temperature range for hydrogen liquefaction applications. As antiferromagnetic compounds typically do not exhibit a large magnetocaloric effect, understanding the magnetic orderings in GdCo2B2 could help uncover more magnetocaloric compounds that rely on antiferromagnetic ordering. GdCo2B2 exhibits four antiferromagnetic phase transitions at 22 K, 18.5 K, 13 K, and 7 K. Due to the difficulty of conducting neutron diffraction measurements on compounds containing affordable natural Gd, the microscopic magnetic structures have so far not been investigated. In this study, by using high energy neutrons and devising special sample preparations for lower energy neutrons, powder neutron diffraction patterns of GdCo2B2 have successfully been measured. A long-period incommensurate magnetic ordering with k1=(0.053100) was seen at 20 K. The propagation vector of the incommensurate structure shifted to k1=(0.07100) at 16 K, and an additional k=(000) ferromagnetic component was observed. At 10 K, two incommensurate propagation vectors of k1=(0.073100) and k2=(0.07310.07310), which shifted to k1=(0.074100) and k2=(0.07410.07410) at 6 K, were observed to coexist. By considering only the k1-modulation, two possible magnetic structures below 10 K are reported to describe the data, either ac-cycloid structure with constant moment at each Gd site or ellipsoidal ab-cycloid structure. Exchange interaction energy calculations indicated that the long-period antiferromagnetic ordering in GdCo2B2 is energetically close to the ferromagnetic state due to the strong competition between ferromagnetic and antiferromagnetic exchange interactions, which plays an essential role for the emergence of the large magnetocaloric effect in GdCo2B2.

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