TY - JOUR
T1 - The crystal structures, magnetic interactions and cryogenic magnetocaloric effects for NaGdXO4 (X=Si, Ti) compounds
AU - Chen, Zuhua
AU - Zhang, Guochun
AU - Wang, Changkun
AU - Gao, Jiahao
AU - Zhang, Yicai
AU - Yu, Shilin
AU - Zhao, Yanan
AU - Li, Zhenxing
AU - Shen, Jun
AU - Tu, Heng
N1 - Publisher Copyright:
© 2024 Elsevier B.V.
PY - 2025/1/5
Y1 - 2025/1/5
N2 - The development of ultra-low temperature magnetic refrigeration technologies demands magnetic refrigeration materials with excellent properties. Hence, improving performances of magnetic refrigerants has always been a significant scientific issue in magnetic refrigeration field. In this article, the relationship of crystal structures, magnetic interactions and magnetocaloric effect (MCE) for NaGdSiO4 and NaGdTiO4 has been investigated. NaGdSiO4 and NaGdTiO4 both crystallizes orthogonal structure, but the significant difference of unit cell parameters and symmetries results in different arrangement of Gd atoms. The distorted crystal structure and weaker magnetic between Gd3+ ions make NaGdSiO4 exhibit larger MCE with the maximum magnetic entropy change (-∆SM) of 49.0 J·kg−1·K−1 at 2.8 K. Comparably speaking, NaGdTiO4, which is a quasi-triangular antiferromagnet, possesses a stronger magnetic interaction between Gd3+ ions with the maximum -∆SM of 31.9 J·kg−1·K−1 at 2.6 K. These results confirm the importance of magnetic interactions for magnetic refrigeration materials, and, more broadly, they highlight the significance of crystal structures in that field.
AB - The development of ultra-low temperature magnetic refrigeration technologies demands magnetic refrigeration materials with excellent properties. Hence, improving performances of magnetic refrigerants has always been a significant scientific issue in magnetic refrigeration field. In this article, the relationship of crystal structures, magnetic interactions and magnetocaloric effect (MCE) for NaGdSiO4 and NaGdTiO4 has been investigated. NaGdSiO4 and NaGdTiO4 both crystallizes orthogonal structure, but the significant difference of unit cell parameters and symmetries results in different arrangement of Gd atoms. The distorted crystal structure and weaker magnetic between Gd3+ ions make NaGdSiO4 exhibit larger MCE with the maximum magnetic entropy change (-∆SM) of 49.0 J·kg−1·K−1 at 2.8 K. Comparably speaking, NaGdTiO4, which is a quasi-triangular antiferromagnet, possesses a stronger magnetic interaction between Gd3+ ions with the maximum -∆SM of 31.9 J·kg−1·K−1 at 2.6 K. These results confirm the importance of magnetic interactions for magnetic refrigeration materials, and, more broadly, they highlight the significance of crystal structures in that field.
KW - Crystal structures
KW - Magnetic interactions
KW - Magnetic refrigeration
KW - Magnetocaloric effect
UR - http://www.scopus.com/inward/record.url?scp=85207599647&partnerID=8YFLogxK
U2 - 10.1016/j.jallcom.2024.177218
DO - 10.1016/j.jallcom.2024.177218
M3 - Article
AN - SCOPUS:85207599647
SN - 0925-8388
VL - 1010
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
M1 - 177218
ER -