TY - JOUR
T1 - Giant refrigeration capacity in Gd5B2C5 compounds with tetragonal structure
AU - Li, Zhenxing
AU - Liu, Yakun
AU - Hu, Zhouhang
AU - Fu, Diyi
AU - Liu, Jun
AU - Mo, Zhaojun
AU - Gao, Xinqiang
AU - Tang, Mingsheng
AU - Shen, Jun
N1 - Publisher Copyright:
Copyright © 2026. Published by Elsevier Ltd.
PY - 2026/6
Y1 - 2026/6
N2 - The search for high-performance magnetic refrigeration materials to promote the application of magnetic refrigeration technology to replace the traditional gas compression refrigeration is an urgent requirement. In this work, Gd5B2C5 compound with tetragonal structure (P4/ncc; space group No. 130) was synthesized and its crystal structure, magnetism, magnetocaloric effects were systematically investigated. It undergoes a second-order magnetic phase transition from ferromagnetic to paramagnetic around approximately 132 K. The maximum magnetic entropy change and refrigeration capacity of Gd5B2C5 compound are 4.5 J·kg−1 K−1, 219.2 J·kg−1, 8.9 J·kg−1 K−1 and 713.8 J·kg−1 under varying magnetic fields of 0–2 T and 0–5 T. It is worth mentioning that the half-peak width of the maximum magnetic entropy change is as high as 110.5 K under a varying magnetic field of 0–5 T, which will benefit the wide temperature span required for refrigeration. The present results indicate that Gd5B2C5 compound is a suitable candidate for practical applications in magnetic refrigeration technology.
AB - The search for high-performance magnetic refrigeration materials to promote the application of magnetic refrigeration technology to replace the traditional gas compression refrigeration is an urgent requirement. In this work, Gd5B2C5 compound with tetragonal structure (P4/ncc; space group No. 130) was synthesized and its crystal structure, magnetism, magnetocaloric effects were systematically investigated. It undergoes a second-order magnetic phase transition from ferromagnetic to paramagnetic around approximately 132 K. The maximum magnetic entropy change and refrigeration capacity of Gd5B2C5 compound are 4.5 J·kg−1 K−1, 219.2 J·kg−1, 8.9 J·kg−1 K−1 and 713.8 J·kg−1 under varying magnetic fields of 0–2 T and 0–5 T. It is worth mentioning that the half-peak width of the maximum magnetic entropy change is as high as 110.5 K under a varying magnetic field of 0–5 T, which will benefit the wide temperature span required for refrigeration. The present results indicate that Gd5B2C5 compound is a suitable candidate for practical applications in magnetic refrigeration technology.
KW - Ferromagnetic
KW - Giant refrigeration capacity
KW - Magnetic refrigeration
KW - Magnetocaloric effect
UR - https://www.scopus.com/pages/publications/105035257773
U2 - 10.1016/j.cryogenics.2026.104345
DO - 10.1016/j.cryogenics.2026.104345
M3 - Article
AN - SCOPUS:105035257773
SN - 0011-2275
VL - 158
JO - Cryogenics
JF - Cryogenics
M1 - 104345
ER -