临界指数
范德瓦尔斯力
凝聚态物理
磁化
铁磁性
Widom缩放
物理
居里温度
缩放比例
相变
顺磁性
重整化群
磁场
量子力学
数学
分子
几何学
作者
Tianyang Yao,W L Qubie,Pushpendra Kumar,Xu Bai,Shixin Hu,Desheng Xue,Junli Zhang
标识
DOI:10.1088/1361-648x/ad4d48
摘要
Abstract The critical behavior of the van der Waals ferromagnet Fe 3.8 GaTe 2 was systematically studied through measurements of isothermal magnetization, with the magnetic field applied along the c -axis. Fe 3.8 GaTe 2 undergoes a non-continuous paramagnetic to ferromagnetic phase transition at the Curie temperature T c ∼ 355 K. A comprehensive analysis of isotherms around T c utilizing the modified Arrott diagram, the Kouvel–Fisher method, the Widom scaling law, and the critical isotherm analysis yielded the critical exponent of β = 0.411, γ = 1.246, and δ = 3.99. These critical exponents are found to be self-consistent and align well with the scaling equation at high magnetic fields, underscoring the reliability and intrinsic nature of these parameters. However, the low-field data deviates from the scaling relation, exhibiting a vertical trend when T < T c . This discrepancy suggests the occurrence of a first-order phase transition in the crystal under a low magnetic field when T < T c . Mössbauer spectra were employed to provide insights into the critical behaviors of magnetic moments at different sites, including (Fe1)A, (Fe1)B, and Fe2. The results are consistent with the isothermal magnetization analysis. Additionally, the renormalization group theory analysis reveals that the spin coupling within the Fe 3.8 GaTe 2 crystal follows the three-dimensional Heisenberg ({d:n} = {3:3}) type with long-range magnetic and exchange interaction decays with a distance as J ( r ) ≈ r −4.80 .
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