The effect of hydrogen bonding on the magnetism quantum behavior of doped Co-MOFs

IF 3.5 3区 化学 Q2 CHEMISTRY, INORGANIC & NUCLEAR Journal of Solid State Chemistry Pub Date : 2025-02-02 DOI:10.1016/j.jssc.2025.125207
Zhenjun Fan , Haoming Ning , Zhenyu Mi , Zhilin Xu , Tianyi Gao , Zhirui Sun , Xiaohui Song
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Abstract

In this paper, the low temperature magnetic behavior of doped Co based metal-organic frameworks (MOFs) single-crystals [(CH3)2NH2]Co1-xMx[HCOO]3 (DMCo1-xMxF) with M = Mg, Zn, Mn, Ni and x = 0.1–0.5 were systematically investigated. It was found that the long-range interactions between magnetic ions were effectively modulated by the type of doping ions, with antiferromagnetic phase transition temperature of 18.5 K for DMCo0.8Ni0.2F, 13.5 K for DMCo0.8Mn0.2F, 14.5 K for DMCo0.9Zn0.1F and 12 K for DMCo0.7Mg0.3F. Abnormally large coercive fields and hysteresis loss in Mg- or Zn- doping samples reveal the existence of single-ion quantum magnets in Co-based MOFs after non-magnetic doping. The coexistence of both long-range magnetic order and individual single-ion quantum magnets was further confirmed by quantum step behavior observed in the low-temperature hysteresis loop for non-magnetic doping (Mg, Zn) samples. A systematic analysis of the changes in bond length, bond angle, and vibrational spectrum of the samples indicates that the enhancement of hydrogen bonding is beneficial for increasing the anisotropy of magnetic single ions, leading to an increase in magnetic hysteresis and coercive fields, exhibiting quantum tunneling behavior of magnetic single ions. For the magnetic doping (Mn, Ni) samples, complex magnetic behavior is exhibited due to competition between magnetic ions. Our research indicates that doping can effectively regulate the quantum behavior of magnetic ions. The strength of hydrogen bonds has a significantly impacts on spin reversal and interactions.

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氢键对掺杂Co-MOFs磁性量子行为的影响
本文系统研究了M = Mg, Zn, Mn, Ni, x = 0.1-0.5掺杂Co基金属有机骨架(MOFs) [(CH3)2NH2]Co1-xMx[HCOO]3 (DMCo1-xMxF)单晶[(CH3)2NH2]的低温磁性行为。结果表明:DMCo0.8Ni0.2F的反铁磁相变温度为18.5 K, DMCo0.8Mn0.2F的反铁磁相变温度为13.5 K, DMCo0.9Zn0.1F的反铁磁相变温度为14.5 K, DMCo0.7Mg0.3F的反铁磁相变温度为12 K。Mg或Zn掺杂样品中存在异常大的矫顽力场和磁滞损失,表明非磁性掺杂后co基mof中存在单离子量子磁体。在非磁掺杂(Mg, Zn)样品的低温磁滞回线中观察到的量子阶跃行为进一步证实了长程磁序和单个单离子量子磁体的共存。系统分析了样品的键长、键角和振动谱的变化,表明氢键的增强有利于磁性单离子各向异性的增加,导致磁滞和矫顽力场的增加,表现出磁性单离子的量子隧穿行为。对于磁性掺杂(Mn, Ni)样品,由于磁性离子之间的竞争,表现出复杂的磁性行为。我们的研究表明,掺杂可以有效地调节磁性离子的量子行为。氢键强度对自旋反转和相互作用有显著影响。
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来源期刊
Journal of Solid State Chemistry
Journal of Solid State Chemistry 化学-无机化学与核化学
CiteScore
6.00
自引率
9.10%
发文量
848
审稿时长
25 days
期刊介绍: Covering major developments in the field of solid state chemistry and related areas such as ceramics and amorphous materials, the Journal of Solid State Chemistry features studies of chemical, structural, thermodynamic, electronic, magnetic, and optical properties and processes in solids.
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