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从有序到无序:稀三角晶格BaCoNbO的磁相演变

From order to disorder: magnetic phase evolution of diluted triangular lattice BaCoNbO.

作者信息

N Akhil, Ranaut Dheeraj, Channarayappa Sharath Kumar, Jaiswal-Nagar D

机构信息

School of Physics, IISER Thiruvananthapuram, Vithura, Thiruvananthapuram 695551, India.

出版信息

J Phys Condens Matter. 2025 Jul 31;37(31). doi: 10.1088/1361-648X/adf36a.

DOI:10.1088/1361-648X/adf36a
PMID:40701170
Abstract

Magnetic lattice dilution in geometrically frustrated systems provides a platform to investigate the presence of unconventional magnetic phases as the dilution is expected to destabilize the conventional magnetic order and creates randomness in exchange interactions. In this context, we have investigated the impact of non-magnetic Zndoping on an effective spin ()-½ geometrically frustrated triangular lattice BaCoNbO. The successful formation of pure single phase and preservation of crystal symmetry is confirmed via x-ray diffraction studies. Magnetic susceptibility measurements confirm the persistence of= ½ state, along with the suppression of antiferromagnetic (AFM) ordering with the critical concentration (= 0.4) corresponding to disordered state. This transition from AFM to disordered state above= 0.4 is further confirmed from isothermal magnetization (()). Along with this, a field-induced transition identical to a spin-flop transition is observed in the saturation region of() curves which become more dominant for higher concentration. The dilution of magnetic lattice results in randomness in exchange interactions with reduced AFM coupling between the spins which lowers the energy barrier for spin reorientation and gives rise to these unique spin-flop transitions. Our results highlight the role of magnetic dilution in tuning the balance between frustration and exchange interactions, offering insight into such field-driven behavior of quantum magnets.

摘要

在几何阻挫系统中进行磁晶格稀释提供了一个平台,用于研究非常规磁相的存在,因为预计稀释会破坏传统磁序并在交换相互作用中产生随机性。在此背景下,我们研究了非磁性锌掺杂对有效自旋()-½几何阻挫三角晶格BaCoNbO的影响。通过X射线衍射研究证实了纯单相的成功形成和晶体对称性的保持。磁化率测量证实了= ½态的持续存在,同时反铁磁(AFM)序随对应无序态的临界浓度(= 0.4)而受到抑制。从等温磁化(())进一步证实了在= 0.4以上从AFM到无序态的这种转变。除此之外,在()曲线的饱和区域观察到与自旋翻转转变相同的场致转变,对于更高浓度,这种转变更为显著。磁晶格的稀释导致交换相互作用的随机性,自旋之间的AFM耦合减弱降低了自旋重新取向的能垒,并产生了这些独特的自旋翻转转变。我们的结果突出了磁稀释在调节阻挫和交换相互作用之间平衡方面的作用,为量子磁体的这种场驱动行为提供了见解。

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