压力诱导的结构和磁性顺序过渡在J1 - J2正方形格子反铁磁体AMoOPOCl (A = K,Rb) 中
Yuanhui Xu1, Rui Cui1, Hongping Jiang1
1Key Laboratory of Applied Chemistry, Yanshan University, Qinhuangdao 066004, P. R. China. xfhao@ysu.edu.cn.
Physical chemistry chemical physics : PCCP
|March 1, 2024
概括
我们研究了压力下的方格格子反铁磁体AMoOPO4Cl. 高压诱导结构转变,由于P3s轨道参与,改变柱状反铁磁顺序为Néel反铁磁顺序.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 量子磁力 量子磁力 量子磁力
背景情况:
- 方格格子反铁磁铁对于探索量子相非常重要.
- AMoOPO4Cl (A = K,Rb) 是量子相的潜在候选者.
- 了解他们在压力下的行为是关键.
研究的目的:
- 在压力下研究AMoOPO4Cl的电子和磁性特性.
- 确定结构和磁性排序进化.
- 阐明磁性顺序转换的机制.
主要方法:
- 一开始的密度函数理论计算.
- 包括电子相关性和范德瓦尔斯力.
- 分析状态密度和旋转密度等表面的密度.
主要成果:
- 柱状反铁磁排序是环境P4/nmm相的基本状态.
- 一个高压P4/n阶段解释了观察到的结构和磁性过渡.
- 过渡涉及P3s轨道激活铁磁超交换相互作用.
结论:
- P4/n阶段是适合AMoOPO4Cl.Cl的高压结构.
- 在压力下的磁交换合中,P3s轨道起着重要的作用.
- 这项工作加深了对正方形格子反铁磁体及其压力诱导过渡的理解.
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