Wang Qi, Zhang Zhilu, Huang Haicai, Song Xinyu, Bu Yuxiang
School of Chemistry and Chemical Engineering, Shandong University, Jinan 250100, P. R. China.
Phys Chem Chem Phys. 2022 Feb 9;24(6):3834-3843. doi: 10.1039/d1cp04597k.
The strain effect on the magnetic response of 2D materials as spintronic devices is always important in actual applications. Due to the intriguing electronic and magnetic properties of two-dimensional (2D) vanadium porphyrin (V-PP) sheets, we studied the strain-induced magnetic coupling changes in 2D V-PP sheets by using the density functional theory method and found intriguing magnetic variation characters. The calculated results indicate that biaxial strain can modulate the magnetic moments of the central transition metal vanadium atoms and more importantly can induce phase transitions among three magnetic modes with four magnetic states (ferromagnetic (FM), ferrimagnetic (FIM), and two antiferromagnetic (AFM: AFM1 featuring a parallel spin lattice AFM2 featuring a crossing spin lattice)) with unique conversion pathways due to their different responses to the strain. As the compressive strain increases, the magnetic characteristics of 2D-VPP transitions as FM → FIM → AFM1 with two critical points (-4.7% and -6%), while the tensile strain can induce the original FM coupling to transition to another AFM state (FM → AFM2) at 5.3%. Analyses of the density of states, spin densities, and Bader charges reveal that the rich magnetic response properties of the system originate from the electron transfer between the central V and the porphyrin ligand induced by strain. This work provides intriguing information regarding the strain-induced magnetic phase transition mechanism and also presents a viable development direction to design 2D porphyrin magnetic semiconductors and spintronic devices.
作为自旋电子器件,二维材料的应变效应在实际应用中对磁响应始终具有重要意义。由于二维钒卟啉(V-PP)片材具有引人入胜的电子和磁性特性,我们采用密度泛函理论方法研究了二维V-PP片材中应变诱导的磁耦合变化,并发现了有趣的磁变化特征。计算结果表明,双轴应变可以调节中心过渡金属钒原子的磁矩,更重要的是,由于三种磁模式对应变的不同响应,双轴应变可以诱导三种磁模式(具有四种磁态,即铁磁(FM)、亚铁磁(FIM)和两种反铁磁(AFM:AFM1具有平行自旋晶格,AFM2具有交叉自旋晶格))之间的相变,并具有独特的转变途径。随着压缩应变增加,二维VPP的磁特性在两个临界点(-4.7%和-6%)处从FM转变为FIM再转变为AFM1,而拉伸应变在5.3%时可诱导原始FM耦合转变为另一种AFM状态(FM→AFM2)。态密度、自旋密度和巴德电荷分析表明,该系统丰富的磁响应特性源于应变诱导的中心V与卟啉配体之间的电子转移。这项工作提供了关于应变诱导磁相变机制的有趣信息,也为设计二维卟啉磁性半导体和自旋电子器件提出了一个可行的发展方向。