School of Physics, State Key Laboratory for Crystal Materials, Shandong University, Jinan 250100, People's Republic of China.
J Phys Chem A. 2011 Sep 8;115(35):9987-92. doi: 10.1021/jp109470r. Epub 2011 Aug 11.
On the basis of density functional theory (DFT) methods, we study the magnetic properties and electronic structures of the armchair (4, 4) and zigzag (8, 0) single-wall SiC nanotubes with various vacancies and boron substitution. The calculation results indicate that a Si vacancy could induce the magnetic moments in both armchair (4, 4) and zigzag (8, 0) single-wall SiC nanotubes, which mainly arise from the p orbital of C atoms surrounding Si vacancy, leading to the ferromagnetic coupling. However, a C vacancy could only bring about the magnetic moment in armchair (4, 4) single-wall SiC nanotube, which mainly originates from the polarization of Si p electrons, leading to the antiferromagnetic coupling. In addition, for both kinds of single-wall SiC nanotubes, magnetic moments can be induced by a boron atom substituting for C atom. When two boron atoms locate nearest neighbored, both kinds of single-wall Si(C, B) nanotubes exhibit antiferromagnetic coupling.
基于密度泛函理论(DFT)方法,我们研究了具有不同空位和硼取代的扶手椅(4,4)和锯齿(8,0)单壁碳化硅纳米管的磁性和电子结构。计算结果表明,硅空位可以在扶手椅(4,4)和锯齿(8,0)单壁碳化硅纳米管中诱导磁矩,主要来源于硅空位周围 C 原子的 p 轨道,导致铁磁耦合。然而,碳空位只能在扶手椅(4,4)单壁碳化硅纳米管中产生磁矩,主要源于 Si p 电子的极化,导致反铁磁耦合。此外,对于这两种单壁碳化硅纳米管,硼原子取代 C 原子可以诱导磁矩。当两个硼原子位于最近邻时,两种单壁 Si(C, B)纳米管都表现出反铁磁耦合。