Datta Soumendu, Kaphle Gopi Chandra, Baral Sayan, Mookerjee Abhijit
Department of Condensed Matter Physics and Material Sciences, S.N. Bose National Centre for Basic Sciences, JD Block, Sector-III, Salt Lake City, Kolkata 700 098, India.
Central Department of Physics, Tribhuvan University, Kathmandu, Nepal.
J Chem Phys. 2015 Aug 28;143(8):084309. doi: 10.1063/1.4929510.
Using density functional theory (DFT) based electronic structure calculations, the effects of morphology of semiconducting nanostructures on the magnetic interaction between two magnetic dopant atoms as well as a possibility of tuning band gaps have been studied in the case of the bi-doped (ZnO)24 nanostructures with the impurity dopant atoms of the 3d late transition metals-Mn, Fe, Co, Ni, and Cu. To explore the morphology effect, three different structures of the host (ZnO)24 nano-system, having different degrees of spatial confinement, have been considered: a two dimensional nanosheet, a one dimensional nanotube, and a finite cage-shaped nanocluster. The present study employs hybrid density functional theory to accurately describe the electronic structure of all the systems. It is shown here that the magnetic coupling between the two dopant atoms remains mostly anti-ferromagnetic in the course of changing the morphology from the sheet geometry to the cage-shaped geometry of the host systems, except for the case of energetically most stable bi-Mn doping, which shows a transition from ferromagnetic to anti-ferromagnetic coupling with decreasing aspect ratio of the host system. The effect of the shape change, however, has a significant effect on the overall band gap variations of both the pristine as well as all the bi-doped systems, irrespective of the nature of the dopant atoms and provides a means for easy tunability of their optoelectronic properties.
利用基于密度泛函理论(DFT)的电子结构计算方法,研究了半导体纳米结构的形态对两个磁性掺杂原子之间磁相互作用的影响,以及在具有3d晚期过渡金属(Mn、Fe、Co、Ni和Cu)杂质掺杂原子的双掺杂(ZnO)24纳米结构中调节带隙的可能性。为了探究形态效应,考虑了主体(ZnO)24纳米体系的三种不同结构,它们具有不同程度的空间限制:二维纳米片、一维纳米管和有限的笼状纳米团簇。本研究采用杂化密度泛函理论来精确描述所有体系的电子结构。结果表明,在主体体系从片状几何形态转变为笼状几何形态的过程中,两个掺杂原子之间的磁耦合大多保持反铁磁性,但能量上最稳定的双Mn掺杂情况除外,它随着主体体系纵横比的减小呈现出从铁磁耦合到反铁磁耦合的转变。然而,形状变化对原始体系以及所有双掺杂体系的整体带隙变化都有显著影响,与掺杂原子的性质无关,并为其光电性质的轻松调节提供了一种手段。