First-Principles Study of Defected Single Layer Hexagonal Boron-Nitride (h-BN)

H. K. Neupane, N. Adhikari
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Abstract

The novel properties of pristine h-BN, oxygen (O) atom impurity defects in h-BN (h-B(N-O) and h-(B-O)N), one boron (1B) atom vacancy defect in h-BN (h-BN_1B) and one nitrogen (1N) atom vacancy defect in h-BN (h-BN_1N) materials are investigated by spin-polarized density functional theory (DFT) using computational tool Quantum ESPRESSO. We found that they are stable materials. From the band structure calculations, we found that all the considered systems are wide bandgap materials. The bandgap energy of pristine h-BN, impurity defects h-B(N-O) and h-(B-O)N, and vacancy defects h-BN_1B and h-BN_1Nmaterials have values 4.98 eV, 4.19 eV& 2.47 eV,and 4.84 eV& 3.62 eV respectively. Also, it is found that h-B(N-O) and h-BN_1N materials have n-type Schottky contact while h-(B-O)N and h-BN_1B materials have p-type Schottky contact. From the analysis ofdensity of states (DOS) and partial density of states (PDOS) calculations, we found that non-magnetic pristine h-BN changes to magnetic h-B(N-O) andh-(B-O)N materials due to presence of impurity defects,and h-BN_1B andh-BN_1N materials due to presence of vacancy defects. Magnetic moments of h-B(N-O), h-(B-O)N, h-BN_1B and h-BN_1N materials are 1.00 µB/cell, 0.94 µB/cell, 3.00 µB/cell and 1.00 µB/cell respectively. They are obtained due to unpaired up and down spins state of electrons in 2p orbital of B and N atoms in the structures.
缺陷单层六方氮化硼(h-BN)的第一性原理研究
利用量子ESPRESSO计算工具,利用自旋极化密度泛函理论(DFT)研究了原始h- bn、h- bn中氧(O)原子杂质缺陷(h- b (N-O)和h-(B-O)N)、h- bn中一个硼(1B)原子空位缺陷(h- bn_1b)和h- bn (h- bn_1n)材料中一个氮(1N)原子空位缺陷(h- bn_1n)的新性质。我们发现它们是稳定的材料。从带结构计算中,我们发现所有考虑的系统都是宽带隙材料。原始h- bn、杂质缺陷h- b (N- o)和h-(B-O)N、空位缺陷h- bn_1b和h- bn_1n材料的能带能分别为4.98 eV、4.19 eV和2.47 eV、4.84 eV和3.62 eV。h- b (N- o)和h- bn_1n材料具有N型肖特基接触,h-(B-O)N和h- bn_1b材料具有p型肖特基接触。通过对态密度(DOS)和偏态密度(PDOS)计算的分析,我们发现,由于杂质缺陷的存在,非磁性原始h-BN转变为磁性h-B(N- o)和h-(B-O)N材料,以及由于空位缺陷的存在,h-BN_1B和h- bn_1n材料。h-B(N- o)、h-(B- o)N、h- bn_1b和h- bn_1n材料的磁矩分别为1.00µB/cell、0.94µB/cell、3.00µB/cell和1.00µB/cell。它们是由于结构中B和N原子的2p轨道上电子的不成对的上下自旋状态而得到的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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