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Native Point Defects in Monolayer Hexagonal Boron Phosphide from First Principles
Journal of Electronic Materials ( IF 2.2 ) Pub Date : 2020-08-09 , DOI: 10.1007/s11664-020-08357-7
Zijiang Luo , Yuandong Ma , Xiuzhang Yang , Bing Lv , Zhibin Gao , Zhao Ding , Xuefei Liu

In this paper, we have investigated the electronic and magnetic properties of four types of native defects under neutral and charged states in a hexagonal boron phosphide (h-BP) monolayer, including boron vacancy (\( V_{\rm{B}} ) \), phosphorus vacancy (\( V_{\rm{P}} ) \), boron on the phosphorus site (\( B_{\rm{P}} ) \) and phosphorus on the boron site (\( P_{\rm{B}} ) \) within the framework of the density functional theory. For the four types of defects, various charge states were investigated, and only 0 and 1 + charge states for all defects are stable within the electronic chemical potential range (i.e. Fermi level range). It is found that \( B_{\rm{P}} \) with the smallest defect formation energy is the most stable defect under both phosphorus-rich and -poor conditions in the whole range of electronic chemical potential. \( V_{\rm{P}} \) and \( P_{\rm{B}} \) are found to be shallow donors (i.e. 1 +/0) but could not be effectively introduced into the h-BP monolayer due to a rather high formation energy, while \( V_{\rm{B}} \) and \( B_{\rm{P}} \) are found to be holes trap centers. Especially, \( B_{\rm{P}} \) with a low defect formation energy, will be produced easily and seriously affect the p-type doping efficiency and conductivity of h-BP. Additionally, \( V_{\rm{B}} \) and \( V_{\rm{P}} \) induce a nonzero magnetic moment while \( P_{\rm{B}} \) and \( B_{\rm{P}} \) show non-magnetic nature in the h-BP monolayer.



中文翻译:

从第一原理的单层六方磷化硼的自然点缺陷。

在本文中,我们研究了六角形磷化硼(h-BP)单层中性和带电状态下四种类型的天然缺陷的电子和磁性,包括硼空位(\(V _ {\ rm {B}}) \),磷空位(\(V _ {\ rm {P}})\),磷位点上的硼(\(B _ {\ rm {P}})\)和硼位点上的磷(\(P_ { \ rm {B}})\)在密度泛函理论的框架内。对于四种类型的缺陷,研究了各种电荷状态,并且所有缺陷的仅0和1 +电荷状态在电子化学势范围(即费米能级范围)内稳定。发现\(B _ {\ rm {P}} \)在整个电子化学势范围内,具有最小缺陷形成能的元素在富磷和贫磷条件下都是最稳定的缺陷。发现\(V _ {\ rm {P}} \)\(P _ {\ rm {B}} \)是浅的供体(即1 + / 0),但不能有效地引入h-BP单层由于相当高的地层能量,发现\(V _ {\ rm {B}} \)\(B _ {\ rm {P}} \)是空穴陷阱的中心。特别是,容易产生缺陷形成能量低的\(B _ {\ rm {P}} \),并且严重影响h-BP的p型掺杂效率和电导率。此外,\(V _ {\ rm {B}} \)\(V _ {\ rm {P}} \)感应非零磁矩,而\(P _ {\ rm {B}} \)\(B _ {\ rm {P}} \)在h-BP单层中显示非磁性。

更新日期:2020-08-10
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