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作 者:Yuming Yang Baohua Teng 杨宇明;滕保华(School of Physics,University of Electronic Science and Technology of China;School of Mathematical Sciences,University of Electronic Science and Technology of China)
机构地区:[1]School of Physics,University of Electronic Science and Technology of China,Chengdu 610054,China [2]School of Mathematical Sciences,University of Electronic Science and Technology of China,Chengdu 611731,China
出 处:《Chinese Physics B》2018年第10期508-511,共4页中国物理B(英文版)
摘 要:In this paper the percolation behavior with a specific concentration of the defects was discussed on the twodimensional graphene lattice. The percolation threshold is determined by a numerical method with a high degree of accuracy. This method is also suitable for locating the percolation critical point on other crystalline structures. Through investigating the evolution of the largest cluster size and the cluster sizes distribution, we find that under various lattice sizes and concentrations of pentagon-heptagon defects there is no apparent change for the percolation properties in graphene lattice.In this paper the percolation behavior with a specific concentration of the defects was discussed on the twodimensional graphene lattice. The percolation threshold is determined by a numerical method with a high degree of accuracy. This method is also suitable for locating the percolation critical point on other crystalline structures. Through investigating the evolution of the largest cluster size and the cluster sizes distribution, we find that under various lattice sizes and concentrations of pentagon-heptagon defects there is no apparent change for the percolation properties in graphene lattice.
关 键 词:PERCOLATION GRAPHENE pentagon-heptagon defect CONCENTRATION
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