石墨烯纳米片中亚晶格状态的不平衡

IF 1.1 Q3 PHYSICS, MULTIDISCIPLINARY Journal of Physics Communications Pub Date : 2023-09-01 DOI:10.1088/2399-6528/ad0022
H Yorikawa
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引用次数: 0

摘要

摘要利用紧密结合方法研究了石墨烯纳米片中π电子的能态。石墨烯是碳原子的二部晶格或蜂窝晶格。据报道,包含空位团簇的整个石墨烯纳米片的亚晶格不平衡Δ N由外边缘和内边缘的亚晶格不平衡组成,这是表征电子态的特征。在非零能态中,电子均匀地分布在亚晶格A和B之间,与Δ N的值无关。相比之下,零能态是∣Δ N∣折叠简并态,其中电子不均匀地分布在亚晶格A或亚晶格b上。偶尔,大型或特定的石墨烯纳米片具有大量的零能态,它们是非零能态和零能态的混合态。
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Sublattice imbalance of states in graphene nanoflakes
Abstract The energy states of π -electrons in a graphene nanoflake obtained from graphene, a well-known bipartite lattice or honeycomb lattice of carbon atoms, are studied using the tight-binding method. It is reported that the sublattice imbalance Δ N of the entire graphene nanoflake including vacancy clusters, which characterizes the electronic states, consists of those of the outer and inner edges. In nonzero-energy states, the electrons are evenly distributed between the sublattices A and B, regardless of the value of Δ N . In contrast, zero-energy states are ∣Δ N ∣-fold degenerate states where the electrons are unevenly distributed on either sublattice A or sublattice B. Occasionally, large or specific graphene nanoflakes have substantial zero-energy states, which are mixed states of the nonzero-energy states and zero-energy states.
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来源期刊
Journal of Physics Communications
Journal of Physics Communications PHYSICS, MULTIDISCIPLINARY-
CiteScore
2.60
自引率
0.00%
发文量
114
审稿时长
10 weeks
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