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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Energy Dispersions and Minimal Conductivity of Bernal Multilayer Graphene
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Energy Dispersions and Minimal Conductivity of Bernal Multilayer Graphene

机译:Bernal多层石墨烯的能量色散和最小电导率

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In this work, we derive the analytical expression of the energy dispersions and minimal conductivity of the Bernal multilayer graphenes with the trigonal warping γ3 taken into consideration. Under unitary transformation, both the Hamiltonian matrix H and current operator partial deriv H/partial deriv k of an N-layer Bernal graphene can be exactly reduced to block diagonal matrices. As the layer number N is even (odd), the 2N X 2N matrix is decomposed into N/2 four by four blocks (one 2 x 2 and (N-1)/2 4 x 4 blocks). Each of the Hamiltonian blocks represents an independent subsystem, which is an equivalent bilayer or a monolayer graphene. The analytical expression of energy dispersions are then obtained. Most importantly, the minimal conductivity, based on the Kubo formula, of Bernal multilayer graphene is equal to the summation of the direct current conductivity of each subsystem. The analytical formula of minimal conductivity is (N/2) 2A/π (e~2/h) [4/π(e~2/h) + ((N - 1)/ 2)24/π(e~2/h)] for even (odd) N, where 24/π (e~2/h) is the conductivity of a bilayer graphene with trigonal warping [Phys. Rev. Lett. 2007, 99, 066802].
机译:在这项工作中,我们推导了考虑三角扭曲γ3的Bernal多层石墨烯的能量色散和最小电导率的解析表达式。在unit变换下,可以精确地减少哈密顿矩阵H和N层Bernal石墨烯的电流算子偏导数H /偏导数k,以阻塞对角矩阵。由于层数N为偶数(奇数),因此将2N X 2N矩阵分解为N / 2个四乘四块(一个2 x 2和(N-1)/ 2 4 x 4个块)。每个汉密尔顿块代表一个独立的子系统,它是等效的双层或单层石墨烯。然后获得能量色散的解析表达式。最重要的是,基于Kubo公式的Bernal多层石墨烯的最小电导率等于每个子系统的直流电导率之和。最小电导率的解析公式为(N / 2)2A /π(e〜2 / h)[4 /π(e〜2 / h)+((N-1)/ 2)24 /π(e〜2对于偶数(奇数)N,其中24 /π(e〜2 / h)是具有三角形翘曲的双层石墨烯的电导率。牧师2007,99,066802]。

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