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arXiv 0908.3371cond-mat.mes-hallcond-mat.mtrl-sci
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双层石墨烯中的栅极可调带隙

Gate-tunable bandgap in bilayer graphene

L. A. Falkovsky

摘要:

双层石墨烯的紧束缚模型用于找到导带和价带之间的间隙,作为栅极电压和施主或受主掺杂的函数。总Hartree能量最小化,并得到了方程的间隙。这个能隙与化学势之比的方程只由屏蔽常数决定。因此,在不存在施主或受主的情况下,间隙与栅极电压或载流子浓度严格成比例。在相反的情况下,当存在施主或受主时,间隙在栅极偏压的电子和空穴侧上表现出不对称行为。与Kuzmenko等人的实验数据的比较表明,良好的协议。

英文摘要:

The tight-binding model of bilayer graphene is used to find the gap between the conduction and valence bands, as a function of both the gate voltage and as the doping by donors or acceptors. The total Hartree energy is minimized and the equation for the gap is obtained. This equation for the ratio of the gap to the chemical potential is determined only by the screening constant. Thus the gap is strictly proportional to the gate voltage or the carrier concentration in the absence of donors or acceptors. In the opposite case, where the donors or acceptors are present, the gap demonstrates the asymmetrical behavior on the electron and hole sides of the gate bias. A comparison with experimental data obtained by Kuzmenko et al demonstrates the good agreement.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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