ITEP, B Cheremushkinskaya street 25, Moscow 117218, Russia and Institute for Theoretical Problems of Microphysics, Moscow State University, Moscow 119899, Russia.
Phys Rev Lett. 2013 Aug 2;111(5):056801. doi: 10.1103/PhysRevLett.111.056801. Epub 2013 Jul 30.
We report on the results of the first-principles numerical study of spontaneous breaking of chiral (sublattice) symmetry in suspended monolayer graphene due to electrostatic interaction, which takes into account the screening of Coulomb potential by electrons on σ orbitals. In contrast to the results of previous numerical simulations with unscreened potential, we find that suspended graphene is in the conducting phase with unbroken chiral symmetry. This finding is in agreement with recent experimental results by the Manchester group [D. C. Elias et al., Nat. Phys. 7, 701 (2011); A. S. Mayorov et al., Nano Lett. 12, 4629 (2012)]. Further, by artificially increasing the interaction strength, we demonstrate that suspended graphene is quite close to the phase transition associated with spontaneous chiral symmetry breaking, which suggests that fluctuations of chirality and nonperturbative effects might still be quite important.
我们报告了基于第一性原理的数值研究结果,该研究探讨了由于静电相互作用导致悬浮单层石墨烯中手性(亚晶格)对称性自发破缺的现象,其中考虑了 σ 轨道上电子对库仑势的屏蔽。与之前未屏蔽势的数值模拟结果相反,我们发现悬浮石墨烯处于手性对称性未破缺的导电相。这一发现与曼彻斯特小组的最近实验结果一致[D. C. Elias 等人,Nat. Phys. 7, 701(2011);A. S. Mayorov 等人,Nano Lett. 12, 4629(2012)]。此外,通过人为地增加相互作用强度,我们证明悬浮石墨烯非常接近与手性对称性自发破缺相关的相变,这表明手性涨落和非微扰效应可能仍然非常重要。