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首页> 外文期刊>Physical review, B >Emergence of massless Dirac quasiparticles in correlated hydrogenated graphene with broken sublattice symmetry
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Emergence of massless Dirac quasiparticles in correlated hydrogenated graphene with broken sublattice symmetry

机译:亚质量的狄拉克准粒子在相关氢化石墨烯中的破坏与亚晶格对称性的出现

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Using the variational cluster approximation (VCA) and the cluster perturbation theory, we study the finite-temperature phase diagram of a half-depleted periodic Anderson model on the honeycomb lattice at half-filling for a model of graphone, i.e., single-side hydrogenated graphene. The ground state of this model is found to be ferromagnetic (FM) semimetal. The origin of this FM state is attributed to the instability of a flat band located at the Fermi energy in the noninteracting limit and is smoothly connected to the Lieb-Mattis-type ferromagnetism. The spin-wave dispersion in the FM state is linear in momentum at zero temperature but becomes quadratic at finite temperatures, implying that the FM state is fragile against thermal fluctuations. Indeed, our VCA calculations find that the paramagnetic (PM) state dominates the finite-temperature phase diagram. More surprisingly, we find that massless Dirac quasiparticles with the linear energy dispersion emerge at the Fermi energy upon introducing the electron correlation U at the impurity sites in the PM phase. The Dirac Fermi velocity is found to be highly correlated to the quasiparticle weight of the emergent massless Dirac quasiparticles at the Fermi energy and monotonically increases with U. These unexpected massless Dirac quasiparticles are also examined with the Hubbard-I approximation and the origin is discussed in terms of the spectral weight redistribution involving a large energy scale of U. Considering an effective quasiparticle Hamiltonian which reproduces the single-particle excitations obtained by the Hubbard-I approximation, we argue that the massless Dirac quasiparticles are protected by the electron correlation. Our finding therefore provides a unique example of the emergence of massless Dirac quasiparticles due to dynamical electron correlations without breaking any spatial symmetry. The experimental implications of our results for graphone as well as a graphene sheet on transition-metal substrates are also briefly discussed.
机译:利用变分簇近似(VCA)和簇扰动理论,研究了石墨烯(单面氢化)模型在半填充时蜂窝网格上半耗尽周期安德森模型的有限温度相图。石墨烯。发现该模型的基态是铁磁(FM)半金属。 FM状态的起因归因于位于非相互作用极限处位于费米能量处的平坦带的不稳定性,并且平滑地连接至利勃·马蒂斯型铁磁性。 FM状态下的自旋波色散在零温度下的动量呈线性,但在有限温度下变为二次方,这意味着FM状态易受热波动的影响。实际上,我们的VCA计算发现,顺磁(PM)状态主导着有限温度相图。更令人惊讶的是,我们发现,当在PM相的杂质位点引入电子相关U时,具有线性能量色散的无质量Dirac准粒子以费米能出现。发现狄拉克费米速度与费米能量处出现的无质量的狄拉克准粒子的拟粒子重量高度相关,并随U单调增加。这些意外的无质量狄拉克准粒子也用Hubbard-I近似进行了检验,并在考虑到大能量尺度的光谱重分布的术语。考虑到有效的准粒子哈密顿量,该哈密顿量再现了通过Hubbard-I近似获得的单粒子激发,我们认为无质量的狄拉克准粒子受到电子相关性的保护。因此,我们的发现提供了一个独特的例子,说明由于动态电子相关性而导致的无质量Dirac准粒子的出现,而没有破坏任何空间对称性。还简要讨论了我们的研究结果对过渡金属衬底上的石墨烯以及石墨烯片的实验意义。

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