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arXiv 1511.05282cond-mat.mes-hallcond-mat.str-el
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玻色狄拉克材料的蜂窝晶格颗粒超导体

Granular Superconductor in a honeycomb lattice as a realization of Bosonic Dirac Material

Saikat Banerjee, J. Fransson, A. M. Black-Schaffer, H. Ågren, A. V. Balatsky

摘要:

本文研究了二维颗粒状超导薄片中相位振荡的低能有效理论。使用石墨烯的例子,我们提出了工程狄拉克节点的玻色子激发的证据:集体玻色子模式的光谱在布里渊区的K和K点交叉,形成狄拉克节点。我们展示了如何获得两种不同类型的集体相位振荡,它们类似于两带超导体中的Leggett和Bogoliubov-Anderson-Gorkov模式。我们发现,狄拉克节点被保存在存在的晶粒间的相互作用,尽管诱导的两个集体模式的定性特征的变化。最后,通过为两个亚晶格选择不同的在位势来打破亚晶格对称性,导致狄拉克节点附近的能隙开口,类似于费米狄拉克材料。玻色子激发的狄拉克节点色散将传统狄拉克锥激发的讨论扩展到玻色子的情形。我们称这种情况为玻色子狄拉克材料(BDM)的代表,类似于文献中广泛讨论的费米狄拉克材料的情况。

英文摘要:

We examine the low energy effective theory of phase oscillations in a two-dimensional granular superconducting sheet where the grains are arranged in honeycomb lattice structure. Using the example of graphene we present the evidence for the engineered Dirac nodes in the bosonic excitations: the spectra of the collective bosonic modes cross at the K and K points in the Brillouin zone and form Dirac nodes. We show how two different types of collective phase oscillations are obtained and that they are analogous to the Leggett and the Bogoliubov-Anderson-Gorkov modes in a two-band superconductor. We show that the Dirac node is preserved in the presence of an inter-grain interaction, despite induced changes of the qualitative features of the two collective modes. Finally, breaking the sublattice symmetry by choosing different on-site potentials for the two sublattices leads to a gap opening near the Dirac node, in analogy with Fermionic Dirac materials. Dirac node dispersion of bosonic excitations is thus expanding the discussion of the conventional Dirac cone excitations to the case of bosons. We call this case as a representative of Bosonic Dirac Materials (BDM), similar to the case of Fermionic Dirac materials extensively discussed in the literature.

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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