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arXiv 2402.02477quant-phcond-mat.mes-hall
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拓扑保护的晶格费米子卡西米尔效应

Topologically protected Casimir effect for lattice fermions

C. W. J. Beenakker

AI总结:

本文提出用无费米子加倍障碍的欧几里得作用量局域离散化方法,避免晶格离散化破坏狄拉克锥拓扑保护,从而防止拓扑绝缘体中卡西米尔效应被指数抑制。

摘要:

电磁卡西米尔效应在拓扑绝缘体中有一个费米子对应物:无质量狄拉克费米子场的零点涨落介导了磁散射体之间的力。卡西米尔力对保持未配对狄拉克锥拓扑保护的无序不敏感。如果狄拉克方程被离散化,这种保护可能被破坏;如果在狄拉克点处打开一个能隙,将导致卡西米尔效应的指数抑制。在这里,我们展示了如何通过应用最近发展的欧几里得作用量的局域离散化来避免这种晶格伪影,该离散化不受哈密顿量局域离散化的费米子加倍障碍的影响。

英文摘要:

The electromagnetic Casimir effect has a fermionic counterpart in topological insulators: Zero-point fluctuations of a massless Dirac fermion field mediate a force between magnetic scatterers. The Casimir force is insensitive to disorder that preserves the topological protection of an unpaired Dirac cone. The protection may be broken if the Dirac equation is discretized, and an exponential suppression of the Casimir effect will result if a gap opens at the Dirac point. Here we show how this lattice artefact may be avoided, by applying a recently developed local discretization of the Euclidean action that does not suffer from the fermion-doubling obstruction of local discretizations of the Hamiltonian.

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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