Kauch A, Pudleiner P, Astleithner K, Thunström P, Ribic T, Held K
Institute of Solid State Physics, TU Wien, 1040 Vienna, Austria.
Institute of Theoretical and Computational Physics, Graz University of Technology, 8010 Graz, Austria.
Phys Rev Lett. 2020 Jan 31;124(4):047401. doi: 10.1103/PhysRevLett.124.047401.
The interaction of light with solids gives rise to new bosonic quasiparticles, with the exciton being-undoubtedly-the most famous of these polaritons. While excitons are the generic polaritons of semiconductors, we show that for strongly correlated systems another polariton is prevalent-originating from the dominant antiferromagnetic or charge density wave fluctuations in these systems. As these are usually associated with a wave vector (π,π,…) or close to it, we propose to call the derived polaritons π-tons. These π-tons yield the leading vertex correction to the optical conductivity in all correlated models studied: the Hubbard, the extended Hubbard model, the Falicov-Kimball, and the Pariser-Parr-Pople model, both in the insulating and in the metallic phase.
光与固体的相互作用产生了新的玻色子准粒子,其中激子无疑是这些极化激元中最著名的。虽然激子是半导体的一般极化激元,但我们表明,对于强关联系统,另一种极化激元很普遍——它源于这些系统中占主导地位的反铁磁或电荷密度波涨落。由于这些通常与波矢(π,π,…)或接近它的波矢相关联,我们建议将导出的极化激元称为π子。在所有研究的关联模型中:哈伯德模型、扩展哈伯德模型、法利科夫-金布尔模型和帕里泽-帕尔-波普尔模型,无论是在绝缘相还是金属相中,这些π子都对光导率产生主要的顶点修正。