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CrSBr中超强耦合 regime下的磁场可调极化激元

Magnetic Field Tunable Polaritons in the Ultrastrong Coupling Regime in CrSBr.

作者信息

Nessi Luca, Occhialini Connor A, Demir Ahmet Kemal, Powalla Lukas, Comin Riccardo

机构信息

Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United States.

Max Planck Institute for Solid State Research, 70569 Stuttgart, Germany.

出版信息

ACS Nano. 2024 Dec 17;18(50):34235-34243. doi: 10.1021/acsnano.4c11799. Epub 2024 Dec 5.

DOI:10.1021/acsnano.4c11799
PMID:39639608
Abstract

Collective excitations of bound electron-hole pairs, i.e., excitons, are ubiquitous in condensed matter systems, and it has been shown that they can strongly couple to other degrees of freedom, such as spin, orbital, and lattice. Among van der Waals materials with pronounced excitonic responses, CrSBr has attracted significant interest due to a very large energy shift of its fundamental bright exciton (at 1.36 eV) under an external magnetic field. This effect has been associated with an increased interlayer electronic hopping when the magnetic order is switched from antiferromagnetic to ferromagnetic by an external magnetic field, enabling its optical detection. In this work, we report the observation of a second bright excitonic resonance (at 1.76 eV), displaying a 5-fold enhancement of the magnetically induced energy shift to ∼100 meV, which we associate to a decreased spatial localization and increased interband nature compared to the fundamental exciton. Moreover, we show how the light-matter interaction reaches the ultrastrong regime where this exciton hybridizes with the cavity modes of photons confined to CrSBr flakes, forming polaritons with a Rabi splitting of Ω ≃ 372 meV, of the same order of magnitude as the one reported for the first exciton. These results expand the understanding of the relationship between the optical response and band structure of CrSBr and clarify the essential ingredients for optimizing magneto-electronic coupling for applications.

摘要

束缚电子 - 空穴对的集体激发,即激子,在凝聚态物质系统中普遍存在,并且已经表明它们可以与其他自由度强烈耦合,例如自旋、轨道和晶格。在具有明显激子响应的范德华材料中,CrSBr因其在外部磁场下基本明亮激子(1.36 eV)的非常大的能量位移而引起了极大的兴趣。这种效应与当磁序通过外部磁场从反铁磁转变为铁磁时层间电子跳跃的增加有关,从而实现了其光学检测。在这项工作中,我们报告了观察到的第二个明亮激子共振(1.76 eV),其磁诱导能量位移增强了5倍,达到约100 meV,我们将其与基本激子相比空间局域化降低和带间性质增加联系起来。此外,我们展示了光与物质的相互作用如何达到超强 regime,其中这种激子与限制在CrSBr薄片中的光子腔模杂交,形成拉比分裂为Ω≃372 meV的极化激元,与报道的第一个激子的量级相同。这些结果扩展了对CrSBr光学响应与能带结构之间关系的理解,并阐明了优化磁电耦合以用于应用的基本要素。

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