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分数量子霍尔液体中手征引力子模式的证据。

Evidence for chiral graviton modes in fractional quantum Hall liquids.

机构信息

School of Physics, National Laboratory of Solid State Microstructures, and Collaborative Innovation Center for Advanced Microstructures, Nanjing University, Nanjing, China.

Department of Physics, Columbia University, New York, NY, USA.

出版信息

Nature. 2024 Apr;628(8006):78-83. doi: 10.1038/s41586-024-07201-w. Epub 2024 Mar 27.

Abstract

Exotic physics could emerge from interplay between geometry and correlation. In fractional quantum Hall (FQH) states, novel collective excitations called chiral graviton modes (CGMs) are proposed as quanta of fluctuations of an internal quantum metric under a quantum geometry description. Such modes are condensed-matter analogues of gravitons that are hypothetical spin-2 bosons. They are characterized by polarized states with chirality of +2 or -2, and energy gaps coinciding with the fundamental neutral collective excitations (namely, magnetorotons) in the long-wavelength limit. However, CGMs remain experimentally inaccessible. Here we observe chiral spin-2 long-wavelength magnetorotons using inelastic scattering of circularly polarized lights, providing strong evidence for CGMs in FQH liquids. At filling factor v = 1/3, a gapped mode identified as the long-wavelength magnetoroton emerges under a specific polarization scheme corresponding to angular momentum S = -2, which persists at extremely long wavelength. Remarkably, the mode chirality remains -2 at v = 2/5 but becomes the opposite at v = 2/3 and 3/5. The modes have characteristic energies and sharp peaks with marked temperature and filling-factor dependence, corroborating the assignment of long-wavelength magnetorotons. The observations capture the essentials of CGMs and support the FQH geometrical description, paving the way to unveil rich physics of quantum metric effects in topological correlated systems.

摘要

奇异物理可能源于几何形状和相关性之间的相互作用。在分数量子霍尔(FQH)态中,人们提出了一种新的集体激发,称为手征引力子模式(CGM),作为量子几何描述下内部量子度量波动的量子。这些模式是凝聚态物质中引力子的类似物,是假设的自旋-2 玻色子。它们的特征是具有手征性 +2 或 -2 的极化状态,并且能量间隙与长波极限中的基本中性集体激发(即磁旋子)重合。然而,CGM 仍然无法通过实验来探测。在这里,我们使用圆偏振光的非弹性散射来观察手征自旋-2 长波磁旋子,为 FQH 液体中的 CGM 提供了强有力的证据。在填充因子 v = 1/3 下,在与角动量 S = -2 对应的特定极化方案下,出现了一个被识别为长波磁旋子的带隙模式,该模式在极长的波长下仍然存在。值得注意的是,在 v = 2/5 时模式的手征性仍然为 -2,但在 v = 2/3 和 3/5 时变为相反。这些模式具有特征能量和尖锐的峰值,具有明显的温度和填充因子依赖性,证实了长波磁旋子的分配。这些观察结果捕捉到了 CGM 的本质,并支持了 FQH 几何描述,为揭示拓扑相关系统中量子度量效应的丰富物理铺平了道路。

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