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全光非平衡途径稳定烧绿石型 iridates 中的磁 Weyl 半金属。

All-optical nonequilibrium pathway to stabilising magnetic Weyl semimetals in pyrochlore iridates.

机构信息

Max Planck Institute for the Structure and Dynamics of Matter, Center for Free Electron Laser Science, 22761, Hamburg, Germany.

Department of Physics, North Carolina State University, Raleigh, 27695-8202, NC, USA.

出版信息

Nat Commun. 2018 Oct 26;9(1):4452. doi: 10.1038/s41467-018-06991-8.

DOI:10.1038/s41467-018-06991-8
PMID:30367073
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6203748/
Abstract

Nonequilibrium many-body dynamics is becoming a central topic in condensed matter physics. Floquet topological states were suggested to emerge in photodressed bands under periodic laser driving. Here we propose a viable nonequilibrium route without requiring coherent Floquet states to reach the elusive magnetic Weyl semimetallic phase in pyrochlore iridates by ultrafast modification of the effective electron-electron interaction with short laser pulses. Combining ab initio calculations for a time-dependent self-consistent light-reduced Hubbard U and nonequilibrium magnetism simulations for quantum quenches, we find dynamically modified magnetic order giving rise to transiently emerging Weyl cones that can be probed by time- and angle-resolved photoemission spectroscopy. Our work offers a unique and realistic pathway for nonequilibrium materials engineering beyond Floquet physics to create and sustain Weyl semimetals. This may lead to ultrafast, tens-of-femtoseconds switching protocols for light-engineered Berry curvature in combination with ultrafast magnetism.

摘要

非平衡多体动力学正成为凝聚态物理的一个核心课题。在周期性激光驱动下,光调制能带中出现了 Floquet 拓扑状态。在这里,我们提出了一种可行的非平衡途径,无需相干 Floquet 态,通过超快改变有效电子-电子相互作用,用短激光脉冲即可在烧绿石型铱酸盐中达到难以捉摸的磁 Weyl 半金属相。通过对含时自洽光还原 Hubbard U 的第一性原理计算和量子猝灭的非平衡磁模拟的结合,我们发现动态修正的磁序导致瞬时出现的 Weyl 锥,其可以通过时间和角度分辨光发射谱进行探测。我们的工作为非平衡材料工程提供了一个独特的、现实的途径,超越了 Floquet 物理,以创造和维持 Weyl 半金属。这可能会导致超快、几十飞秒的切换协议,用于用光工程设计 Berry 曲率,结合超快磁学。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/a47a466ab350/41467_2018_6991_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/be7e95d8ce9b/41467_2018_6991_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/62e32665095b/41467_2018_6991_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/f0ee60f17eff/41467_2018_6991_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/a47a466ab350/41467_2018_6991_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/be7e95d8ce9b/41467_2018_6991_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/62e32665095b/41467_2018_6991_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/f0ee60f17eff/41467_2018_6991_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ebf4/6203748/a47a466ab350/41467_2018_6991_Fig4_HTML.jpg

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