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正方- Kagome晶格反铁磁体中的无隙自旋液体

Gapless spin liquid in a square-kagome lattice antiferromagnet.

作者信息

Fujihala Masayoshi, Morita Katsuhiro, Mole Richard, Mitsuda Setsuo, Tohyama Takami, Yano Shin-Ichiro, Yu Dehong, Sota Shigetoshi, Kuwai Tomohiko, Koda Akihiro, Okabe Hirotaka, Lee Hua, Itoh Shinichi, Hawai Takafumi, Masuda Takatsugu, Sagayama Hajime, Matsuo Akira, Kindo Koichi, Ohira-Kawamura Seiko, Nakajima Kenji

机构信息

Tokyo University of Science, Department of Physics, Tokyo, 162-8601, Japan.

Tokyo University of Science, Department of Applied Physics, Tokyo, 125-8585, Japan.

出版信息

Nat Commun. 2020 Jul 9;11(1):3429. doi: 10.1038/s41467-020-17235-z.

DOI:10.1038/s41467-020-17235-z
PMID:32647219
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7347939/
Abstract

Observation of a quantum spin liquid (QSL) state is one of the most important goals in condensed-matter physics, as well as the development of new spintronic devices that support next-generation industries. The QSL in two dimensional quantum spin systems is expected to be due to geometrical magnetic frustration, and thus a kagome-based lattice is the most probable playground for QSL. Here, we report the first experimental results of the QSL state on a square-kagome quantum antiferromagnet, KCuAlBiO(SO)Cl. Comprehensive experimental studies via magnetic susceptibility, magnetisation, heat capacity, muon spin relaxation (μSR), and inelastic neutron scattering (INS) measurements reveal the formation of a gapless QSL at very low temperatures close to the ground state. The QSL behavior cannot be explained fully by a frustrated Heisenberg model with nearest-neighbor exchange interactions, providing a theoretical challenge to unveil the nature of the QSL state.

摘要

观测量子自旋液体(QSL)态是凝聚态物理领域最重要的目标之一,同时对于支持下一代产业的新型自旋电子器件的发展也至关重要。二维量子自旋系统中的QSL预计源于几何磁阻挫,因此基于 Kagome 的晶格是QSL最有可能出现的体系。在此,我们报道了在正方 Kagome 量子反铁磁体 KCuAlBiO(SO)Cl 上关于QSL态的首个实验结果。通过磁化率、磁化强度、热容量、μ子自旋弛豫(μSR)和非弹性中子散射(INS)测量进行的全面实验研究表明,在非常接近基态的低温下形成了无隙QSL。具有最近邻交换相互作用的阻挫海森堡模型无法完全解释QSL行为,这为揭示QSL态的本质带来了理论挑战。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/9f1273d7c065/41467_2020_17235_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/ebf183335151/41467_2020_17235_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/070a5973ca17/41467_2020_17235_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/5742d9e4b120/41467_2020_17235_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/f711d440d2d1/41467_2020_17235_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/9f1273d7c065/41467_2020_17235_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/ebf183335151/41467_2020_17235_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/070a5973ca17/41467_2020_17235_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/5742d9e4b120/41467_2020_17235_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/f711d440d2d1/41467_2020_17235_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0766/7347939/9f1273d7c065/41467_2020_17235_Fig5_HTML.jpg

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本文引用的文献

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探测人工量子磁体中的共振价键态。
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