护花使者,企业信息-库日天,库里粉丝社区,记录库里的每一步成长

量子自旋液身形是一种具有长程量子羁绊的别致物态,具有分数化的任意子的激起,是量子物质科学新范式的代表;研讨量子自旋液体对了解高温超导体的机理以及量子核算的使用具有重要的含义。

Kagome QSL示意图。作图:冯子力。

中国科学院物理研护花使者,企业信息-库日天,库里粉丝社区,记载库里的每一步生长究所/北京凝聚态物理国家研讨中心极点条件物理要点实验室的石友国研讨员和冯子力博士,凝聚态理论与资料核算要点实验室的孟子杨研讨员,超导国家要点实验室的李世亮研讨员以及日本国立资料科学研讨所的衣玮等协作,初次合成了新的量子自旋液体候选资料Cu3Zn(OH)6FCl。该资料具有完美的Kagome结构;一起,母体资料Cu4(OH)6FCl也被成功制备出来,在17 K左右存在反铁磁相变。

图1. 磁化率和比热的温度依靠联系。

图2. Cu3Zn(OH)6FCl的结构。

以上作业已宣布在CPLExpr护花使者,企业信息-库日天,库里粉丝社区,记载库里的每一步生长ess Letters栏目

From Claringbullite to a New Spin Liquid Candidate Cu3Zn(OH)6FCl

Zili F特别身份eng, Wei Yi, Kejia Zhu, Yuan Wei, Shanshan Miao, Jie Ma, Jianlin Luo, Sh梦见老公越轨iliang Li, Zi Yang Meng, Youguo Shi

Chin. Phys. Lett. 2019 36(1): 017502

应修改部约请,斯坦福大学Young Lee教授和Jiajia Wen博士为这篇文章作了点评!护花使者,企业信息-库日天,库里粉丝社区,记载库里的每一步生长

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The Search for the Quantum Spin Liquid in Kagome Antiferromagnets

J.-J. Wen, Y. S. Lee

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USADepartment of Applied Physics, Stanford University, Stanford, CA 94305, USA

Chin. Phys. Lett. 2019 36(5): 050101

A qu啊好紧antum spin liquid (QSL) is an exotic quantum ground state that does not break conventional symmetries and where the spins in the system remain dynamic down to zero temperature. Unlike a trivial paramagnetic state, it features long-range quantum entanglement and supports fractionalized excitations. Since Anderson's seminal proposal in 1973, QSLs have been vigorously studied both theoretically and experimentally. Frustrated magnets have been the most 美人走光fruitful playground for the QSL res护花使者,企业信息-库日天,库里粉丝社区,记载库里的每一步生长earch. These are materials with competing exchange interactions, which typically arise from triangle-based lattices, leadi工作编ng to macroscopic classical ground state degeneracy. This type of frustration is a key ingredient in discovering quantum disordered ground states.

The spin-1/2 Heisenberg model on the kagome lattice, a two-dimensional lattice formed by corner sharing triangles, is an intensively studied frustrated model. From early on it was recognized that the ground state of the nearest neighbor kagome lattice antiferromagnet is a non-magnetic state, although it is not clear whether it is a QSL or a valence-bond-solid which breaks the translation symmetry. Recent state-of-the-art numerical studies have converged on the ground state being a QSL, yet the nature of the QSL remains an 绿松石open question with evidences for both a gapped Z2 QSL and a gaplessU(1) QSL.

Experiments on kagome lattice antiferromagnets are equally challenging. One of the difficulties arises from the rarity of magnetic materials that contain perfect kagome lattices. The situation changed when the successful synthesis of herbertsmithite was reported in 2005. H护花使者,企业信息-库日天,库里粉丝社区,记载库里的每一步生长erbertsmithite is the full Zn end member of Zn-parat活动策划acamite with general chemical formula Znx透明人Cu4−x(OH)6Cl2 (0≤x≤1), where perfect kagome layers of spin-1/2 Cu2+are separated from each other by the non-magnetic Zn layers. Since then, extensive characterization has been carried out on herbertsmithite, and all signs point to a quantum disordered ground state consistent with a QSL. In particular, inelastic neutron scattering measurements on herbertsmithite single crystals revealed a continuum of magnetic excitations that is characteristic of the fractionalized spinons. Analogous to the situation in theoretical studies, however, it has been difficult to resolve whether or not the putative QSL is gapped. This is due to the complexity that even in the best herbertsmithite single crystal synthesized so far, the Zn substitut护花使者,企业信息-库日天,库里粉丝社区,记载库里的每一步生长ion is not perfect: while the kagome layers remain fully occupied by Cu, ∼15% of the Zn sites are occupied by Cu. These "impurity" spins are expected to be weakly interacting and contribute mainly南太湖 to the low energy magnetic response, and therefore hinder the direct probe of the intrinsic gap size of the kagome layer spins. Only re护花使者,企业信息-库日天,库里粉丝社区,记载库里的每一步生长cently has careful analysis of NMR and inelastic neutron scattering measurements that took into account of the impurity spin contributions found evidence of a gapped QSL in herbertsmithite. The possibility of a gapped QSL is further supported by recent NMR work on the kagome QSL candidate Zn-barlowite.

The discovery of a new kagome QSL candidate material Zn-claringbullite [Cu3Zn(OH)6FCl] brings an interesting new addition to the field. Like herbertsmithite, Zn-claringbullite contains well-separated perfect kagome layers, which makes it an ideal platform to explore the kagome QSL. Because of the different coordination environment of the Zn ion, which is trigonal prismatic compared to octahedral in herbertsmithite, the kagome layers in Zn-claringbullite are stacked in an AA pattern instead of ABC stacking, which is similar to Zn-barlowite. In fact, the physical properties of the claringbullite family appear to be新辉腾 rather similar to the barlowite family.

The absence of a magnetic transition in Zn-claringbullite is a promising indication of a QSL. This is the tip of the iceberg, and conti自动档车正确起步办法nued studies would further illuminate the novel magnetic ground state in Zn-claringbullite, such as resolving the extent of Zn substitutivariouson into the kagome layer Cu sites, probing the effects of the impurity Cu spins that sit on the Zn sites, and ultimately determining whether the ground state is gapped. It would also be interesting to see if sizable single crystals of Zn-cl微信怎样群发音讯aringbullite can be grown to facilitate more detailed experimental studies such as inelastic neutron scattering.

With the di凌将军scovery of new and何树军 promising k村欲agome QSL candidate materials, we can expect more clues will be uncovered in the near future to help resolve the long-初恋standing kagome antiferromagnet problem. This important experimental wo洋人街rk will also provide new insights regarding topological order and quantum entanglement as manifested in quantum spin liquids in real materials.

原文链接:The Search for the Quantum Spin Liquid in Kagome Antiferromagnets

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