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      Spin-lattice decoupling in a triangular-lattice quantum spin liquid

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          Abstract

          A quantum spin liquid (QSL) is an exotic state of matter in condensed-matter systems, where the electron spins are strongly correlated, but conventional magnetic orders are suppressed down to zero temperature because of strong quantum fluctuations. One of the most prominent features of a QSL is the presence of fractionalized spin excitations, called spinons. Despite extensive studies, the nature of the spinons is still highly controversial. Here we report magnetocaloric-effect measurements on an organic spin-1/2 triangular-lattice antiferromagnet, showing that electron spins are decoupled from a lattice in a QSL state. The decoupling phenomena support the gapless nature of spin excitations. We further find that as a magnetic field is applied away from a quantum critical point, the number of spin states that interact with lattice vibrations is strongly reduced, leading to weak spin–lattice coupling. The results are compared with a model of a strongly correlated QSL near a quantum critical point.

          Abstract

          A number of materials have been proposed as realizations of exotic quantum spin liquids but many important properties are difficult to establish. Isono et al. show evidence for spin-lattice decoupling in an organic material, which may help resolve conflicting results about the existence of a spin-excitation gap.

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          Resonating valence bonds: A new kind of insulator?

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            Fractionalized excitations in the spin liquid state of a kagom\'{e} lattice antiferromagnet

            New physics can emerge in magnetic materials where quantum fluctuations are enhanced due to reduced dimensionality and strong frustration. One long sought example is the resonating-valence-bond (RVB) state, where atomic magnetic moments are strongly correlated but do not order or freeze even in the limit of T -> 0. The RVB ground state does not break conventional symmetries, such as lattice translation or spin-rotation. The realization of such a quantum spin liquid in two-dimensions would represent a new state of matter. It is believed that spin liquid physics plays a role in the phenomenon of high-Tc superconductivity, and the topological properties of the spin liquid state may have applications in the field of quantum information. We present neutron scattering measurements of the spin excitations on single crystal samples of the spin-1/2 kagom\'{e} lattice antiferromagnet ZnCu3(OD)6Cl2 (also called herbertsmithite). Our observation of a spinon continuum in a two-dimensional magnet is remarkable first. The results serve as a key fingerprint of the quantum spin liquid state in herbertsmithite.
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              Spin Liquid State in an Organic Mott Insulator with Triangular Lattice

              \(^{1}\)H NMR and static susceptibility measurements have been performed in an organic Mott insulator with nearly isotropic triangular lattice, \(\kappa\)-(BEDT-TTF)\(_{2}\)Cu\(_{2}\)(CN)\(_{3}\), which is a model system of frustrated quantum spins. The static susceptibility is described by the spin \(S\) = 1/2 antiferromagnetic triangular-lattice Heisenberg model with the exchange constant \(J\) \(\sim\) 250 K. Regardless of the large magnetic interactions, the \(^{1}\)H NMR spectra show no indication of long-range magnetic ordering down to 32 mK, which is four-orders of magnitude smaller than \(J\). These results suggest that a quantum spin liquid state is realized in the close proximity of the superconducting state appearing under pressure.
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                Author and article information

                Contributors
                takayuki.isono@riken.jp
                UJI.Shinya@nims.go.jp
                Journal
                Nat Commun
                Nat Commun
                Nature Communications
                Nature Publishing Group UK (London )
                2041-1723
                17 April 2018
                17 April 2018
                2018
                : 9
                : 1509
                Affiliations
                [1 ]ISNI 0000 0001 0789 6880, GRID grid.21941.3f, National Institute for Materials Science, ; Tsukuba, Ibaraki 305-0003 Japan
                [2 ]ISNI 0000 0001 2151 536X, GRID grid.26999.3d, Department of Applied Physics, , University of Tokyo, ; Bunkyo-ku, Tokyo, 113-8656 Japan
                [3 ]Present Address: Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama, 351-0198 Japan
                Author information
                http://orcid.org/0000-0002-9542-6316
                http://orcid.org/0000-0001-9239-0621
                http://orcid.org/0000-0001-5992-0125
                Article
                4005
                10.1038/s41467-018-04005-1
                5904176
                29666404
                17415dc4-2b1a-41ad-884b-23d2e4b5cd4c
                © The Author(s) 2018

                Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

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                : 24 April 2017
                : 27 March 2018
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