Rearrangement of uncorrelated valence bonds evidenced by low-energy spin excitations in YbMgGaO4

DC-magnetization data measured down to 40 mK speak against conventional freezing and reinstate YbMgGaO\(_4\) as a triangular spin-liquid candidate. Magnetic susceptibility measured parallel and perpendicular to the \(c\)-axis reaches constant values below 0.1 and 0.2 K, respectively, thus indicating...

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Published inarXiv.org
Main Authors Li, Yuesheng, Bachus, Sebastian, Liu, Benqiong, Radelytskyi, Igor, Bertin, Alexandre, Schneidewind, Astrid, Tokiwa, Yoshifumi, Tsirlin, Alexander A, Gegenwart, Philipp
Format Paper Journal Article
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 22.03.2019
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Summary:DC-magnetization data measured down to 40 mK speak against conventional freezing and reinstate YbMgGaO\(_4\) as a triangular spin-liquid candidate. Magnetic susceptibility measured parallel and perpendicular to the \(c\)-axis reaches constant values below 0.1 and 0.2 K, respectively, thus indicating the presence of gapless low-energy spin excitations. We elucidate their nature in the triple-axis inelastic neutron scattering experiment that pinpoints the low-energy (\(E\) \(\leq\) \(J_0\) \(\sim\) 0.2 meV) part of the excitation continuum present at low temperatures (\(T\) \(<\) \(J_0\)/\(k_B\)), but \emph{completely} disappearing upon warming the system above \(T\) \(\gg\) \(J_0\)/\(k_B\). In contrast to the high-energy part at \(E\) \(>\) \(J_0\) that is rooted in the breaking of nearest-neighbor valence bonds and persists to temperatures well above \(J_0\)/\(k_B\), the low-energy one originates from the rearrangement of the valence bonds and thus from the propagation of unpaired spins. We further extend this picture to herbertsmithite, the spin-liquid candidate on the kagome lattice, and argue that such a hierarchy of magnetic excitations may be a universal feature of quantum spin liquids.
Bibliography:Phys. Rev. Lett. 122, 137201 (2019)
ISSN:2331-8422
DOI:10.48550/arxiv.1903.09574