Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurements

The spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} [ET: bis(ethylenedithio)tetrathiafulvalene] does not exhibit magnetic ordering down to a very low temperature, but shows a mysterious anomaly at 6 K. The origin of the so-called 6-K anomaly is still under debate. We carried out nuclear quadrupole re...

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Main Authors: T. Kobayashi, Q.-P. Ding, H. Taniguchi, K. Satoh, A. Kawamoto, Y. Furukawa
Format: Article
Language:English
Published: American Physical Society 2020-10-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.2.042023
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author T. Kobayashi
Q.-P. Ding
H. Taniguchi
K. Satoh
A. Kawamoto
Y. Furukawa
author_facet T. Kobayashi
Q.-P. Ding
H. Taniguchi
K. Satoh
A. Kawamoto
Y. Furukawa
author_sort T. Kobayashi
collection DOAJ
description The spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} [ET: bis(ethylenedithio)tetrathiafulvalene] does not exhibit magnetic ordering down to a very low temperature, but shows a mysterious anomaly at 6 K. The origin of the so-called 6-K anomaly is still under debate. We carried out nuclear quadrupole resonance (NQR) measurements on the copper sites of the insulating layers, which are sensitive to the charge dynamics unlike conventional spin-1/2 nuclear magnetic resonance (NMR). The main finding of this Rapid Communication is that the observation of a sharp peak behavior in the nuclear spin-lattice relaxation rate T_{1}^{−1} of ^{63}Cu NQR at 6 K while T_{1}^{−1} of both ^{13}C and ^{1}H NMR show no clear anomaly. This behavior can be understood as a second-order phase transition related to charge disproportionation in the ET layers.
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spelling doaj.art-6cc1dcd451974faabe8c2371bbbeb1c52024-04-12T17:03:19ZengAmerican Physical SocietyPhysical Review Research2643-15642020-10-012404202310.1103/PhysRevResearch.2.042023Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurementsT. KobayashiQ.-P. DingH. TaniguchiK. SatohA. KawamotoY. FurukawaThe spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} [ET: bis(ethylenedithio)tetrathiafulvalene] does not exhibit magnetic ordering down to a very low temperature, but shows a mysterious anomaly at 6 K. The origin of the so-called 6-K anomaly is still under debate. We carried out nuclear quadrupole resonance (NQR) measurements on the copper sites of the insulating layers, which are sensitive to the charge dynamics unlike conventional spin-1/2 nuclear magnetic resonance (NMR). The main finding of this Rapid Communication is that the observation of a sharp peak behavior in the nuclear spin-lattice relaxation rate T_{1}^{−1} of ^{63}Cu NQR at 6 K while T_{1}^{−1} of both ^{13}C and ^{1}H NMR show no clear anomaly. This behavior can be understood as a second-order phase transition related to charge disproportionation in the ET layers.http://doi.org/10.1103/PhysRevResearch.2.042023
spellingShingle T. Kobayashi
Q.-P. Ding
H. Taniguchi
K. Satoh
A. Kawamoto
Y. Furukawa
Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurements
Physical Review Research
title Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurements
title_full Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurements
title_fullStr Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurements
title_full_unstemmed Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurements
title_short Charge disproportionation in the spin-liquid candidate κ-(ET)_{2}Cu_{2}(CN)_{3} at 6 K revealed by ^{63}Cu NQR measurements
title_sort charge disproportionation in the spin liquid candidate κ et 2 cu 2 cn 3 at 6 k revealed by 63 cu nqr measurements
url http://doi.org/10.1103/PhysRevResearch.2.042023
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