Anisotropic charge dynamics in the Quantum spin-liguid candidate Kappa -(BEDT-TTF) sub(2) Cu sub(2)(CN) sub(3)
We have in detail characterized the anisotropic charge response of the dimer Mott insulator Kappa -(BEDT-TTF) sub(2) Cu sub(2)(CN) sub(3) by dc conductivity, Hall effect, and dielectric spectroscopy. At room temperature, the Hall coefficient is positive and close to the value expected from stoichiom...
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Published in: | Physical review. B, Condensed matter and materials physics Vol. 90; no. 19 |
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Main Authors: | , , , , , , , , , , , , , |
Format: | Journal Article |
Language: | English |
Published: |
15-11-2014
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Subjects: | |
Online Access: | Get full text |
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Summary: | We have in detail characterized the anisotropic charge response of the dimer Mott insulator Kappa -(BEDT-TTF) sub(2) Cu sub(2)(CN) sub(3) by dc conductivity, Hall effect, and dielectric spectroscopy. At room temperature, the Hall coefficient is positive and close to the value expected from stoichiometry; the temperature behavior follows the dc resistivity [rho](T). Within the planes the dc conductivity is well described by variable-range hopping in two dimensions; this model, however, fails for the out-of-plane direction. An unusually broad in-plane dielectric relaxation is detected below about 60 K; it slows down much faster than the dc conductivity following an Arrhenius law. At around 17 K, we can identify a pronounced dielectric anomaly concomitantly with anomalous features in the mean relaxation time and spectral broadening. The out-of-plane relaxation, on the other hand, shows a much weaker dielectric anomaly; it closely follows the temperature behavior of the respective dc resistivity. At lower temperatures, the dielectric constant becomes smaller both within and perpendicular to the planes; also, the relaxation levels off. The observed behavior bears features of relaxorlike ferroelectricity. Because heterogeneities impede its long-range development, only a weak-tunneling-like dynamics persists at low temperatures. We suggest that the random potential and domain structure gradually emerge due to the coupling to the anion network. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 content type line 23 ObjectType-Feature-2 |
ISSN: | 1098-0121 1550-235X |