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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Sheptyakov, D.
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (8/8 displayed)
- 2020Intermediate magnetic phase of the magnetoelectric compound (Ca, Sr) BaCo4O7 described with the superspace formalismcitations
- 2016Ba3 Mx Ti3−x O9 (M = Ir, Rh): A family of 5d/4d-based diluted quantum spin liquidscitations
- 2015Sc2Ga2CuO7citations
- 2015Sc2Ga2CuO7: A possible quantum spin liquid near the percolation thresholdcitations
- 2012On the high-temperature phase of barbituric acidcitations
- 2012Ionic conductivity in the Mg intercalated fullerene polymer Mg2C60citations
- 2012Reversible hydrogen absorption in sodium intercalated fullerenescitations
- 2011Silicon Location in Silicate-Substituted Calcium Phosphate Ceramics Determined by Neutron Diffractioncitations
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article
Sc2Ga2CuO7
Abstract
Sc<sub>2</sub>Ga<sub>2</sub>CuO<sub>7</sub> (SGCO) crystallizes in a hexagonal structure (space group: P6<sub>3</sub>/mmc), which can be seen as<br/>an alternating stacking of single and double triangular layers. Combining neutron, x-ray, and resonant x-ray diffraction, we establish that the single triangular layers are mainly populated by nonmagnetic Ga<sup>3+</sup> ions (85%<br/>Ga and 15% Cu), while the bilayers have comparable population of Cu<sup>2+</sup> and Ga<sup>3+</sup> ions (43% Cu and 57% Ga). Our susceptibility measurements in the temperature range 1.8–400 K give no indication of any spin-freezing or magnetic long-range order (LRO). We infer an effective paramagnetic moment μ<sub>eff</sub> = 1.79 ± 0.09μ<sub>B</sub> and a Curie-Weiss temperature θ<sub>CW</sub> of about −44 K, suggesting antiferromagnetic interactions between the Cu<sup>2+</sup>(S =<br/>1/2) ions. Low-temperature neutron powder diffraction data showed no evidence for LRO down to 1.5 K. In our specific heat data as well, no anomalies were found down to 0.35 K, in the field range 0–140 kOe. The magnetic specific heat C<sub>m</sub>, exhibits a broad maximum at around 2.5 K followed by a nearly power law C<sub>m</sub> ∝ T<sup>α</sup> behavior at lower temperatures, with α increasing from 0.3 to 1.9 as a function of field for fields up to 90 kOe and then remaining at 1.9 for fields up to 140 kOe. Our results point to a disordered ground state in SGCO.