0000000000824049

AUTHOR

Mikhail Eremets

showing 4 related works from this author

Exotic magnetism in the alkali sesquioxidesRb4O6andCs4O6

2009

Among the various alkali oxides the sesquioxides ${\text{Rb}}_{4}{\text{O}}_{6}$ and ${\text{Cs}}_{4}{\text{O}}_{6}$ are of special interest. Electronic-structure calculations using the local spin-density approximation predicted that ${\text{Rb}}_{4}{\text{O}}_{6}$ should be a half-metallic ferromagnet, which was later contradicted when an experimental investigation of the temperature-dependent magnetization of ${\text{Rb}}_{4}{\text{O}}_{6}$ showed a low-temperature magnetic transition and differences between zero-field-cooled and field-cooled measurements. Such behavior is known from spin glasses and frustrated systems. ${\text{Rb}}_{4}{\text{O}}_{6}$ and ${\text{Cs}}_{4}{\text{O}}_{6}$ c…

PhysicsCrystallographyCharge orderingMagnetizationSpin glassUnpaired electronCondensed matter physicsMagnetismValencyCrystal structureCondensed Matter PhysicsAntibonding molecular orbitalElectronic Optical and Magnetic MaterialsPhysical Review B
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Pressure-restored superconductivity in Cu-substituted FeSe

2011

Copper doping of FeSe destroys its superconductivity at ambient pressure, even at low doping levels. Here we report the pressure-dependent transport and structural properties of Fe${}_{1.01\ensuremath{-}x}$Cu${}_{x}$Se with 3$%$ and 4$%$ Cu doping and find that the superconductivity is restored. Metallic resistivity behavior, absent in Cu-doped FeSe, is also restored. At the low pressure of 1.5 GPa, superconductivity is seen at 6 K for 4$%$ Cu doping, somewhat lower than the 8 K ${T}_{c}$ of undoped FeSe. ${T}_{c}$ reaches its maximum of 31.3 K at 7.8 GPa, lower than the maximum superconducting temperature in the undoped material under pressure (${T}_{c}$ max of 37 K) but still very high. X…

DiffractionSuperconductivityMaterials scienceCondensed matter physicsDopingCondensed Matter PhysicsCopper dopingElectronic Optical and Magnetic MaterialsMetalLattice constantElectrical resistivity and conductivityvisual_artvisual_art.visual_art_mediumAmbient pressurePhysical Review B
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Local electronic structure rearrangements and strong anharmonicity in YH3 under pressures up to 180 GPa

2021

The authors acknowledge the ESRF program committee (Grenoble, France) for the opportunity to perform XAFS and XRD measurements. We are grateful to Prof. Dr Marek Tkacz from the Institute of Physical Chemistry, PAS Kasprzaka 44/52, 01-224 Warsaw, Poland, for high quality YH3 samples and to Dr. José A. Flores-Livas for a fruitful discussion. A.P.M. and A.A.I. acknowledge the Russian Foundation for the Basic Research (grant No 18-02-40001_mega) for financial support. J.P., A.K., and I.P. would like to thank the support of the Latvian Council of Science project No. lzp-2018/2-0353. ISSP UL acknowledge the European Union’s Horizon 2020 Framework Programme H2020-WIDESPREAD-01-20l 6-2017-TeamingPh…

Materials scienceHydrogenScienceGeneral Physics and Astronomychemistry.chemical_element02 engineering and technology01 natural sciencesGeneral Biochemistry Genetics and Molecular BiologyCondensed Matter::Materials Science0103 physical sciencesAtomPhysics::Atomic and Molecular Clusters:NATURAL SCIENCES:Physics [Research Subject Categories]Physics::Atomic PhysicsPhysics::Chemical Physics010306 general physicsMultidisciplinaryExtended X-ray absorption fine structureHydrideQAnharmonicityGeneral ChemistryYttrium021001 nanoscience & nanotechnologyXANESX-ray absorption fine structurechemistryChemical physics0210 nano-technologyNature Communications
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Conventional superconductivity at 203 kelvin at high pressures in the sulfur hydride system.

2015

A superconductor is a material that can conduct electricity without resistance below a superconducting transition temperature, Tc. The highest Tc that has been achieved to date is in the copper oxide system: 133 kelvin at ambient pressure and 164 kelvin at high pressures. As the nature of superconductivity in these materials is still not fully understood (they are not conventional superconductors), the prospects for achieving still higher transition temperatures by this route are not clear. In contrast, the Bardeen-Cooper-Schrieffer theory of conventional superconductivity gives a guide for achieving high Tc with no theoretical upper bound--all that is needed is a favourable combination of …

SuperconductivityMultidisciplinaryRoom-temperature superconductorCondensed matter physicsHydrogenChemistryTransition temperaturechemistry.chemical_elementMineralogyMetallic hydrogenMagnetic susceptibilityElectrical resistivity and conductivityCondensed Matter::SuperconductivityDensity of statesNature
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