Search results for "magnetization"

showing 10 items of 550 documents

A Comparative Structural and Magnetic Study of Three Compounds Based on the Cluster Unit M4Cl8(THF)6 (M=Mn, Fe, Co)

2001

Treatment of anhydrous M Cl 2 phases with THF under refluxing conditions leads to excision of the clusters M 4 Cl 8 (THF) 6 ( M =Fe (1), Co (3)) and dimensional reduction to the chain of clusters, {Mn 4 Cl 8 (THF) 6 (Mn(THF) 2 Cl 2 } ∞ , (2). All three compounds were isolated in high yields as crystalline materials and subjected to comprehensive magnetic studies. X-ray structures of the three compounds were performed to verify the nature of the compounds, but only the Mn derivative is discussed in detail due to the fact that the structures of the Fe and Co clusters were reported earlier. The molecular structures of M 4 Cl 8 (THF) 6 ( M =Fe, Co) consist of a rhombic arrrangement of metal ion…

StereochemistryCrystal structureCondensed Matter PhysicsMagnetic susceptibilityElectronic Optical and Magnetic MaterialsInorganic ChemistryMetalCrystallographyMagnetizationchemistry.chemical_compoundchemistryOctahedronvisual_artMaterials ChemistryCeramics and Compositesvisual_art.visual_art_mediumMoleculeAntiferromagnetismPhysical and Theoretical ChemistryTetrahydrofuranJournal of Solid State Chemistry
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Structural and magnetic characterization of the tridimensional network [Fe(HCO2)3]n·nHCO2H

2013

In this work we report the structural and magnetic characterization of a new three-dimensional porous metal–organic framework (MOF) based on iron(III) and the formate anion, [Fe(HCO2)3]n·nHCO2H (1), which was obtained by solvothermal synthesis. The tridimensional structure crystallizes in the trigonal space group Rc and is formed by highly regular octahedral Fe(OHCO)6 units. These units contain six equal Fe–O distances, with angles slightly different from 90° or 180°. The packing of 1 corresponds to a 3D covalent network defined by face sharing between the parallelepipeds, which are formed by the interactions of Fe(OHCO)6 units through formate ligands, thus generating a 41263 topology. This…

StereochemistrySolvothermal synthesisBridging ligandGeneral ChemistryCatalysischemistry.chemical_compoundCrystallographyMagnetizationchemistryFerromagnetismNetwork covalent bondingMaterials ChemistryAntiferromagnetismFormateSpin cantingNew Journal of Chemistry
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Langmuir-Blodgett Films of Magnetic Clusters

1999

Abstract The mixed-valence manganese clusters [Mn12O12(carboxylato)16] have been organized in a multilayer architecture. Indeed, well-defined Langmuir-Blodgett (LB) films of the acetate and the benzoate Mn12 clusters can be obtained using behenic acid as organic matrix. Here, we report the magnetic properties of these multilayers, which present a marked hysteresis at 2 K.

Stereochemistrychemistry.chemical_elementManganeseCondensed Matter PhysicsMagnetic hysteresisMagnetic susceptibilityLangmuir–Blodgett filmMagnetizationHysteresischemistry.chemical_compoundCrystallographychemistryCarboxylateBehenic acidMolecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals
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A facile semi-open method for synthesis of non-centrosymmetric superconducting Li2(Pd,Pt)3B bulks and thin films

2010

Abstract Non-centrosymmetric superconductor Li 2 (Pd 1− x Pt x ) 3 B, x  = 0–1 was synthesized from mixtures of the elements. A simple semi-open method is proposed using endings-pressed stainless steel tubes placed in a high-vacuum furnace. Heating regime employed a short-time overheating at 900 °C and a slow cooling step between T s and 550 °C within 3 h. To adequately compensate Li-losses and attain maximum critical temperature, the optimum T s and starting Li-content were found to change from 720 to 740 °C and from Li 2.4 to Li 2.6 , respectively, when x was changing from 0 to 1. It was shown that placing Li separately in the tube also produces superconducting samples, Li being supplied …

SuperconductivityMagnetizationMaterials scienceSlow coolingSuperconducting thin filmsAnalytical chemistryHeat treatedEnergy Engineering and Power TechnologySemi openElectrical and Electronic EngineeringThin filmCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsPhysica C: Superconductivity and its Applications
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Superconductivity and magnetism in Rb0.8Fe1.6Se2under pressure

2012

High-pressure magnetization, structural and 57Fe M\"ossbauer studies were performed on superconducting Rb0.8Fe1.6Se2.0 with Tc = 32.4 K. The superconducting transition temperature gradually decreases on increasing pressure up to 5.0 GPa followed by a marked step-like suppression of superconductivity near 6 GPa. No structural phase transition in the Fe vacancy-ordered superstructure is observed in synchrotron XRD studies up to 15.6 GPa, while the M\"ossbauer spectra above 5 GPa reveal the appearance of a new paramagnetic phase and significant changes in the magnetic and electronic properties of the dominant antiferromagnetic phase, coinciding with the disappearance of superconductivity. Thes…

SuperconductivityMaterials scienceCondensed matter physicsMagnetismCondensed Matter PhysicsSynchrotronPhysics::GeophysicsElectronic Optical and Magnetic Materialslaw.inventionCondensed Matter::Materials ScienceParamagnetismMagnetizationlawCondensed Matter::SuperconductivityPhase (matter)AntiferromagnetismCondensed Matter::Strongly Correlated ElectronsSuperstructure (condensed matter)Physical Review B
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Vortex-system ordering during magnetisation measurements in YBa2Cu3O7−δ films at low temperatures

2007

Abstract Zero-field-cooling dc magnetisation relaxation measurements performed on optimally doped epitaxial YBa 2 Cu 3 O 7− δ films with the external magnetic field H oriented parallel to the c -axis reveal the ordering of the creeping vortex-system in the low temperature T domain, due to the macroscopic currents induced in the sample. This dynamic ordering manifests itself through the appearance of a maximum in the T variation of the normalised vortex-creep activation energy. The location of this maximum in the H – T plane describes a well-defined current induced order–disorder line. Our results suggest the absence of a static elastic vortex glass in disordered high-temperature superconduc…

SuperconductivityMaterials scienceCondensed matter physicsRelaxation (NMR)DopingEnergy Engineering and Power TechnologyActivation energyCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsMagnetic fieldVortexMagnetizationCondensed Matter::SuperconductivityElectrical and Electronic EngineeringScalingPhysica C: Superconductivity
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Vortex creep crossover in YBCO/PrBCO superlattices during standard magnetization relaxation measurements

2011

We investigated the relaxation of the irreversible magnetization in a series of 200?nm thick YBa2Cu3O7/PrBa2Cu3O7 [(YBCO)n/(PrBCO)m] superlattices, where the thickness m of the nonsuperconducting PrBCO layer (measured in unit cells) was kept to m = 4 (sufficient to decouple the superconducting YBCO layers), whereas the thickness n of the YBCO layer was varied between 2 and 20 unit cells. The analysis of standard zero-field-cooling dc magnetization relaxation data obtained in the low temperature T region with the applied magnetic field H oriented along the c axis reveals the occurrence of a crossover elastic (collective) vortex creep at low T?plastic vortex creep at high T, generated by the …

SuperconductivityMaterials scienceCondensed matter physicsSuperlatticeRelaxation (NMR)Metals and AlloysQuantum vortexCondensed Matter PhysicsVortexMagnetizationCreepCondensed Matter::SuperconductivityMaterials ChemistryCeramics and CompositesElectrical and Electronic EngineeringThin filmSuperconductor Science and Technology
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Origin of the fast magnetization relaxation at low temperatures in HTS with strong pinning

2010

The temperature T variation of the normalized magnetization relaxation rate S in high-temperature superconductors (HTS) with strong vortex pinning exhibits a maximum in the low-T range. This was reported for various HTS, and the origin of the faster relaxation at low T appearing in standard magnetization relaxation measurements was usually related to specific pinning properties of the investigated specimens. Since the observed behaviour seems to be characteristic to all HTS with enhanced pinning (generated by random and/or correlated disorder), we show that the S(T) maximum can be explained in terms of classic collective vortex creep. The influence of thermo-magnetic instabilities in the lo…

SuperconductivityMaterials scienceFlux pinningCondensed matter physicsRelaxation (NMR)Energy Engineering and Power TechnologyCondensed Matter PhysicsInstabilityElectronic Optical and Magnetic MaterialsVortexMagnetizationCreepCondensed Matter::SuperconductivityElectrical and Electronic EngineeringPinning forcePhysica C: Superconductivity and its Applications
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On the determination of vortex creep parameters in superconductors using standard magnetization relaxation data

2011

The relaxation of the irreversible magnetic moment m(t) in YBa2Cu3O7 (YBCO) films was investigated as a function of temperature T and the external magnetic field H along the c axis applied in zero-field cooling conditions, for the determination of vortex creep parameters. The data analysis was performed using the T and current density dependence of the normalized vortex creep activation energy, or by the fit of the m(t) data with the well known interpolation formula in the framework of the general vortex creep equation. It was found that (i) even for specimens with strong static pinning the characteristic pinning energy remains small in the low-T range, where the vortex creep appearing in s…

SuperconductivityMaterials scienceMagnetic momentCondensed matter physicsRelaxation (NMR)Metals and AlloysCondensed Matter PhysicsPhysics::GeophysicsMagnetic fieldVortexMagnetizationCreepCondensed Matter::SuperconductivityMaterials ChemistryCeramics and CompositesElectrical and Electronic EngineeringCurrent densitySuperconductor Science and Technology
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Improvement of the critical current density of spark plasma sintered MgB2by C60addition

2010

We investigated the influence of fullerene (C60) addition on the superconducting parameters of MgB2 bulk samples obtained by spark plasma sintering (SPS). It was found that 1.5?wt% C60 addition leads to the reduction of the critical temperature by a few K, whereas the magnetically determined critical current density increases by approximately one order of magnitude in an applied magnetic field H = 70?kOe at temperature T = 10?K. This indicates substitution of B by C in C60 added MgB2 processed by SPS, contrary to some data reported in the literature obtained using conventional methods. For our relatively large specimens, the occurrence of macroscale flux jumps was observed over a wide (H, T…

SuperconductivityMaterials scienceMagnetic momentCondensed matter physicsRelaxation (NMR)Metals and AlloysSpark plasma sinteringFluxPlasmaCondensed Matter PhysicsMagnetizationCondensed Matter::SuperconductivityMaterials ChemistryCeramics and CompositesElectrical and Electronic EngineeringOrder of magnitudeSuperconductor Science and Technology
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