Search results for "Transition Temperature"

showing 10 items of 137 documents

Fabrication of superconducting tantalum nitride thin films using infra-red pulsed laser deposition

2013

We report the successful fabrication of superconducting tantalum nitride (TaN) thin films using a pulsed laser deposition technique with 1064 nm radiation. Films with thickness $ \sim $ 100 nm deposited on MgO (100) single crystals and on oxidized silicon (SiO$_{2} $) substrates exhibited a superconducting transition temperature of $\sim $ 8 K and 6 K, respectively. The topography of these films were investigated using atomic force and scanning electron microscopy, revealing fairly large area particulate free and smooth surfaces, while the structure of the films were investigated using standard $ \theta -2 \theta $ and glancing angle X-ray diffraction techniques. For films grown on MgO a fa…

Materials scienceSiliconScanning electron microscopeAnalytical chemistrychemistry.chemical_elementFOS: Physical sciences02 engineering and technology01 natural sciencesPulsed laser depositionSuperconductivity (cond-mat.supr-con)chemistry.chemical_compoundTantalum nitride0103 physical sciencesThin film010306 general physicsta116Deposition (law)Condensed Matter - Materials Scienceta114Condensed matter physicsTransition temperatureCondensed Matter - SuperconductivityHexagonal phaseMaterials Science (cond-mat.mtrl-sci)Surfaces and Interfaces021001 nanoscience & nanotechnologyCondensed Matter PhysicsSurfaces Coatings and Filmschemistry0210 nano-technology
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Lattice-Site-Specific Spin Dynamics in Double PerovskiteSr2CoOsO6

2014

Magnetic properties and spin dynamics have been studied for the structurally ordered double perovskite Sr2CoOsO6. Neutron diffraction, muon-spin relaxation, and ac-susceptibility measurements reveal two antiferromagnetic (AFM) phases on cooling from room temperature down to 2 K. In the first AFM phase, with transition temperature TN1=108  K, cobalt (3d7, S=3/2) and osmium (5d2, S=1) moments fluctuate dynamically, while their average effective moments undergo long-range order. In the second AFM phase below TN2=67  K, cobalt moments first become frozen and induce a noncollinear spin-canted AFM state, while dynamically fluctuating osmium moments are later frozen into a randomly canted state at…

Materials scienceSpin dynamicsCondensed matter physicsTransition temperatureNeutron diffractionGeneral Physics and Astronomychemistry.chemical_element02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesCondensed Matter::Materials Sciencechemistry.chemical_compoundchemistryLattice (order)0103 physical sciencesAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsOsmium010306 general physics0210 nano-technologyCobaltAFm phasePhysical Review Letters
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Guest Effect on Nanopatterned Spin-Crossover Thin Films

2011

International audience; Nanopatterned thin films of the metal–organic framework {Fe(bpac)[Pt(CN)4]} (bpac=bis(4‐pyridyl)acetylene) are elaborated by the combination of a sequential assembly process and a lithographic method. Raman microspectroscopy is used to probe the temperature dependence of the spin state of the iron(II) ions in the films (40–90 nm in thickness), and reveals an incomplete but cooperative spin transition comparable to that of the bulk material. Adsorption/desorption of pyridine guest molecules is found to have a substantial influence on the spin‐crossover properties of the thin layers. This interplay between host–guest and spin‐crossover properties in thin films and nano…

Materials scienceSpin statesSpin transitionNanotechnology02 engineering and technologyMicroscopy Atomic ForceSpectrum Analysis Raman010402 general chemistry01 natural sciencesBiomaterialssymbols.namesakeSpin crossoverMetals HeavyDesorptionTransition TemperatureGeneral Materials ScienceThin film[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/MicroelectronicsCyanidesThin layersTransition temperatureGeneral Chemistry021001 nanoscience & nanotechnologyNanostructures0104 chemical sciencessymbolsPhysical chemistrySpin Labels0210 nano-technologyRaman spectroscopyBiotechnology
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Equilibrium phase behavior of polyethylene oxide and of its mixtures with tetrahydronaphthalene or/and poly(ethylene oxide-block-dimethylsiloxane)

2002

Liquid/solid and liquid/liquid (LL) transition temperatures were measured by means of an automated device that monitors the light passing through the systems as a function of T at different constant cooling or heating rates q. For pure polyethylene oxide (PEO) crystallization and melting temperatures depend on |q|0.3 and become identical at the equilibrium transition temperature Tm=61.0 °C in the limit of infinitely slow cooling/heating. The reduction of Tm for PEO dissolved in tetrahydronaphthalene (THN) yields information on the Flory–Huggins interaction parameter ξ between these two compounds; ξ results negative and decreases markedly with rising polymer concentration. A tentative explan…

Materials scienceSpinodal decompositionTransition temperatureAnalytical chemistryOxideGeneral Physics and AstronomyFlory–Huggins solution theorylaw.inventionchemistry.chemical_compoundchemistrylawPolymer chemistryPolymer blendPhysical and Theoretical ChemistryCrystallizationSolubilityPhase diagramThe Journal of Chemical Physics
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TeO2 liquid phase: Viscosity measurements and evaluation of the thermal conductivity from crystal growth experiments

2008

Current applications of paratellurite TeO{sub 2} in optics and nuclear physics require improving the yield and optical quality of synthesized single crystals. Modelling of the growth process is a useful tool for such purpose, however, involving the knowledge of several thermodynamic parameters of both solid and liquid phase of the compound. This work describes the determination of two main unknown ones, namely dynamic viscosity {eta} and thermal conductivity {lambda}{sub l} of the liquid phase. Measurements of {eta} are performed by means of a specifically designed apparatus; over a 40 K temperature interval above the melting point we find a mean value of 0.028 Pa.s. This data is used in co…

Materials scienceYield (engineering)Mechanical EngineeringTransition temperatureMineralogyThermodynamicsCrystal growthAtmospheric temperature rangeCondensed Matter PhysicsLambdaViscosityThermal conductivityMechanics of MaterialsMelting pointGeneral Materials ScienceMaterials Research Bulletin
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Phase coexistence in a triolein-phosphatidylcholine system. Implications for lysosomal membrane properties.

2010

The effects of tri- and monoglycerides on phospholipid (POPC) membranes were studied using spectroscopical methods. Triolein was found to form two types of POPC-rich membranes, both with POPC or as a three-component system with monopalmitin. These two membrane types were determined as co-existing phases based on their spontaneous and stable separation and named heavy and light phase according to their sedimentation behaviour. Marked differences were seen in the physical properties of these phases, even though only minor compositional variation was detected. The light, less polar phase was found to be less ordered and more fluid and seemed to allow significantly lower amount of water penetra…

Membrane FluidityLipid BilayersPhospholipidCalorimetryBiochemistryPhase TransitionGlycerideschemistry.chemical_compoundPhosphatidylcholineMembrane fluidityTransition TemperatureTrioleinMolecular BiologyPOPCChromatographyCalorimetry Differential ScanningOrganic ChemistryElectron Spin Resonance SpectroscopyWaterCell BiologyPenetration (firestop)MembranechemistryBiophysicsPhosphatidylcholineslipids (amino acids peptides and proteins)LysosomesTrioleinChemistry and physics of lipids
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Temperature and pressure dependence of quercetin-3-O-palmitate interaction with a model phospholipid membrane: film balance and scanning probe micros…

2004

The molecular interaction of quercetin-3-O-palmitate (QP) with dimyristoylphosphatidylcholine (DMPC) has been studied. Film balance measurements of the average molecular area vs QP molar fraction in DMPC/QP mixed monolayers showed that relevant positive deviations from ideality, i.e., a less dense monolayer packing, occurred for a temperature of 10 degrees C, below the critical melting transition temperature of DMPC monolayers T c m approximately equal 20 degrees C), while ideal behavior was observed at 37 degrees C, above this phase transition temperature. The positive deviation observed at low temperatures in the average molecular area increased with the surface pressure. Scanning probe m…

Membrane FluiditySurface PropertiesLipid BilayersAnalytical chemistryPhospholipidPalmitic AcidPhase separationPalmitic AcidsSurface pressureMole fractionMicroscopy Atomic ForcePhase TransitionBiomaterialsScanning probe microscopychemistry.chemical_compoundMembrane LipidsColloid and Surface ChemistryMonolayerLangmuir-Blodgett monolayersMolecular StructureTransition temperatureTemperatureQuercetin palmitateSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsLangmuir–Blodgett monolayerMembranechemistryAluminum SilicatesQuercetinMicaStress MechanicalDimyristoylphosphatidylcholineAlgorithmsScanning force microscopy
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Monte Carlo calculation of free energy for a fcc lattice-gas model

1990

A face-centered-cubic Ising lattice-gas model with nearest- and next-nearest-neighbor interactions is studied, and an accurate determination of the transition temperature for the discontinuous order-disorder transition is obtained. This model is of interest in the studies of phase diagrams for metallic alloys. The location of the transition was previously not known accurately, and its estimation has a number of applications. Very accurate absolute free-energy densities for the two coexisting phases have been obtained from a combination of the standard thermodynamic integration method and the method of sampling finite-size dependence. The latent-heat also is calculated with good precision.

Metallic alloyMaterials scienceLattice (order)Latent heatTransition temperatureMonte Carlo methodThermodynamic integrationIsing modelStatistical physicsPhase diagramPhysical Review B
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Prevalence and genotypes of Borrelia burgdorferi sensu lato infection in Ixodes ricinus ticks in southern Norway.

2010

From April to October 2007, host-seeking Ixodes ricinus ticks were collected from 4 locations in southern Norway: Farsund, Mandal, Sogne and Tromoy. Two hundred and ten larvae, 1130 nymphs and 449 adults were investigated for infection with Borrelia burgdorferi sensu lato (s.l.) by real-time polymerase chain reaction (PCR) amplification of the 16S rRNA gene. The total percentage of B. burgdorferi s.l. in nymphal and adult ticks was determined to be 31.3% in Farsund, 25.2% in Mandal, 22.3% in Sogne and 22.1% in Tromoy. Larvae were pooled in groups of 10 before analysis, and Borrelia infection was detected in 1 of the 21 larvae pools. B. burgdorferi s.l. were genotyped by melting curve analys…

Microbiology (medical)DNA BacterialNymphIxodes ricinusGenotypeDNA RibosomalPolymerase Chain Reactionlaw.inventionBorrelia burgdorferi GrouplawBorreliaRNA Ribosomal 16Sparasitic diseasesPrevalenceAnimalsCluster AnalysisTransition TemperatureAcariBorrelia burgdorferiPolymerase chain reactionGeneral Immunology and MicrobiologybiologyIxodesNorwayParasitiformesGeneral MedicineSequence Analysis DNAbacterial infections and mycosesbiology.organism_classificationVirologyBacterial Typing TechniquesInfectious DiseasesLarvaIxodesDNA IntergenicIxodidaeScandinavian journal of infectious diseases
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Gelation behavior of 5-chloro-8-hydroxyquinoline, an antituberculosis agent, in aqueous alcohol solutions

2012

It was shown that 5-chloro-8-hydroxyquinoline, an antituberculosis agent, gels aqueous alcohol solutions efficiently. Thermal stability and gel-to-sol transition temperature of 1% gel in CD3OD/D2O (2:1) was studied by 1H-NMR. Fibrous structures of four xerogels have been characterized by scanning electron microscope. peerReviewed

Microbiology (medical)gelScanning electron microscope5-kloori-8-hydroksikinoliinigel; 5-chloro-8-hydroxyquinoline; <em>Mycobacterium </em><em>tuberculosis</em>gelationBiochemistryMicrobiologyArticle5-chloro-8-hydroxyquinolinechemistry.chemical_compoundOrganic chemistryPharmacology (medical)Thermal stabilityGeneral Pharmacology Toxicology and Pharmaceuticsta116Aqueous alcoholgeelin muodostusTransition temperature5-chloro-8-hydoxyquinolinelcsh:RM1-950Antituberculosis agent8-HydroxyquinolineMycobacterium tuberculosisInfectious Diseaseslcsh:Therapeutics. PharmacologychemistryNuclear chemistryAntibiotics
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