Search results for "Magnetic Structure"

showing 10 items of 40 documents

Electronic structure calculations in ordered and disordered solids with spiral magnetic order

2011

A scheme to calculate the electronic structure of systems having a spiral magnetic structure is presented. The approach is based on the Korringa-Kohn-Rostoker Green's function formalism which allows, in combination with the coherent potential approximation alloy theory, dealing with chemically disordered materials. It is applied to the magnetic random alloys Fe${}_{x}$Ni${}_{1\ensuremath{-}x}$, Fe${}_{x}$Co${}_{1\ensuremath{-}x}$, and Fe${}_{x}$Mn${}_{1\ensuremath{-}x}$. For these systems the stability of their magnetic structure was analyzed. For Fe${}_{x}$Ni${}_{1\ensuremath{-}x}$ the spin stiffness for was determined as a function of concentration that was found in satisfying agreement w…

PhysicsCondensed matter physicsMagnetic structureAlloyElectronic structureengineering.materialCondensed Matter PhysicsMagnetic susceptibilityElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceParamagnetismMuffin-tin approximationSpin waveengineeringCoherent potential approximationPhysical Review B
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Alloying-induced transition from local-moment to itinerant heavy fermion magnetism in Ce(Cu1−xNix)2Ge2

1990

Abstract A monotonous increase of the Kondo temperature in Ce(Cu1−xNix)2Ge2 from 7 (x = 0) to 30 K (x = 1) is accompanied by drastic changes of ground state properties: for x⩽0.2, a modulated magnetic structure (q01 = (0.28, 0.28, 0.54)) involving Kondo-reduced local Ce moments ( μ s = 0.74μ B Ce for x = 0) forms below TN1(x). TN1 = 4. 1 K for CeCu2Ge2 is strongly depressed upon increasing x. At x ≲ 0.2, a different modulation develops below TN2(x) which becomes maximum (≃4 K) for x = 0.5. Since this is characterized by a very small value of q02 (=(0, 0, 0.13) at x = 0.5) and a gradually decreasing ordered moment (reaching μs ≲ 0.2μB/Ce for x ⩾0.65), we ascribe it to “heavy fermion band mag…

PhysicsCondensed matter physicsMagnetic structureMagnetismHeavy fermionMoment (physics)Electrical and Electronic EngineeringAtomic physicsCondensed Matter PhysicsGround stateElectronic Optical and Magnetic MaterialsLocal momentPhysica B: Condensed Matter
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Hyperfine structure measurements of neutral niobium with Fourier transform spectroscopy

2010

Aims. We report on experimental studies of hyperfine structure splitting of neutral niobium.Methods. We used high-resolution Fourier transform spectroscopy to record a spectrum of niobium produced with a hollow cathode discharge lamp in the range of wavenumbers from 10 000 cm-1 to 30 000 cm-1 .Results. The magnetic dipole hyperfine structure constants A were determined for the 109 levels of odd parity by analyzing the profiles of 224 spectral lines. The A  values of 57 of these level are reported for the first time.

PhysicsGas-discharge lampMagnetic structureNiobiumchemistry.chemical_elementAstronomy and AstrophysicsFourier transform spectroscopylaw.inventionsymbols.namesakeFourier transformchemistrySpace and Planetary SciencelawsymbolsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsSpectroscopyHyperfine structureMagnetic dipoleAstronomy and Astrophysics
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Magnetic order in a Kondo lattice: A neutron scattering study of CeCu2Ge2

1989

Elastic and inelastic neutron scattering studies of the Kondo lattice CeCu2Ge2 were performed. AtTN=4.1 K an incommensurate magnetic order develops with an ordering wave vectorq0=(0.28, 0.28, 0.54) and an ordered moment µs=0.74 µB. The crystalline electric field splits the 4f1-J-multiplet of the Ce ion into a ground state doublet and a quartet at 191 K. The wave function of the ground state yields an ordered moment of 1.54µB. Thus, due to the onset of the formation of a Kondo singlet the magnetic moment is considerably reduced. The magnetic relaxation rate Λ was investigated via quasielastic neutron scattering. The temperature dependence of Λ(T) is characteristic of heavy-fermion systems wi…

PhysicsNeutron magnetic momentCondensed matter physicsMagnetic structureInelastic scatteringNeutron scatteringCondensed Matter PhysicsInelastic neutron scatteringElectronic Optical and Magnetic MaterialsMagnetizationQuasielastic neutron scatteringCondensed Matter::Strongly Correlated ElectronsGeneral Materials ScienceKondo effectZeitschrift f�r Physik B Condensed Matter
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Neutron diffraction study of the heavy fermion superconductors UM2Al3(M=Pd, Ni)

1992

An elastic neutron scattering study was performed on the new superconducting heavy fermion systems UPd2Al3 and UNi2Al3. The neutron diffraction patterns reveal unambiguously long range antiferromagnetic order in UPd2Al3 with an ordered magnetic momentμ U = (0.85±0.03)μ B , which coexists with the superconducting state. This is by far the largestμ U value observed for any heavy fermion superconductor. For UNi2Al3, no long-range magnetic order could be observed for temperaturesT≧1.5 K, yielding an upper limit of the ordered moment of 0.2μ B .

PhysicsSuperconductivityRange (particle radiation)Magnetic structureCondensed matter physicsMagnetic momentNeutron diffractionAntiferromagnetismGeneral Materials ScienceHeavy fermion superconductorNeutron scatteringCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsZeitschrift f�r Physik B Condensed Matter
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Photoabsorption and MXCD in photoemission microscopy for characterisation of advanced materials

1999

Abstract We applied chemical and magnetic sensitive photoemission electron microscopy (PEEM) to investigate surfaces of advanced materials. PEEM at low photon energies provides a high spatial resolution, but suffers from the lack of information about the chemical composition of the imaged surface. Such information can be obtained by PEEM via tuning the photon energy to X-ray absorption edges. To apply spectromicroscopy we acquired and subtracted microscopic images using photon energies just below and at the edges. The resulting difference gives a micro-image of the lateral distribution of a specific element. Microspectroscopy is performed by recording the intensity of secondary electrons in…

RadiationPhotonMagnetic structurebusiness.industryChemistryAnalytical chemistryPhoton energyDichroismRadiationCondensed Matter PhysicsAtomic and Molecular Physics and OpticsSecondary electronsElectronic Optical and Magnetic MaterialsPhotoemission electron microscopyOpticsPhysical and Theoretical ChemistryAbsorption (electromagnetic radiation)businessSpectroscopyJournal of Electron Spectroscopy and Related Phenomena
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θ0 thermal Josephson junction

2017

We predict the thermal counterpart of the anomalous Josephson effect in superconductor/ferromagnet/superconductor junctions with non-coplanar magnetic texture. The heat current through the junction is shown to have the phase-sensitive interference component proportional to $\cos(\theta - \theta_0)$, where $\theta$ is the Josephson phase difference and $\theta_0$ is the texture-dependent phase shift. In the generic tri-layer magnetic structure with the spin-filtering tunnel barrier $\theta_0$ is determined by the spin chirality of magnetic configuration and can be considered as the direct manifestation of the energy transport with participation of spin-triplet Cooper pairs. In case of the id…

SuperconductivityJosephson effectPhysicsHeat currentJosephson junctionsCondensed matter physicsMagnetic structureta114Condensed Matter - Superconductivity02 engineering and technology021001 nanoscience & nanotechnologyCoupling (probability)conductors (matter)01 natural sciencesCooper pairsFerromagnetismCondensed Matter::Superconductivitymagnetism0103 physical sciencesCooper pair010306 general physics0210 nano-technologySpin-½Physical Review B
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Density Functional Theory Calculations On Magnetic Properties Of Actinide Compounds

2011

ABSTRACTWe have performed a detailed analysis of the magnetic (collinear and noncollinear) order and atomic and electron structures of UO2, PuO2 and UN on the basis of density functional theory with the Hubbard electron correlation correction (DFT+U). We have shown that the 3-k magnetic structure of UO2 is stabilized for the Hubbard parameter value of U=4.6 eV (while J=0.5 eV) when Dudarev’s formalism is used. UO2 keeps cubic shape in this structure. Two O atoms nearest to each U atom in direction of its magnetic moment move toward this U atom. Neither UN nor PuO2 shows the energetical preference for the rhombohedral distortion, in contrast to UO2, and, thus, no complex 3-k magnetic structu…

Tetragonal crystal systemMaterials scienceMagnetic momentCondensed matter physicsElectronic correlationMagnetic structureAtomDensity functional theoryElectronElectronic structureMRS Proceedings
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Neutron-scattering studies on CeM2Ge2(M=Ag, Au, and Ru)

1992

The results of elastic, quasielastic, and inelastic neutron-scattering studies on polycrystalline CeM 2 Ge 2 (M=Ag, Au, and Ru) are presented. All compounds reveal long-range magnetic order at low temperatures. Ferromagnetic (M=Ru), antiferromagnetic (M=Au), and incommensurate (M=Ag) structures were detected. Using time-of-flight (TOF) techniques, the crystalline electric-field splittings were determined. With high-resolution TOF experiments the temperature and wave-vector dependence of the magnetic relaxation rate was studied

chemistry.chemical_classificationElastic scatteringMaterials scienceCondensed matter physicsMagnetic structureNuclear TheoryAnalytical chemistryNeutron scatteringInelastic scatteringchemistryFerromagnetismAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsCrystalliteNuclear ExperimentInorganic compoundPhysical Review B
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Electronic and magnetic structure ofLa0.875Sr0.125MnO3calculated by means of hybrid density-functional theory

2007

We present the results of ab initio calculations on magnetic and electronic structures of La1�xSrxMnO3 at low doping, x =1/8. Using the B3LYP hybrid exchange-correlation functional within the framework of densityfunctional theory, we predict a ferromagnetic ground state for La0.875Sr0.125MnO3 in both the low-temperature orthorhombic and the high-temperature pseudocubic phases. This is in contrast to its parent compound LaMnO3, for which we find in agreement with experiment the layered antiferromagnetic state to be the most stable one. The calculated density of states and bond population analysis suggest a tendency of formation of half-metallic spin states in the band gap of both structures.

education.field_of_studyMaterials scienceCondensed matter physicsMagnetic structureSpin statesPopulationCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceAb initio quantum chemistry methodsDensity of statesAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsDensity functional theoryGround stateeducationPhysical Review B
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