Search results for "FERROMAGNET"

showing 10 items of 995 documents

High-spin polarization of Heusler alloys

2006

Fermi surface of a half-metal compound with cubic Fm–3m symmetry: Heusler alloy or double perovskite.The inset shows the spin resolved density of state for a CCFA Heusler compound. ( This illustration appears on the cover of the print edition. ) This cluster issue of Journal of Physics D: Applied Physics is devoted to magnetic Heusler alloys. This class of materials is currently considered to contain the most attractive half-metallic ferromagnets due to their high Curie temperatures and their structural relation to conventional semiconductors. The first compound to be identified as a half-metallic ferromagnet, by de Groot et al back in 1983, was the half-Heusler alloy NiMnSb. After a period…

Acoustics and UltrasonicsCondensed matter physicsMagnetoresistanceSpin polarizationChemistryFermi surfaceengineering.materialCondensed Matter PhysicsHeusler compoundSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsMagnetizationFerromagnetismengineeringCurie temperatureHalf-metal
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Off-stoichiometry in Co2FeSi thin films sputtered from stoichiometric targets revealed by nuclear magnetic resonance

2009

Co2FeSi is predicted to be a half-metallic ferromagnet with an extraordinary high magnetic moment and Curie temperature. However, a low tunnel magneto-resistance ratio, a lower spin polarization and a lower magnetic moment were experimentally observed in thin film samples. Consequently, thin Co2FeSi films of different groups were studied using spin-echo nuclear magnetic resonance (NMR). NMR probes the local hyperfine fields of the active atoms, which strongly depend on the local environment. NMR is thus able to reveal the next neighbouring shells of the Co-59 nuclei in the Co2FeSi thin films. As expected, our NMR study shows the main resonance line corresponding to Co-59 nuclei in the L2(1)…

Acoustics and UltrasonicsMagnetic momentCondensed matter physicsSpin polarizationChemistryResonanceCondensed Matter PhysicsFerromagnetic resonanceSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceNuclear magnetic resonanceSpin echoCurie temperatureCondensed Matter::Strongly Correlated ElectronsThin filmHyperfine structureJournal of Physics D: Applied Physics
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High spin polarization in Co2CrAl–Cr superlattice

2009

The electronic structure, magnetic properties and interface effects in Co2CrAl?Cr superstructures have been investigated by the use of first principle calculations. The results show that at the interface, a large magnetic moment and a high spin polarization can be induced by a strong ferromagnetic exchange interaction at the Cr?Co interface. However, at the CrAl?Cr interface, both the magnetic moment and the spin polarization of the Cr atoms are decreased due to a Cr?Cr antiferromagnetic interaction. It can also be found that the interface effect is only a short range effect. So, high spin polarization in Co2CrAl?Cr superlattice can be obtained. Based on this theoretical analysis, a large g…

Acoustics and UltrasonicsSpin polarizationCondensed matter physicsMagnetic momentMagnetoresistanceChemistryMagnetismSuperlatticeGiant magnetoresistanceCondensed Matter PhysicsSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceFerromagnetismAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsComputer Science::DatabasesJournal of Physics D: Applied Physics
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Ferromagnetic gyroscopes for tests of fundamental physics

2020

A ferromagnetic gyroscope (FG) is a ferromagnet whose angular momentum is dominated by electron spin polarization and that will precess under the action of an external torque, such as that due to a magnetic field. Here we model and analyze FG dynamics and sensitivity, focusing on practical schemes for experimental realization. In the case of a freely floating FG, we model the transition from dynamics dominated by libration in relatively high externally applied magnetic fields, to those dominated by precession at relatively low applied fields. Measurement of the libration frequency enables in situ measurement of the magnetic field and a technique to reduce the field below the threshold for w…

Angular momentumgyroscopePhysics and Astronomy (miscellaneous)Field (physics)Atomic Physics (physics.atom-ph)Materials Science (miscellaneous)physics beyond the standard modelFOS: Physical sciencesApplied Physics (physics.app-ph)01 natural sciences530Physics - Atomic Physics010305 fluids & plasmasMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesLibrationddc:530Electrical and Electronic Engineering010306 general physicsLarmor precessionSuperconductivityPhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsMeissner effectFerromagnetism gyroscope physics beyond the standard model Meissner effectPhysics - Applied PhysicsferromagnetismAtomic and Molecular Physics and OpticsMagnetic fieldMeissner effectFerromagnetismPrecessionQuantum Physics (quant-ph)
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Dynamic magnetic materials based on the cationic coordination polymer [Cu(btix)2]n(2n+) [btix = 1,4-bis(triazol-1-ylmethyl)benzene]: tuning the struc…

2012

A three-dimensional coordination polymer, [Cu(btix)(2)(BF(4))(2)](n) [btix = 1,4-bis(triazol-1-ylmethyl)benzene], with antiferromagnetic interactions occurring via the organic ligand, has been prepared and characterized. It has been shown to permit the exchange of anionic species in the crystalline network with modification of the magnetic properties. Coordinated BF(4)(-) can be reversibly exchanged by different anions with (NO(3)(-) and Cl(-)) or without (PF(6)(-) and ClO(4)(-)) dynamic response of the organic ligand, which acts as the only linker between the metal centers. Interestingly, an irreversible exchange occurs with N(3)(-) anions to generate a new coordination polymer, [Cu(btix)(…

AnionsModels MolecularIon exchangeMolecular StructureLigandCoordination polymerPolymersInorganic chemistryCationic polymerizationAb initioCrystallography X-RayMagnetic susceptibilitylaw.inventionInorganic Chemistrychemistry.chemical_compoundCrystallographyMagnetic FieldschemistrylawCationsOrganometallic CompoundsAntiferromagnetismPhysical and Theoretical ChemistryElectron paramagnetic resonanceCopperInorganic chemistry
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Influence of the anions on the structure and magnetic properties of a series of bis(µ-diphexono)-bridged linear trinuclear copper(II) complexes: an e…

2011

The reaction of H(2)L (N,N'-dimethyl-N,N'-bis(2-hydroxy-3-methoxy-5-methylbenzyl)-ethylenediamine) with different copper salts, in methanol and using a H(2)L/Cu = 2 : 3 molar ratio, led to four new bis(μ-diphenoxo)-bridged Cu(3) complexes of general formula [{Cu(S)(μ-L)}(2)Cu(H(2)O)(2n)]X(2) (S = CH(3)OH, n = 1 and X = BF(4)(-) for (1) or ClO(4)(-) for (2); S = Br(3)(-) anion and n = 1 without any X species for (3); S = H(2)O, n = 0 and X = NO(3)(-) for (4)). The use in the same reaction conditions of 4,4'-bipyridine (4,4'-bipy) as connector led to the chain complex [{Cu(μ-4,4'-bipy)(0.5)(μ-L)}(2)Cu(H(2)O)(2n)](ClO(4))(2)·17H(2)O (5). The structure of the centrosymmetric trinuclear unit in …

AnionsSteric effectsChemistryInorganic chemistryMolecular Conformationchemistry.chemical_elementEthylenediamineModels TheoreticalCrystallography X-RayCopperMagnetic susceptibilityInorganic ChemistryMetalMagneticsCrystallographychemistry.chemical_compoundCoordination Complexesvisual_artOctahedral molecular geometryAtomvisual_art.visual_art_mediumAntiferromagnetismta116CopperDalton Transactions
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Spin Frustration in Triangular Cu 3 II Complexes with 6‐Methyl‐2‐pyridyloxime as Ligand – Synthesis, Structural, and Magnetic Characterization

2013

In the present work, new examples of μ3-OH/oximato Cu3 triangles have been obtained by treatment of different copper salts with 6-methyl-2-pyridylaldoxime [6-MepyC(H)NOH, 6-mepaoH]. Depending on the anion, the compounds [Cu3(OH)(6-mepao)3(O2CPh)2] (1), [Cu6(OH)2(6-mepao)6(NO3)3](NO3)·H2O (2·H2O) and [Cu6(OH)2(6-mepao)6(ClO4)3](ClO4) (3) formed and were characterized. Complex 1 is an isolated triangle, whereas 2 and 3 are hexanuclear compounds with two triangular subunits linked by anionic bridges. Susceptibility measurements show very strong antiferromagnetic interactions and the presence of antisymmetric exchange at low temperature. The magnetic properties of these frustrated triangles hav…

Antisymmetric exchangeLigandChemistrymedia_common.quotation_subjectFrustrationchemistry.chemical_elementCopperlaw.inventionInorganic ChemistryMagnetizationCrystallographyNuclear magnetic resonancelawAntiferromagnetismSpin (physics)Electron paramagnetic resonancemedia_commonEuropean Journal of Inorganic Chemistry
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[Mnii2(bpym)(H2O)8]4+ and [Miv(CN)8]4– (M = Mo and W) as building blocks in designing bpym- and cyanide-bridged bimetallic three-dimensional networks…

2002

One-pot reaction between the dinuclear [MnII2(bpym)(H2O)8]4+ complex and the mononuclear [MIV(CN)8]4− unit (M = Mo and W; bpym = 2,2′-bipyrimidine) in aqueous solution yields the novel heterobimetallic complexes of formula {(μ-bpym)[Mn(H2O)]2-(μ-NC)6M(CN)2} with M = Mo (1) and W (2). 1 and 2 are isostructural three-dimensional compounds where the manganese atoms are bridged by bisbidentate bpym and hexakismonodentate octacyanometalate units. Variable-temperature magnetic susceptibility data of 1 and 2 show the occurrence of a significant antiferromagnetic coupling between the high spin manganese(II) ions through bridging bpym (Jca. −1.1 cm−1, the exchange Hamiltonian being defined as H = −J…

Aqueous solutionCyanidechemistry.chemical_elementGeneral ChemistryManganeseMagnetic susceptibilityCatalysisAntiferromagnetic couplingchemistry.chemical_compoundCrystallographychemistryComputational chemistryMaterials ChemistryIsostructuralBimetallic stripNew Journal of Chemistry
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Oxalate and 2,2′-bipyrimidine as bis-chelating ligands in the honeycomb layered compound {[Fe2(bpym)(ox)2]·5H2O}n

2002

The novel two-dimensional iron(II) compound of formula {[Fe2(bpym)(ox)2]·5H2O}n (1) [bpym = 2,2′-bipyrimidine and ox = oxalate dianion] is obtained by reaction of oxalic acid, iron(II) chloride and 2,2′-bipyrimidine in aqueous solution. The structure of 1 is made up of oxalato-bridged iron(II) chains cross-linked by bischelating bpym affording a honeycomb lattice. Variable-temperature magnetic susceptibility data of 1 show the occurrence of relatively large antiferromagnetic interactions between the high spin iron(II) ions separated by more than 5.5 A through bridging bpym [Jbpym = −4.0(2) cm−1] and ox [Jox = ca. −7.8(2) cm−1] ligands. These values compare well with those obtained in the ir…

Aqueous solutionDenticityChemistryLigandInorganic chemistryOxalic acidGeneral ChemistryChlorideMagnetic susceptibilityCatalysisOxalateCrystallographychemistry.chemical_compoundMaterials ChemistrymedicineAntiferromagnetismmedicine.drugNew Journal of Chemistry
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2D and 3D coordination polymers based on 2,2′-bipyrimidine and cyanide bridging ligands incorporating coordinated and guest ammonia molecules. Synthe…

2005

The coordination polymers {[Ni(CN)4]2[(Ni(NH3)2)2(bpym)]·2H2O}n1 and {[Cu2(CN)2(bpym)]·NH3}n2 have been prepared from the reactions of M(NO3)2·nH2O [Cu(II), n = 3 and M = Ni(II), n = 6] with NaCN and bpym (2,2′-bipyrimidine) in concentrated aqueous ammonia, respectively. The structure of 1 is made of bipyrimidine bridged centrosymmetric dinuclear [Ni(NH3)2(μ-bpym)Ni(NH3)2] fragments connected by four [Ni(CN)4]2− anions giving rise to a 2D framework. Layers, which adopt a stair-like conformation, are stacked with an ABAB… repeat pattern. Water molecules are located in the interlayer space and are involved in hydrogen bond interactions with the non-bridging cyanide groups of the [Ni(CN)4]2− a…

Aqueous solutionHydrogen bondChemistryCyanideInorganic chemistryGeneral ChemistryCrystal structureCatalysisIonCrystallographychemistry.chemical_compoundOctahedronMaterials ChemistryAntiferromagnetismMoleculeNew Journal of Chemistry
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