Search results for "Susceptibility"

showing 10 items of 912 documents

Room-temperature paramagnetoelectric effect in magnetoelectric multiferroics Pb(Fe1/2Nb1/2)O3 and its solid solution with PbTiO3

2015

We have observed the magnetoelectric (ME) response at room temperature and above in high-resistive ceramics made of multiferroic Pb(Fe1/2Nb1/2)O3 (PFN) and PFN-based solid solution 0.91PFN-0.09PbTiO3 (PFN-PT). The value of the paramagnetoelectric (PME) coefficient shows a pronounced maximum near the ferroelectric-to-paraelectric phase transition temperature, T C, and then decreases sharply to zero for T > T C. The maximal PME coefficient in PFN is about 4 × 10−18 s/A. The theoretical description of the PME effect, within the framework of a Landau theory of phase transitions allowing for realistic temperature dependences of spontaneous polarization, dielectric and magnetic susceptibilities, …

Phase transitionMaterials scienceFOS: Physical sciences02 engineering and technologyDielectric01 natural sciencesCondensed Matter::Materials ScienceCondensed Matter::Superconductivity0103 physical sciencesGeneral Materials ScienceMultiferroicsCeramic010306 general physicsCondensed Matter - Materials ScienceCondensed matter physicsMechanical EngineeringMaterials Science (cond-mat.mtrl-sci)021001 nanoscience & nanotechnologyMagnetic susceptibilityLandau theoryMagnetic fieldMechanics of Materialsvisual_artvisual_art.visual_art_medium0210 nano-technologySolid solution
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Crystallographic, electronic structure and magnetic properties of the GdTAl; T=Co, Ni and Cu ternary compounds

2000

Abstract Single phase GdCoAl, GdCuAl and single crystal GdNiAl samples of good quality were synthesized. The electrical resistivity, magnetization and AC susceptibility as a function of temperature revealed in all these compounds a ferromagnetic ordering at 100, 83 and 60 K, respectively. A magnetic transition, probably to a non-colinear structure was observed in GdNiAl at 31 K as well as the presence of the third magnetic transition at 14 K, while in the GdCuAl compound an evidence of similar transition was found at 23 K. In GdNiAl a transition between two different crystallographic phases of ZrNiAl-type was observed at 220 K. The transition was accompanied by rapid jumps of crystal lattic…

Phase transitionMaterials scienceFermi levelCondensed Matter PhysicsMagnetic susceptibilityElectronic Optical and Magnetic MaterialsCrystallographyMagnetizationsymbols.namesakeTransition pointElectrical resistivity and conductivityDensity of statessymbolsCondensed Matter::Strongly Correlated ElectronsSingle crystalJournal of Magnetism and Magnetic Materials
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Anisotropies and magnetic phase transitions in insulating antiferromagnets determined by a Spin-Hall magnetoresistance probe

2019

Antiferromagnets possess a number of intriguing and promising properties for electronic devices, which include a vanishing net magnetic moment and thus insensitivity to large magnetic fields and characteristic terahertz frequency dynamics. However, probing the antiferromagnetic ordering is challenging without synchrotron-based facilities. Here, we determine the material parameters of the insulating iron oxide hematite, α-Fe2O3, using the surface sensitive spin-Hall magnetoresistance (SMR). Combined with a simple analytical model, we extract the antiferromagnetic anisotropies and the bulk Dzyaloshinskii-Moriya field over a wide range of temperatures and magnetic fields. Across the Morin phas…

Phase transitionMaterials scienceMagnetoresistanceQC1-999General Physics and AstronomyFOS: Physical sciencesLarge scale facilities for research with photons neutrons and ionslcsh:Astrophysics02 engineering and technologyPhysics and Astronomy(all)Astrophysics01 natural sciences0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)lcsh:QB460-466Antiferromagnetism010306 general physicsSpin (physics)AnisotropySpin-½Magnetic momentCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsPhysics021001 nanoscience & nanotechnologyMagnetic susceptibilitylcsh:QC1-999Magnetic fieldQB460-466Condensed Matter::Strongly Correlated Electrons0210 nano-technologylcsh:Physics
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High-Spin → Low-Spin Relaxation in [Fe(bpp)2](CF3SO3)2 H2O after LIESST and Thermal Spin-State Trapping—Dynamics of Spin Transition Versus Dynamics o…

1996

The iron(II) complex [Fe(bpp)2]-(CF3SO3)2 H2O (bpp = 2,6-bis(pyrazolyl-3-yl)pyridine) shows a thermal spin transition associated with a hysteresis of approximately 140 K width. The transition temperatures T1/2 (where the fraction of HS species γHS = 0.5) are 147 K and ≈285 K in the cooling and heating directions, respectively. The compound shows the LIESST and reverse-LIESST effects at low temperatures. The relaxation of the metastable HS states generated by LIESST was observed quantitatively at temperatures between 77.5 and 85 K by Mossbauer spectroscopy. Metastable HS states can also be generated by rapid cooling of the sample. The relaxation of the metastable HS states formed by thermal …

Phase transitionSpin statesChemistryOrganic ChemistryRelaxation (NMR)Analytical chemistrySpin transitionGeneral ChemistryMolecular physicsMagnetic susceptibilityCatalysisLIESSTSpin crossoverMetastabilityChemistry - A European Journal
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Spin crossover star-shaped metallomesogens of iron(II).

2014

Three new types of spin crossover (SCO) metallomesogens of Fe-II based on symmetric tripod ligands and their magnetic and structural properties are reported here. These were obtained by condensation of tris(2-aminoethyl)-amin (tren) with the aldehyde derived from 3-alkoxy-6-methylpyridine (mpyN, N (number of carbon atoms in n-alkyl chains) = 8, 18), 1-alkyl-1H-imidazole (imN, N = 4, 16, 18, 20, 22), or 1-alkyl-1H-benzimidazole (bimN, N = 6, 14, 16, 18, 20). A complex derived from 1-octadecyl-1H-naphtho[2,3-d]imidazole (nim18) retains the high spin state at any temperature. Single crystals of the short-chain complexes were investigated by a combination of X-ray crystallography, magnetic meas…

Phase transitionTHERMAL-BEHAVIORSpin statesMOSSBAUER-SPECTROSCOPYLIQUID-CRYSTALLINE PROPERTIESCalorimetryCOMPLEX-COMPOUNDSSERIESMAGNETIC-SUSCEPTIBILITYMagnetic susceptibilityPOLYMORPHISMInorganic ChemistryCrystalchemistry.chemical_compoundCrystallographyROOM-TEMPERATUREchemistrySpin crossoverFISICA APLICADAMössbauer spectroscopyPHASE-TRANSITIONImidazolePhysical and Theoretical ChemistryTHERMAL-BEHAVIOR; SYSTEMSYSTEMInorganic chemistry
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Magnetism and variable temperature and pressure crystal structures of a linear oligonuclear cobalt bis-semiquinonate

2016

The crystal structure of the first oligomeric cobalt dioxolene complex, Co3(3,5-DBSQ)2((t)BuCOO)4(NEt3)2, 1, where DBSQ is 3,5-di-tert-butyl-semiquinonate, has been studied at various temperatures between 20 and 200 K. Despite cobalt-dioxolene complexes being generally known for their extensive ability to exhibit valence tautomerism (VT), we show here that the molecular geometry of compound 1 is essentially unchanged over the full temperature range, indicating the complete absence of electron transfer between ligand and metal. Magnetic susceptibility measurements clearly support the lack of VT between 8 and 300 K. The crystal structure is also determined at elevated pressures in the range f…

Phase transitionValence (chemistry)010405 organic chemistryChemistryCrystal structure010402 general chemistry01 natural sciencesMagnetic susceptibility0104 chemical sciencesInorganic ChemistryCrystallographyTrigonal bipyramidal molecular geometryElectron transferMolecular geometryCoordination geometryDalton Transactions
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Polymorphism in a π stacked Blatter radical: structures and magnetic properties of 3-(phenyl)-1-(pyrid-2-yl)-1,4-dihydrobenzo[ e ][1,2,4]triazin-4-yl

2020

International audience; 3-(Phenyl)-1-(pyrid-2-yl)-1,4-dihydrobenzo[e][1,2,4]triazin-4-yl (2) demonstrates the first example of polymorphism in the family of Blatter radicals. Two polymorphs, 2α and 2β, have been identified and characterized by single crystal X-ray diffractometry and magnetic susceptibility measurements to investigate their magnetism–structure correlations. Both polymorphs form one-dimensional (1D) π stacks of evenly spaced radicals with distinctly different π–π overlap modes. Within the 1D π stacks, radicals are located at evenly interplanar distances, 3.461 Å for 2α and 3.430 Å for 2β. Magnetic susceptibility studies indicate that both polymorphs exhibit antiferromagnetic …

Phase transitionmagneettiset ominaisuudetMaterials scienceSpins010405 organic chemistry[CHIM.ORGA]Chemical Sciences/Organic chemistryRadicalGeneral Chemistryvapaat radikaalitkiteet010402 general chemistryCondensed Matter Physics01 natural sciencesMagnetic susceptibility0104 chemical sciencesCrystallographyPolymorphism (materials science)[CHIM.CRIS]Chemical Sciences/CristallographyAntiferromagnetismGeneral Materials ScienceSingle crystalQuantumorgaaniset yhdisteet
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Analytical representations for relaxation functions of glasses

2002

Analytical representations in the time and frequency domains are derived for the most frequently used phenomenological fit functions for non-Debye relaxation processes. In the time domain the relaxation functions corresponding to the complex frequency dependent Cole-Cole, Cole-Davidson and Havriliak-Negami susceptibilities are also represented in terms of $H$-functions. In the frequency domain the complex frequency dependent susceptibility function corresponding to the time dependent stretched exponential relaxation function is given in terms of $H$-functions. The new representations are useful for fitting to experiment.

PhysicsCondensed Matter - Materials ScienceMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesFunction (mathematics)Disordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsExponential functionFrequency domainMaterials ChemistryCeramics and CompositesRelaxation (physics)Time domainStatistical physicsSusceptibility function
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Strongly interacting matter under external magnetic fields within nonlocal NJL-type models

2017

We study the behavior of strongly interacting matter under an external magnetic field in the context of nonlocal Nambu-Jona-Lasinio (NJL) -like models. We find that at zero temperature the condensates display the well-known Magnetic Catalysis effect, showing a good quantitative agreement with lattice QCD (LQCD) results. Moreover, when extended to finite temperature we find that (contrary to what happens in the local NJL model) the Inverse Magnetic Catalysis (IMC) effect is naturally incorporated. We also analyze the magnetic susceptibility of the QCD vacuum in the limit of small magnetic field, considering two different model parametrizations, and compare our numerical results to those obta…

PhysicsCondensed matter physics010308 nuclear & particles physicsMagnetic catalysisPhysicsQC1-999QCD vacuumHigh Energy Physics::PhenomenologyFísicaInverseContext (language use)Lattice QCD01 natural sciencesMagnetic susceptibilityMagnetic fieldQuantum electrodynamics0103 physical sciencesHadronic systemsLimit (mathematics)010306 general physicsCiencias ExactasMagnetic catalysis effectEPJ Web of Conferences
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Structure-property relations in the distorted ordered double perovskite Sr2InReO6

2011

The rock-salt ordered type double perovskite Sr${}_{2}$InReO${}_{6}$ is systematically investigated by means of powder x-ray diffraction, neutron powder diffraction, temperature-dependent electrical transport, heat capacity and magnetic susceptibility measurements, and electronic band structure calculations. The crystal structure of Sr${}_{2}$InReO${}_{6}$ is revised to be monoclinic (cryolite structure type, space group $P$2${}_{1}$/$n$) with all structural distortions according to the high-symmetry aristotype due to tilting of the InO${}_{6}$ and ReO${}_{6}$ octahedra, respectively. Sr${}_{2}$InReO${}_{6}$ is a Mott insulator with variable-range hopping. Two 5$d$ electrons are unpaired an…

PhysicsCondensed matter physicsAntiferromagnetismElectronic structureCrystal structureType (model theory)Condensed Matter PhysicsElectronic band structureMagnetic susceptibilityHeat capacityElectronic Optical and Magnetic MaterialsMonoclinic crystal systemPhysical Review B
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