Search results for "Magnetization"

showing 10 items of 550 documents

Multiferroics by Rational Design: Implementing Ferroelectricity in Molecule-Based Magnets

2012

Multiferroics (MF) are materials that exhibit simultaneouslyseveral ferroic order parameters. Among the multiferroicmaterials, those combining antiferro- or ferroelectricity (FE)and antiferro-, ferri-, or ferromagnetism (FM) within thesame material are highly desirable: the coexistence of thepolar and magnetic orders paves the way towards four-levelmemories while their interactions through the magnetoelec-tric effect makes it possible to control the magnetization byelectric fields and hence to develop electronically tuneablemagnetic devices, which are an essential feature for spin-tronics.

PhysicsMolecular magnetsCondensed matter physics010405 organic chemistryRational designGeneral MedicineGeneral Chemistry010402 general chemistry01 natural sciencesFerroelectricity[ CHIM ] Chemical SciencesCatalysis0104 chemical sciencesMagnetizationNuclear magnetic resonanceFerromagnetism[CHIM]Chemical SciencesMultiferroicsMolecule-based magnets
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Crystal time-reversal symmetry breaking and spontaneous Hall effect in collinear antiferromagnets

2020

Identification of a previously overlooked spontaneous Hall effect mechanism creates opportunities in low-dissipation spintronics.

PhysicsMultidisciplinaryCondensed matter physicseducationMaterials ScienceSciAdv r-articles02 engineering and technologyCondensed Matter PhysicsCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnology01 natural sciencesSymmetry (physics)CrystalMagnetizationFerromagnetismT-symmetryHall effect0103 physical sciencesAntiferromagnetismSymmetry breaking010306 general physics0210 nano-technologypsychological phenomena and processesResearch ArticlesResearch ArticleScience Advances
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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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Erratum to: “A quark model analysis of orbital angular momentum” [Phys. Lett. B 460 (1999) 8–16]

2000

PhysicsNuclear and High Energy PhysicsAngular momentumTotal angular momentum quantum numberQuantum electrodynamicsAngular momentum couplingOrbital motionRotational transitionAngular momentum operatorOrbital magnetizationAzimuthal quantum numberPhysics Letters B
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Neutron Fermi liquids under the presence of a strong magnetic field with effective nuclear forces

2009

Landau's Fermi liquid parameters are calculated for non-superfluid pure neutron matter in the presence of a strong magnetic field at zero temperature. The particle-hole interactions in the system, where a net magnetization may be present, are characterized by these parameters in the framework of a multipolar formalism. We use either zero- or finite-range effective nuclear forces to describe the nuclear interaction. Using the obtained Fermi liquid parameters, the contribution of a strong magnetic field on some bulk magnitudes such as isothermal compressibility and spin susceptibility is also investigated.

PhysicsNuclear and High Energy PhysicsFermi contact interactionNuclear TheoryCondensed matter physicsFOS: Physical sciencesFísicaQuantum oscillationsNuclear matterNuclear Theory (nucl-th)MagnetizationNuclear forceNeutronFermi liquid theoryFermi gas
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Atomic beam magnetic resonance apparatus for systematic measurement of hyperfine structure anomalies (Bohr-Weisskopf effect)

1993

Abstract An atomic beam magnetic resonance (ABMR) apparatus has been constructed at Orsay, and has been installed at the CERN PS Booster ISOLDE mass separator facility for “on-line” work with radioactive isotopes in a program to measure hyperfine structure anomalies (the Bohr-Weisskopf effect) over long isotopic chains. The hfs anomalies result from the effect of the spatial distribution of the nuclear magnetization on the atomic hfs interaction. Constructional details of the system are described: emphasis is placed on the measurement of nuclear g-factors by a triple resonance, laser state selected, ABMR method. A precision better than 10−4 for gI values has been obtained in stable atomic b…

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementThermal ionizationMass spectrometryLaserlaw.inventionBohr modelNuclear physicsMagnetizationsymbols.namesakechemistrylawCaesiumsymbolsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsDetectors and Experimental TechniquesAtomic physicsNuclear ExperimentInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Systematic measurements of the bohr-weisskpf effect at isolde

1992

The hyperfine anomaly gives an insight into the coupling of spin and orbital magnetic moments in the nucleus. More precisely, the nuclear magnetization is expressible through the nuclear wave functions with which is tested not only the magnetic moment operator, but also the tensor product [s×C2]1. The experiment can then be expected to be of value in testing the nuclear structure theory. The greatest value of these measurements is gained when these are made systematically over a large number of isotopes. We propose to initiate a program at ISOLDE to measure the hyperfine anomaly systematically in the heavy alkali elements. The experimental setup to achieve, in particular, a precise measurem…

PhysicsNuclear and High Energy PhysicsMagnetic momentNuclear structureCondensed Matter PhysicsAtomic and Molecular Physics and OpticsBohr modelNuclear physicsMagnetizationsymbols.namesakeNuclear magnetic momentsymbolsPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsAnomaly (physics)Nuclear ExperimentSpin (physics)Hyperfine structureHyperfine Interactions
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Magnetic dipole moments near 132Sn: new measurement on 135I by NMR/ON

1998

Abstract On-line low temperature nuclear orientation (OLNO) experiments have been performed on the isotope 135 I using the technique of nuclear magnetic resonance on oriented nuclei (NMR/ON). The magnetic moment of the 7 2 + ground state has been measured to be μ( 7 2 + 135 I ) = 2.940(2) μ N , thereby extending the known data on these states in odd- A I isotopes up to the neutron shell closure at N = 82. Shell-model calculations have been performed for the magnetic moments of 7 2 + states in the N = 82 isotones using free-nucleon and effective g -factors. The effective g -factors are obtained from a perturbation calculation that includes corrections for core polarisation and meson-exchange…

PhysicsNuclear and High Energy PhysicsMagnetizationMagnetic energyMagnetic momentNeutron magnetic momentProton magnetic momentNuclear TheoryNuclear magnetic momentAtomic physicsNuclear ExperimentMagnetic dipoleElectron magnetic dipole momentNuclear Physics A
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The magnetic shielding for the neutron decay spectrometer aSPECT

2014

Abstract Many experiments in nuclear and neutron physics are confronted with the problem that they use a superconducting magnetic spectrometer which potentially affects other experiments by their stray magnetic field. The retardation spectrometer a SPECT consists, inter alia, of a superconducting magnet system that produces a strong longitudinal magnetic field of up to 6.2 T. In order not to disturb other experiments in the vicinity of a SPECT, we had to develop a magnetic field return yoke for the magnet system. While the return yoke must reduce the stray magnetic field, the internal magnetic field and its homogeneity should not be affected. As in many cases, the magnetic shielding for a S…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectromagnetMagnetic energyDemagnetizing fieldForce between magnetsFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)law.inventionComputational physicsNuclear physicsMagnetizationlawMagnetElectromagnetic shieldingMagnetic pressureNuclear Experiment (nucl-ex)InstrumentationNuclear Experiment
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Magnetic hyperfine anomaly in muonic193Ir

1977

The nuclear decay of the 5/2+ 139 keV state to the 3/2+ ground state was observed in muonic193Ir. The hyperfine splitting of the 3/2+ state and 5/2+ state was determined to be 640±100 eV and 1280±160 eV, respectively. The ground state splitting is about twice that of a point nucleus, an anomaly never observed this large. This is mainly due to the different radial distribution of spin and orbital magnetization of a d3/2 proton configuration for which these contributions nearly cancel to zero in the magnetic moment. But calculations including configuration mixing and coupling to a vibrating or a deformed core show deviations. The groundstate anomaly is in line with that observed by the Mossba…

PhysicsNuclear and High Energy PhysicsProtonMagnetic momentCondensed Matter PhysicsAtomic and Molecular Physics and OpticsMössbauer spectroscopyPhysical and Theoretical ChemistryAtomic physicsAnomaly (physics)Spin (physics)Ground stateOrbital magnetizationHyperfine structureHyperfine Interactions
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