0000000000181537

AUTHOR

G. Sparn

showing 6 related works from this author

LOCAL-MOMENT AND ITINERANT ANTIFERROMAGNETISM IN THE HEAVY-FERMION SYSTEM CE(CU1-XNIX)2GE2

1992

Elastic and inelastic neutron-scattering studies on the system Ce(Cu1−xNix)2Ge2 are reported. These measurements are complemented by measurements of the magnetic susceptibility, high-field magnetization, heat capacity, thermal expansion, electrical resistivity and thermopower. The results reveal an interesting T-x phase diagram consisting of two different antiferromagnetic phases for x 0.5. Further experimental evidence for different types of antiferromagnetic ordering derives from a line-shape analysis of the quasielastic neutron-scattering intensity, from magnetization and thermopower experiments.

MagnetizationMaterials scienceCondensed matter physicsMagnetismElectrical resistivity and conductivityNeutron diffractionGeneral Physics and AstronomyAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsHeat capacityMagnetic susceptibilityPhase diagram
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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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Alloying experiments on heavy fermion compounds

1990

Abstract This paper is intended to demonstrate the usefulness of controlled alloying for the understanding of heavy-fermion physics: (1) Th-substitution for Ce in CeCu2Si2 emphasizes the dominating role of the dopant-induced strain fields in generating incoherent scattering and pair breaking, (2) replacement of Cu by Ni in Ce(Cu1-xNix)2Ge2 leads to phenomena which are interpreted as derived from a transition between local-moment and itinerant heavy-fermion magnetism, and (3) increasing Cu concentration in UCu4+xAl8-x is accompanied by an antiferromagnetic to nonmagnetic transition near xcr = 1.5 similar to what has been found before for several Ce-based systems. A heavy Fermi-liquid phase w…

Materials scienceCondensed matter physicsMagnetismHeavy fermionIncoherent scatterQuasiparticleAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCoherence (physics)
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Instabilities in heavy-fermion systems

1992

Abstract We review (i) an itinerant antiferromagnetic phase transition below 4 K in Ni-rich Ce(Cu 1− x Ni x ) 2 Ge 2 systems, (ii) the coincidence at T = 0.63 K of both a structural lattice instability in “as-grown” (non-superconducting) CeCu 2 Si 2 single crystals and bulk superconductivity in annealed ones as well as (iii) antiferromagnetic and superconducting transitions at T N = 4.6 K and T c = 1 K, respectively, in the heavy-fermion compound UNi 2 Al 3 .

SuperconductivityPhysicsPhase transitionCondensed matter physicsCondensed Matter::SuperconductivityLattice (order)Heavy fermionAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsCondensed Matter PhysicsInstabilityElectronic Optical and Magnetic Materials
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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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Magnetic order in the heavy fermion system Ce(Cu1−xNix)2Ge2

1990

Abstract The magnetic phase diagram of the heavy fermion (HF) systems Ce(Cu 1−x Ni x ) 2 Ge 2 is discussed utilizing results of transport, thermodynamic and neutron-scattering measurements. While the Kondo temperature increases monotonically with x, a complex x-dependence is found for the Neel temperature, associated with a transition from local-moment to itinerant HF magnetism.

PhysicsCondensed matter physicsMagnetismMagnetic orderMonotonic functionCondensed Matter PhysicsMagnetic phase diagramElectronic Optical and Magnetic MaterialsHeavy fermionOrder (group theory)Condensed Matter::Strongly Correlated ElectronsElectrical and Electronic EngineeringNéel temperatureMagnetic impurityPhysica B: Condensed Matter
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