Ivica Aviani

Kondo effect in Ce x La 1 − x Cu 2.05 Si 2 intermetallics

The magnetic susceptibility and susceptibility anisotropy of the quasibinary alloy system

Kondo effect inCexLa1−xCu2.05Si2intermetallics

{mathrm{Ce}}_{x}{mathrm{La}}_{1ensuremath{-}x}{mathrm{Cu}}_{2.05}{mathrm{Si}}_{2}

Kondo effect in CexLa1-xCu2.05Si intermetallics

have been studied for low concentration of Ce ions. The single-ion description is found to be valid for

MAGNETIC PROPERTIES OF CEXLA1-XCU2.05SI2

xl~0.09.

Spin-dimer-like Magnetic Coupling in the Infinite-chain Compound CA0.85CUO2

The experimental results are discussed in terms of the degenerate Coqblin-Schrieffer model with a crystalline electric field splitting ensuremath{Delta}ensuremath{simeq}330 K. The properties of the model, obtained by combining the lowest-order scaling and the perturbation theory, provide a satisfactory description of the experimental data down to 30 K. The experimental results between 20 K and 2 K are explained by the exact solution of the Kondo model for an effective doublet.

Reentrant quantum criticality in Yb2Pd2Sn

The magnetic susceptibility and susceptibility anisotropy of the quasibinary alloy system

Macroscopic and microscopic investigation of the antiferromagnetic phase of TbB6

{mathrm{Ce}}_{x}{mathrm{La}}_{1ensuremath{-}x}{mathrm{Cu}}_{2.05}{mathrm{Si}}_{2}

[M_6Br_(12)(H_2O)_6][HgBr_2X_2]×12H_2O, M = Nb, Ta, X = Cl, Br, I - Spojevi s poluvodičkim svojstvima

have been studied for low concentration of Ce ions. The single-ion description is found to be valid for

Magnetic properties of Ce x La 1- x Cu 2.05Si 2

xl~0.09.

Magnetic properties of YbInCu 4

The experimental results are discussed in terms of the degenerate Coqblin-Schrieffer model with a crystalline electric field splitting ensuremath{Delta}ensuremath{simeq}330 K. The properties of the model, obtained by combining the lowest-order scaling and the perturbation theory, provide a satisfactory description of the experimental data down to 30 K. The experimental results between 20 K and 2 K are explained by the exact solution of the Kondo model for an effective doublet.