Alim Ormeci

Magnetic and structural transitions in layered iron arsenide systems: AFe2As2 versus RFeAsO

Resistivity, specific-heat, and magnetic-susceptibility measurements performed on

Strong coupling between magnetic and structural order parameters in SrFe2As2

{\text{SrFe}}_{2}{\text{As}}_{2}

AFe2As2 (A = Ca, Sr, Ba, Eu) and SrFe2-xTMxAs2 (TM = Mn, Co, Ni): crystal structure, charge doping, magnetism and superconductivity

samples evidence a behavior very similar to that observed in LaFeAsO and

Crystal structure and transport properties of Ba8Ge43□3

{\text{BaFe}}_{2}{\text{As}}_{2}

High temperature thermoelectric properties of the type-I clathrate Ba8NixGe46-x-ysquarey

, with the difference being that the formation of the spin-density wave and the lattice deformation occur in a pronounced first-order transition at

Synthesis, Crystal Structure, and Physical Properties of the Type-I Clathrate Ba8−δNix□ySi46–x–y

{T}_{0}=205\text{ }\text{K}

Dumbbells of Five-Connected Silicon Atoms and Superconductivity in the Binary Silicides MSi3 (M = Ca, Y, Lu)

. Comparing further data evidences that the Fe magnetism is stronger in

Synthesis of the intermetallic clathrate Na2Ba6Si46 by oxidation of Na2BaSi4 with HCl

{\text{SrFe}}_{2}{\text{As}}_{2}

Dumbbells of Five-Connected Ge Atoms and Superconductivity in CaGe3

and in

Preparation, phase stability and structure of the C36 Laves phase Nb1-xCo2+x

{\text{EuFe}}_{2}{\text{As}}_{2}