Abstract

The electronic structure and magnetic ordering in La$_{1-x}$Pr$_x$Co$_2$P$_2$ ($x=$0, 0.25, and 1) phosphides have been studied theoretically using the fully relativistic spin-polarized Dirac linear muffin-tin orbital (LMTO) band-structure method. The X-ray absorption and X-ray magnetic circular dichroism spectra at the Co$L_{2,3}$ and Pr$M_{4,5}$ edges have been investigated theoretically within the framework of the LSDA+$U$ method. The core-hole effect in the final state as well as the effects of the electric quadrupole $E_2$ and magnetic dipole $M_1$ transitions have been investigated. Good agreement with experimental measurements has been found.

Highlights

  • Ternary intermetallics AT2X2, where A − alkali, alkali-earth, rare-earth, or actinide metal, T − transition metal, and X − nonmetal, often demonstrate intrinsically complex magnetic structures and a wide variety of physical properties

  • The spin magnetic moments at the Pr and Co sites are aligned along the c axis with the antiparallel magnetic coupling between the neighboring planes resulting in antiferromagnetism

  • The E2 transitions are much weaker than the electric dipole transitions E1. They are almost invisible in the XAS and have a very small effect on the XMCD spectra at the Pr M4,5 edges

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Summary

Introduction

Ternary intermetallics AT2X2, where A − alkali, alkali-earth, rare-earth, or actinide metal, T − transition metal, and X − nonmetal, often demonstrate intrinsically complex magnetic structures and a wide variety of physical properties They belong to the ThCr2Si2 structure type and can be conveniently represented as materials built by stacking covalently bonded transition metal-metalloid T2X2 layers, made of edge-sharing TX4 tetrahedra, with ionic A atoms. SmMn2Ge2 becomes ferromagnetic below 348 K and undergoes a transition to an antiferromagnetic state at 196 K, followed by a re-entrant ferromagnetic transition at 64 K [7] This peculiar magnetic behavior stems from the layered structure and the presence of two magnetic sublattices in these materials and was later observed for a number of rare-earth manganese germanides and silicides [8,9,10,11]. The isotypic phosphides were prepared much later [12] and the investigations of their magnetic properties have started only recently

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