Intermetallics of the types REPd3 X 2 and REPt3 X 2 (RE=La–Nd, Sm, Gd, Tb; X=In, Sn) with substructures featuring tin and In atoms in distorted square-planar coordination

Author:

Engelbert Simon1,Stegemann Frank1,Bönnighausen Judith1,Klenner Steffen1,Janka Oliver1,Pöttgen Rainer1

Affiliation:

1. Institut für Anorganische und Analytische Chemie , Universität Münster , Corrensstrasse 30, 48149 Münster , Germany

Abstract

Abstract The intermetallic compounds RET 3 X 2 (RE = La–Nd, Sm, Gd, Tb; T = Pd, Pt; X = In, Sn) have been synthesized from the elements by arc-melting and subsequent annealing sequences in tube or induction furnaces. The samples were characterized through Guinier powder diffraction patterns, and several structures were refined from single crystal X-ray diffractometer data. These indium and tin intermetallics crystallize with the orthorhombic CePd3In2-type structure, space group Pnma. The palladium (platinum) and indium (tin) atoms in the RET 3 X 2 structures build up complex three-dimensional [T 3 X 2] δ polyanionic networks in which the rare earth atoms fill cavities. The striking structural motifs concern the indium, respectively tin substructures, in which part of the indium and tin atoms have distorted square planar homoatomic coordination environments: In1In12In22 units in PrPd3In2 with interatomic distances 325 pm In1–In1 and 332 pm In1–In2 as well as Sn1Sn12Sn22 units in PrPt3Sn2 with the larger distances of 356 pm for Sn1–Sn1 and of 344 pm for Sn1–Sn2. Temperature dependent magnetic susceptibility measurements have indicated Pauli paramagnetism or diamagnetism for the lanthanum compounds, van-Vleck paramagnetism for SmPt3In2 and Curie-Weiss paramagnetism for the remaining compounds. Antiferromagnetic ordering was detected at T N = 4.0(1) K for CePt3In2 and at T N = 3.5(1) K for SmPt3In2. CePt3In2 shows a metamagnetic transition at an external magnetic field of 47(3) kOe.

Publisher

Walter de Gruyter GmbH

Subject

General Chemistry

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