β-HfCuGeA new polymorph of HfCuGe with a novel structure type

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Abstract

The structure and elementary physical properties of a new intermetallic compound, β-HfCuGe, are reported. β-HfCuGe has a tetragonal structure (space group I4/mmm) with lattice constants of a=3.7634(11)Å and c=13.499(4) Å. The structure, which consists of double layers of Hf stacked with edge-sharing CuGe4 squares, is not typical for intermetallic compounds and appears to be a new structure type. The compound is a weak paramagnet and a normal metal down to 0.4 K.

Graphical abstract

Crystal structure of β-HfCuGe (right) and the coordination of the different atoms in β-HfCuGe (left).

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Highlights

► Layered intermetallic compound. ► BCC Hf layers and square planar CuGe network. ► Metallic conductor and paramagnetic.

Introduction

There are four previously reported compounds in the Hf–Cu–Ge ternary system. The 1:1:1 compound HfCuGe crystallizes in the TiNiSi structure type (space group Pnma) [1], Hf2CuGe4 crystallizes in space group Cmcm [2], Cu4Hf3Ge2 crystallizes in the Fe2P structure type with the space group P6¯2m [3] and HfCuGe2 crystallizes in space group P4/nmm [4]. Among these, HfCuGe2 is a layered compound with alternating layers of Hf–Ge–Cu2–Ge–Hf–Ge2. Hf2CuGe4 also consists of layers but with a different stacking order. Fe2P-type Cu4Hf3Ge2 consists of alternating Cu–Ge and Cu–Hf layers. In none of these compounds are two layers of the same element adjacent. In the previously reported form of HfCuGe, which has the TiNiSi structure type, the layers include all three atom types. To the best of the authors’ knowledge the properties of those phases have not yet been reported.

Here we report the crystal structure and properties of a new phase in the Hf–Cu–Ge ternary system with the composition 1:1:1. This polymorph of HfCuGe crystallizes in a new structure type that is quite different from the known Hf–Cu–Ge compounds. The layers consist of edge sharing CuGe4 squares alternating with two Hf metal layers; both structural components are unusual for ternary intermetallic compounds.

Section snippets

Experimental details

Samples of β-HfCuGe were prepared by three different methods. The first of these was arc melting and annealing. Stoichiometric amounts of Hf (99.6%), Cu (99.99%) and Ge (99.9999%) pieces were arc melted in an argon atmosphere. A Zr sponge was co-heated in the system to bind remaining oxygen. The buttons were melted three times, and turned over after each melt process to yield homogeneous samples. The polycrystalline ingots obtained were annealed in an evacuated quartz tube at 900 °C for 2 week.

Results and discussion

β-HfCuGe appears as a gray-metallic bulk ingot. It is stable in air and water. Single crystal diffraction studies resulted in the determination of the structure in the tetragonal space group I4/mmm (No. 139) with the lattice constants a=3.7643(11) Å and c=13.499(4) Å. The crystallographic data are given in Table 1 and structural details are given in Table 2 [8]. The reflection intensity statistics could not reliably predict the space group of this novel structure, so it was initially solved in

Summary

We have reported a new polymorph of HfCuGe and discussed its crystallographic and physical properties. β-HfCuGe crystallizes in a structure with adjacent Hf layers and a square planar network of Cu and Ge. It shows metallic conductivity and is an intrinsic Pauli paramagnet with a low density of states at the Fermi level. The presence of adjacent Hf layers suggests that β-HfCuGe may form a hydride under the appropriate conditions.

Acknowledgments

This research was supported by the Department of Energy, Division of Basic Energy Sciences, Grant DE-FG02-98-ER45706.

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