Structural properties of two deuterides LaY2Ni9D12.8 and CeY2Ni9D7.7 determined by neutron powder diffraction and X-ray absorption spectroscopy

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Abstract

The crystal structure of two deuterides RY2Ni9Dx (R=La; x=12.8 and R=Ce; x=7.7) have been investigated by means of neutron powder diffraction and X-ray absorption spectroscopy. The structures are best described in the space group R3̄m. The deuterium location has been determined for both compounds. The nature and the occupancy factors of the different D sites are presented. Comparisons are made between the La-based deuteride and the Ce-one in relation with the crystal structure of the intermetallic compounds. Differences in site occupancies within the RM2 and RM5 building units of the PuNi3-type structure are discussed and heterogeneous mixed valence state is reported for the cerium compound.

Introduction

Intermetallic compounds RMn (R=rare earth or transition metal, M=transition metal, n=1, 2, 3 or 5) are able to store reversibly large amount of hydrogen and are potential materials for energy storage either by solid-gas [1], [2] or electrochemical routes [3], [4]. Nowadays, new interests are devoted to RM3-type compounds with the recent discovery of new compounds in ternary systems like RM2Ni9 (R=rare earth or Ca; M=Mg, Ca, Ti or Y) [5], [6], [7], [8], [9], [10], [11]. These compounds crystallize in an ordered variant of the PuNi3-type rhombohedral structure (R3̄m space group) [12] and can be described as a stacking of CaCu5 (Haucke phase) and MgZn2 (Laves phase) units [13] as shown in Fig. 1. Few hydrides have been investigated from a structural point of view in the RM3 family. For the RNi3 system (R=Ho, Er, Y), the PuNi3-type structure is generally preserved upon hydrogenation and neither decomposition nor structural changes are reported. From the neutron diffraction (ND) analysis of HoNi3D1.8, Burnasheva et al. [14] found two occupied sites: 71% of the deuterium lies in the interstice 18h1 and the remaining atoms are located in the site 6c1. However, for CeNi3H3 the hydride phase is formed with a huge uniaxial expansion of the cell (δa/a=−0.80%, δc/c=30.76%) [15]. Recently, Yartys and coworkers [16], [17] found an orthorhombic symmetry lowering into Pmcn space group for the deuteride CeNi3D2.7 and reported that deuterium was located only within the CeNi2 units. In the RCo3 system, two homogeneity domains are reported for YCo3. The beta phase YCo3Dx exists for 1⩽x⩽1.9 and was described in the R3̄m space group by Benham et al. [18] with significant uniaxial volume expansion (δa/a=−0.07%, δc/c=9.72%) attributed to the filling of the RM2 units only. Indeed, all deuterium atoms were found in the tetrahedral site 36i1 in agreement with the exclusive hydrogenation of RM2 units. The gamma phase YCo3D3.8 was investigated by Bartashevich [19]. Less anisotropic volume expansion was observed (δa/a=4.44%, δc/c=8.27%) and, in addition to the site 36i1 reported for the beta phase, significant occupations for sites 18h2 and 36i2 within the RM5 units were found. A small orthorhombic distortion comparable to that observed in RCo5 hydrides [20] was also reported. According to these works, it is expected that the beta phase corresponds to the filling of the RM2 units followed by the filling of the RM5 units in the gamma phase.

To our knowledge, no structural data have been reported so far on ternary RM2Ni9-type deuterides. In this paper, we will present the structural properties of the two deuterides LaY2Ni9D12.8 and CeY2Ni9D7.7 determined by neutron powder diffraction (NPD) and X-ray absorption spectroscopy (XAS). Differences in site occupancies within the RM2 and RM5 building units of the PuNi3-type structure are also discussed.

Section snippets

Experimental

The alloys RY2Ni9 (R=La, Ce) were prepared following the procedure described in [10]. Metallographic examination, powder X-ray diffraction experiments (XRD) (Bruker AXS D8 θ–θ diffractometer, CuKα radiation, flat plate, Bragg–Brentano geometry, 2θ-range 20–120°, step size 0.02°, backscattered rear graphite monochromator) and elemental analysis by electron probe micro-analysis (EPMA) were performed to check the homogeneity of the alloys. Deuterated samples have been loaded by solid–gas reaction

Results

The compositions of the alloys obtained by EPMA (see Table 1) are homogeneous and close to the nominal ones. XRD analysis confirms that both samples are single phase and adopt the rhombohedral PuNi3-type structure as previously described in [10].

This structure can be described as an intergrowth between RM5 unit (Haücke phase) and RM2 (Laves phase) ones. Among the two available crystallographic sites for R atoms, lanthanum occupies preferentially the site 3a leading to an ordered ternary

Discussion

The ternary compound LaY2Ni9 absorbs more than 1 D/metal, a value very close to the mean one generally observed in other metallic hydrides. Deuterium is equally distributed within the RMi units and the cell volume expansion is isotropic. The overall δV/Vs (around 26%) are in agreement with value observed in metallic hydrides. If one looks to the nature of the deuterium occupied sites, it is worth to note that they are very similar to those reported for the binary compounds: 4h, 6m, 12n and 12o

Conclusions

The crystal structure of the two deuterides LaY2Ni9D12.8 and CeY2Ni9D7.7 have been determined. It is observed that the lanthanum compound exhibits an isotropic behaviour with occupation of both RMi units, whereas for the cerium compound anisotropy is related to the exclusive occupation of RM2 units by deuterium. From these results, it can be established that:

  • Isotropic cell volume expansion is related to full hydrogenation of both RMi units whereas anisotropic behaviour is obtained when hydrogen

Acknowledgements

The authors wish to thank Mrs. F. Briaucourt and Mr. E. Leroy for technical assistance, Mr. R. Cortes for his help during X-ray absorption experiment in LURE and Mrs. F. Bourée-Vigneron for neutron data acquisition in LLB.

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