Refinement. R[F 2 >2(F 2 )] = wr(f 2 ) = S = reflections

Transcription

1 Acta Crystallographica Section E Structure Reports Online ISSN Zr 3 NiSb 7 : a new antimony-enriched ZrSb 2 derivative V. Romaka, a * A. Tkachuk b and L. Romaka a measured reflections 1722 independent reflections Refinement R[F 2 >2(F 2 )] = wr(f 2 ) = S = reflections Table 1 Selected bond lengths (Å). inorganic compounds 1500 reflections with I > 2(I) R int = parameters max = 2.12 e Å 3 min = 2.89 e Å 3 a Department of Inorganic Chemistry, Ivan Franko National University of Lviv, Kyryla i Mefodiya Street 6, Lviv, Ukraine, and b Department of Chemistry, University of Alberta, Edmonton, Alberta, Canada T6G 2G2 Correspondence romakav@yahoo.com Received 27 June 2008; accepted 2 July 2008 Key indicators: single-crystal X-ray study; T = 295 K; mean (Sb Ni) = Å; R factor = 0.025; wr factor = 0.054; data-to-parameter ratio = Single crystals of trizirconium nickel heptaantimonide were synthesized from the constituent elements by arc-melting. The compound crystallizes in a unique structure type and belongs to the family of two-layer structures. All crystallographically unique atoms (3 Zr, 1 Ni and 7 Sb) are located at sites with m symmetry. The structure contains Zr 2 Ni 2 Sb 5 and Zr 4 Sb 9 fragments and might be described as a new ZrSb 2 derivative with a high Sb content. Related literature The structure of ZrSb 2 was described by Garcia & Corbett (1988). For related antimonides, see: Romaka et al. (2007); Tkachuk et al. (2007). For related literature, see: Emsley (1991). Zr1 Sb4 i (6) Zr1 Sb (8) Zr1 Sb1 ii (8) Zr1 Sb3 iii (7) Zr1 Sb7 iii (6) Zr1 Sb (8) Zr2 Sb6 iv (6) Zr2 Sb4 iii (6) Zr2 Sb2 iv (6) Zr2 Sb2 ii (8) Zr2 Sb (8) Zr3 Sb1 iv (6) Zr3 Sb3 iv (7) Zr3 Sb5 iv (6) Zr3 Sb6 v (8) Zr3 Sb3 vi (9) Ni1 Sb (10) Ni1 Sb2 iv (7) Ni1 Sb1 iv (7) Ni1 Sb4 vi (10) Sb1 Sb (8) Sb1 Sb3 vii (6) Sb1 Sb4 viii (6) Sb2 Sb2 ix (7) Sb2 Sb4 viii (6) Sb5 Sb7 iii (6) Sb5 Sb6 iv (6) Sb6 Sb7 i (6) Symmetry codes: (i) x þ 1 2 ; y þ 1; z 1 2 ; (ii) x þ 1 2 ; y; z þ 1 2 ; (iii) x þ 1 2 ; y; z 1 2 ; (iv) x þ 1 2 ; y; z þ 1 2 ; (v) x; y; z þ 1; (vi) x þ 1 2 ; y; z þ 3 2 ; (vii) x; y þ 1; z þ 1; (viii) x; y; z þ 1; (ix) x; y; z. Data collection: SMART (Bruker, 2000); cell refinement: SAINT- Plus (Bruker, 2000); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: SHELXL97. The work was in part supported by the Ministry of Ukraine for Education and Science (grant No. 0106U001299). Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2182). Experimental Crystal data Zr 3 NiSb 7 M r = Orthorhombic, Pnma a = (19) Å b = (4) Å c = (15) Å Data collection Bruker SMART 1000 diffractometer V = (18) Å 3 Z =4 Mo K radiation = mm 1 T = 295 (2) K mm Absorption correction: numerical (SHELXTL; Sheldrick, 2008) T min = 0.057, T max = References Brandenburg, K. (1999). DIAMOND. Crystal Impact GbR, Bonn, Germany. Bruker (2000). SMART and SAINT-Plus. Bruker AXS Inc., Madison, Wisconsin, USA. Emsley, J. (1991). The Elements, 2nd ed. Oxford: Clarendon Press. Garcia, E. & Corbett, J. D. (1988). J. Solid State Chem. 73, Romaka, L., Tkachuk, A. & Stadnyk, Yu. (2007). 11th Scientific Conference L viv Chemistry Reading 2007, Collected Abstracts, p. H37. L viv: Publishing Center of Ivan Franko National University. Sheldrick, G. M. (2008). Acta Cryst. A64, Tkachuk, A., Romaka, L. & Stadnyk, Yu. (2007). 10th International Conference on Crystal Chemistry of Intermetallic Compounds, L viv (Ukraine), Collected Abstracts, p. 71. L viv: Publishing Center of Ivan Franko National University. doi: /s Romaka et al. i47

2 [doi: /s ] Zr 3 NiSb 7 : a new antimony-enriched ZrSb 2 derivative V. Romaka, A. Tkachuk and L. Romaka S1. Comment Antimony based intermetallics attract interest due to interesting thermoelectric properties of some phases, e.g. antimonides with MgAgAs and Y 3 Au 3 Sb 4 type structures. The investigation of new intermetallic phases is useful for the development of new materials, and the accurate determination of their crystal structures is a basic requirement for a better understanding of the corresponding physical properties. Investigation of the Zr Ni Sb ternary system revealed the presence of several compounds in the Sb-enriched area (Romaka et al., 2007), including the new title antimonide with composition Zr 27 Ni 9 Sb 64 (in % at ). Interatomic distances (Table 1) between Sb atoms are in good agreement with the sum of the atomic radius (Emsley, 1991), whereas the majority of Zr Sb and all Ni Sb distances are somewhat shortened. Such shortening may be explained by partial covalent bonding which appears to be significant between Ni Sb atoms because their contact distances are rather close to the sum of their covalent radii (2.56 Å). As the majority of ternary intermetallics are constructed from the fragments of their most stable binary compounds, the structure analysis of the antimonides Zr 3 NiSb 7 and the already known Zr 2 NiSb 3 (Tkachuk et al., 2007) in the Sb-enriched area shows that both can be derived from the binary compound ZrSb 2 (Garcia & Corbett, 1988), which crystallizes in the PbCl 2 structure type. Zr 3 NiSb 7 belongs to the family of two-layer structures. It may be represented as a net of trigonal prisms formed by Sb atoms that are bridged by nickel atoms (Fig. 1a). Such an arrangement is very similar to that in the binary ZrSb 2 structure (Fig. 1b). The coordination polyhedra are distorted tri-capped trigonal prisms for the Zr atoms, and distorted octahedra for Ni atoms. In an alternative description, the Zr 3 NiSb 7 structure contains fragments of the hypothetical "Zr 2 Ni 2 Sb 5 " and "Zr 4 Sb 9 " structures (Fig. 2) which are so far unknown for the ternary Zr Ni Sb or binary Zr Sb systems. The main feature of the Zr 3 NiSb 7 structure is the absence of covalent bonding between antimony atoms in contrast to the ZrSb 2 structure. The general conclusion is that the presence of Ni atoms intensifies the interaction between Zr/Ni and Sb and, at the same time, reduces the bonding between Sb atoms. One may speculate that the composition of the Zr 3 NiSb 7 compound may be the boundary limit of some solid solutions based on ZrSb 2. However, the detailed study of the phase equilibria in the Zr Ni Sb system did not show a formation of any substitutional or interstitial solid solution. Moreover, the diffraction patterns of Zr 3 NiSb 7 and ZrSb 2 are rather different. S2. Experimental A sample with nominal composition Zr 30 Ni 10 Sb 60 was prepared by arc-melting the constituent elements Zr (99.99 wt.%), Ni (99.99 wt.%), and Sb (99.99 wt.%) on a water-cooled copper hearth under a protective Ti-gettered argon atmosphere. 5 wt.% excess of Sb was required to compensate the evaporative loss during arc-melting. The ingot was annealed at 870 K for 720 h in an evacuated silica ampoule, and finally quenched in cold water. A crystal of the title compound suitable for single-crystal X-ray diffraction was extracted directly from the annealed sample. The chemical composition of the crystal was determined on the basis of an energy dispersive X-ray spectroscopical analysis using a Hitachi S-2700 sup-1

3 scanning electron microscope. The result of the analysis is in good aggreement with the composition calculated from the structural refinement: Measured: 24.5 (8) % at Zr, 11.3 (6) % at Ni, 64.2 (16) % at Sb; calculated Zr 27 % at, Ni 9% at, Sb 64 % at. S3. Refinement The highest remaining electron density peak and the deepest hole are located 0.80 Å from Sb1 and 1.78 Å from Ni1, respectively. The structure solution and refinement were also performed in the non-centrosymmetric space group Pna2 1, but were less satisfactory and resulted in larger R indices and atomic displacement parameters. Figure 1 (a). Projection of the Zr 3 NiSb 7 structure onto the (010) plane with displacement ellipsoids drawn at the 95% probability level. [Symmetry codes: (i) x, 1 - y, -1/2 + z; (iv) x, -y, z; (vi) 1/2 + x, y, z]; (b) Projection of the ZrSb 2 structure onto the (010) plane. sup-2

4 Figure 2 The stacked "Zr 2 Ni 2 Sb 5 " and "Zr 4 Sb 9 " fragments in the Zr 3 NiSb 7 structure. trizirconium nickel heptaantimonide Crystal data Zr 3 NiSb 7 M r = Orthorhombic, Pnma Hall symbol: -P 2ac 2n a = (19) Å b = (4) Å c = (15) Å V = (18) Å 3 Z = 4 Data collection Bruker SMART 1000 diffractometer Radiation source: fine-focus sealed tube Graphite monochromator φ and ω scans Absorption correction: numerical (SHELXTL; Sheldrick, 2008) T min = 0.057, T max = F(000) = 2020 D x = Mg m 3 Mo Kα radiation, λ = Å Cell parameters from 4956 reflections θ = µ = mm 1 T = 295 K Needle, silver mm measured reflections 1722 independent reflections 1500 reflections with I > 2σ(I) R int = θ max = 30.5, θ min = 2.3 h = k = 5 5 l = sup-3

5 Refinement Refinement on F 2 Least-squares matrix: full R[F 2 > 2σ(F 2 )] = wr(f 2 ) = S = reflections 68 parameters 0 restraints Primary atom site location: structure-invariant direct methods Secondary atom site location: difference Fourier map w = 1/[σ 2 (F o2 ) + (0.0223P) P] where P = (F o 2 + 2F c2 )/3 (Δ/σ) max = Δρ max = 2.12 e Å 3 Δρ min = 2.89 e Å 3 Extinction correction: SHELXL97 (Sheldrick, 2008), Fc * =kfc[ xfc 2 λ 3 /sin(2θ)] -1/4 Extinction coefficient: (5) Special details Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. Refinement. Refinement of F 2 against ALL reflections. The weighted R-factor wr and goodness of fit S are based on F 2, conventional R-factors R are based on F, with F set to zero for negative F 2. The threshold expression of F 2 > σ(f 2 ) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F 2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å 2 ) x y z U iso */U eq Zr (4) (5) (14) Zr (4) (5) (13) Zr (4) (5) (14) Ni (5) (6) (18) Sb (3) (3) (11) Sb (2) (3) (10) Sb (3) (3) (11) Sb (3) (3) (10) Sb (3) (3) (11) Sb (2) (3) (11) Sb (3) (4) (11) Atomic displacement parameters (Å 2 ) U 11 U 22 U 33 U 12 U 13 U 23 Zr (3) (3) (3) (2) Zr (3) (3) (3) (2) Zr (3) (3) (3) (2) Ni (4) (5) (4) (3) Sb (2) (2) (2) (15) Sb (2) (2) (2) (15) Sb (2) (2) (2) (16) Sb (2) (2) (2) (15) Sb (2) (2) (2) (15) Sb (2) (2) (2) (15) sup-4

6 Sb (2) (3) (3) (16) Geometric parameters (Å, º) Zr1 Sb4 i (6) Sb2 Ni1 ii (7) Zr1 Sb4 ii (6) Sb2 Zr2 ii (6) Zr1 Sb (8) Sb2 Zr2 i (6) Zr1 Sb1 iii (8) Sb2 Zr2 viii (8) Zr1 Sb3 ii (7) Sb2 Sb2 xi (7) Zr1 Sb3 i (7) Sb2 Sb2 xii (7) Zr1 Sb7 ii (6) Sb2 Sb4 x (6) Zr1 Sb7 i (6) Sb2 Sb4 ix (6) Zr1 Sb (8) Sb3 Zr3 ii (7) Zr2 Sb6 iv (6) Sb3 Zr3 i (7) Zr2 Sb6 v (6) Sb3 Zr1 v (7) Zr2 Sb4 ii (6) Sb3 Zr1 iv (7) Zr2 Sb4 i (6) Sb3 Zr3 xiii (9) Zr2 Sb2 v (6) Sb3 Sb1 ix (6) Zr2 Sb2 iv (6) Sb3 Sb1 x (6) Zr2 Sb2 iii (8) Sb4 Ni1 xiii (10) Zr2 Sb (8) Sb4 Zr2 v (6) Zr2 Sb (9) Sb4 Zr2 iv (6) Zr3 Sb1 iv (6) Sb4 Zr1 iv (6) Zr3 Sb1 v (6) Sb4 Zr1 v (6) Zr3 Sb3 v (7) Sb4 Sb1 x (6) Zr3 Sb3 iv (7) Sb4 Sb1 ix (6) Zr3 Sb5 iv (6) Sb4 Sb2 x (6) Zr3 Sb5 v (6) Sb4 Sb2 ix (6) Zr3 Sb6 vi (8) Sb5 Zr3 ii (6) Zr3 Sb3 vii (9) Sb5 Zr3 i (6) Zr3 Ni (12) Sb5 Sb7 ii (6) Ni1 Sb (10) Sb5 Sb7 i (6) Ni1 Sb2 iv (7) Sb5 Sb6 v (6) Ni1 Sb2 v (7) Sb5 Sb6 iv (6) Ni1 Sb1 v (7) Sb6 Zr2 ii (6) Ni1 Sb1 iv (7) Sb6 Zr2 i (6) Ni1 Sb4 vii (10) Sb6 Zr3 xiv (8) Sb1 Ni1 ii (7) Sb6 Sb5 ii (6) Sb1 Ni1 i (7) Sb6 Sb5 i (6) Sb1 Zr3 i (6) Sb6 Sb7 i (6) Sb1 Zr3 ii (6) Sb6 Sb7 ii (6) Sb1 Zr1 viii (8) Sb7 Zr1 iv (6) Sb1 Sb (8) Sb7 Zr1 v (6) Sb1 Sb3 ix (6) Sb7 Sb5 v (6) Sb1 Sb3 x (6) Sb7 Sb5 iv (6) Sb1 Sb4 x (6) Sb7 Sb6 iv (6) Sb1 Sb4 ix (6) Sb7 Sb6 v (6) Sb2 Ni1 i (7) sup-5

7 Sb4 i Zr1 Sb4 ii (2) Ni1 i Sb2 Zr2 viii (2) Sb4 i Zr1 Sb (11) Ni1 ii Sb2 Zr2 viii (2) Sb4 ii Zr1 Sb (11) Zr2 ii Sb2 Zr2 viii (17) Sb4 i Zr1 Sb1 iii (16) Zr2 i Sb2 Zr2 viii (17) Sb4 ii Zr1 Sb1 iii (16) Ni1 i Sb2 Sb (19) Sb6 Zr1 Sb1 iii (3) Ni1 ii Sb2 Sb (19) Sb4 i Zr1 Sb3 ii (3) Zr2 ii Sb2 Sb (17) Sb4 ii Zr1 Sb3 ii (15) Zr2 i Sb2 Sb (17) Sb6 Zr1 Sb3 ii (19) Zr2 viii Sb2 Sb (19) Sb1 iii Zr1 Sb3 ii (16) Ni1 i Sb2 Sb2 xi (3) Sb4 i Zr1 Sb3 i (15) Ni1 ii Sb2 Sb2 xi (17) Sb4 ii Zr1 Sb3 i (3) Zr2 ii Sb2 Sb2 xi (17) Sb6 Zr1 Sb3 i (19) Zr2 i Sb2 Sb2 xi (2) Sb1 iii Zr1 Sb3 i (16) Zr2 viii Sb2 Sb2 xi (16) Sb3 ii Zr1 Sb3 i (2) Sb1 Sb2 Sb2 xi (17) Sb4 i Zr1 Sb7 ii (3) Ni1 i Sb2 Sb2 xii (17) Sb4 ii Zr1 Sb7 ii (15) Ni1 ii Sb2 Sb2 xii (3) Sb6 Zr1 Sb7 ii (16) Zr2 ii Sb2 Sb2 xii (2) Sb1 iii Zr1 Sb7 ii (10) Zr2 i Sb2 Sb2 xii (16) Sb3 ii Zr1 Sb7 ii (15) Zr2 viii Sb2 Sb2 xii (16) Sb3 i Zr1 Sb7 ii (3) Sb1 Sb2 Sb2 xii (17) Sb4 i Zr1 Sb7 i (15) Sb2 xi Sb2 Sb2 xii (2) Sb4 ii Zr1 Sb7 i (3) Ni1 i Sb2 Sb4 x (3) Sb6 Zr1 Sb7 i (16) Ni1 ii Sb2 Sb4 x (2) Sb1 iii Zr1 Sb7 i (10) Zr2 ii Sb2 Sb4 x (12) Sb3 ii Zr1 Sb7 i (3) Zr2 i Sb2 Sb4 x (2) Sb3 i Zr1 Sb7 i (15) Zr2 viii Sb2 Sb4 x (14) Sb7 ii Zr1 Sb7 i (2) Sb1 Sb2 Sb4 x (12) Sb4 i Zr1 Sb (19) Sb2 xi Sb2 Sb4 x (15) Sb4 ii Zr1 Sb (19) Sb2 xii Sb2 Sb4 x (2) Sb6 Zr1 Sb (2) Ni1 i Sb2 Sb4 ix (2) Sb1 iii Zr1 Sb (3) Ni1 ii Sb2 Sb4 ix (3) Sb3 ii Zr1 Sb (11) Zr2 ii Sb2 Sb4 ix (2) Sb3 i Zr1 Sb (11) Zr2 i Sb2 Sb4 ix (12) Sb7 ii Zr1 Sb (16) Zr2 viii Sb2 Sb4 ix (14) Sb7 i Zr1 Sb (16) Sb1 Sb2 Sb4 ix (12) Sb6 iv Zr2 Sb6 v (2) Sb2 xi Sb2 Sb4 ix (2) Sb6 iv Zr2 Sb4 ii (14) Sb2 xii Sb2 Sb4 ix (15) Sb6 v Zr2 Sb4 ii (3) Sb4 x Sb2 Sb4 ix (15) Sb6 iv Zr2 Sb4 i (3) Zr3 ii Sb3 Zr3 i (2) Sb6 v Zr2 Sb4 i (14) Zr3 ii Sb3 Zr1 v (2) Sb4 ii Zr2 Sb4 i (2) Zr3 i Sb3 Zr1 v (17) Sb6 iv Zr2 Sb2 v (3) Zr3 ii Sb3 Zr1 iv (16) Sb6 v Zr2 Sb2 v (15) Zr3 i Sb3 Zr1 iv (2) Sb4 ii Zr2 Sb2 v (3) Zr1 v Sb3 Zr1 iv (2) Sb4 i Zr2 Sb2 v (15) Zr3 ii Sb3 Zr3 xiii (18) Sb6 iv Zr2 Sb2 iv (15) Zr3 i Sb3 Zr3 xiii (18) sup-6

8 Sb6 v Zr2 Sb2 iv (3) Zr1 v Sb3 Zr3 xiii (19) Sb4 ii Zr2 Sb2 iv (15) Zr1 iv Sb3 Zr3 xiii (19) Sb4 i Zr2 Sb2 iv (3) Zr3 ii Sb3 Sb1 ix (2) Sb2 v Zr2 Sb2 iv (2) Zr3 i Sb3 Sb1 ix (13) Sb6 iv Zr2 Sb2 iii (11) Zr1 v Sb3 Sb1 ix (16) Sb6 v Zr2 Sb2 iii (11) Zr1 iv Sb3 Sb1 ix (2) Sb4 ii Zr2 Sb2 iii (16) Zr3 xiii Sb3 Sb1 ix (13) Sb4 i Zr2 Sb2 iii (16) Zr3 ii Sb3 Sb1 x (13) Sb2 v Zr2 Sb2 iii (17) Zr3 i Sb3 Sb1 x (2) Sb2 iv Zr2 Sb2 iii (17) Zr1 v Sb3 Sb1 x (2) Sb6 iv Zr2 Sb (17) Zr1 iv Sb3 Sb1 x (15) Sb6 v Zr2 Sb (17) Zr3 xiii Sb3 Sb1 x (13) Sb4 ii Zr2 Sb (19) Sb1 ix Sb3 Sb1 x (15) Sb4 i Zr2 Sb (19) Ni1 xiii Sb4 Zr2 v (2) Sb2 v Zr2 Sb (11) Ni1 xiii Sb4 Zr2 iv (2) Sb2 iv Zr2 Sb (12) Zr2 v Sb4 Zr2 iv (2) Sb2 iii Zr2 Sb (3) Ni1 xiii Sb4 Zr1 iv (2) Sb6 iv Zr2 Sb (15) Zr2 v Sb4 Zr1 iv (2) Sb6 v Zr2 Sb (15) Zr2 iv Sb4 Zr1 iv (17) Sb4 ii Zr2 Sb (12) Ni1 xiii Sb4 Zr1 v (2) Sb4 i Zr2 Sb (12) Zr2 v Sb4 Zr1 v (17) Sb2 v Zr2 Sb (18) Zr2 iv Sb4 Zr1 v (2) Sb2 iv Zr2 Sb (18) Zr1 iv Sb4 Zr1 v (2) Sb2 iii Zr2 Sb (2) Ni1 xiii Sb4 Sb1 x (16) Sb5 Zr2 Sb (2) Zr2 v Sb4 Sb1 x (2) Sb1 iv Zr3 Sb1 v (2) Zr2 iv Sb4 Sb1 x (13) Sb1 iv Zr3 Sb3 v (3) Zr1 iv Sb4 Sb1 x (16) Sb1 v Zr3 Sb3 v (15) Zr1 v Sb4 Sb1 x (2) Sb1 iv Zr3 Sb3 iv (16) Ni1 xiii Sb4 Sb1 ix (16) Sb1 v Zr3 Sb3 iv (3) Zr2 v Sb4 Sb1 ix (13) Sb3 v Zr3 Sb3 iv (2) Zr2 iv Sb4 Sb1 ix (2) Sb1 iv Zr3 Sb5 iv (16) Zr1 iv Sb4 Sb1 ix (2) Sb1 v Zr3 Sb5 iv (3) Zr1 v Sb4 Sb1 ix (16) Sb3 v Zr3 Sb5 iv (3) Sb1 x Sb4 Sb1 ix (15) Sb3 iv Zr3 Sb5 iv (14) Ni1 xiii Sb4 Sb2 x (16) Sb1 iv Zr3 Sb5 v (3) Zr2 v Sb4 Sb2 x (2) Sb1 v Zr3 Sb5 v (15) Zr2 iv Sb4 Sb2 x (16) Sb3 v Zr3 Sb5 v (14) Zr1 iv Sb4 Sb2 x (13) Sb3 iv Zr3 Sb5 v (3) Zr1 v Sb4 Sb2 x (2) Sb5 iv Zr3 Sb5 v (2) Sb1 x Sb4 Sb2 x (14) Sb1 iv Zr3 Sb6 vi (13) Sb1 ix Sb4 Sb2 x (17) Sb1 v Zr3 Sb6 vi (13) Ni1 xiii Sb4 Sb2 ix (16) Sb3 v Zr3 Sb6 vi (19) Zr2 v Sb4 Sb2 ix (16) Sb3 iv Zr3 Sb6 vi (19) Zr2 iv Sb4 Sb2 ix (2) Sb5 iv Zr3 Sb6 vi (17) Zr1 iv Sb4 Sb2 ix (2) Sb5 v Zr3 Sb6 vi (17) Zr1 v Sb4 Sb2 ix (13) Sb1 iv Zr3 Sb3 vii (16) Sb1 x Sb4 Sb2 ix (17) Sb1 v Zr3 Sb3 vii (16) Sb1 ix Sb4 Sb2 ix (14) sup-7

9 Sb3 v Zr3 Sb3 vii (18) Sb2 x Sb4 Sb2 ix (15) Sb3 iv Zr3 Sb3 vii (18) Zr3 ii Sb5 Zr3 i (2) Sb5 iv Zr3 Sb3 vii (12) Zr3 ii Sb5 Zr (2) Sb5 v Zr3 Sb3 vii (12) Zr3 i Sb5 Zr (2) Sb6 vi Zr3 Sb3 vii (3) Zr3 ii Sb5 Zr (16) Sb1 iv Zr3 Ni (15) Zr3 i Sb5 Zr (16) Sb1 v Zr3 Ni (15) Zr2 Sb5 Zr (2) Sb3 v Zr3 Ni (18) Zr3 ii Sb5 Sb7 ii (16) Sb3 iv Zr3 Ni (18) Zr3 i Sb5 Sb7 ii (2) Sb5 iv Zr3 Ni (2) Zr2 Sb5 Sb7 ii (17) Sb5 v Zr3 Ni (2) Zr1 Sb5 Sb7 ii (15) Sb6 vi Zr3 Ni (3) Zr3 ii Sb5 Sb7 i (2) Sb3 vii Zr3 Ni (2) Zr3 i Sb5 Sb7 i (16) Sb7 Ni1 Sb2 iv (3) Zr2 Sb5 Sb7 i (17) Sb7 Ni1 Sb2 v (3) Zr1 Sb5 Sb7 i (15) Sb2 iv Ni1 Sb2 v (3) Sb7 ii Sb5 Sb7 i (18) Sb7 Ni1 Sb1 v (3) Zr3 ii Sb5 Sb6 v (2) Sb2 iv Ni1 Sb1 v (4) Zr3 i Sb5 Sb6 v (16) Sb2 v Ni1 Sb1 v (16) Zr2 Sb5 Sb6 v (14) Sb7 Ni1 Sb1 iv (3) Zr1 Sb5 Sb6 v (16) Sb2 iv Ni1 Sb1 iv (16) Sb7 ii Sb5 Sb6 v (2) Sb2 v Ni1 Sb1 iv (4) Sb7 i Sb5 Sb6 v (11) Sb1 v Ni1 Sb1 iv (3) Zr3 ii Sb5 Sb6 iv (16) Sb7 Ni1 Sb4 vii (4) Zr3 i Sb5 Sb6 iv (2) Sb2 iv Ni1 Sb4 vii (2) Zr2 Sb5 Sb6 iv (14) Sb2 v Ni1 Sb4 vii (2) Zr1 Sb5 Sb6 iv (16) Sb1 v Ni1 Sb4 vii (2) Sb7 ii Sb5 Sb6 iv (11) Sb1 iv Ni1 Sb4 vii (2) Sb7 i Sb5 Sb6 iv (2) Sb7 Ni1 Zr (3) Sb6 v Sb5 Sb6 iv (18) Sb2 iv Ni1 Zr (17) Zr2 ii Sb6 Zr2 i (2) Sb2 v Ni1 Zr (17) Zr2 ii Sb6 Zr (17) Sb1 v Ni1 Zr (2) Zr2 i Sb6 Zr (17) Sb1 iv Ni1 Zr (2) Zr2 ii Sb6 Zr3 xiv (19) Sb4 vii Ni1 Zr (3) Zr2 i Sb6 Zr3 xiv (19) Ni1 ii Sb1 Ni1 i (3) Zr1 Sb6 Zr3 xiv (2) Ni1 ii Sb1 Zr3 i (3) Zr2 ii Sb6 Sb5 ii (16) Ni1 i Sb1 Zr3 i (2) Zr2 i Sb6 Sb5 ii (2) Ni1 ii Sb1 Zr3 ii (2) Zr1 Sb6 Sb5 ii (17) Ni1 i Sb1 Zr3 ii (3) Zr3 xiv Sb6 Sb5 ii (14) Zr3 i Sb1 Zr3 ii (2) Zr2 ii Sb6 Sb5 i (2) Ni1 ii Sb1 Zr1 viii (2) Zr2 i Sb6 Sb5 i (16) Ni1 i Sb1 Zr1 viii (2) Zr1 Sb6 Sb5 i (17) Zr3 i Sb1 Zr1 viii (19) Zr3 xiv Sb6 Sb5 i (14) Zr3 ii Sb1 Zr1 viii (19) Sb5 ii Sb6 Sb5 i (18) Ni1 ii Sb1 Sb (19) Zr2 ii Sb6 Sb7 i (2) Ni1 i Sb1 Sb (19) Zr2 i Sb6 Sb7 i (16) Zr3 i Sb1 Sb (18) Zr1 Sb6 Sb7 i (16) Zr3 ii Sb1 Sb (18) Zr3 xiv Sb6 Sb7 i (15) sup-8

10 Zr1 viii Sb1 Sb (19) Sb5 ii Sb6 Sb7 i (2) Ni1 ii Sb1 Sb3 ix (2) Sb5 i Sb6 Sb7 i (11) Ni1 i Sb1 Sb3 ix (18) Zr2 ii Sb6 Sb7 ii (16) Zr3 i Sb1 Sb3 ix (17) Zr2 i Sb6 Sb7 ii (2) Zr3 ii Sb1 Sb3 ix (2) Zr1 Sb6 Sb7 ii (16) Zr1 viii Sb1 Sb3 ix (14) Zr3 xiv Sb6 Sb7 ii (15) Sb2 Sb1 Sb3 ix (14) Sb5 ii Sb6 Sb7 ii (11) Ni1 ii Sb1 Sb3 x (18) Sb5 i Sb6 Sb7 ii (2) Ni1 i Sb1 Sb3 x (2) Sb7 i Sb6 Sb7 ii (18) Zr3 i Sb1 Sb3 x (2) Ni1 Sb7 Zr1 iv (10) Zr3 ii Sb1 Sb3 x (17) Ni1 Sb7 Zr1 v (10) Zr1 viii Sb1 Sb3 x (14) Zr1 iv Sb7 Zr1 v (2) Sb2 Sb1 Sb3 x (13) Ni1 Sb7 Sb5 v (2) Sb3 ix Sb1 Sb3 x (16) Zr1 iv Sb7 Sb5 v (2) Ni1 ii Sb1 Sb4 x (2) Zr1 v Sb7 Sb5 v (16) Ni1 i Sb1 Sb4 x (3) Ni1 Sb7 Sb5 iv (2) Zr3 i Sb1 Sb4 x (17) Zr1 iv Sb7 Sb5 iv (16) Zr3 ii Sb1 Sb4 x (12) Zr1 v Sb7 Sb5 iv (2) Zr1 viii Sb1 Sb4 x (14) Sb5 v Sb7 Sb5 iv (18) Sb2 Sb1 Sb4 x (13) Ni1 Sb7 Sb6 iv (2) Sb3 ix Sb1 Sb4 x (18) Zr1 iv Sb7 Sb6 iv (16) Sb3 x Sb1 Sb4 x (14) Zr1 v Sb7 Sb6 iv (2) Ni1 ii Sb1 Sb4 ix (3) Sb5 v Sb7 Sb6 iv (2) Ni1 i Sb1 Sb4 ix (2) Sb5 iv Sb7 Sb6 iv (12) Zr3 i Sb1 Sb4 ix (12) Ni1 Sb7 Sb6 v (2) Zr3 ii Sb1 Sb4 ix (17) Zr1 iv Sb7 Sb6 v (2) Zr1 viii Sb1 Sb4 ix (14) Zr1 v Sb7 Sb6 v (16) Sb2 Sb1 Sb4 ix (13) Sb5 v Sb7 Sb6 v (12) Sb3 ix Sb1 Sb4 ix (14) Sb5 iv Sb7 Sb6 v (2) Sb3 x Sb1 Sb4 ix (18) Sb6 iv Sb7 Sb6 v (18) Sb4 x Sb1 Sb4 ix (15) Ni1 Sb7 Zr (2) Ni1 i Sb2 Ni1 ii (3) Zr1 iv Sb7 Zr (2) Ni1 i Sb2 Zr2 ii (3) Zr1 v Sb7 Zr (2) Ni1 ii Sb2 Zr2 ii (2) Sb5 v Sb7 Zr (11) Ni1 i Sb2 Zr2 i (2) Sb5 iv Sb7 Zr (11) Ni1 ii Sb2 Zr2 i (3) Sb6 iv Sb7 Zr (14) Zr2 ii Sb2 Zr2 i (2) Sb6 v Sb7 Zr (14) Symmetry codes: (i) x+1/2, y+1, z 1/2; (ii) x+1/2, y, z 1/2; (iii) x+1/2, y, z+1/2; (iv) x+1/2, y, z+1/2; (v) x+1/2, y+1, z+1/2; (vi) x, y, z+1; (vii) x+1/2, y, z+3/2; (viii) x 1/2, y, z+1/2; (ix) x, y+1, z+1; (x) x, y, z+1; (xi) x, y, z; (xii) x, y+1, z; (xiii) x 1/2, y, z+3/2; (xiv) x, y, z 1. sup-9