Abstract
New alkaline earth-gold-aluminides were synthesized from the elements in sealed tantalum or quartz ampoules in muffle furnaces at maximum annealing temperatures of 1325 K. The structures were refined from single crystal X-ray diffractometer data. SrAu3Al2 crystallizes in an ordered version of the LT-SrZn5 structure: Pnma, a = 1315.9(3), b = 549.0(1), c = 684.5(3) pm, wR2 = 0.0232, 930 F2 values, 35 variables. SrAu2.83Al2.17 (a = 1065.0(2), b = 845.0(2), c = 548.1(1) pm, wR2 = 0.0416, 452 F2 values, 22 variables) and BaAu2.89Al2.11 (a = 1096.1(3), b = 835.7(3), c = 554.0(1) pm, wR2 = 0.0280, 501 F2 values, 22 variables) both adopt the BaZn5 type, space group Cmcm with Au/Al mixing on the 4c site. The gold and aluminum atoms in both types form three-dimensional networks of condensed tetrahedra with the strontium and barium atoms in large cavities. BaAu7.09Al5.91 is a new member of the NaZn13 type: Fm3̅c, a = 1257.6(2) pm, wR2 = 0.0267, 168 F2 values, 12 variables. Both the 96i and 8b sites show Au/Al mixing. The crystal chemical details are discussed.
1 Introduction
Gold-aluminum intermetallics have widely been studied in microelectronics, since the aurides Al2Au5 (called white plague) and Al2Au (called purple plague) frequently occur at solder joints through inter-diffusion processes at higher temperatures. The main problem with auride formation at the interfaces concerns drastic differences in the electrical conductivity as compared to the pure metals as well as the brittleness of the intermetallic compound which might lead to cracks at the joints.
Apart from these technical applications, gold intermetallics display a rich crystal chemistry and fascinating bonding peculiarities, a consequence of relativistic effects [1–4]. If a highly electropositive element (alkali (A), alkaline earth (AE) or rare earth (RE) metal) reacts with gold and a p element of the 3rd, 4th, or 5th main group (E), structures with one-, two-, or three-dimensional [AuxEy] polyanions form. Typical examples are the linear phosphido-aurate ions [AuP2]5– in K5[AuP2] [5], the planar 2D [AuP]2– and [Au2Sn]6– polyanions in SrAuP [6] and Er2Au2Sn [7], or the wurtzite-related three-dimensional [AuSn]3– network in CeAuSn [8].
So far, the systems AE-Au-Al have only scarcely been studied. Few compounds with calcium and strontium have been reported: TiNiSi-type CaAuAl [9], CaAu0.8Ga3.2 and CaAu0.9Ga3.1 with BaAl4-type structure [10, 11], CaAu3Al7 [12], and the large series of aluminum-rich Ca3Au6+xAl26T (T = Ti, Zr, Hf, V, Nb, Cr, Mo, W, Mn, Re) and Sr3Au6+xAl26T (T = Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Mn, Re) [12, 13] compounds with a stuffed variant of the cubic BaCd11 type. Further strontium compounds were reported recently. Sr2Au6Al3 [14] is the first representative of the Sr2Au6Zn3 type with Al3 triangles. This structural motif also occurs in SrAu4.06Al2.94, SrAu5.05Al1.95, Sr2Au7.32Al1.67, and Sr2Au6.18Al2.82 [15]. The triangles show small degrees of Au/Al mixing.
When searching for further representatives of this structural family we obtained a series of by-products with different structure types, namely SrAu3Al2, SrAu2.83Al2.17, BaAu2.89Al2.11 and BaAu7.09Al5.91. The synthesis and crystal chemistry of these aluminides are reported herein.
2 Experimental
2.1 Synthesis
Starting materials for the syntheses of the ternary aluminides were sublimed ingots of strontium (Aldrich, >99 %), barium rods (Alfa Aesar 99.9 %), pieces of a gold bar (Heraeus, >99.9 %) and aluminum chips (Koch Chemicals, >99.99 %). The strontium granules and the barium rod were cut into smaller pieces under paraffin oil (dried over sodium wire) and subsequently washed with n-hexane. These pieces were kept in Schlenk tubes under argon prior to the reactions. The argon was purified over titanium sponge (900 K), silica gel, and molecular sieves.
The ternary compounds were obtained from reactions of the elements in sealed high-melting metal or quartz tubes. The following compounds were obtained (starting compositions and container materials in parentheses): SrAu3Al2 (3:7.2:3; tantalum), SrAu2.83Al2.17 (1:4:3; tantalum), BaAu2.89Al2.11 (1:4:3; quartz) and BaAu7.09Al5.91 (1:3:2; quartz). The tantalum ampoules were sealed in an arc-melting furnace [16] under an argon pressure of ca. 700 mbar and sealed in quartz tubes for protection against oxidation.
The containers were subsequently placed in a muffle furnace, rapidly heated to 1325 K and kept at this temperature for a few minutes. The tubes were then cooled to 825 K at a rate of 60 K h−1, kept there for another 9 h, followed by radiative heat loss by switching off the power supply. The polycrystalline samples were separated mechanically from the crucible material. All samples show metallic luster and are stable in air over weeks.
2.2 X-ray diffraction
The polycrystalline samples were characterized through Guinier powder patterns (Enraf-Nonius camera, type FR 552): imaging plate detector, Fujifilm BAS-1800, CuKα1 radiation, and α-quartz (a = 491.30, c = 540.46 pm) as an internal standard. The lattice parameters (Table 1) were obtained from least-squares refinements. Correct indexing of the patterns was ensured through a comparison of the experimental patterns with calculated ones [17].
Crystal data and structure refinement parameters for SrAu3Al2, SrAu2.83(1)Al2.17(1), BaAu2.89(1)Al2.11(1), and BaAu7.09(1)Al5.91(1).
Empirical formula | SrAu3Al2 | SrAu2.83(1)Al2.17(1) | BaAu2.89(1)Al2.11(1) | BaAu7.09(1)Al5.91(1) |
Space group; Z | Pnma; 4 | Cmcm; 4 | Cmcm; 4 | Fm3̅c; 8 |
Molar mass, g mol−1 | 732.48 | 703.58 | 764.18 | 1692.43 |
Unit cell dimensions (single crystal data) | ||||
a, pm | 1315.84(3) | 1064.99(4) | 1097.40(7) | 1257.6(2) |
b, pm | 549.46(2) | 844.96(4) | 836.54(5) | b = a |
c, pm | 684.34(2) | 548.13(3) | 556.31(4) | c = a |
V, nm3 | 0.4948 | 0.4932 | 0.5107 | 1.9889 |
Unit cell dimensions (powder data) | ||||
a, pm | 1315.9(3) | 1065.0(2) | 1096.1(3) | – |
b, pm | 549.0(1) | 845.0(2) | 835.7(3) | – |
c, pm | 684.5(3) | 548.1(1) | 554.0(1) | – |
V, nm3 | 0.4945 | 0.4933 | 0.5075 | – |
Calculated density, g cm−3 | 9.84 | 9.48 | 10.00 | 11.30 |
Crystal size, μm3 | 35 × 35 × 45 | 25 × 35 × 40 | 30 × 35 × 50 | 40 × 45 × 45 |
Diffractometer | IPDS-II | IPDS-II | IPDS-II | IPDS-II |
Wave length; λ, pm | MoKα; 71.073 | MoKα; 71.073 | MoKα; 71.073 | MoKα; 71.073 |
Transm. ratio (max/min) | 0.507/0.117 | 0.735/0.354 | 0.366/0.147 | 0.193/0.045 |
Absorption coefficient, mm−1 | 99.6 | 94.9 | 91.2 | 108.4 |
F(000), e | 1204 | 1159 | 1248 | 5541 |
θ range, deg | 3–32 | 3–31 | 3–32 | 3–32 |
Range in hkl | ±19, ±8, ±10 | ±15, ±12, −7 | ±16, ±12, −8 | ±18, ±18, +18 |
Total no. reflections | 3207 | 1530 | 1670 | 2868 |
Independent reflections/Rint | 930/0.0371 | 452/0.0280 | 501/0.0277 | 168/0.0602 |
Refl. with I > 2 σ(I)/Rσ | 797/0.0311 | 377/0.0257 | 423/0.0282 | 130/0.0320 |
Data/ref. parameters | 930/35 | 452/22 | 501/22 | 168/12 |
Goodness-of-fit on F2 | 0.825 | 0.978 | 0.911 | 0.860 |
Final R1/wR2 [I > 2 σ(I)] | 0.0137/0.0228 | 0.0179/0.0408 | 0.0164/0.0274 | 0.0191/0.0259 |
Final R1/wR2 (all data) | 0.0191/0.0232 | 0.0239/0.0416 | 0.0233/0.0280 | 0.0308/0.0267 |
Extinction coefficient | 0.00090(2) | 0.0021(1) | 0.00082(4) | 0.00021(1) |
Largest diff. peak/hole, e Å−3 | 1.74/–1.49 | 2.83/–4.41 | 2.87/–2.53 | 1.77/–1.68 |
Irregularly shaped single crystals with conchoidal fracture were selected from the crushed samples and glued to thin quartz fibers using bees wax. The crystals were first studied on a Buerger camera (using white Mo radiation) to check their quality. Intensity data were collected at room temperature on a Stoe IPDS-II image plate system (graphite-monochromatized MoKα radiation; λ = 71.073 pm) in oscillation mode. Numerical absorption corrections were applied to the data sets. Details about the data collections and the crystallographic parameters are summarized in Table 1.
2.3 Structure refinements
The SrAu3Al2 data set showed a primitive orthorhombic lattice and the systematic extinctions were compatible with space group Pnma. Orthorhombic C-centered lattices were observed for the SrAu2.83Al2.17 and BaAu2.89Al2.11 data sets and space group Cmcm was found to be correct during the structure refinements. The starting atomic parameters were deduced from interpretations of Direct Methods with Shelxs-97 [18], and the structures were refined with full-matrix least-squares on F2 using Shelxl-97 [19] with anisotropic atomic displacement parameters for all atoms. A comparison with substances known from the literature showed Wyckoff sequence dc4 for SrAu3Al2 and gec2 for SrAu2.83Al2.17 and BaAu2.89Al2.11, indicating isotypism with LT-SrZn5 (Pnma) and BaZn5 (Cmcm) [20–22] with complete or partial Au/Al ordering on the zinc sites. The mixed occupancies of the SrAu2.83Al2.17 and BaAu2.89Al2.11 structures were refined through a least-squares variable in the final cycles. BaAu7.09Al5.91 showed a face-centered cubic lattice and space group Fm3̅c (NaZn13 type [23]). Refinement of the occupancy parameters revealed Au/Al mixing for the 96i and the 8b sites. The final difference Fourier syntheses revealed no residual peaks. The refined atomic positions, displacement parameters, and interatomic distances are given in Tables 2–6.
Atomic positions of SrAu3Al2, SrAu2.83(1)Al2.17(1), BaAu2.89(1)Al2.11(1), and BaAu7.09(1)Al5.91(1).
Atom | Wyckoff site | x | y | z | Mixed site Au/Al (%) |
---|---|---|---|---|---|
SrAu3Al2 | |||||
Sr | 4c | 0.41092(5) | 1/4 | 0.84775(9) | |
Au1 | 4c | 0.21732(2) | 1/4 | 0.15326(3) | |
Au2 | 4c | 0.19338(2) | 1/4 | 0.55707(3) | |
Au3 | 4c | 0.00879(2) | 1/4 | 0.09486(4) | |
Al1 | 8d | 0.3500(1) | 0.0004(3) | 0.3577(2) | |
SrAu2.83(1)Al2.17(1) | |||||
Sr | 4c | 0 | 0.6758(1) | 1/4 | |
Au1 | 8g | 0.18851(3) | 0.28797(4) | 1/4 | |
Au2 | 4c | 0 | 0.06612(7) | 1/4 | 83.0(5)/17.0(5) |
Al | 8e | 0.2060(3) | 0 | 0 | |
BaAu2.89(1)Al2.11(1) | |||||
Ba | 4c | 0 | 0.66727(8) | 1/4 | |
Au1 | 8g | 0.19509(2) | 0.28922(4) | 1/4 | |
Au2 | 4c | 0 | 0.07496(5) | 1/4 | 89.4(4)/11.6(4) |
Al3 | 8e | 0.1969(2) | 0 | 0 | |
BaAu7.09(1)Al5.91(1) | |||||
Ba | 8a | 1/4 | 1/4 | 1/4 | |
Au1/Al1 | 96i | 0 | 0.12546(4) | 0.17830(4) | 58.2(6)/41.8(6) |
Au2/Al2 | 8b | 0 | 0 | 0 | 10.1(6)/89.9(6) |
Anisotropic displacement parameters (pm2) of SrAu3Al2, SrAu2.83(1)Al2.17(1), BaAu2.89(1)Al2.11(1) and BaAu7.09(1)Al5.91(1).
Atom | Wyckoff site | U11 | U22 | U33 | U12 | U13 | U23 | Ueq |
---|---|---|---|---|---|---|---|---|
SrAu3Al2 | ||||||||
Sr | 4c | 111(3) | 90(3) | 126(3) | 0 | 31(2) | 0 | 109(1) |
Au1 | 4c | 70(1) | 97(1) | 74(1) | 0 | –15(1) | 0 | 80(1) |
Au2 | 4c | 164(1) | 79(1) | 72(2) | 0 | 25(1) | 0 | 105(1) |
Au3 | 4c | 57(1) | 76(1) | 164(1) | 0 | 10(1) | 0 | 99(1) |
Al1 | 8d | 72(7) | 40(6) | 85(5) | –9(5) | –12(5) | 2(5) | 65(2) |
SrAu2.83(1)Al2.17(1) | ||||||||
Sr | 4c | 112(5) | 131(5) | 117(5) | 0 | 0 | 0 | 120(2) |
Au1 | 8g | 150(2) | 100(2) | 91(2) | 47(1) | 0 | 0 | 114(1) |
Au2 | 4c | 60(3) | 104(2) | 448(5) | 0 | 0 | 0 | 204(3) |
Al | 8e | 134(12) | 100(10) | 50(10) | 0 | 0 | 14(8) | 95(5) |
BaAu2.89(1)Al2.11(1) | ||||||||
Ba | 4c | 110(2) | 111(3) | 115(3) | 0 | 0 | 0 | 112(1) |
Au1 | 8g | 132(1) | 88(1) | 95(1) | –29(1) | 0 | 0 | 105(1) |
Au2 | 4c | 69(2) | 107(2) | 195(3) | 0 | 0 | 0 | 124(2) |
Al3 | 8e | 109(9) | 82(9) | 62(10) | 0 | 0 | 3(7) | 84(4) |
BaAu7.09(1)Al5.91(1) | ||||||||
Ba | 8a | 122(4) | U11 | U11 | 0 | 0 | 0 | U11 |
Au1/Al1 | 96i | 190(3) | 266(3) | 345(3) | 0 | 0 | 68(2) | 267(2) |
Au2/Al2 | 8b | 167(15) | U11 | U11 | 0 | 0 | 0 | U11 |
Interatomic distances (pm) in SrAu3Al2.
Sr: | 1 | Au3 | 329.2(1) | Au3: | 2 | Al | 252.0(2) |
1 | Au1 | 329.6(1) | 1 | Au1 | 277.3(1) | ||
2 | Au2 | 338.7(1) | 2 | Al | 282.5(2) | ||
2 | Au3 | 341.3(1) | 2 | Au3 | 304.5(1) | ||
1 | Au2 | 348.6(1) | 1 | Sr | 329.2(1) | ||
2 | Au1 | 348.6(1) | 2 | Sr | 341.3(1) | ||
2 | Al | 369.9(2) | Al: | 1 | Au3 | 252.0(2) | |
2 | Al | 371.0(2) | 1 | Au2 | 254.0(2) | ||
2 | Al | 371.1(2) | 1 | Au1 | 260.1(2) | ||
1 | Au2 | 377.4(1) | 1 | Au1 | 262.4(1) | ||
2 | Al | 383.5(2) | 1 | Al | 274.1(3) | ||
Au1: | 2 | Al | 260.1(2) | 1 | Al | 274.9(2) | |
2 | Al | 262.4(1) | 1 | Au3 | 282.5(2) | ||
1 | Au3 | 277.3(1) | 1 | Au2 | 282.6(2) | ||
1 | Au2 | 278.2(1) | 1 | Sr | 369.9(2) | ||
2 | Au2 | 305.8(1) | 1 | Sr | 371.0(2) | ||
1 | Sr | 329.6(1) | 1 | Sr | 371.1(2) | ||
2 | Sr | 348.6(1) | 1 | Sr | 383.5(2) | ||
Au2: | 2 | Al | 254.0(2) | ||||
1 | Au1 | 278.2(1) | |||||
2 | Al | 282.6(2) | |||||
2 | Au1 | 305.8(1) | |||||
2 | Sr | 338.7(1) | |||||
1 | Sr | 348.6(1) | |||||
1 | Sr | 377.4(1) |
All distances of the first coordination spheres are listed. Standard deviations are given in parentheses.
Interatomic distances (pm) in SrAu2.83(1)Al2.17(1).
Sr: | 1 | Au2 | 329.8(2) | Au2: | 4 | Al3 | 264.7(3) |
4 | Au1 | 341.1(1) | 2 | Au1 | 274.7(1) | ||
2 | Au2 | 345.0(1) | 2 | Au2 | 296.0(1) | ||
2 | Au2 | 350.2(1) | 1 | Sr | 329.8(2) | ||
4 | Al | 372.6(3) | 2 | Sr | 350.2(1) | ||
4 | Al | 376.8(2) | Al: | 2 | Au1 | 252.0(1) | |
2 | Au1 | 384.3(1) | 2 | Au2 | 264.7(3) | ||
2 | Sr | 404.2(2) | 2 | Al | 274.1(1) | ||
Au1: | 2 | Al | 252.0(1) | 2 | Au1 | 279.9(1) | |
1 | Au2 | 274.7(1) | 2 | Sr | 372.6(3) | ||
2 | Al | 279.9(1) | 2 | Sr | 376.8(2) | ||
2 | Au1 | 310.5(1) | |||||
2 | Sr | 341.1(1) | |||||
1 | Sr | 345.0(1) |
All distances of the first coordination spheres are listed. Standard deviations are given in parentheses. Note the Au/Al mixing on site 4c (Table 3).
Interatomic distances (pm) in BaAu7.09(1)Al5.91(1).
Ba: | 24 | Au1/Al1 | 362.6(1) |
Au1/Al1: | 2 | Au1/Al1 | 255.6(1) |
1 | Au2/Al2 | 274.2(1) | |
4 | Au1/Al1 | 282.1(1) | |
2 | Au1/Al1 | 286.9(1) | |
1 | Au1/Al1 | 315.6(1) | |
1 | Au1/Al1 | 361.4(1) | |
2 | Ba | 362.6(1) | |
Au2/Al2: | 12 | Au1/Al1 | 274.2(1) |
All distances of the first coordination spheres are listed. Standard deviations are given in parentheses.
Further details of the crystal structure investigations may be obtained from Fachinformationszentrum Karlsruhe, 76344 Eggenstein-Leopoldshafen, Germany (fax: +49-7247-808-666; e-mail: crysdata@fiz-karlsruhe.de, http://www.fiz-karlsruhe.de/request_for_deposited_data.html) on quoting the deposition numbers CSD-429904 (SrAu3Al2), CSD-429905 (SrAu2.83Al2.17), CSD-429906 (BaAu2.89Al2.11) and CSD-429907 (BaAu7.09Al5.91).
2.4 EDX data
The crystals of SrAu3Al2, SrAu2.83Al2.17, BaAu2.89Al2.11 and BaAu7.09Al5.91 studied on the diffractometer were semiquantitatively analyzed by EDX using a Zeiss EVO® MA10 scanning electron microscope in variable pressure mode. SrF2, BaF2, Au, and Al2O3 were used as standards. The experimentally observed compositions were all within ±3 at.-% close to the ones refined from the single crystal X-ray data. The standard deviations result from the irregular surface of the crystals (conchoidal fracture). No impurity elements (especially from the container material) were detected.
3 Results and discussion
Phase analytical studies in the systems AE-Au-Al led to four new ternary compounds with pronounced three-dimensional polyanionic networks formed by the gold and aluminum atoms. The new compounds crystallize with three different structure types which will be discussed separately.
We start our discussion with the structure of SrAu3Al2. The gold and aluminum atoms show complete ordering and one can describe the SrAu3Al2 structure as a ternary ordered version of the low-temperature (LT) modification of SrZn5 [21]. So far only few ternary examples are known for that structure type: RbAu3Ga2 and CsAu3Ga2 with complete gold-gallium ordering [24] as well as BaPd1.57Zn3.43 and BaAu1.41Zn3.59 with pronounced Pd/Zn and Au/Zn mixing, respectively [25].
A view of the SrAu3Al2 structure approximately along the b axis is presented in Fig. 1. The shortest interatomic distances occur between the gold and aluminum atoms (252–262 pm). They compare well with the sum of the covalent radii of 259 pm [26]. Additionally we observe Au–Au (277–306 pm) and Al–Al (274–275 pm) contacts, which are close to the respective distances in the elements (286 pm in fcc aluminum and 288 pm in fcc gold) [27]. Together, the gold and aluminum atoms built up a three-dimensional network of condensed tetrahedra. The larger strontium atoms fill the cavities within this network. They have 18 nearest Au/Al neighbors. As expected from the course of the electronegativities, the nine nearest neighbors are gold atoms (329–349 pm Sr–Au). A similar bonding situation has been observed for Sr2Au3In4 (308–355 pm Sr–Au) [28], SrAuSn (327–341 pm Sr–Au) [29] and Sr2Au6Al3 (325–335 pm Sr–Au) [14]. All of these distances compare well with the sum of the covalent radii of 326 pm for Sr + Au [26].

The structures of SrAu3Al2, SrAu2.83Al2.17 and BaAu2.89Al2.11. Alkaline earth, gold and aluminum atoms are drawn as medium grey, blue and magenta circles, respectively. Mixed occupied sites are marked by segments. The tetrahedral gold-aluminum substructures are emphasized.
With a lower gold content we obtained SrAu2.83Al2.17 which crystallizes with the BaZn5 structure [21], space group Cmcm, similar to the barium compound BaAu2.89Al2.11. This structural arrangement has previously been reported for BaAg2.4Al2.6 [30] and KAu3.08Ga1.92 [31]. It is remarkable, that all four ternary representatives show one mixed occupied site; the 4c site for the three aluminum compounds but the 8e site for the gallium one.
Exemplarily we discuss the SrAu2.83Al2.17 structure for the series of BaZn5-related phases. A view of the structure approximately along the c axis is presented in Fig. 2. The gross structural features and the course of the interatomic distances (see Tables 4 and 5) are very similar to the fully ordered variant SrAu3Al2 discussed above. The mixed occupied sites correspond to the common atom of the corner-sharing tetrahedra. The only peculiarity that should be mentioned are the enhanced U33 parameters of the Au2 positions. This might be a hint for some short-range order.

The crystal structure of BaAu7.09Al5.91 (NaZn13 type, Fm3̅c). Barium sites are drawn in medium grey color, the mixed occupied Au/Al sites in black and white segments. The left-hand drawing emphasizes packing of Au2/Al2 centered icosahedra and barium centered 24-atom snub cubes. The polyhedral subunits and their connectivity through tetrahedra are emphasized at the right-hand part.
The fourth compound crystallizes with the cubic NaZn13 type structure. Both zinc sites (96i and 8b) show Au/Al mixing, leading to the composition BaAu7.09Al5.91 for the investigated crystal. Besides the solid solution BaAuxZn13–x [32], BaAu7.09Al5.91 is one of the few gold-containing members with NaZn13-type structure. The crystal chemistry and chemical bonding of binary and ternary NaZn13 type phases are well documented [33, 34]. Herein we only briefly discuss the structural peculiarities of BaAu7.09Al5.91. The unit cell of BaAu7.09Al5.91 is shown in Fig. 2. The basic polyhedral building units are Au2/Al2 centered icosahedra and barium centered 24-atom snub cubes which are packed in a CsCl manner. Due to different orientations of the icosahedra, a 2 × 2 × 2 superstructure occurs. Another geometrical description would be an fcc packing of icosahedra with icosahedra of the other orientation in all octahedral voids and the 24-atom snub cubes in all tetrahedral voids. Although these explanations are of purely geometrical nature, they offer an easy way to illustrate the large unit cell which comprises 112 atoms. BaAu7.09Al5.91 crystallizes with the undistorted cubic NaZn13 type. Several ordering variants forcing symmetry reductions are summarized in ref. [35].
Since both network sites (96i with almost equal occupancy and 8b with predominant aluminum occupancy) show Au/Al mixing, we can only discuss average distances (Table 6). They compare well with the sum of the covalent radii of Au + Al of 259 pm as well as with fcc gold (288 pm), similar to the three phases discussed above. The differently oriented icosahedra are connected via short Au/Al–Au/Al distances forming tetrahedra between the larger polyhedra.
Finally we draw back to the formulæ of SrAu3Al2, SrAu2.83Al2.17, BaAu2.89Al2.11, and BaAu7.09Al5.91 which are written in the classical style for ternary aluminides/intermetallic aluminum compounds [4]. However, keeping the course of the Pauling electronegativities [25] of gold (2.54) and aluminum (1.61) in mind, we can safely ascribe auridic character to the gold atoms, similar to many other series of related intermetallic gold compounds, e.g. RE4Mg3Au10 [36].
Acknowledgments
This work was supported by the Deutsche Forschungsgemeinschaft. B.G. is indebted to the Fonds der Chemischen Industrie and the NRW Forschungsschule Molecules and Materials – A Common Design Principle for PhD fellowships.
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©2015 by De Gruyter
Artikel in diesem Heft
- Frontmatter
- In this Issue
- Helical chain Ag(I) complexes with a tridentate N-donor ligand: syntheses, structural characterization, and properties
- A 3D mixed-valence Cu(I)/Cu(II) coordination polymer constructed by 2-(2-fluorophenyl)-1H-imidazo[4,5-f][1,10]phenanthroline and 1,3-benzenedicarboxylate
- 1,8-Naphthalimide derivative-based turn-off fluorescent probe for the detection of picrate in organic aqueous media
- Fluxional behaviour of tricyclo[2.2.1.02,6]heptaphosphide trisanion: a DFT investigation
- l-Valinate hydrates of nickel, copper and zinc – a structural study
- Pyridinium ylides in the one-pot synthesis of a new quinoline/indolizine hybrid
- Ternary aurides RE4Mg3Au10 (RE = La, Ce, Pr) and RE4Cd3Au10 (RE = Y, La–Nd, Sm, Gd–Dy) – ordering variants of the Zr7Ni10 type
- The structure of a coordination polymer constructed of manganese(II) biphenyl-4, 4′-dicarboxylate
- Alkaline earth-gold-aluminides: synthesis and structure of SrAu3Al2, SrAu2.83Al2.17, BaAu2.89Al2.11 and BaAu7.09Al5.91
- Phosphanchalkogenide und ihre Metallkomplexe. III. Halogenierungsprodukte der Gold(I)komplexe Ph3PEAuX (E = S oder Se; X = Cl, Br oder I)
- Synthesis and structural characterization of the new rare-earth borosilicates Pr3BSi2O10 and Tb3BSi2O10
Artikel in diesem Heft
- Frontmatter
- In this Issue
- Helical chain Ag(I) complexes with a tridentate N-donor ligand: syntheses, structural characterization, and properties
- A 3D mixed-valence Cu(I)/Cu(II) coordination polymer constructed by 2-(2-fluorophenyl)-1H-imidazo[4,5-f][1,10]phenanthroline and 1,3-benzenedicarboxylate
- 1,8-Naphthalimide derivative-based turn-off fluorescent probe for the detection of picrate in organic aqueous media
- Fluxional behaviour of tricyclo[2.2.1.02,6]heptaphosphide trisanion: a DFT investigation
- l-Valinate hydrates of nickel, copper and zinc – a structural study
- Pyridinium ylides in the one-pot synthesis of a new quinoline/indolizine hybrid
- Ternary aurides RE4Mg3Au10 (RE = La, Ce, Pr) and RE4Cd3Au10 (RE = Y, La–Nd, Sm, Gd–Dy) – ordering variants of the Zr7Ni10 type
- The structure of a coordination polymer constructed of manganese(II) biphenyl-4, 4′-dicarboxylate
- Alkaline earth-gold-aluminides: synthesis and structure of SrAu3Al2, SrAu2.83Al2.17, BaAu2.89Al2.11 and BaAu7.09Al5.91
- Phosphanchalkogenide und ihre Metallkomplexe. III. Halogenierungsprodukte der Gold(I)komplexe Ph3PEAuX (E = S oder Se; X = Cl, Br oder I)
- Synthesis and structural characterization of the new rare-earth borosilicates Pr3BSi2O10 and Tb3BSi2O10