Download citation
Download citation
link to html
Electron diffraction is a complementary technique to single-crystal X-ray diffraction and powder X-ray diffraction for structure solution of unknown crystals. Crystals too small to be studied by single-crystal X-ray diffraction or too complex to be solved by powder X-ray diffraction can be studied by electron diffraction. The main drawbacks of electron diffraction have been the difficulties in collecting complete three-dimensional electron diffraction data by conventional electron diffraction methods and the very time-consuming data collection. In addition, the intensities of electron diffraction suffer from dynamical scattering. Recently, a new electron diffraction method, rotation electron diffraction (RED), was developed, which can overcome the drawbacks and reduce dynamical effects. A complete three-dimensional electron diffraction data set can be collected from a sub-micrometre-sized single crystal in less than 2 h. Here the RED method is applied for ab initio structure determination of an unknown complex intermetallic phase, the pseudo-decagonal (PD) quasicrystal approximant Al37.0(Co,Ni)15.5, denoted as PD2. RED shows that the crystal is F-centered, with a = 46.4, b = 64.6, c = 8.2 Å. However, as with other approximants in the PD series, the reflections with odd l indices are much weaker than those with l even, so it was decided to first solve the PD2 structure in the smaller, primitive unit cell. The basic structure of PD2 with unit-cell parameters a = 23.2, b = 32.3, c = 4.1 Å and space group Pnmm has been solved in the present study. The structure with c = 8.2 Å will be taken up in the near future. The basic structure contains 55 unique atoms (17 Co/Ni and 38 Al) and is one of the most complex structures solved by electron diffraction. PD2 is built of characteristic 2 nm wheel clusters with fivefold rotational symmetry, which agrees with results from high-resolution electron microscopy images. Simulated electron diffraction patterns for the structure model are in good agreement with the experimental electron diffraction patterns obtained by RED.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600576713029294/he5621sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600576713029294/he5621sup2.hkl
Contains datablock pd70

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S1600576713029294/he5621sup3.pdf
Table S1 Atomic coordinates of the PD2 quasicrystal approximant structure in Al-Co-Ni

CCDC reference: 968428

Computing details top

Program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
(I) top
Crystal data top
Al18.50Co7.75Ni0γ = 90°
Mr = 956.75V = 3075.7 (2) Å3
a = 23.2010 (3) ÅZ = 8
b = 32.3100 (3) ÅF(000) = 5282
c = 4.1030 (3) ÅDx = 4.132 Mg m3
α = 90°µ = 0.00 mm1
β = 90°T = 293 K
Data collection top
Radiation source: fine-focus sealed tubeRint = 0.332
Graphite monochromatorθmax = 0.7°, θmin = 0.1°
8073 measured reflectionsh = 2223
1799 independent reflectionsk = 3232
1738 reflections with I > 2σ(I)l = 44
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullPrimary atom site location: structure-invariant direct methods
R[F2 > 2σ(F2)] = 0.429Secondary atom site location: difference Fourier map
wR(F2) = 0.702 w = 1/[σ2(Fo2) + (0.1P)2]
where P = (Fo2 + 2Fc2)/3
S = 4.16(Δ/σ)max = 0.435
1799 reflectionsΔρmax = 1.98 e Å3
156 parametersΔρmin = 2.56 e Å3
Crystal data top
Al18.50Co7.75Ni0β = 90°
Mr = 956.75γ = 90°
a = 23.2010 (3) ÅV = 3075.7 (2) Å3
b = 32.3100 (3) ÅZ = 8
c = 4.1030 (3) ŵ = 0.00 mm1
α = 90°T = 293 K
Data collection top
8073 measured reflectionsRint = 0.332
1799 independent reflectionsθmax = 0.7°
1738 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.4290 restraints
wR(F2) = 0.702(Δ/σ)max = 0.435
S = 4.16Δρmax = 1.98 e Å3
1799 reflectionsΔρmin = 2.56 e Å3
156 parameters
Special details top

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 F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 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 (Å2) top
xyzUiso*/Ueq
Co10.5322 (8)0.3655 (5)0.75000.011 (5)*
Co20.1625 (8)0.5570 (4)0.25000.000 (4)*
Co30.1506 (11)0.3217 (7)0.75000.036 (6)*
Co40.483 (3)0.25000.25000.11 (2)*
Co50.0231 (12)0.25000.25000.014 (7)*
Co60.8568 (16)0.25000.25000.036 (9)*
Co70.3368 (8)0.3177 (5)0.75000.007 (5)*
Co80.3365 (8)0.5580 (5)0.25000.007 (5)*
Co90.6654 (8)0.2968 (5)0.25000.009 (5)*
Co100.2866 (10)0.4383 (6)0.25000.019 (5)*
Co110.0316 (7)0.4842 (5)0.25000.007 (5)*
Co120.0290 (7)0.3673 (5)0.75000.003 (4)*
Co130.4693 (7)0.4855 (5)0.25000.000 (4)*
Co140.2149 (10)0.4374 (6)0.25000.024 (6)*
Co150.7823 (8)0.3225 (5)0.25000.007 (4)*
Co160.3489 (12)0.3730 (8)0.25000.042 (7)*
Co170.1461 (9)0.3701 (6)0.25000.018 (5)*
Al180.1242 (15)0.4487 (10)0.25000.070 (9)*
Al190.3562 (7)0.5114 (5)0.25000.009 (4)*
Al200.1804 (19)0.25000.75000.062 (12)*
Al210.4087 (14)0.3674 (10)0.75000.068 (9)*
Al220.601 (2)0.3254 (14)0.75000.124 (17)*
Al230.1072 (11)0.2947 (8)0.25000.046 (7)*
Al240.0260 (9)0.3993 (6)0.25000.026 (5)*
Al250.635 (2)0.25000.75000.084 (15)*
Al260.8343 (7)0.2914 (5)0.25000.006 (4)*
Al270.7078 (19)0.3135 (13)0.75000.101 (12)*
Al280.5056 (8)0.2895 (6)0.75000.022 (5)*
Al290.089 (2)0.5142 (14)0.75000.121 (16)*
Al300.4997 (14)0.3206 (9)0.25000.067 (9)*
Al310.0029 (10)0.4357 (6)0.75000.030 (6)*
Al320.1978 (8)0.4841 (5)0.25000.013 (5)*
Al330.2614 (11)0.5582 (7)0.75000.045 (7)*
Al340.7553 (18)0.25000.25000.066 (11)*
Al350.0787 (14)0.6043 (9)0.25000.067 (8)*
Al360.301 (3)0.25000.75000.12 (2)*
Al370.425 (2)0.5191 (14)0.25000.121 (16)*
Al380.243 (2)0.3192 (17)0.75000.18 (3)*
Al390.4982 (12)0.4398 (7)0.75000.046 (7)*
Al400.3023 (12)0.6248 (8)1.25000.048 (7)*
Al410.2956 (10)0.3892 (7)0.75000.042 (6)*
Al420.1994 (9)0.3981 (6)0.75000.025 (5)*
Al430.0709 (12)0.25000.25000.027 (7)*
Al440.6113 (14)0.4137 (10)0.75000.070 (9)*
Al450.176 (4)0.540 (2)0.25000.25 (4)*
Al460.2935 (18)0.4836 (12)0.25000.094 (12)*
Al470.0081 (12)0.3227 (8)0.25000.055 (7)*
Al480.586 (3)0.25000.25000.13 (2)*
Al490.1015 (11)0.3330 (8)0.75000.053 (7)*
Al500.0764 (14)0.3650 (9)0.75000.061 (8)*
Al510.407 (3)0.4230 (19)0.25000.16 (2)*
Al520.027 (2)0.2876 (13)0.75000.124 (17)*
Al530.1959 (19)0.6177 (13)0.75000.100 (13)*
Al540.381 (3)0.25000.75000.15 (3)*
Al550.401 (3)0.2906 (17)0.25000.16 (3)*
Bond lengths (Å) top
Co1—Al222.05 (5)Al26—Al43viii2.57 (3)
Co1—Al442.41 (4)Al26—Al26v2.68 (3)
Co1—Al392.53 (3)Al26—Al49vii2.87 (2)
Co1—Al282.53 (2)Al26—Al49viii2.87 (2)
Co1—Al302.62 (2)Al26—Al53xiii3.02 (5)
Co1—Al30i2.62 (2)Al26—Al27ii3.02 (5)
Co1—Al212.87 (4)Al26—Al34ii3.06 (3)
Co2—Al452.15 (2)Al26—Al343.06 (3)
Co2—Al45i2.15 (2)Al27—Co9i2.34 (2)
Co2—Al53i2.11 (4)Al27—Co15i2.70 (3)
Co2—Al29i2.19 (5)Al27—Al40xii2.87 (3)
Co2—Al33i2.29 (3)Al27—Al40xiii2.87 (3)
Co2—Al322.49 (2)Al27—Al26i3.02 (5)
Co2—Al352.47 (4)Al27—Al343.10 (3)
Co3—Al502.22 (4)Al27—Al34i3.10 (3)
Co3—Al382.16 (6)Al27—Al53xii3.15 (6)
Co3—Al202.42 (3)Al28—Al30i2.289 (15)
Co3—Al23ii2.45 (2)Al28—Al302.289 (15)
Co3—Al232.45 (2)Al28—Co4i2.475 (18)
Co3—Co172.581 (19)Al28—Al28iv2.55 (4)
Co3—Co17ii2.581 (19)Al28—Al483.05 (5)
Co3—Al422.72 (3)Al28—Al48i3.05 (5)
Co3—Al523.08 (5)Al29—Co2ii2.19 (5)
Co4—Al302.32 (3)Al29—Co11ii2.63 (3)
Co4—Al30iii2.32 (3)Al29—Co11xiv2.80 (5)
Co4—Al282.475 (18)Al29—Al32ii2.70 (5)
Co4—Al28iii2.475 (18)Al29—Al35ii2.92 (5)
Co4—Al28iv2.475 (18)Al29—Al452.99 (7)
Co4—Al28ii2.475 (18)Al29—Al45ii2.99 (7)
Co4—Al482.40 (9)Al29—Al18ii3.06 (4)
Co4—Al55iii2.31 (7)Al29—Al313.23 (5)
Co4—Al552.31 (7)Al29—Al31xvi3.37 (4)
Co5—Al432.18 (4)Al30—Al28ii2.289 (15)
Co5—Al232.43 (3)Al30—Al552.49 (6)
Co5—Al23v2.43 (3)Al30—Co1ii2.62 (2)
Co5—Al52i2.39 (2)Al30—Al483.03 (6)
Co5—Al52vi2.39 (2)Al30—Al22ii3.12 (4)
Co5—Al522.39 (2)Al30—Al21ii3.31 (4)
Co5—Al52v2.39 (2)Al31—Al24ii2.424 (16)
Co5—Al47v2.46 (3)Al31—Co11ii2.667 (17)
Co5—Al472.46 (3)Al31—Co11xiv2.71 (3)
Co6—Al342.35 (5)Al31—Al502.85 (4)
Co6—Al26v2.504 (12)Al31—Al35xiv3.08 (3)
Co6—Al26i2.504 (12)Al31—Al35xv3.08 (3)
Co6—Al262.504 (12)Al31—Al29xvi3.37 (4)
Co6—Al26iii2.504 (12)Al31—Al29xiv3.37 (4)
Co6—Al43vii2.65 (3)Al32—Co14i2.578 (16)
Co6—Al43viii2.65 (3)Al32—Al33i2.81 (3)
Co6—Al49vii2.85 (3)Al32—Al42i2.78 (3)
Co6—Al49ix2.85 (3)Al32—Al29i2.70 (5)
Co6—Co15iii2.91 (3)Al32—Al45i2.77 (5)
Co6—Co152.91 (3)Al32—Al452.77 (5)
Co7—Al542.42 (4)Al32—Al18i2.91 (3)
Co7—Al362.34 (3)Al32—Al46i3.02 (3)
Co7—Al212.32 (4)Al33—Co2ii2.29 (3)
Co7—Al55i2.68 (4)Al33—Al532.45 (5)
Co7—Al552.68 (4)Al33—Al19ii2.67 (3)
Co7—Al412.50 (3)Al33—Co8ii2.69 (2)
Co7—Co16i2.74 (2)Al33—Al32ii2.81 (3)
Co7—Co162.74 (2)Al33—Al45ii2.91 (6)
Co7—Al38i2.98 (4)Al33—Al452.91 (6)
Co7—Al38x2.98 (4)Al33—Al44xii3.09 (4)
Co8—Al40i2.30 (3)Al33—Al40i3.12 (3)
Co8—Al372.40 (5)Al33—Al403.12 (3)
Co8—Al44xi2.55 (2)Al33—Al46ii3.25 (3)
Co8—Al44xii2.55 (2)Al34—Co15iii2.43 (2)
Co8—Al462.60 (4)Al34—Co9iii2.58 (4)
Co8—Al192.585 (14)Al34—Al26i3.06 (3)
Co8—Al19ii2.585 (14)Al34—Al26iii3.06 (3)
Co8—Al332.69 (2)Al34—Al26v3.06 (3)
Co8—Al33i2.69 (2)Al34—Al27iii3.10 (3)
Co9—Al272.34 (2)Al34—Al27iv3.10 (3)
Co9—Al27ii2.34 (2)Al35—Al24xv2.43 (4)
Co9—Al482.39 (6)Al35—Co12xiv2.53 (2)
Co9—Al40xiii2.64 (3)Al35—Co12xv2.53 (2)
Co9—Al342.58 (4)Al35—Al53i2.75 (5)
Co9—Al22ii2.71 (3)Al35—Al47xv2.87 (4)
Co9—Al222.71 (3)Al35—Al49xv2.93 (3)
Co9—Al25ii2.645 (17)Al35—Al49xiv2.93 (3)
Co9—Al252.645 (17)Al35—Al29i2.92 (5)
Co9—Co152.84 (3)Al35—Al31xiv3.08 (3)
Co10—Al42i2.40 (3)Al35—Al31xv3.08 (3)
Co10—Co162.56 (3)Al36—Al541.87 (10)
Co10—Al46i2.53 (2)Al36—Co7iv2.34 (3)
Co10—Al462.53 (2)Al36—Al38v3.31 (5)
Co10—Al322.54 (3)Al36—Al38x3.31 (5)
Co10—Al41ii2.601 (18)Al36—Al38iii3.31 (5)
Co10—Al412.601 (18)Al36—Al38i3.31 (5)
Co10—Co142.64 (2)Al37—Co13xii2.46 (5)
Co10—Co14i2.64 (2)Al37—Co13ii2.54 (3)
Co10—Al512.85 (6)Al37—Al19ii2.61 (3)
Co10—Al192.86 (3)Al37—Al44xi3.10 (4)
Co11—Al182.44 (4)Al37—Al44xii3.10 (4)
Co11—Al29i2.63 (3)Al37—Al39xi3.03 (4)
Co11—Al292.63 (3)Al37—Al39xii3.03 (4)
Co11—Al312.667 (17)Al37—Al39ii3.08 (5)
Co11—Al31i2.667 (17)Al37—Al463.25 (6)
Co11—Al31xiv2.71 (3)Al38—Al422.75 (6)
Co11—Al29xiv2.80 (5)Al38—Co7ii2.98 (4)
Co11—Co11xiv2.72 (2)Al38—Co7xvii2.98 (4)
Co11—Co11xv2.72 (2)Al38—Co16ii3.00 (6)
Co11—Al242.75 (3)Al38—Al41ii3.29 (5)
Co12—Al492.02 (3)Al38—Al41xvii3.29 (5)
Co12—Al312.33 (3)Al38—Al36xvii3.31 (5)
Co12—Al502.45 (4)Al38—Al36ii3.31 (5)
Co12—Al35xiv2.53 (2)Al39—Co13xi2.53 (3)
Co12—Al35xv2.53 (2)Al39—Co13i2.614 (18)
Co12—Al47ii2.555 (19)Al39—Al442.76 (4)
Co12—Al472.555 (19)Al39—Al37xi3.03 (4)
Co12—Al242.628 (16)Al39—Al37xii3.03 (4)
Co12—Al24ii2.628 (16)Al39—Al37i3.08 (5)
Co12—Al522.88 (4)Al39—Al512.99 (5)
Co13—Al39xi2.53 (3)Al39—Al51i2.99 (5)
Co13—Al37xii2.46 (5)Al40—Co8ii2.30 (3)
Co13—Al37i2.54 (3)Al40—Co9xiii2.64 (3)
Co13—Al372.54 (3)Al40—Co15xiii2.60 (3)
Co13—Al39ii2.614 (18)Al40—Al27xii2.87 (3)
Co13—Al392.614 (18)Al40—Al27xiii2.87 (3)
Co13—Al512.48 (6)Al40—Al33ii3.12 (3)
Co13—Co13xi2.67 (2)Al40—Al44xii3.13 (3)
Co13—Co13xii2.67 (2)Al40—Al44xiii3.13 (3)
Co13—Al192.76 (2)Al40—Al53ii3.22 (4)
Co14—Al182.14 (4)Al40—Al533.22 (4)
Co14—Al462.36 (4)Al41—Co16i2.45 (2)
Co14—Al422.439 (15)Al41—Co14i2.43 (3)
Co14—Al42i2.439 (15)Al41—Co10i2.601 (18)
Co14—Al41ii2.43 (3)Al41—Al42i3.05 (2)
Co14—Al322.578 (16)Al41—Al42x3.05 (2)
Co14—Al32ii2.578 (16)Al41—Al46i3.05 (5)
Co14—Co10ii2.64 (2)Al41—Al38i3.29 (5)
Co14—Co172.70 (3)Al41—Al38x3.29 (5)
Co15—Al342.43 (2)Al42—Co10ii2.40 (3)
Co15—Al262.583 (15)Al42—Co14ii2.439 (15)
Co15—Al26i2.583 (15)Al42—Co17ii2.561 (18)
Co15—Al40xiii2.60 (3)Al42—Al32ii2.78 (3)
Co15—Al27ii2.70 (3)Al42—Al503.05 (4)
Co15—Al272.70 (3)Al42—Al41ii3.05 (2)
Co15—Al49vii2.72 (3)Al42—Al41xvii3.05 (2)
Co15—Al53xii2.86 (3)Al42—Al18ii3.15 (3)
Co15—Al53xiii2.86 (3)Al43—Al26xviii2.57 (3)
Co16—Al512.11 (6)Al43—Al26xix2.57 (3)
Co16—Al552.92 (6)Al43—Co6xx2.65 (3)
Co16—Al41ii2.45 (2)Al43—Co6xix2.65 (3)
Co16—Al412.45 (2)Al43—Al472.76 (3)
Co16—Al212.48 (3)Al43—Al47v2.76 (3)
Co16—Al21ii2.48 (3)Al43—Al52i3.29 (4)
Co16—Co7ii2.74 (2)Al43—Al523.29 (4)
Co16—Al38i3.00 (6)Al43—Al52v3.29 (4)
Co17—Al42i2.561 (18)Al43—Al52vi3.29 (4)
Co17—Al422.561 (18)Al44—Al19xi2.53 (4)
Co17—Al182.59 (4)Al44—Co8xi2.55 (2)
Co17—Co3i2.581 (19)Al44—Co8xii2.55 (2)
Co17—Al502.62 (2)Al44—Al37xi3.10 (4)
Co17—Al50i2.62 (2)Al44—Al37xii3.10 (4)
Co17—Al232.60 (3)Al44—Al33xii3.09 (4)
Co17—Al242.94 (3)Al44—Al40xii3.13 (3)
Al18—Al242.78 (4)Al44—Al40xiii3.13 (3)
Al18—Al322.91 (3)Al45—Co2ii2.15 (2)
Al18—Al32ii2.91 (3)Al45—Al32ii2.77 (5)
Al18—Al423.15 (3)Al45—Al33i2.91 (6)
Al18—Al42i3.15 (3)Al45—Al29i2.99 (7)
Al18—Al29i3.06 (4)Al45—Al53i3.28 (7)
Al18—Al293.06 (4)Al45—Al533.28 (7)
Al18—Al453.18 (8)Al45—Al463.27 (9)
Al19—Al44xi2.53 (4)Al46—Co10ii2.53 (2)
Al19—Al37i2.61 (3)Al46—Al19ii2.67 (3)
Al19—Al372.61 (3)Al46—Al32ii3.02 (3)
Al19—Co8i2.585 (14)Al46—Al41ii3.05 (5)
Al19—Al33i2.67 (3)Al46—Al33i3.25 (3)
Al19—Al462.67 (3)Al47—Al522.48 (3)
Al19—Al46i2.67 (3)Al47—Al52i2.48 (3)
Al19—Al513.09 (7)Al47—Co12i2.555 (19)
Al20—Co3vi2.42 (3)Al47—Al35xv2.87 (4)
Al20—Al382.67 (6)Al47—Al493.00 (3)
Al20—Al38vi2.67 (6)Al47—Al49i3.00 (3)
Al20—Al23vi3.03 (3)Al47—Al50i3.15 (3)
Al20—Al23ii3.03 (3)Al48—Al25ii2.35 (4)
Al20—Al23v3.03 (3)Al48—Co9iii2.39 (6)
Al20—Al233.03 (3)Al48—Al30iii3.03 (6)
Al21—Co16i2.48 (3)Al48—Al28iii3.05 (5)
Al21—Al412.72 (4)Al48—Al28ii3.05 (5)
Al21—Al51i2.73 (4)Al48—Al28iv3.05 (5)
Al21—Al512.73 (4)Al48—Al22iii3.20 (4)
Al21—Al553.22 (4)Al49—Co15xx2.72 (3)
Al21—Al55i3.22 (4)Al49—Co6xx2.85 (3)
Al21—Al393.13 (4)Al49—Al26xx2.87 (2)
Al21—Al303.31 (4)Al49—Al26xix2.87 (2)
Al21—Al30i3.31 (4)Al49—Al35xv2.93 (3)
Al22—Al272.52 (6)Al49—Al35xiv2.93 (3)
Al22—Al252.56 (5)Al49—Al47ii3.00 (3)
Al22—Al282.49 (5)Al49—Al523.32 (5)
Al22—Co9i2.71 (3)Al49—Al53xvi3.40 (4)
Al22—Al442.87 (6)Al49—Al53xiv3.40 (4)
Al22—Al483.20 (4)Al50—Co17ii2.62 (2)
Al22—Al48i3.20 (4)Al50—Al24ii2.61 (2)
Al22—Al30i3.12 (4)Al50—Al522.75 (5)
Al22—Al303.12 (4)Al50—Al47ii3.15 (3)
Al23—Co3i2.45 (2)Al50—Al23ii3.14 (3)
Al23—Al472.82 (4)Al51—Al21ii2.73 (4)
Al23—Al522.78 (3)Al51—Al39ii2.99 (5)
Al23—Al52i2.78 (3)Al51—Al41ii3.48 (5)
Al23—Al23v2.89 (5)Al52—Co5ii2.39 (2)
Al23—Al20i3.03 (3)Al52—Al47ii2.48 (3)
Al23—Al50i3.14 (3)Al52—Al52vi2.43 (8)
Al23—Al503.14 (3)Al52—Al23ii2.78 (3)
Al24—Al31i2.424 (16)Al52—Al43ii3.29 (4)
Al24—Al312.424 (16)Al53—Co2ii2.11 (4)
Al24—Al35xv2.43 (4)Al53—Al35ii2.75 (5)
Al24—Al472.60 (3)Al53—Co15xii2.86 (3)
Al24—Al502.61 (2)Al53—Co15xiii2.86 (3)
Al24—Al50i2.61 (2)Al53—Al26xiii3.02 (5)
Al24—Co12i2.628 (16)Al53—Al27xii3.15 (6)
Al25—Al48i2.35 (4)Al53—Al45ii3.28 (7)
Al25—Al482.35 (4)Al53—Al40i3.22 (4)
Al25—Al22iv2.56 (5)Al53—Al49xvi3.40 (4)
Al25—Al272.66 (5)Al54—Co7iv2.42 (4)
Al25—Al27iv2.66 (5)Al54—Al55i2.48 (3)
Al25—Co9i2.645 (18)Al54—Al55iii2.48 (3)
Al25—Co9iii2.645 (18)Al54—Al55iv2.48 (3)
Al25—Co9iv2.645 (18)Al54—Al552.48 (3)
Al25—Al28iv3.26 (5)Al55—Co7ii2.68 (4)
Al25—Al283.26 (5)Al55—Al54ii2.48 (3)
Al26—Co6ii2.504 (12)Al55—Al21ii3.22 (4)
Al26—Co15ii2.583 (15)
Symmetry codes: (i) x, y, z+1; (ii) x, y, z1; (iii) x, y+1/2, z+1/2; (iv) x, y+1/2, z+3/2; (v) x, y+1/2, z1/2; (vi) x, y+1/2, z3/2; (vii) x+1, y, z+1; (viii) x+1, y, z; (ix) x+1, y+1/2, z1/2; (x) x, y, z+2; (xi) x+1, y+1, z+1; (xii) x+1, y+1, z; (xiii) x+1, y+1, z1; (xiv) x, y+1, z1; (xv) x, y+1, z; (xvi) x, y+1, z2; (xvii) x, y, z2; (xviii) x1, y+1/2, z1/2; (xix) x1, y, z; (xx) x1, y, z1.

Experimental details

Crystal data
Chemical formulaAl18.50Co7.75Ni0
Mr956.75
Crystal system, space group?, ?
Temperature (K)293
a, b, c (Å)23.2010 (3), 32.3100 (3), 4.1030 (3)
α, β, γ (°)90, 90, 90
V3)3075.7 (2)
Z8
Radiation type?, λ = 0.02508 Å
µ (mm1)0.00
Crystal size (mm) × ×
Data collection
Diffractometer?
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
8073, 1799, 1738
Rint0.332
θmax (°)0.7
(sin θ/λ)max1)0.508
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.429, 0.702, 4.16
No. of reflections1799
No. of parameters156
(Δ/σ)max0.435
Δρmax, Δρmin (e Å3)1.98, 2.56

Computer programs: SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997).

 

Follow J. Appl. Cryst.
Sign up for e-alerts
Follow J. Appl. Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds