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We report the crystal structure analyses of CaAlSi from single-crystal and powder X-ray diffraction and the existence of two commensurately modulated phases, a sixfold and a fivefold modulated structure. This polymorphism seems to be correlated to the thermal history of the sample. We describe both modulated structures using a three-dimensional and a (3 + 1)-dimensional formalism.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768106025900/ck5016sup1.cif
Contains datablocks global, 6-fold_superstructure_298K, 5-fold_superstructure_298K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768106025900/ck50166-foldsup2.hkl
Contains datablock 6-fold_superstructure_(298K)

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768106025900/ck50165-foldsup3.hkl
Contains datablock 5-fold_superstructure_(298K)

Computing details top

For both compounds, data collection: X-AREA (Stoe, 2002); cell refinement: FullProf Suite (Rodriguez-Carvajal); data reduction: X-RED (Stoe, 1996); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ATOMS Version 5.1; software used to prepare material for publication: WinGX 1.64.05 (Farrugia, 1999).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
[Figure 8]
[Figure 9]
[Figure 10]
(6-fold_superstructure_298K) top
Crystal data top
AlSiCaDx = 2.383 Mg m3
Dm = 2.383 Mg m3
Dm measured by not measured
Mr = 95.15Melting point: 0 K
Hexagonal, P6m2Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P -6 2Cell parameters from 23 reflections
a = 4.17720 (4) Åθ = 10.1–47.2°
c = 26.3246 (4) ŵ = 2.76 mm1
V = 397.80 (1) Å3T = 298 K
Z = 6Cuboid, metallic dark grey
F(000) = 2820.18 × 0.16 × 0.15 × 0 (radius) mm
Data collection top
STOE IPDS 2
diffractometer
233 reflections with I > 2σ(I)
rotation method scansRint = 0.049
Absorption correction: empirical (using intensity measurements)
X-SHAPE (Stoe & Cie, 1996)
θmax = 27.1°, θmin = 1.6°
Tmin = 0.557, Tmax = 0.660h = 55
3136 measured reflectionsk = 55
429 independent reflectionsl = 3333
Refinement top
Refinement on F20 constraints
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.013P)2]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.03(Δ/σ)max < 0.001
wR(F2) = 0.082Δρmax = 0.25 e Å3
S = 1.96Δρmin = 0.29 e Å3
429 reflectionsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
31 parametersAbsolute structure parameter: 0.1 (3)
0 restraints
Crystal data top
AlSiCaZ = 6
Mr = 95.15Mo Kα radiation
Hexagonal, P6m2µ = 2.76 mm1
a = 4.17720 (4) ÅT = 298 K
c = 26.3246 (4) Å0.18 × 0.16 × 0.15 × 0 (radius) mm
V = 397.80 (1) Å3
Data collection top
STOE IPDS 2
diffractometer
429 independent reflections
Absorption correction: empirical (using intensity measurements)
X-SHAPE (Stoe & Cie, 1996)
233 reflections with I > 2σ(I)
Tmin = 0.557, Tmax = 0.660Rint = 0.049
3136 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.030 restraints
wR(F2) = 0.082Δρmax = 0.25 e Å3
S = 1.96Δρmin = 0.29 e Å3
429 reflectionsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
31 parametersAbsolute structure parameter: 0.1 (3)
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Ca1000.08205 (12)0.0160 (6)
Ca2000.24927 (15)0.0151 (6)
Ca3000.41729 (14)0.0172 (7)
SI10.33330.666700.038 (2)0.5
SI20.66670.333300.0147 (14)0.5
SI30.33330.66670.1605 (2)0.0217 (12)0.5
SI40.66670.33330.17111 (19)0.0145 (12)0.5
SI50.33330.66670.32802 (15)0.0128 (10)0.5
SI60.66670.33330.3412 (2)0.0219 (11)0.5
SI70.33330.66670.50.0084 (11)0.5
SI80.66670.33330.50.039 (3)0.5
AL10.33330.666700.038 (2)0.5
AL20.66670.333300.0147 (14)0.5
AL30.33330.66670.1605 (2)0.0217 (12)0.5
AL40.66670.33330.17111 (19)0.0145 (12)0.5
AL50.33330.66670.32802 (15)0.0128 (10)0.5
AL60.66670.33330.3412 (2)0.0219 (11)0.5
AL70.33330.66670.50.0084 (11)0.5
AL80.66670.33330.50.039 (3)0.5
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ca10.0189 (9)0.0189 (9)0.0104 (11)0.0094 (5)00
Ca20.0158 (8)0.0158 (8)0.0139 (10)0.0079 (4)00
Ca30.0156 (9)0.0156 (9)0.0202 (14)0.0078 (5)00
SI10.0141 (19)0.0141 (19)0.086 (7)0.0071 (10)00
SI20.0130 (18)0.0130 (18)0.018 (3)0.0065 (9)00
SI30.0168 (14)0.0168 (14)0.032 (3)0.0084 (7)00
SI40.0073 (12)0.0073 (12)0.029 (3)0.0036 (6)00
SI50.0115 (13)0.0115 (13)0.015 (2)0.0057 (7)00
SI60.0127 (12)0.0127 (12)0.040 (3)0.0063 (6)00
SI70.0048 (15)0.0048 (15)0.015 (3)0.0024 (7)00
SI80.0088 (18)0.0088 (18)0.101 (8)0.0044 (9)00
AL10.0141 (19)0.0141 (19)0.086 (7)0.0071 (10)00
AL20.0130 (18)0.0130 (18)0.018 (3)0.0065 (9)00
AL30.0168 (14)0.0168 (14)0.032 (3)0.0084 (7)00
AL40.0073 (12)0.0073 (12)0.029 (3)0.0036 (6)00
AL50.0115 (13)0.0115 (13)0.015 (2)0.0057 (7)00
AL60.0127 (12)0.0127 (12)0.040 (3)0.0063 (6)00
AL70.0048 (15)0.0048 (15)0.015 (3)0.0024 (7)00
AL80.0088 (18)0.0088 (18)0.101 (8)0.0044 (9)00
Bond lengths (Å) top
Ca1—SI33.175 (4)Ca3—Ca3iii4.1772
Ca1—AL3i3.175 (4)Ca3—Ca3viii4.355 (7)
Ca1—SI3i3.175 (4)SI1—AL2v2.4117
Ca1—AL3ii3.175 (4)SI1—AL2iii2.4117
Ca1—SI3ii3.175 (4)SI1—SI2v2.4117
Ca1—AL2ii3.238 (2)SI1—SI2iii2.4117
Ca1—AL1ii3.238 (2)SI1—SI22.4117
Ca1—SI2ii3.238 (2)SI1—Ca1iv3.238 (2)
Ca1—SI1ii3.238 (2)SI1—Ca1v3.238 (2)
Ca1—AL2iii3.238 (2)SI1—Ca1vii3.238 (2)
Ca1—AL1i3.238 (2)SI1—Ca1ix3.238 (2)
Ca1—SI2iii3.238 (2)SI1—Ca1x3.238 (2)
Ca1—SI1i3.238 (2)SI1—SI34.224 (5)
Ca1—SI23.238 (2)SI2—AL1vi2.4117
Ca1—SI13.238 (2)SI2—AL1i2.4117
Ca1—SI43.363 (5)SI2—SI1vi2.4117
Ca1—AL4iii3.363 (5)SI2—SI1i2.4117
Ca1—SI4iii3.363 (5)SI2—Ca1iv3.238 (2)
Ca1—AL4ii3.363 (5)SI2—Ca1vi3.238 (2)
Ca1—SI4ii3.363 (5)SI2—Ca1vii3.238 (2)
Ca1—Ca1ii4.1772SI2—Ca1xi3.238 (2)
Ca1—Ca1iv4.1772SI2—Ca1x3.238 (2)
Ca1—Ca1v4.1772SI2—SI44.504 (5)
Ca1—Ca1iii4.1772SI3—AL4v2.4279 (7)
Ca1—Ca1i4.1772SI3—SI4v2.4279 (7)
Ca1—Ca1vi4.1772SI3—AL4iii2.4279 (6)
Ca1—Ca1vii4.320 (7)SI3—SI4iii2.4279 (6)
Ca1—Ca24.402 (5)SI3—SI42.4279 (7)
Ca2—AL4ii3.170 (4)SI3—Ca1v3.175 (4)
Ca2—SI4ii3.170 (4)SI3—Ca1iv3.175 (4)
Ca2—AL4iii3.170 (4)SI3—Ca2iv3.359 (5)
Ca2—SI4iii3.170 (4)SI3—Ca2v3.359 (5)
Ca2—SI43.170 (4)SI3—SI54.411 (5)
Ca2—SI53.180 (4)SI4—AL3i2.4279 (6)
Ca2—AL5i3.180 (4)SI4—SI3i2.4279 (6)
Ca2—SI5i3.180 (4)SI4—AL3vi2.4279 (7)
Ca2—AL5ii3.180 (4)SI4—SI3vi2.4279 (7)
Ca2—SI5ii3.180 (4)SI4—Ca2iv3.170 (4)
Ca2—AL3ii3.359 (5)SI4—Ca2vi3.170 (4)
Ca2—SI3ii3.359 (5)SI4—Ca1vi3.363 (5)
Ca2—AL3i3.359 (5)SI4—Ca1iv3.363 (5)
Ca2—SI3i3.359 (5)SI4—SI64.479 (8)
Ca2—SI33.359 (5)SI5—AL6v2.4367 (9)
Ca2—SI63.417 (5)SI5—SI6v2.4367 (9)
Ca2—AL6iii3.417 (5)SI5—AL6iii2.4367 (9)
Ca2—SI6iii3.417 (5)SI5—SI6iii2.4367 (9)
Ca2—AL6ii3.417 (5)SI5—SI62.4367 (9)
Ca2—SI6ii3.417 (5)SI5—Ca2v3.180 (4)
Ca2—Ca2iv4.1772SI5—Ca2iv3.180 (4)
Ca2—Ca2ii4.1772SI5—Ca3iv3.367 (4)
Ca2—Ca2i4.1772SI5—Ca3v3.367 (4)
Ca2—Ca2iii4.1772SI5—SI74.527 (4)
Ca2—Ca2vi4.1772SI6—AL5i2.4367 (9)
Ca2—Ca2v4.1772SI6—SI5i2.4367 (9)
Ca2—Ca34.423 (5)SI6—AL5vi2.4367 (9)
Ca3—AL6ii3.134 (5)SI6—SI5vi2.4367 (9)
Ca3—SI6ii3.134 (5)SI6—Ca3iv3.134 (5)
Ca3—AL6iii3.134 (5)SI6—Ca3vi3.134 (5)
Ca3—SI6iii3.134 (5)SI6—Ca2vi3.417 (5)
Ca3—SI63.134 (5)SI6—Ca2iv3.417 (5)
Ca3—SI83.249 (2)SI6—SI84.179 (6)
Ca3—SI73.249 (2)SI7—AL8v2.4117
Ca3—AL8iii3.249 (2)SI7—AL8iii2.4117
Ca3—AL7i3.249 (2)SI7—SI8v2.4117
Ca3—SI8iii3.249 (2)SI7—SI8iii2.4117
Ca3—SI7i3.249 (2)SI7—SI82.4117
Ca3—AL8ii3.249 (2)SI7—Ca3xii3.249 (2)
Ca3—AL7ii3.249 (2)SI7—Ca3xiii3.249 (2)
Ca3—SI8ii3.249 (2)SI7—Ca3v3.249 (2)
Ca3—SI7ii3.249 (2)SI7—Ca3viii3.249 (2)
Ca3—AL5ii3.367 (4)SI7—Ca3iv3.249 (2)
Ca3—SI5ii3.367 (4)SI8—AL7vi2.4117
Ca3—AL5i3.367 (4)SI8—AL7i2.4117
Ca3—SI5i3.367 (4)SI8—SI7vi2.4117
Ca3—SI53.367 (4)SI8—SI7i2.4117
Ca3—Ca3iv4.1772SI8—Ca3xii3.249 (2)
Ca3—Ca3ii4.1772SI8—Ca3xiv3.249 (2)
Ca3—Ca3i4.1772SI8—Ca3vi3.249 (2)
Ca3—Ca3vi4.1772SI8—Ca3viii3.249 (2)
Ca3—Ca3v4.1772SI8—Ca3iv3.249 (2)
Symmetry codes: (i) x, y1, z; (ii) x1, y1, z; (iii) x1, y, z; (iv) x+1, y+1, z; (v) x, y+1, z; (vi) x+1, y, z; (vii) x, y, z; (viii) x, y, z+1; (ix) x, y+1, z; (x) x+1, y+1, z; (xi) x+1, y, z; (xii) x+1, y+1, z+1; (xiii) x, y+1, z+1; (xiv) x+1, y, z+1.
(5-fold_superstructure_298K) top
Crystal data top
AlSiCaDx = 2.383 Mg m3
Dm = 2.383 Mg m3
Dm measured by not measured
Mr = 95.15Melting point: 0 K
Hexagonal, P6m2Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P -6 2Cell parameters from 23 reflections
a = 4.17720 (4) Åθ = 10.1–47.2°
c = 21.9372 (3) ŵ = 2.76 mm1
V = 331.50 (1) Å3T = 298 K
Z = 5Cuboid, metallic dark grey
F(000) = 2350.21 × 0.20 × 0.18 × 0 (radius) mm
Data collection top
STOE IPDS 2
diffractometer
340 reflections with I > 2σ(I)
rotation method scansRint = 0.058
Absorption correction: empirical (using intensity measurements)
X-SHAPE (Stoe & Cie, 1996)
θmax = 29.2°, θmin = 1.9°
Tmin = 0.531, Tmax = 0.607h = 55
4754 measured reflectionsk = 55
422 independent reflectionsl = 3030
Refinement top
Refinement on F20 constraints
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.023P)2]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.035(Δ/σ)max < 0.001
wR(F2) = 0.086Δρmax = 0.46 e Å3
S = 1.99Δρmin = 0.41 e Å3
422 reflectionsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
26 parametersAbsolute structure parameter: 0.5 (4)
0 restraints
Crystal data top
AlSiCaZ = 5
Mr = 95.15Mo Kα radiation
Hexagonal, P6m2µ = 2.76 mm1
a = 4.17720 (4) ÅT = 298 K
c = 21.9372 (3) Å0.21 × 0.20 × 0.18 × 0 (radius) mm
V = 331.50 (1) Å3
Data collection top
STOE IPDS 2
diffractometer
422 independent reflections
Absorption correction: empirical (using intensity measurements)
X-SHAPE (Stoe & Cie, 1996)
340 reflections with I > 2σ(I)
Tmin = 0.531, Tmax = 0.607Rint = 0.058
4754 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0350 restraints
wR(F2) = 0.086Δρmax = 0.46 e Å3
S = 1.99Δρmin = 0.41 e Å3
422 reflectionsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
26 parametersAbsolute structure parameter: 0.5 (4)
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Ca10000.0202 (6)
Ca2000.19941 (8)0.0160 (4)
Ca3000.40126 (5)0.0165 (5)
Si10.33330.66670.08767 (12)0.0210 (5)0.5
Si20.66670.33330.10556 (8)0.0120 (6)0.5
Si30.33330.66670.29191 (9)0.0122 (5)0.5
Si40.66670.33330.30909 (12)0.0241 (7)0.5
Si50.33330.66670.50.0136 (6)0.5
Si60.66670.33330.50.0472 (14)0.5
Al10.33330.66670.08767 (12)0.0210 (5)0.5
Al20.66670.33330.10556 (8)0.0120 (6)0.5
Al30.33330.66670.29191 (9)0.0122 (5)0.5
Al40.66670.33330.30909 (12)0.0241 (7)0.5
Al50.33330.66670.50.0136 (6)0.5
Al60.66670.33330.50.0472 (14)0.5
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ca10.0203 (10)0.0203 (10)0.0202 (10)0.0101 (5)00
Ca20.0155 (5)0.0155 (5)0.0169 (5)0.0078 (3)00
Ca30.0189 (7)0.0189 (7)0.0116 (6)0.0095 (3)00
Si10.0137 (8)0.0137 (8)0.0356 (9)0.0068 (4)00
Si20.0097 (8)0.0097 (8)0.0167 (7)0.0048 (4)00
Si30.0088 (7)0.0088 (7)0.0189 (7)0.0044 (3)00
Si40.0150 (10)0.0150 (10)0.0422 (10)0.0075 (5)00
Si50.0088 (9)0.0088 (9)0.0231 (12)0.0044 (4)00
Si60.0137 (14)0.0137 (14)0.114 (4)0.0068 (7)00
Al10.0137 (8)0.0137 (8)0.0356 (9)0.0068 (4)00
Al20.0097 (8)0.0097 (8)0.0167 (7)0.0048 (4)00
Al30.0088 (7)0.0088 (7)0.0189 (7)0.0044 (3)00
Al40.0150 (10)0.0150 (10)0.0422 (10)0.0075 (5)00
Al50.0088 (9)0.0088 (9)0.0231 (12)0.0044 (4)00
Al60.0137 (14)0.0137 (14)0.114 (4)0.0068 (7)00
Bond lengths (Å) top
Ca1—Si13.0846 (17)Ca3—Al5v3.2416 (8)
Ca1—Al1i3.0846 (17)Ca3—Si6v3.2416 (8)
Ca1—Si1i3.0846 (17)Ca3—Si5v3.2416 (8)
Ca1—Al1ii3.0846 (17)Ca3—Al3v3.4016 (15)
Ca1—Al1iii3.0846 (17)Ca3—Si3v3.4016 (15)
Ca1—Si1ii3.0846 (17)Ca3—Al3iii3.4016 (15)
Ca1—Si1iii3.0846 (17)Ca3—Si3iii3.4016 (15)
Ca1—Al1iv3.0846 (17)Ca3—Si33.4016 (15)
Ca1—Al1v3.0846 (17)Ca3—Ca3viii4.1772
Ca1—Si1iv3.0846 (17)Ca3—Ca3v4.1772
Ca1—Si1v3.0846 (17)Ca3—Ca3iii4.1772
Ca1—Si23.3435 (12)Ca3—Ca3ix4.1772
Ca1—Al2i3.3435 (12)Ca3—Ca3x4.1772
Ca1—Si2i3.3435 (12)Ca3—Ca3vii4.1772
Ca1—Al2vi3.3435 (12)Ca3—Ca3xi4.332 (2)
Ca1—Al2vii3.3435 (12)Si1—Al2x2.4434 (4)
Ca1—Si2vi3.3435 (12)Si1—Si2x2.4434 (4)
Ca1—Si2vii3.3435 (12)Si1—Al2vii2.4434 (4)
Ca1—Al2iv3.3435 (12)Si1—Si2vii2.4434 (4)
Ca1—Si2v3.3435 (12)Si1—Si22.4434 (4)
Ca1—Si2iv3.3435 (12)Si1—Ca1x3.0846 (17)
Ca1—Al2v3.3435 (12)Si1—Ca1viii3.0846 (17)
Ca1—Ca1viii4.1772Si1—Ca2viii3.439 (3)
Ca1—Ca1v4.1772Si1—Ca2x3.439 (3)
Ca1—Ca1iii4.1772Si2—Al1iii2.4434 (4)
Ca1—Ca1ix4.1772Si2—Si1iii2.4434 (4)
Ca1—Ca1vii4.1772Si2—Al1ix2.4434 (4)
Ca1—Ca1x4.1772Si2—Si1ix2.4434 (4)
Ca1—Ca2iv4.3746 (18)Si2—Ca2viii3.1710 (14)
Ca1—Ca24.3746 (18)Si2—Ca2ix3.1710 (14)
Ca2—Si33.1518 (15)Si2—Ca1ix3.3435 (12)
Ca2—Al3iii3.1518 (15)Si2—Ca1viii3.3435 (12)
Ca2—Si3iii3.1518 (15)Si3—Al4x2.4410 (3)
Ca2—Al3v3.1518 (15)Si3—Si4x2.4410 (3)
Ca2—Si3v3.1518 (15)Si3—Al4vii2.4410 (3)
Ca2—Al2v3.1710 (14)Si3—Si4vii2.4410 (3)
Ca2—Si2v3.1710 (14)Si3—Si42.4410 (3)
Ca2—Al2vii3.1710 (14)Si3—Ca2x3.1518 (15)
Ca2—Si2vii3.1710 (14)Si3—Ca2viii3.1518 (15)
Ca2—Si23.1710 (14)Si3—Ca3viii3.4016 (15)
Ca2—Si43.407 (2)Si3—Ca3x3.4016 (15)
Ca2—Al4vii3.407 (2)Si4—Al3iii2.4410 (3)
Ca2—Si4vii3.407 (2)Si4—Si3iii2.4410 (3)
Ca2—Al4v3.407 (2)Si4—Al3ix2.4410 (3)
Ca2—Si4v3.407 (2)Si4—Si3ix2.4410 (3)
Ca2—Si1v3.439 (3)Si4—Ca3viii3.1472 (18)
Ca2—Al1v3.439 (3)Si4—Ca3ix3.1472 (18)
Ca2—Al1iii3.439 (3)Si4—Ca2ix3.407 (2)
Ca2—Si1iii3.439 (3)Si4—Ca2viii3.407 (2)
Ca2—Si13.439 (3)Si5—Al6x2.4117
Ca2—Ca2v4.1772Si5—Al6vii2.4117
Ca2—Ca2viii4.1772Si5—Si6x2.4117
Ca2—Ca2x4.1772Si5—Si6vii2.4117
Ca2—Ca2vii4.1772Si5—Si62.4117
Ca2—Ca2iii4.1772Si5—Ca3xii3.2416 (8)
Ca2—Ca2ix4.1772Si5—Ca3xiii3.2416 (8)
Ca2—Ca34.4280 (18)Si5—Ca3x3.2416 (8)
Ca3—Al4v3.1472 (18)Si5—Ca3xi3.2416 (8)
Ca3—Si4v3.1472 (18)Si5—Ca3viii3.2416 (8)
Ca3—Al4vii3.1472 (18)Si6—Al5ix2.4117
Ca3—Si4vii3.1472 (18)Si6—Al5iii2.4117
Ca3—Si43.1472 (18)Si6—Si5ix2.4117
Ca3—Si63.2416 (8)Si6—Si5iii2.4117
Ca3—Si53.2416 (8)Si6—Ca3xii3.2416 (8)
Ca3—Al6vii3.2416 (8)Si6—Ca3xiv3.2416 (8)
Ca3—Al5iii3.2416 (8)Si6—Ca3ix3.2416 (8)
Ca3—Si6vii3.2416 (8)Si6—Ca3xi3.2416 (8)
Ca3—Si5iii3.2416 (8)Si6—Ca3viii3.2416 (8)
Ca3—Al6v3.2416 (8)
Symmetry codes: (i) x1, y1, z; (ii) x, y1, z; (iii) x, y1, z; (iv) x, y, z; (v) x1, y1, z; (vi) x1, y, z; (vii) x1, y, z; (viii) x+1, y+1, z; (ix) x+1, y, z; (x) x, y+1, z; (xi) x, y, z+1; (xii) x+1, y+1, z+1; (xiii) x, y+1, z+1; (xiv) x+1, y, z+1.

Experimental details

(6-fold_superstructure_298K)(5-fold_superstructure_298K)
Crystal data
Chemical formulaAlSiCaAlSiCa
Mr95.1595.15
Crystal system, space groupHexagonal, P6m2Hexagonal, P6m2
Temperature (K)298298
a, c (Å)4.17720 (4), 26.3246 (4)4.17720 (4), 21.9372 (3)
V3)397.80 (1)331.50 (1)
Z65
Radiation typeMo KαMo Kα
µ (mm1)2.762.76
Crystal size (mm)0.18 × 0.16 × 0.15 × 0 (radius)0.21 × 0.20 × 0.18 × 0 (radius)
Data collection
DiffractometerSTOE IPDS 2
diffractometer
STOE IPDS 2
diffractometer
Absorption correctionEmpirical (using intensity measurements)
X-SHAPE (Stoe & Cie, 1996)
Empirical (using intensity measurements)
X-SHAPE (Stoe & Cie, 1996)
Tmin, Tmax0.557, 0.6600.531, 0.607
No. of measured, independent and
observed [I > 2σ(I)] reflections
3136, 429, 233 4754, 422, 340
Rint0.0490.058
(sin θ/λ)max1)0.6410.686
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.03, 0.082, 1.96 0.035, 0.086, 1.99
No. of reflections429422
No. of parameters3126
Δρmax, Δρmin (e Å3)0.25, 0.290.46, 0.41
Absolute structureFlack H D (1983), Acta Cryst. A39, 876-881Flack H D (1983), Acta Cryst. A39, 876-881
Absolute structure parameter0.1 (3)0.5 (4)

Computer programs: X-AREA (Stoe, 2002), FullProf Suite (Rodriguez-Carvajal), X-RED (Stoe, 1996), SHELXL97 (Sheldrick, 1997), ATOMS Version 5.1, WinGX 1.64.05 (Farrugia, 1999).

 

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