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The crystal structure of synthetic K2Sc[Si2O6]F has been solved and refined as an incommensurately modulated structure in (3 + 2)-dimensional superspace. This paper describes the tetragonal structure in the superspace group P42/mnm(α,α,0)000s(−α,α,0)0000 [a = 8.9878 (1), c = 8.2694 (2) Å, V = 668.01 (2) Å3] with modulation wavevectors q1 = 0.2982 (4)(a* + b*) and q2 = 0.2982 (4)(−a* + b*). Structure refinement taking into account the modulation of positional and ADP parameters for all atoms from 3074 observed main hkl00 and satellite reflections hklmn of first order with single, m·n = 0, and mixed, m·n = ±1, indices converged to a final R value of 0.0514. The structure is a mixed octahedral–tetrahedral framework composed of [ScO4F2] octahedra, [Si4O12] rings and K in variable coordination. Due to the modulation the O atoms move into and out of the first coordination sphere of K leading to a minimum of five and a maximum of 10 interatomic K—O distances up to 3.1 Å. Although this feature is comparable to observations in modulated fresnoite and melilite group compounds, these structures differ from K2Sc[Si2O6]F with respect to their topology. On temperature increase the intensity of the satellite reflections decreases until they disappear just above 443 K. The high-temperature normal structure, in space group P42/mnm, is identical to the room-temperature average structure of K2Sc[Si2O6]F.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520615024865/dk5040sup1.cif
Contains datablocks global, I_rt, II_rt_incom, II_473K, II_rt, III_223K, III_173K

txt

Text file https://doi.org/10.1107/S2052520615024865/dk5040sup2.txt
CIF file of crystal I average structure room Temperature

txt

Text file https://doi.org/10.1107/S2052520615024865/dk5040sup3.txt
CIF file of crystal II high temperature normal structure

txt

Text file https://doi.org/10.1107/S2052520615024865/dk5040sup4.txt
CIF file of crystal II average room temperature structure

txt

Text file https://doi.org/10.1107/S2052520615024865/dk5040sup5.txt
CIF file crystal III modulated structure -50°

txt

Text file https://doi.org/10.1107/S2052520615024865/dk5040sup6.txt
CIF file crystal III modulated structure -100°

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520615024865/dk5040sup7.pdf
Supporting tables and figures

B-IncStrDB reference: 11562ExhL04

CCDC references: 1453444; 1453445; 1453446; 1453447; 1453448; 1453449

Computing details top

Data collection: CrysAlis PRO, Agilent Technologies, Version 1.171.35.19 (release 27-10-2011 CrysAlis171 .NET) (compiled Oct 27 2011,15:02:11) for I_rt; CrysAlis PRO, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) for II_rt_incom, III_223K, III_173K. Cell refinement: CrysAlis PRO, Agilent Technologies, Version 1.171.35.19 (release 27-10-2011 CrysAlis171 .NET) (compiled Oct 27 2011,15:02:11) for I_rt; CrysAlis PRO, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) for II_rt_incom, III_223K, III_173K. Data reduction: CrysAlis PRO, Agilent Technologies, Version 1.171.35.19 (release 27-10-2011 CrysAlis171 .NET) (compiled Oct 27 2011,15:02:11) for I_rt; CrysAlis PRO, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) for II_rt_incom, III_223K, III_173K.

(I_rt) top
Crystal data top
FK2O6ScSi2F(000) = 576
Mr = 294.3Dx = 2.935 Mg m3
Tetragonal, P42/m21/n2/mMo Kα radiation, λ = 0.7107 Å
Hall symbol: -P 4n;-2nCell parameters from 3764 reflections
a = 8.9780 (2) Åθ = 3.2–28.3°
c = 8.2608 (3) ŵ = 2.72 mm1
V = 665.86 (3) Å3T = 293 K
Z = 4
Data collection top
Xcalibur, Ruby, Gemini ultra
diffractometer
473 independent reflections
Radiation source: Enhance (Mo) X-ray Source457 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.024
Detector resolution: 10.3575 pixels mm-1θmax = 28.4°, θmin = 3.2°
ω scansh = 1111
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.19 (release 27-10-2011 CrysAlis171 .NET) (compiled Oct 27 2011,15:02:11) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 912
Tmin = 0.655, Tmax = 1l = 1110
4745 measured reflections
Refinement top
Refinement on F0 restraints
R[F2 > 2σ(F2)] = 0.0350 constraints
wR(F2) = 0.047Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 3.77(Δ/σ)max = 0.009
473 reflectionsΔρmax = 0.46 e Å3
38 parametersΔρmin = 1.56 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sc0.500.250.0037 (2)
K10.79325 (8)0.20675 (8)00.0201 (3)
K20.34266 (8)0.34266 (8)00.0314 (3)
Si0.12239 (6)0.12239 (6)0.19665 (9)0.0043 (2)
O1000.2594 (3)0.0184 (9)
O20.1163 (2)0.1163 (2)00.0200 (8)
F0.5000.0197 (9)
O30.0725 (2)0.28126 (17)0.2593 (2)0.0234 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sc0.0045 (3)0.0045 (3)0.0020 (5)000
K10.0250 (4)0.0250 (4)0.0101 (5)0.0144 (4)00
K20.0408 (5)0.0408 (5)0.0124 (6)0.0332 (6)00
Si0.0050 (3)0.0050 (3)0.0030 (5)0.0013 (3)0.00030 (18)0.00030 (18)
O10.0242 (14)0.0242 (14)0.0068 (16)0.0167 (13)00
O20.0276 (12)0.0276 (12)0.0048 (15)0.0142 (14)00
F0.0377 (18)0.0187 (15)0.0028 (14)0.0021 (10)00
O30.0380 (11)0.0083 (8)0.0240 (10)0.0094 (8)0.0065 (8)0.0056 (6)
Bond lengths (Å) top
Sc—F2.0652 (2)K1—O3viii2.8091 (19)
Sc—Fi2.0652 (2)K2—O1ix2.818 (2)
Sc—O3ii2.0704 (16)K2—O1x2.818 (2)
Sc—O3iii2.0704 (16)K2—O22.874 (2)
Sc—O3iv2.0704 (16)Si—O11.6381 (10)
Sc—O3v2.0704 (16)Si—O21.6264 (7)
K1—O3vi2.8091 (19)Si—O31.5820 (17)
K1—O3iii2.8091 (19)Si—O3v1.5820 (17)
K1—O3vii2.8091 (19)
Symmetry codes: (i) y+1/2, x1/2, z+1/2; (ii) x+1/2, y1/2, z+1/2; (iii) x+1/2, y+1/2, z+1/2; (iv) y+1, x, z; (v) y, x, z; (vi) y+1/2, x+1/2, z1/2; (vii) y+1/2, x+1/2, z+1/2; (viii) x+1/2, y+1/2, z1/2; (ix) y+1/2, x+1/2, z1/2; (x) x+1/2, y+1/2, z+1/2.
(II_rt_incom) top
Crystal data top
FK2O6ScSi2F(000) = 576
Mr = 294.3Dx = 2.926 Mg m3
Tetragonal, P42/m21/n2/mMo Kα radiation, λ = 0.71069 Å
q1 = 0.298200a* + 0.298200b*; q2 = -0.298200a* + 0.298200b*Cell parameters from 6650 reflections
a = 8.9878 (1) Åθ = 3–23.2°
c = 8.2694 (2) ŵ = 2.71 mm1
V = 668.01 (2) Å3T = 293 K
Z = 40.36 × 0.23 × 0.09 mm
† Symmetry operations: (1) x1, x2, x3, x4, x5; (2) −x1, −x2, x3, −x4, −x5; (3) −x2+1/2, x1+1/2, x3+1/2, −x5+1/2, x4+1/2; (4) x2+1/2, −x1+1/2, x3+1/2, x5+1/2, −x4+1/2; (5) −x1+1/2, x2+1/2, −x3+1/2, x5, x4; (6) x1+1/2, −x2+1/2, −x3+1/2, −x5, −x4; (7) x2, x1, −x3, x4+1/2, −x5+1/2; (8) −x2, −x1, −x3, −x4+1/2, x5+1/2; (9) −x1, −x2, −x3, −x4, −x5; (10) x1, x2, −x3, x4, x5; (11) x2+1/2, −x1+1/2, −x3+1/2, x5+1/2, −x4+1/2; (12) −x2+1/2, x1+1/2, −x3+1/2, −x5+1/2, x4+1/2; (13) x1+1/2, −x2+1/2, x3+1/2, −x5, −x4; (14) −x1+1/2, x2+1/2, x3+1/2, x5, x4; (15) −x2, −x1, x3, −x4+1/2, x5+1/2; (16) x2, x1, x3, x4+1/2, −x5+1/2.

Data collection top
Xcalibur, Ruby, Gemini ultra
diffractometer
3223 independent reflections
Radiation source: Enhance (Mo) X-ray Source3074 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.059
Detector resolution: 10.3575 pixels mm-1θmax = 26.7°, θmin = 1.4°
ω scansh = 1111
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1111
Tmin = 0.649, Tmax = 1l = 1010
43219 measured reflections
Refinement top
Refinement on F0 constraints
R[F2 > 2σ(F2)] = 0.052Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
wR(F2) = 0.064(Δ/σ)max = 0.140
S = 4.21Δρmax = 0.79 e Å3
3223 reflectionsΔρmin = 0.75 e Å3
268 parametersExtinction correction: B-C type 1 Gaussian isotropic (Becker & Coppens, 1974)
0 restraintsExtinction coefficient: 76000 (17000)
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sc0.500.250.00838 (13)
K10.79314 (4)0.20686 (4)00.02308 (13)
K20.34293 (4)0.34293 (4)00.03292 (14)
Si0.12224 (3)0.12224 (3)0.19667 (5)0.00955 (12)
O1000.25974 (18)0.0182 (3)
O20.11643 (12)0.11643 (12)00.0217 (3)
F0.5000.0235 (4)
O30.07264 (8)0.28094 (9)0.25906 (8)0.02148 (19)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sc0.0090 (2)0.0090 (2)0.0072 (3)000
K10.0263 (2)0.0263 (2)0.0167 (3)0.00903 (16)00
K20.0402 (2)0.0402 (2)0.0184 (3)0.0235 (2)00
Si0.01040 (19)0.01040 (19)0.0078 (2)0.00047 (11)0.00024 (7)0.00024 (7)
O10.0199 (5)0.0199 (5)0.0149 (8)0.0093 (4)00
O20.0281 (5)0.0281 (5)0.0089 (6)0.0091 (5)00
F0.0322 (7)0.0296 (8)0.0086 (7)0.0030 (5)00
O30.0266 (3)0.0132 (3)0.0247 (4)0.0046 (2)0.0014 (2)0.0033 (2)
Geometric parameters (Å, º) top
AverageMinimumMaximum
K2—O3i3.074 (2)2.897 (2)3.376 (2)
K2—O3ii3.084 (2)2.897 (2)3.376 (2)
K2—O3iii3.074 (2)2.897 (2)3.376 (2)
K2—O3iv3.084 (2)2.897 (2)3.376 (2)
O2v—K1—O2vi58.72 (9)57.83 (9)59.60 (9)
O3—K2—O3i105.76 (6)99.71 (6)111.89 (7)
O3—K2—O3ii90.52 (6)83.99 (6)96.27 (6)
O3—K2—O3vii99.92 (6)98.07 (6)101.87 (6)
O3—K2—O3viii81.50 (6)74.10 (6)88.81 (7)
O3—K2—O3iii55.02 (5)51.10 (5)58.83 (6)
O3—K2—O3iv148.76 (7)144.06 (7)154.44 (6)
O3—K2—O3ix47.38 (5)46.52 (5)48.24 (5)
O3i—K2—O3ii154.67 (7)153.64 (7)155.68 (8)
O3i—K2—O3vii90.68 (6)83.99 (6)96.27 (6)
O3i—K2—O3viii55.02 (6)51.10 (5)58.83 (6)
O3i—K2—O3iii80.67 (7)76.59 (6)83.47 (7)
O3i—K2—O3iv93.77 (6)92.50 (6)94.96 (5)
O3i—K2—O3ix148.94 (7)144.06 (7)154.44 (6)
O3ii—K2—O3vii105.60 (6)99.71 (6)111.89 (7)
O3ii—K2—O3viii148.76 (7)144.06 (7)154.44 (6)
O3ii—K2—O3iii93.77 (6)92.50 (6)94.96 (5)
O3ii—K2—O3iv80.73 (7)76.59 (6)83.47 (7)
O3ii—K2—O3ix54.84 (6)51.10 (5)58.83 (6)
O3vii—K2—O3viii47.38 (5)46.52 (5)48.24 (5)
O3vii—K2—O3iii148.94 (7)144.06 (7)154.44 (6)
O3vii—K2—O3iv54.84 (5)51.10 (5)58.83 (6)
O3vii—K2—O3ix81.41 (6)74.10 (6)88.81 (7)
O3viii—K2—O3iii105.76 (6)99.71 (6)111.89 (7)
O3viii—K2—O3iv90.52 (6)83.99 (6)96.27 (6)
O3viii—K2—O3ix99.92 (6)98.07 (6)101.87 (6)
O3iii—K2—O3iv154.67 (7)153.64 (7)155.68 (8)
O3iii—K2—O3ix90.68 (6)83.99 (6)96.27 (6)
O3iv—K2—O3ix105.60 (6)99.71 (6)111.89 (7)
K1x—O2—K1vi121.24 (11)117.84 (10)124.67 (11)
K1x—O2—O2xi60.53 (9)57.77 (9)63.97 (9)
K1vi—O2—O2xi60.72 (9)57.77 (9)63.97 (9)
Symmetry codes: (i) x2+1/2, x1+1/2, x31/2, x5+1/2, x4+1/2; (ii) x1+1/2, x2+1/2, x3+1/2, x5, x4; (iii) x2+1/2, x1+1/2, x3+1/2, x5+1/2, x4+1/2; (iv) x1+1/2, x2+1/2, x31/2, x5, x4; (v) x1+1, x2, x3, x4, x5; (vi) x1+1, x2, x3, x4, x5; (vii) x2, x1, x3, x4+1/2, x5+1/2; (viii) x1, x2, x3, x4, x5; (ix) x2, x1, x3, x4+1/2, x5+1/2; (x) x11, x2, x3, x4, x5; (xi) x1, x2, x3, x4, x5.
(II_473K) top
Crystal data top
FK2O6ScSi2Z = 4
Mr = 294.3F(000) = 576
Tetragonal, P42/m21/n2/mDx = 2.920 Mg m3
Hall symbol: -P 4n;-2nMo Kα radiation, λ = 0.71069 Å
a = 8.9939 (5) ŵ = 2.71 mm1
c = 8.2758 (7) ÅT = 293 K
V = 669.43 (8) Å3
Data collection top
IPDS Stoe
diffractometer
401 reflections with I > 3σ(I)
Radiation source: X-ray tubeRint = 0.053
Graphite monochromatorθmax = 26.7°, θmin = 3.2°
??integration method?? scansh = 1111
4724 measured reflectionsk = 1111
406 independent reflectionsl = 1010
Refinement top
Refinement on F0 restraints
R[F2 > 2σ(F2)] = 0.0260 constraints
wR(F2) = 0.038Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 3.59(Δ/σ)max = 0.018
406 reflectionsΔρmax = 0.40 e Å3
38 parametersΔρmin = 0.89 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sc10.500.250.0098 (2)
Si0.12240 (5)0.12240 (5)0.19636 (6)0.01029 (19)
K10.79357 (6)0.20643 (6)00.0300 (2)
K20.34265 (7)0.34265 (7)00.0415 (3)
O2bz0.1163 (2)0.1163 (2)00.0292 (6)
Obxx000.2592 (3)0.0241 (7)
F0.500.50.0281 (8)
Ot0.07257 (17)0.28140 (13)0.25854 (15)0.0255 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sc10.0112 (3)0.0112 (3)0.0070 (4)000
Si0.0113 (3)0.0113 (3)0.0083 (4)0.0002 (2)0.00030 (13)0.00030 (13)
K10.0344 (4)0.0344 (4)0.0211 (4)0.0133 (4)00
K20.0501 (5)0.0501 (5)0.0243 (5)0.0311 (5)00
O2bz0.0398 (10)0.0398 (10)0.0079 (11)0.0147 (12)00
Obxx0.0287 (11)0.0287 (11)0.0148 (13)0.0147 (10)00
F0.0341 (14)0.0424 (15)0.0079 (11)0.0047 (9)00
Ot0.0348 (7)0.0140 (6)0.0277 (8)0.0066 (5)0.0022 (6)0.0042 (4)
Geometric parameters (Å, º) top
Sc1—F2.0689 (3)Si—Otv1.5845 (13)
Sc1—Fi2.0689 (3)K1—Otvi2.8206 (15)
Sc1—Otii2.0728 (13)K1—Otiii2.8206 (15)
Sc1—Otiii2.0728 (13)K1—Otvii2.8206 (15)
Sc1—Otiv2.0728 (13)K1—Otviii2.8206 (15)
Sc1—Otv2.0728 (13)K2—O2bz2.8788 (19)
Si—O2bz1.6269 (6)K2—Obxxix2.8245 (17)
Si—Obxx1.6413 (8)K2—Obxxx2.8245 (17)
Si—Ot1.5845 (13)
F—Sc1—Fi180.0 (5)O2bz—Si—Obxx105.74 (10)
F—Sc1—Otii91.95 (3)O2bz—Si—Ot110.20 (8)
F—Sc1—Otiii91.95 (3)O2bz—Si—Otv110.20 (8)
F—Sc1—Otiv88.05 (3)Obxx—Si—Ot108.23 (7)
F—Sc1—Otv88.05 (3)Obxx—Si—Otv108.23 (7)
Fi—Sc1—Otii88.05 (3)Ot—Si—Otv113.89 (8)
Fi—Sc1—Otiii88.05 (3)Otvi—K1—Otiii116.57 (4)
Fi—Sc1—Otiv91.95 (3)Otvi—K1—Otvii90.22 (4)
Fi—Sc1—Otv91.95 (3)Otvi—K1—Otviii56.18 (4)
Otii—Sc1—Otiii176.09 (5)Otiii—K1—Otvii56.18 (4)
Otii—Sc1—Otiv90.07 (6)Otiii—K1—Otviii90.22 (4)
Otii—Sc1—Otv90.07 (6)Otvii—K1—Otviii116.57 (4)
Otiii—Sc1—Otiv90.07 (6)O2bz—K2—Obxxix135.12 (3)
Otiii—Sc1—Otv90.07 (6)O2bz—K2—Obxxx135.12 (3)
Otiv—Sc1—Otv176.09 (5)Obxxix—K2—Obxxx89.76 (5)
Symmetry codes: (i) y+1/2, x1/2, z1/2; (ii) x+1/2, y1/2, z+1/2; (iii) x+1/2, y+1/2, z+1/2; (iv) y+1, x, z; (v) y, x, z; (vi) y+1/2, x+1/2, z1/2; (vii) y+1/2, x+1/2, z+1/2; (viii) x+1/2, y+1/2, z1/2; (ix) y+1/2, x+1/2, z1/2; (x) x+1/2, y+1/2, z+1/2.
(II_rt) top
Crystal data top
FK2O6ScSi2Z = 4
Mr = 294.3F(000) = 576
Tetragonal, P42/m21/n2/mDx = 2.926 Mg m3
Hall symbol: -P 4n;-2nMo Kα radiation, λ = 0.71069 Å
a = 8.9878 (1) ŵ = 2.71 mm1
c = 8.2694 (2) ÅT = 293 K
V = 668.01 (2) Å3
Data collection top
Radiation source: X-ray tubeθmax = 26.6°, θmin = 3.2°
3100 measured reflectionsh = 1111
264 independent reflectionsk = 1111
264 reflections with I > 3σ(I)l = 1010
Rint = 0.053
Refinement top
Refinement on F0 constraints
R[F2 > 2σ(F2)] = 0.029Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
wR(F2) = 0.053(Δ/σ)max = 0.027
S = 3.95Δρmax = 0.19 e Å3
264 reflectionsΔρmin = 0.24 e Å3
40 parametersExtinction correction: B-C type 1 Gaussian isotropic (Becker & Coppens, 1974)
0 restraintsExtinction coefficient: 100000 (30000)
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sc0.500.250.0087 (3)
K10.79325 (5)0.20675 (5)00.0256 (4)
K20.34263 (6)0.34263 (6)00.0365 (4)
Si0.12233 (4)0.12233 (4)0.19652 (6)0.0093 (3)
O1000.2604 (3)0.0237 (8)
O20.11596 (17)0.11596 (17)00.0239 (6)
F0.5000.0249 (9)
O30.07211 (18)0.28113 (15)0.25936 (14)0.0281 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sc0.0106 (6)0.0106 (6)0.0050 (7)000
K10.0313 (6)0.0313 (6)0.0142 (7)0.0137 (3)00
K20.0467 (6)0.0467 (6)0.0159 (7)0.0328 (4)00
Si0.0109 (6)0.0109 (6)0.0062 (6)0.00103 (16)0.00025 (10)0.00025 (10)
O10.0286 (13)0.0286 (13)0.0140 (16)0.0173 (9)00
O20.0343 (10)0.0343 (10)0.0031 (10)0.0152 (11)00
F0.0402 (17)0.0261 (14)0.0084 (17)0.0008 (8)00
O30.0420 (9)0.0159 (8)0.0265 (9)0.0083 (5)0.0053 (6)0.0061 (4)
Bond lengths (Å) top
Sc—F2.0674 (1)K1—O3viii2.8146 (14)
Sc—Fi2.0674 (1)K2—O1ix2.8156 (19)
Sc—O3ii2.0726 (14)K2—O1x2.8156 (19)
Sc—O3iii2.0726 (14)K2—O22.8811 (16)
Sc—O3iv2.0726 (14)Si—O11.6421 (9)
Sc—O3v2.0726 (14)Si—O21.6271 (5)
K1—O3vi2.8146 (14)Si—O31.5846 (14)
K1—O3iii2.8146 (14)Si—O3v1.5846 (14)
K1—O3vii2.8146 (14)
Symmetry codes: (i) y+1/2, x1/2, z+1/2; (ii) x+1/2, y1/2, z+1/2; (iii) x+1/2, y+1/2, z+1/2; (iv) y+1, x, z; (v) y, x, z; (vi) y+1/2, x+1/2, z1/2; (vii) y+1/2, x+1/2, z+1/2; (viii) x+1/2, y+1/2, z1/2; (ix) y+1/2, x+1/2, z1/2; (x) x+1/2, y+1/2, z+1/2.
(III_223K) top
Crystal data top
FK2O6ScSi2F(000) = 576
Mr = 294.3Dx = 2.940 Mg m3
Tetragonal, P42/m21/n2/mMo Kα radiation, λ = 0.7107 Å
q1 = 0.298600a* + 0.298600b*; q2 = -0.298600a* + 0.298600b*Cell parameters from 4774 reflections
a = 8.9705 (4) Åθ = 3.0–29.3°
c = 8.2615 (4) ŵ = 2.73 mm1
V = 664.80 (5) Å3T = 293 K
Z = 40.46 × 0.41 × 0.31 mm
† Symmetry operations: (1) x1, x2, x3, x4, x5; (2) −x1, −x2, x3, −x4, −x5; (3) −x2+1/2, x1+1/2, x3+1/2, −x5+1/2, x4+1/2; (4) x2+1/2, −x1+1/2, x3+1/2, x5+1/2, −x4+1/2; (5) −x1+1/2, x2+1/2, −x3+1/2, x5, x4; (6) x1+1/2, −x2+1/2, −x3+1/2, −x5, −x4; (7) x2, x1, −x3, x4+1/2, −x5+1/2; (8) −x2, −x1, −x3, −x4+1/2, x5+1/2; (9) −x1, −x2, −x3, −x4, −x5; (10) x1, x2, −x3, x4, x5; (11) x2+1/2, −x1+1/2, −x3+1/2, x5+1/2, −x4+1/2; (12) −x2+1/2, x1+1/2, −x3+1/2, −x5+1/2, x4+1/2; (13) x1+1/2, −x2+1/2, x3+1/2, −x5, −x4; (14) −x1+1/2, x2+1/2, x3+1/2, x5, x4; (15) −x2, −x1, x3, −x4+1/2, x5+1/2; (16) x2, x1, x3, x4+1/2, −x5+1/2.

Data collection top
Xcalibur, Ruby, Gemini ultra
diffractometer
4131 independent reflections
Radiation source: Enhance (Mo) X-ray Source1684 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.054
Detector resolution: 10.3575 pixels mm-1θmax = 29.4°, θmin = 3.0°
ω scansh = 1211
Absorption correction: analytical
CrysAlisPro, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. (Clark, R. C. & Reid, J. S. (1995). Acta Cryst. A51, 887-897)
k = 1012
Tmin = 0.406, Tmax = 0.552l = 1010
36339 measured reflections
Refinement top
Refinement on F0 constraints
R[F2 > 2σ(F2)] = 0.040Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
wR(F2) = 0.063(Δ/σ)max = 0.037
S = 1.32Δρmax = 1.69 e Å3
4131 reflectionsΔρmin = 1.73 e Å3
187 parametersExtinction correction: B-C type 1 Gaussian isotropic (Becker & Coppens, 1974)
0 restraintsExtinction coefficient: 8000 (200)
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sc0.500.250.00436 (14)
K10.79288 (5)0.20712 (5)00.01446 (17)
K20.34291 (5)0.34291 (5)00.0234 (2)
Si0.12243 (4)0.12243 (4)0.19662 (7)0.00510 (15)
O1000.2591 (3)0.0103 (5)
O20.11661 (15)0.11661 (15)00.0127 (5)
F0.5000.0134 (5)
O30.07265 (12)0.28124 (11)0.25894 (14)0.0121 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sc0.00438 (19)0.00438 (19)0.0043 (3)000
K10.0162 (2)0.0162 (2)0.0109 (4)0.0061 (3)00
K20.0288 (3)0.0288 (3)0.0125 (4)0.0191 (3)00
Si0.0052 (2)0.0052 (2)0.0049 (3)0.00006 (19)0.00002 (15)0.00002 (15)
O10.0110 (7)0.0110 (7)0.0087 (12)0.0048 (8)00
O20.0170 (7)0.0170 (7)0.0039 (12)0.0055 (8)00
F0.0199 (9)0.0154 (9)0.0048 (10)0.0019 (7)00
O30.0144 (6)0.0070 (5)0.0148 (7)0.0026 (4)0.0008 (5)0.0022 (4)
Bond lengths (Å) top
AverageMinimumMaximum
Sc—F2.0700 (14)2.060 (3)2.0820 (17)
Sc—Fi2.0702 (14)2.060 (3)2.0820 (17)
Sc—O3ii2.078 (5)2.054 (5)2.100 (6)
Sc—O3iii2.078 (5)2.054 (5)2.100 (6)
Sc—O3iv2.078 (5)2.054 (5)2.100 (6)
Sc—O3v2.078 (5)2.054 (5)2.100 (6)
K1—O2vi3.026 (9)2.879 (9)3.218 (9)
K1—O2vii3.022 (9)2.879 (9)3.218 (9)
K1—O3viii2.808 (7)2.708 (7)2.941 (7)
K1—O3iii2.815 (7)2.708 (7)2.940 (7)
K1—O3ix2.808 (7)2.708 (7)2.941 (7)
K1—O3x2.815 (7)2.708 (7)2.940 (7)
K2—O1xi2.825 (5)2.650 (6)2.996 (5)
K2—O1xii2.825 (5)2.650 (6)2.996 (5)
K2—O22.888 (9)2.802 (9)2.952 (9)
K2—O33.280 (7)2.832 (7)3.716 (7)
K2—O3xi3.068 (7)2.812 (7)3.569 (7)
K2—O3iii3.087 (7)2.812 (7)3.569 (7)
K2—O3xiii3.295 (7)2.832 (7)3.716 (7)
K2—O3xiv3.280 (7)2.832 (7)3.716 (7)
K2—O3xv3.068 (7)2.812 (7)3.569 (7)
K2—O3x3.087 (7)2.812 (7)3.569 (7)
K2—O3v3.295 (7)2.832 (7)3.716 (7)
Si—O11.647 (4)1.630 (4)1.664 (4)
Si—O21.632 (2)1.622 (3)1.641 (2)
Si—O31.590 (6)1.572 (6)1.608 (6)
Si—O3v1.590 (6)1.572 (6)1.608 (6)
Symmetry codes: (i) x2+1/2, x11/2, x3+1/2, x5+1/2, x4+1/2; (ii) x1+1/2, x21/2, x3+1/2, x5, x4; (iii) x1+1/2, x2+1/2, x3+1/2, x5, x4; (iv) x2+1, x1, x3, x4+1/2, x5+1/2; (v) x2, x1, x3, x4+1/2, x5+1/2; (vi) x1+1, x2, x3, x4, x5; (vii) x1+1, x2, x3, x4, x5; (viii) x2+1/2, x1+1/2, x31/2, x5+1/2, x4+1/2; (ix) x2+1/2, x1+1/2, x3+1/2, x5+1/2, x4+1/2; (x) x1+1/2, x2+1/2, x31/2, x5, x4; (xi) x2+1/2, x1+1/2, x31/2, x5+1/2, x4+1/2; (xii) x1+1/2, x2+1/2, x3+1/2, x5, x4; (xiii) x2, x1, x3, x4+1/2, x5+1/2; (xiv) x1, x2, x3, x4, x5; (xv) x2+1/2, x1+1/2, x3+1/2, x5+1/2, x4+1/2.
(III_173K) top
Crystal data top
FK2O6ScSi2F(000) = 576
Mr = 294.3Dx = 2.942 Mg m3
Tetragonal, P42/m21/n2/mMo Kα radiation, λ = 0.71073 Å
q1 = 0.298700a* + 0.298700b*; q2 = -0.298700a* + 0.298700b*Cell parameters from 5195 reflections
a = 8.9622 (4) Åθ = 3–29.3°
c = 8.2705 (4) ŵ = 2.72 mm1
V = 664.30 (5) Å3T = 293 K
Z = 40.45 × 0.37 × 0.21 mm
† Symmetry operations: (1) x1, x2, x3, x4, x5; (2) −x1, −x2, x3, −x4, −x5; (3) −x2+1/2, x1+1/2, x3+1/2, −x5+1/2, x4+1/2; (4) x2+1/2, −x1+1/2, x3+1/2, x5+1/2, −x4+1/2; (5) −x1+1/2, x2+1/2, −x3+1/2, x5, x4; (6) x1+1/2, −x2+1/2, −x3+1/2, −x5, −x4; (7) x2, x1, −x3, x4+1/2, −x5+1/2; (8) −x2, −x1, −x3, −x4+1/2, x5+1/2; (9) −x1, −x2, −x3, −x4, −x5; (10) x1, x2, −x3, x4, x5; (11) x2+1/2, −x1+1/2, −x3+1/2, x5+1/2, −x4+1/2; (12) −x2+1/2, x1+1/2, −x3+1/2, −x5+1/2, x4+1/2; (13) x1+1/2, −x2+1/2, x3+1/2, −x5, −x4; (14) −x1+1/2, x2+1/2, x3+1/2, x5, x4; (15) −x2, −x1, x3, −x4+1/2, x5+1/2; (16) x2, x1, x3, x4+1/2, −x5+1/2.

Data collection top
Xcalibur, Ruby, Gemini ultra
diffractometer
3986 independent reflections
Radiation source: Enhance (Mo) X-ray Source2178 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.056
Detector resolution: 10.3575 pixels mm-1θmax = 29.4°, θmin = 3.0°
ω scansh = 1112
Absorption correction: analytical
CrysAlisPro, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. (Clark, R. C. & Reid, J. S. (1995). Acta Cryst. A51, 887-897)
k = 1212
Tmin = 0.443, Tmax = 0.676l = 119
38281 measured reflections
Refinement top
Refinement on F0 constraints
R[F2 > 2σ(F2)] = 0.050Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
wR(F2) = 0.067(Δ/σ)max = 0.034
S = 1.82Δρmax = 2.77 e Å3
3986 reflectionsΔρmin = 3.32 e Å3
187 parametersExtinction correction: B-C type 1 Gaussian isotropic (Becker & Coppens, 1974)
0 restraintsExtinction coefficient: 9100 (400)
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sc0.500.250.00357 (15)
K10.79283 (5)0.20717 (5)00.01151 (17)
K20.34303 (5)0.34303 (5)00.0179 (2)
Si0.12251 (4)0.12251 (4)0.19664 (7)0.00440 (15)
O1000.2586 (3)0.0082 (5)
O20.11637 (16)0.11637 (16)00.0111 (5)
F0.5000.0107 (5)
O30.07260 (12)0.28133 (11)0.25896 (14)0.0099 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sc0.0030 (2)0.0030 (2)0.0047 (3)000
K10.0123 (3)0.0123 (3)0.0100 (4)0.0045 (3)00
K20.0214 (3)0.0214 (3)0.0110 (4)0.0137 (3)00
Si0.0040 (2)0.0040 (2)0.0051 (3)0.0001 (2)0.00002 (15)0.00002 (15)
O10.0081 (7)0.0081 (7)0.0085 (12)0.0034 (8)00
O20.0140 (7)0.0140 (7)0.0052 (12)0.0033 (9)00
F0.0143 (9)0.0114 (9)0.0063 (10)0.0021 (7)00
O30.0103 (5)0.0054 (5)0.0139 (7)0.0018 (4)0.0006 (5)0.0017 (4)
Bond lengths (Å) top
AverageMinimumMaximum
Sc—F2.0737 (13)2.062 (2)2.0868 (15)
Sc—Fi2.0739 (13)2.062 (2)2.0868 (15)
Sc—O3ii2.078 (5)2.051 (5)2.104 (5)
Sc—O3iii2.077 (5)2.051 (5)2.104 (5)
Sc—O3iv2.078 (5)2.051 (5)2.104 (5)
Sc—O3v2.077 (5)2.051 (5)2.104 (5)
K1—O2vi3.025 (8)2.863 (8)3.250 (8)
K1—O2vii3.021 (8)2.863 (8)3.250 (8)
K1—O3viii2.809 (7)2.701 (7)2.951 (7)
K1—O3iii2.817 (7)2.701 (7)2.951 (7)
K1—O3ix2.809 (7)2.701 (7)2.951 (7)
K1—O3x2.817 (7)2.701 (7)2.951 (7)
K2—O1xi2.830 (4)2.641 (5)3.011 (5)
K2—O1xii2.830 (4)2.641 (5)3.011 (5)
K2—O22.897 (9)2.800 (9)2.958 (9)
K2—O33.282 (7)2.772 (7)3.766 (7)
K2—O3xi3.067 (7)2.787 (7)3.676 (6)
K2—O3iii3.090 (7)2.787 (7)3.676 (6)
K2—O3xiii3.299 (7)2.772 (7)3.766 (7)
K2—O3xiv3.282 (7)2.772 (7)3.766 (7)
K2—O3xv3.067 (7)2.787 (7)3.676 (6)
K2—O3x3.090 (7)2.787 (7)3.676 (6)
K2—O3v3.299 (7)2.772 (7)3.766 (7)
Si—O11.648 (4)1.630 (6)1.668 (5)
Si—O21.636 (2)1.624 (2)1.648 (2)
Si—O31.591 (6)1.574 (6)1.610 (6)
Si—O3v1.592 (6)1.574 (6)1.610 (6)
Symmetry codes: (i) x2+1/2, x11/2, x3+1/2, x5+1/2, x4+1/2; (ii) x1+1/2, x21/2, x3+1/2, x5, x4; (iii) x1+1/2, x2+1/2, x3+1/2, x5, x4; (iv) x2+1, x1, x3, x4+1/2, x5+1/2; (v) x2, x1, x3, x4+1/2, x5+1/2; (vi) x1+1, x2, x3, x4, x5; (vii) x1+1, x2, x3, x4, x5; (viii) x2+1/2, x1+1/2, x31/2, x5+1/2, x4+1/2; (ix) x2+1/2, x1+1/2, x3+1/2, x5+1/2, x4+1/2; (x) x1+1/2, x2+1/2, x31/2, x5, x4; (xi) x2+1/2, x1+1/2, x31/2, x5+1/2, x4+1/2; (xii) x1+1/2, x2+1/2, x3+1/2, x5, x4; (xiii) x2, x1, x3, x4+1/2, x5+1/2; (xiv) x1, x2, x3, x4, x5; (xv) x2+1/2, x1+1/2, x3+1/2, x5+1/2, x4+1/2.
 

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