Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
Kermesite, Sb2S2O, is a desymmetrized order–disorder (OD) structure of layers. Two data sets were recorded using twinned crystals from Pezinok, Slovakia (named as Pz21, Pz24). The primitive unit cell is triclinic, P\bar 1, Z = 4, cell parameters are a = 8.1416 (3), b = 10.6968 (3), c = 5.7835 (2) Å, α = 102.758 (3), β = 110.657 (3), γ = 101.020 (3)°, Robs = 0.0243 (Pz21), and a = 8.1372 (2), b = 10.6969 (2), c = 5.7840 (1) Å, α = 102.787 (2), β = 110.606 (2), γ = 100.983 (2)°, Robs = 0.0321 (Pz24). The structure can also be described in the non-standard pseudo-monoclinic octuple (Z = 32), F-centered (Kupčík) cell with extra points in {1\over 4},{1\over 4},0; {1\over 4},{3\over 4},{1\over 2}; {3\over 4},{1\over 4},{1\over 2}; {3\over 4},{3\over 4},0, with parameters a = 21.6466 (9), b = 8.1416 (3), c = 20.3824 (9) Å, α = 90.079 (4), β = 101.985 (5), γ = 89.948 (4)° (Pz21), and a = 21.6558 (5), b = 8.1372 (2), c = 20.3859 (8) Å, α = 90.028 (3), β = 101.994 (3), γ = 89.986 (2)° (Pz24). The structure is built of layers parallel to the bc plane, stacked along the a vector of the octuple cell, composed of ribbons parallel to the b vector: (i) ribbon of two strips of SbO5 flattened quadrangular pyramids, sharing apical edges; (ii) ribbon of edge-sharing corrugated lozenges SbO3S. Basal S atoms of pyramids share corners of lozenges. Sb atoms are displaced out of coordination polyhedra into the inter-layer space. The OD layer comprises adjacent halves of the structure building layers. The layer group is A(1)2/m1, the protocell is defined by b, c, (a/4)sin β. The MDO1 (4A) polytype is generated by repetition of the {\bf t}_{(1,\, {1\over 4},\,0)} [or alternatively {\bf t}_{(1,\,-{1\over 4}, \, 0)}] translation. The co-existence of two kinds of domains give rise to the twinning. The twin operation is 2[010], twin index 2. The total continuation of [. a2 .] generates the MDO2 (2M) polytype, space group A12/a1. Simulated and real diffraction patterns are presented. The important values (edges, angles) and displacements of atoms due to the desymmetrization were evaluated. The comparison with structures of stibnite, bismuthinite and aikinite is added.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052519213024238/wf5108sup1.cif
Contains datablocks global, I, II, III, IV

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052519213024238/wf5108Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052519213024238/wf5108IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052519213024238/wf5108IIIsup4.hkl
Contains datablock III

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052519213024238/wf5108IVsup5.hkl
Contains datablock IV

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052519213024238/wf5108sup6.pdf
Commented responses of the CheckCIF/PLATON report of CIFs corresponding to the data sets of two twinned crystals with various ratio of domains refined in two axial settings

Experimental top

Refinement top

Crystal data, data collection and structure refinement details are summarized in Table 1.

Results and discussion top

Computing details top

Data collection: CrysAlis CCD, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46) for (I). Cell refinement: CrysAlis RED, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46) for (I). Data reduction: CrysAlis RED, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46) for (I).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
[Figure 8]
[Figure 9]
[Figure 10]
[Figure 11]
[Figure 12]
[Figure 13]
[Figure 14]
[Figure 15]
[Figure 16]
(I) top
Crystal data top
OS2Sb2Z = 4
Mr = 323.6F(000) = 568
Triclinic, P1Dx = 4.892 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.7107 Å
a = 8.1416 (3) ÅCell parameters from 6328 reflections
b = 10.6968 (3) Åθ = 2.9–32.6°
c = 5.7835 (2) ŵ = 13.06 mm1
α = 102.758 (3)°T = 293 K
β = 110.657 (3)°Acicular, red
γ = 101.020 (3)°0.65 × 0.05 × 0.03 mm
V = 439.23 (3) Å3
Data collection top
Xcalibur, Atlas, Gemini ultra
diffractometer
4465 independent reflections
Radiation source: Enhance (Mo) X-ray Source2604 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.050
Detector resolution: 10.3784 pixels mm-1θmax = 32.7°, θmin = 2.9°
ω scansh = 1112
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
k = 1616
Tmin = 0.109, Tmax = 0.667l = 88
12651 measured reflections
Refinement top
Refinement on F0 restraints
R[F2 > 2σ(F2)] = 0.0240 constraints
wR(F2) = 0.027Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 1.12(Δ/σ)max = 0.020
4465 reflectionsΔρmax = 1.15 e Å3
92 parametersΔρmin = 1.34 e Å3
Crystal data top
OS2Sb2γ = 101.020 (3)°
Mr = 323.6V = 439.23 (3) Å3
Triclinic, P1Z = 4
a = 8.1416 (3) ÅMo Kα radiation
b = 10.6968 (3) ŵ = 13.06 mm1
c = 5.7835 (2) ÅT = 293 K
α = 102.758 (3)°0.65 × 0.05 × 0.03 mm
β = 110.657 (3)°
Data collection top
Xcalibur, Atlas, Gemini ultra
diffractometer
4465 independent reflections
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
2604 reflections with I > 3σ(I)
Tmin = 0.109, Tmax = 0.667Rint = 0.050
12651 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.02492 parameters
wR(F2) = 0.0270 restraints
S = 1.12Δρmax = 1.15 e Å3
4465 reflectionsΔρmin = 1.34 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sb10.16840 (3)0.63146 (2)0.03891 (5)0.01099 (8)
Sb20.66034 (3)0.62984 (2)0.01365 (5)0.01159 (9)
Sb30.12564 (4)0.85374 (3)0.63183 (5)0.01335 (9)
Sb40.65245 (4)0.91530 (3)0.67939 (5)0.01500 (9)
S10.81008 (13)0.70292 (9)0.49744 (18)0.0144 (3)
S20.28992 (13)0.69210 (9)0.51780 (18)0.0144 (3)
S30.04760 (13)0.90934 (9)0.22597 (18)0.0131 (3)
S40.51998 (13)0.91063 (9)0.22786 (18)0.0134 (3)
O10.8979 (4)0.5681 (2)0.0301 (5)0.0133 (10)
O20.4149 (3)0.5711 (2)0.0761 (5)0.0139 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sb10.01034 (11)0.00907 (10)0.01308 (11)0.00190 (9)0.00565 (9)0.00207 (8)
Sb20.00983 (11)0.00940 (11)0.01518 (12)0.00219 (9)0.00562 (9)0.00297 (8)
Sb30.01271 (12)0.01414 (12)0.01179 (11)0.00299 (9)0.00518 (9)0.00210 (8)
Sb40.01470 (12)0.01523 (12)0.01497 (12)0.00354 (10)0.00588 (10)0.00568 (9)
S10.0125 (4)0.0144 (4)0.0147 (4)0.0010 (3)0.0068 (4)0.0019 (3)
S20.0149 (4)0.0153 (4)0.0128 (4)0.0063 (4)0.0051 (4)0.0031 (3)
S30.0115 (4)0.0122 (4)0.0137 (4)0.0018 (3)0.0044 (3)0.0034 (3)
S40.0135 (4)0.0131 (4)0.0124 (4)0.0033 (3)0.0053 (3)0.0021 (3)
O10.0116 (12)0.0058 (11)0.0226 (14)0.0032 (9)0.0088 (11)0.0010 (9)
O20.0092 (12)0.0064 (11)0.0259 (15)0.0018 (9)0.0093 (11)0.0015 (10)
Geometric parameters (Å, º) top
Sb1—S22.4695 (10)Sb3—S22.4932 (12)
Sb1—O1i2.155 (3)Sb3—S32.4446 (11)
Sb1—O1ii2.010 (3)Sb3—S3iii3.2176 (11)
Sb1—O22.178 (3)Sb3—S4iv3.1624 (10)
Sb2—S12.4878 (10)Sb4—S12.9878 (12)
Sb2—O12.138 (3)Sb4—S23.1080 (10)
Sb2—O22.156 (3)Sb4—S3iv2.5757 (10)
Sb2—O2ii2.011 (2)Sb4—S42.4330 (10)
Sb3—S1i2.5021 (10)Sb4—S4iv2.6106 (12)
S2—Sb1—O1i87.49 (8)S2—Sb3—S395.10 (4)
S2—Sb1—O1ii96.06 (9)S2—Sb3—S3iii172.74 (3)
S2—Sb1—O286.12 (8)S2—Sb3—S4iv88.26 (3)
O1i—Sb1—O1ii72.76 (11)S3—Sb3—S3iii81.50 (3)
O1i—Sb1—O2143.57 (11)S3—Sb3—S4iv78.73 (3)
O1ii—Sb1—O272.33 (11)S3iii—Sb3—S4iv84.80 (3)
S1—Sb2—O185.53 (8)S1—Sb4—S288.60 (3)
S1—Sb2—O282.81 (7)S1—Sb4—S3iv88.02 (3)
S1—Sb2—O2ii102.01 (9)S1—Sb4—S486.20 (3)
O1—Sb2—O2140.35 (11)S1—Sb4—S4iv172.04 (3)
O1—Sb2—O2ii73.16 (11)S2—Sb4—S3iv174.97 (3)
O2—Sb2—O2ii72.49 (12)S2—Sb4—S484.22 (3)
S1i—Sb3—S2102.34 (3)S2—Sb4—S4iv87.39 (3)
S1i—Sb3—S394.15 (3)S3iv—Sb4—S491.84 (3)
S1i—Sb3—S3iii84.35 (3)S3iv—Sb4—S4iv95.51 (3)
S1i—Sb3—S4iv167.80 (3)S4—Sb4—S4iv86.56 (4)
Symmetry codes: (i) x1, y, z; (ii) x+1, y+1, z; (iii) x, y+2, z+1; (iv) x+1, y+2, z+1.
(II) top
Crystal data top
OS2Sb2Z = 32
Mr = 323.6F(000) = 568
Triclinic, X1Dx = 4.892 Mg m3
Hall symbol: -XMo Kα radiation, λ = 0.7107 Å
a = 21.6466 (9) ÅCell parameters from 6328 reflections
b = 8.1416 (3) Åθ = 2.9–32.6°
c = 20.3824 (9) ŵ = 13.06 mm1
α = 90.079 (4)°T = 293 K
β = 101.985 (5)°Acicular, red
γ = 89.948 (4)°0.65 × 0.05 × 0.03 mm
V = 3513.8 (3) Å3
Data collection top
Oxford Diffraction CCD
diffractometer
4465 independent reflections
Radiation source: X-ray tube2604 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.050
Detector resolution: 10.3784 pixels mm-1θmax = 32.7°, θmin = 2.9°
ω scansh = 3131
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
k = 1211
Tmin = 0.109, Tmax = 0.667l = 3030
12651 measured reflections
Refinement top
Refinement on F0 restraints
R[F2 > 2σ(F2)] = 0.0240 constraints
wR(F2) = 0.027Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 1.11(Δ/σ)max = 0.028
4465 reflectionsΔρmax = 1.14 e Å3
92 parametersΔρmin = 1.36 e Å3
Crystal data top
OS2Sb2γ = 89.948 (4)°
Mr = 323.6V = 3513.8 (3) Å3
Triclinic, X1Z = 32
a = 21.6466 (9) ÅMo Kα radiation
b = 8.1416 (3) ŵ = 13.06 mm1
c = 20.3824 (9) ÅT = 293 K
α = 90.079 (4)°0.65 × 0.05 × 0.03 mm
β = 101.985 (5)°
Data collection top
Oxford Diffraction CCD
diffractometer
4465 independent reflections
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
2604 reflections with I > 3σ(I)
Tmin = 0.109, Tmax = 0.667Rint = 0.050
12651 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.02492 parameters
wR(F2) = 0.0270 restraints
S = 1.11Δρmax = 1.14 e Å3
4465 reflectionsΔρmin = 1.36 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sb10.101846 (13)0.74919 (3)0.184271 (11)0.01093 (7)
Sb20.095969 (13)0.25053 (3)0.185079 (12)0.01153 (7)
Sb30.194521 (13)0.00426 (3)0.073117 (13)0.01342 (7)
Sb40.191022 (13)0.49623 (3)0.042365 (13)0.01508 (8)
S10.19864 (5)0.24005 (12)0.14855 (5)0.0144 (3)
S20.20641 (5)0.76251 (12)0.15394 (5)0.0144 (3)
S30.07915 (5)0.01372 (12)0.04532 (5)0.0131 (3)
S40.07931 (5)0.51459 (12)0.04468 (5)0.0134 (3)
O10.11552 (13)0.0016 (3)0.21593 (12)0.0132 (8)
O20.12622 (14)0.4969 (3)0.21445 (12)0.0139 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sb10.01415 (12)0.00977 (11)0.00899 (11)0.00102 (9)0.00265 (8)0.00054 (8)
Sb20.01548 (13)0.00951 (11)0.00931 (11)0.00001 (10)0.00190 (8)0.00064 (8)
Sb30.01422 (12)0.01274 (12)0.01434 (13)0.00091 (10)0.00537 (9)0.00037 (9)
Sb40.01398 (13)0.01547 (13)0.01544 (13)0.00021 (10)0.00226 (9)0.00140 (9)
S10.0176 (5)0.0124 (4)0.0144 (4)0.0028 (4)0.0057 (3)0.0026 (3)
S20.0145 (5)0.0144 (4)0.0153 (4)0.0015 (4)0.0049 (3)0.0027 (3)
S30.0143 (4)0.0129 (4)0.0122 (4)0.0002 (4)0.0030 (3)0.0018 (3)
S40.0144 (4)0.0136 (4)0.0131 (4)0.0005 (4)0.0047 (3)0.0001 (3)
O10.0244 (15)0.0091 (12)0.0057 (11)0.0003 (11)0.0021 (10)0.0020 (9)
O20.0276 (16)0.0069 (11)0.0064 (11)0.0003 (12)0.0017 (10)0.0002 (9)
Geometric parameters (Å, º) top
Sb1—S22.4696 (11)Sb3—S2iii2.4935 (10)
Sb1—O1i2.155 (3)Sb3—S32.4446 (10)
Sb1—O1ii2.010 (2)Sb3—S3iv3.2171 (10)
Sb1—O22.178 (3)Sb3—S4iv3.1618 (10)
Sb2—S12.4876 (11)Sb4—S12.9874 (10)
Sb2—O12.139 (3)Sb4—S23.1073 (10)
Sb2—O22.156 (3)Sb4—S3iv2.5762 (10)
Sb2—O2ii2.011 (2)Sb4—S42.4330 (11)
Sb3—S12.5026 (10)Sb4—S4v2.6111 (10)
S2—Sb1—O1i87.48 (8)S2iii—Sb3—S395.10 (3)
S2—Sb1—O1ii96.07 (9)S2iii—Sb3—S3iv172.74 (3)
S2—Sb1—O286.12 (8)S2iii—Sb3—S4iv88.25 (3)
O1i—Sb1—O1ii72.75 (10)S3—Sb3—S3iv81.49 (3)
O1i—Sb1—O2143.56 (9)S3—Sb3—S4iv78.75 (3)
O1ii—Sb1—O272.33 (10)S3iv—Sb3—S4iv84.80 (2)
S1—Sb2—O185.53 (8)S1—Sb4—S288.60 (3)
S1—Sb2—O282.83 (8)S1—Sb4—S3iv88.02 (3)
S1—Sb2—O2ii102.00 (9)S1—Sb4—S486.20 (3)
O1—Sb2—O2140.36 (9)S1—Sb4—S4v172.05 (3)
O1—Sb2—O2ii73.16 (10)S2—Sb4—S3iv174.97 (3)
O2—Sb2—O2ii72.49 (10)S2—Sb4—S484.23 (3)
S1—Sb3—S2iii102.35 (3)S2—Sb4—S4v87.39 (3)
S1—Sb3—S394.14 (3)S3iv—Sb4—S491.83 (3)
S1—Sb3—S3iv84.35 (3)S3iv—Sb4—S4v95.52 (3)
S1—Sb3—S4iv167.81 (3)S4—Sb4—S4v86.57 (3)
Symmetry codes: (i) x, y+1, z; (ii) x+1/4, y+3/4, z+1/2; (iii) x, y1, z; (iv) x+1/4, y+1/4, z; (v) x+1/4, y+5/4, z.
(III) top
Crystal data top
OS2Sb2Z = 4
Mr = 323.6F(000) = 568
Triclinic, P1Dx = 4.892 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.7107 Å
a = 8.1372 (2) ÅCell parameters from 12220 reflections
b = 10.6969 (3) Åθ = 3.8–32.7°
c = 5.7840 (1) ŵ = 13.06 mm1
α = 102.787 (2)°T = 293 K
β = 110.6063 (19)°Acicular, red
γ = 100.9833 (19)°0.95 × 0.07 × 0.01 mm
V = 439.24 (2) Å3
Data collection top
Oxford Diffraction CCD
diffractometer
4591 independent reflections
Radiation source: X-ray tube3769 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.079
Detector resolution: 10.3784 pixels mm-1θmax = 32.7°, θmin = 3.8°
ω scansh = 1112
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
k = 1616
Tmin = 0.048, Tmax = 0.779l = 88
24475 measured reflections
Refinement top
Refinement on F0 restraints
R[F2 > 2σ(F2)] = 0.0320 constraints
wR(F2) = 0.038Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 2.19(Δ/σ)max = 0.017
4591 reflectionsΔρmax = 2.33 e Å3
92 parametersΔρmin = 2.62 e Å3
Crystal data top
OS2Sb2γ = 100.9833 (19)°
Mr = 323.6V = 439.24 (2) Å3
Triclinic, P1Z = 4
a = 8.1372 (2) ÅMo Kα radiation
b = 10.6969 (3) ŵ = 13.06 mm1
c = 5.7840 (1) ÅT = 293 K
α = 102.787 (2)°0.95 × 0.07 × 0.01 mm
β = 110.6063 (19)°
Data collection top
Oxford Diffraction CCD
diffractometer
4591 independent reflections
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
3769 reflections with I > 3σ(I)
Tmin = 0.048, Tmax = 0.779Rint = 0.079
24475 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.03292 parameters
wR(F2) = 0.0380 restraints
S = 2.19Δρmax = 2.33 e Å3
4591 reflectionsΔρmin = 2.62 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sb10.16830 (7)0.63147 (3)0.03899 (5)0.01036 (13)
Sb20.66029 (7)0.62981 (3)0.01367 (5)0.01097 (13)
Sb30.12564 (5)0.85373 (3)0.63172 (5)0.01265 (11)
Sb40.65275 (5)0.91541 (3)0.67960 (6)0.01425 (12)
S10.8098 (3)0.70294 (12)0.4978 (2)0.0139 (4)
S20.2896 (3)0.69203 (13)0.5174 (2)0.0139 (4)
S30.0478 (2)0.90942 (12)0.2258 (2)0.0123 (4)
S40.5202 (2)0.91063 (13)0.2286 (2)0.0128 (4)
O10.8989 (9)0.5687 (3)0.0304 (6)0.0140 (13)
O20.4155 (8)0.5712 (3)0.0745 (6)0.0136 (13)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sb10.0092 (2)0.01020 (13)0.01315 (12)0.0048 (2)0.00585 (18)0.00260 (9)
Sb20.0088 (2)0.01046 (14)0.01513 (13)0.0051 (2)0.00574 (18)0.00345 (10)
Sb30.01101 (15)0.01518 (15)0.01180 (12)0.00504 (16)0.00517 (12)0.00248 (10)
Sb40.01211 (16)0.01672 (16)0.01490 (13)0.00506 (16)0.00553 (13)0.00613 (11)
S10.0108 (6)0.0153 (5)0.0149 (5)0.0022 (6)0.0068 (6)0.0023 (4)
S20.0135 (7)0.0158 (5)0.0139 (5)0.0077 (6)0.0062 (5)0.0034 (4)
S30.0099 (6)0.0130 (5)0.0137 (4)0.0031 (5)0.0045 (5)0.0041 (4)
S40.0126 (7)0.0138 (5)0.0123 (4)0.0054 (5)0.0055 (5)0.0024 (4)
O10.0088 (19)0.0107 (15)0.0225 (16)0.0025 (19)0.0087 (19)0.0017 (12)
O20.0083 (19)0.0098 (15)0.0228 (15)0.0025 (19)0.0092 (18)0.0009 (12)
Geometric parameters (Å, º) top
Sb1—S22.4683 (12)Sb3—S22.491 (2)
Sb1—O1i2.146 (7)Sb3—S32.4463 (14)
Sb1—O1ii2.016 (3)Sb3—S3iii3.2168 (18)
Sb1—O22.184 (7)Sb3—S4iv3.1626 (16)
Sb2—S12.4904 (11)Sb4—S12.9834 (19)
Sb2—O12.141 (7)Sb4—S23.1125 (17)
Sb2—O22.144 (7)Sb4—S3iv2.5721 (17)
Sb2—O2ii2.013 (3)Sb4—S42.4312 (12)
Sb3—S1i2.5044 (18)Sb4—S4iv2.6101 (19)
S2—Sb1—O1i87.49 (10)S2—Sb3—S395.09 (5)
S2—Sb1—O1ii96.08 (10)S2—Sb3—S3iii172.81 (5)
S2—Sb1—O286.34 (10)S2—Sb3—S4iv88.34 (5)
O1i—Sb1—O1ii72.7 (2)S3—Sb3—S3iii81.52 (5)
O1i—Sb1—O2143.82 (15)S3—Sb3—S4iv78.66 (4)
O1ii—Sb1—O272.6 (2)S3iii—Sb3—S4iv84.78 (4)
S1—Sb2—O185.50 (10)S1—Sb4—S288.50 (5)
S1—Sb2—O282.98 (10)S1—Sb4—S3iv88.16 (5)
S1—Sb2—O2ii101.77 (10)S1—Sb4—S486.23 (5)
O1—Sb2—O2140.58 (16)S1—Sb4—S4iv171.89 (3)
O1—Sb2—O2ii73.6 (2)S2—Sb4—S3iv174.97 (4)
O2—Sb2—O2ii72.1 (2)S2—Sb4—S484.11 (5)
S1i—Sb3—S2102.31 (5)S2—Sb4—S4iv87.35 (5)
S1i—Sb3—S394.21 (5)S3iv—Sb4—S491.91 (5)
S1i—Sb3—S3iii84.32 (5)S3iv—Sb4—S4iv95.50 (5)
S1i—Sb3—S4iv167.75 (5)S4—Sb4—S4iv86.43 (5)
Symmetry codes: (i) x1, y, z; (ii) x+1, y+1, z; (iii) x, y+2, z+1; (iv) x+1, y+2, z+1.
(IV) top
Crystal data top
OS2Sb2Z = 32
Mr = 323.6F(000) = 4544
Triclinic, X1Dx = 4.892 Mg m3
Hall symbol: -XMo Kα radiation, λ = 0.7107 Å
a = 21.6558 (5) ÅCell parameters from 12220 reflections
b = 8.1372 (2) Åθ = 3.8–32.7°
c = 20.3859 (8) ŵ = 13.06 mm1
α = 90.028 (3)°T = 293 K
β = 101.994 (3)°Acicular, red
γ = 89.986 (2)°0.95 × 0.07 × 0.01 mm
V = 3513.92 (19) Å3
Data collection top
Oxford Diffraction CCD
diffractometer
4591 independent reflections
Radiation source: X-ray tube3769 reflections with I > 3σ(I)
Graphite monochromatorRint = 0.079
Detector resolution: 10.3784 pixels mm-1θmax = 32.7°, θmin = 3.8°
ω scansh = 3232
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
k = 1211
Tmin = 0.048, Tmax = 0.779l = 3030
24475 measured reflections
Refinement top
Refinement on F0 restraints
R[F2 > 2σ(F2)] = 0.0320 constraints
wR(F2) = 0.038Weighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
S = 2.19(Δ/σ)max = 0.033
4591 reflectionsΔρmax = 2.34 e Å3
93 parametersΔρmin = 2.58 e Å3
Crystal data top
OS2Sb2γ = 89.986 (2)°
Mr = 323.6V = 3513.92 (19) Å3
Triclinic, X1Z = 32
a = 21.6558 (5) ÅMo Kα radiation
b = 8.1372 (2) ŵ = 13.06 mm1
c = 20.3859 (8) ÅT = 293 K
α = 90.028 (3)°0.95 × 0.07 × 0.01 mm
β = 101.994 (3)°
Data collection top
Oxford Diffraction CCD
diffractometer
4591 independent reflections
Absorption correction: gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
3769 reflections with I > 3σ(I)
Tmin = 0.048, Tmax = 0.779Rint = 0.079
24475 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.03293 parameters
wR(F2) = 0.0380 restraints
S = 2.19Δρmax = 2.34 e Å3
4591 reflectionsΔρmin = 2.58 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sb10.101874 (14)0.74931 (7)0.184267 (14)0.01034 (8)
Sb20.095971 (14)0.25058 (7)0.185095 (14)0.01094 (8)
Sb30.194498 (14)0.00428 (5)0.073132 (16)0.01268 (8)
Sb40.191048 (14)0.49601 (5)0.042299 (17)0.01427 (9)
S10.19871 (6)0.2404 (3)0.14853 (6)0.0139 (3)
S20.20635 (6)0.7627 (2)0.15398 (6)0.0139 (3)
S30.07910 (5)0.0140 (2)0.04529 (6)0.0123 (3)
S40.07948 (6)0.5145 (2)0.04468 (6)0.0128 (3)
O10.11543 (16)0.0008 (8)0.21564 (16)0.0140 (9)
O20.12582 (16)0.4959 (8)0.21441 (16)0.0136 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sb10.01397 (13)0.00697 (13)0.01016 (14)0.00034 (19)0.00273 (10)0.0022 (2)
Sb20.01522 (13)0.00689 (13)0.01042 (14)0.00146 (19)0.00199 (10)0.0022 (2)
Sb30.01408 (13)0.00977 (13)0.01525 (15)0.00021 (12)0.00551 (10)0.00157 (16)
Sb40.01381 (13)0.01195 (14)0.01679 (16)0.00090 (13)0.00256 (11)0.00019 (17)
S10.0177 (5)0.0098 (6)0.0153 (5)0.0021 (6)0.0058 (4)0.0015 (6)
S20.0155 (5)0.0112 (6)0.0158 (5)0.0014 (5)0.0049 (4)0.0040 (6)
S30.0137 (5)0.0103 (6)0.0129 (5)0.0008 (6)0.0027 (4)0.0008 (6)
S40.0142 (5)0.0114 (7)0.0137 (5)0.0003 (6)0.0048 (4)0.0022 (6)
O10.0250 (17)0.0064 (14)0.0106 (15)0.000 (2)0.0039 (13)0.000 (2)
O20.0259 (17)0.0052 (14)0.0098 (15)0.0009 (19)0.0042 (13)0.000 (2)
Geometric parameters (Å, º) top
Sb1—S22.4683 (13)Sb3—S2iii2.4907 (18)
Sb1—O1i2.146 (7)Sb3—S32.4463 (12)
Sb1—O1ii2.016 (3)Sb3—S3iv3.2166 (16)
Sb1—O22.184 (6)Sb3—S4iv3.1623 (16)
Sb2—S12.4903 (14)Sb4—S12.9833 (17)
Sb2—O12.142 (7)Sb4—S23.1122 (17)
Sb2—O22.144 (6)Sb4—S3iv2.5722 (17)
Sb2—O2ii2.013 (3)Sb4—S42.4312 (13)
Sb3—S12.5045 (18)Sb4—S4v2.6103 (17)
S2—Sb1—O1i87.49 (11)S2iii—Sb3—S395.09 (5)
S2—Sb1—O1ii96.08 (10)S2iii—Sb3—S3iv172.81 (5)
S2—Sb1—O286.34 (11)S2iii—Sb3—S4iv88.33 (5)
O1i—Sb1—O1ii72.7 (2)S3—Sb3—S3iv81.52 (4)
O1i—Sb1—O2143.82 (13)S3—Sb3—S4iv78.67 (4)
O1ii—Sb1—O272.6 (2)S3iv—Sb3—S4iv84.78 (4)
S1—Sb2—O185.50 (11)S1—Sb4—S288.50 (5)
S1—Sb2—O282.98 (11)S1—Sb4—S3iv88.16 (5)
S1—Sb2—O2ii101.77 (10)S1—Sb4—S486.23 (5)
O1—Sb2—O2140.58 (14)S1—Sb4—S4v171.90 (4)
O1—Sb2—O2ii73.6 (2)S2—Sb4—S3iv174.97 (4)
O2—Sb2—O2ii72.1 (2)S2—Sb4—S484.12 (5)
S1—Sb3—S2iii102.32 (5)S2—Sb4—S4v87.34 (5)
S1—Sb3—S394.20 (5)S3iv—Sb4—S491.91 (5)
S1—Sb3—S3iv84.32 (5)S3iv—Sb4—S4v95.51 (5)
S1—Sb3—S4iv167.75 (4)S4—Sb4—S4v86.43 (5)
Symmetry codes: (i) x, y+1, z; (ii) x+1/4, y+3/4, z+1/2; (iii) x, y1, z; (iv) x+1/4, y+1/4, z; (v) x+1/4, y+5/4, z.

Experimental details

(I)(II)(III)(IV)
Crystal data
Chemical formulaOS2Sb2OS2Sb2OS2Sb2OS2Sb2
Mr323.6323.6323.6323.6
Crystal system, space groupTriclinic, P1Triclinic, X1Triclinic, P1Triclinic, X1
Temperature (K)293293293293
a, b, c (Å)8.1416 (3), 10.6968 (3), 5.7835 (2)21.6466 (9), 8.1416 (3), 20.3824 (9)8.1372 (2), 10.6969 (3), 5.7840 (1)21.6558 (5), 8.1372 (2), 20.3859 (8)
α, β, γ (°)102.758 (3), 110.657 (3), 101.020 (3)90.079 (4), 101.985 (5), 89.948 (4)102.787 (2), 110.6063 (19), 100.9833 (19)90.028 (3), 101.994 (3), 89.986 (2)
V3)439.23 (3)3513.8 (3)439.24 (2)3513.92 (19)
Z432432
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)13.0613.0613.0613.06
Crystal size (mm)0.65 × 0.05 × 0.030.65 × 0.05 × 0.030.95 × 0.07 × 0.010.95 × 0.07 × 0.01
Data collection
DiffractometerXcalibur, Atlas, Gemini ultra
diffractometer
Oxford Diffraction CCD
diffractometer
Oxford Diffraction CCD
diffractometer
Oxford Diffraction CCD
diffractometer
Absorption correctionGaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
Gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
Gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
Gaussian
Jana2006 (Petricek, Dusek & Palatinus, 2000)
Tmin, Tmax0.109, 0.6670.109, 0.6670.048, 0.7790.048, 0.779
No. of measured, independent and
observed [I > 3σ(I)] reflections
12651, 4465, 2604 12651, 4465, 2604 24475, 4591, 3769 24475, 4591, 3769
Rint0.0500.0500.0790.079
(sin θ/λ)max1)0.7600.7600.7600.760
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.024, 0.027, 1.12 0.024, 0.027, 1.11 0.032, 0.038, 2.19 0.032, 0.038, 2.19
No. of reflections4465446545914591
No. of parameters92929293
Δρmax, Δρmin (e Å3)1.15, 1.341.14, 1.362.33, 2.622.34, 2.58

Computer programs: CrysAlis CCD, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46), CrysAlis RED, Oxford Diffraction Ltd., Version 1.171.33.55 (release 05-01-2010 CrysAlis171 .NET) (compiled Jan 5 2010,16:28:46).

 

Subscribe to Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. B
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds