Download citation
Download citation
link to html
Crystals of the title dysprosium tin sulfide oxide, Dy8SnS13S1-xOx [x = 0.39 (4)], were obtained unintentionally from the Dy-Sn-S system. A statistical mixture of sulfur and oxygen was assumed for one position in the structure. S and O atoms surround each of the eight symmetrically non-equivalent dysprosium atoms. The Sn atoms are located in tetra­hedral surroundings of sulfur atoms. Trigonal prisms and tetra­hedra are connected to each other by their edges. All atoms are situated in mirror planes.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807063416/pk2066sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807063416/pk2066Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](Sn-S) = 0.004 Å
  • Disorder in main residue
  • R factor = 0.026
  • wR factor = 0.038
  • Data-to-parameter ratio = 16.2

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT220_ALERT_2_B Large Non-Solvent S Ueq(max)/Ueq(min) ... 4.25 Ratio
Alert level C PLAT041_ALERT_1_C Calc. and Rep. SumFormula Strings Differ .... ? PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ? PLAT045_ALERT_1_C Calculated and Reported Z Differ by ............ 0.25 Ratio PLAT068_ALERT_1_C Reported F000 Differs from Calcd (or Missing)... ? PLAT077_ALERT_4_C Unitcell contains non-integer number of atoms .. ? PLAT220_ALERT_2_C Large Non-Solvent Dy Ueq(max)/Ueq(min) ... 2.81 Ratio PLAT301_ALERT_3_C Main Residue Disorder ......................... 3.00 Perc. PLAT850_ALERT_2_C Check Flack Parameter Exact Value 0.00 and su .. 0.20
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 26.72 From the CIF: _reflns_number_total 2287 Count of symmetry unique reflns 1198 Completeness (_total/calc) 190.90% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 1089 Fraction of Friedel pairs measured 0.909 Are heavy atom types Z>Si present yes PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 8 ALERT level C = Check and explain 4 ALERT level G = General alerts; check 6 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 3 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

An attempt to synthesize Dy2SnS5, a compound with the La2SnS5 type structure was unsuccessful, resulting in a multiphase product. However, the formation of the new compound, Dy8SnS13S1 - xOx (x = 0.39 (4)) was achieved. The structure of this compound was investigated by means of single-crystal X-ray diffraction. In the initial stage of refinement, the composition Dy8SnS14 was assumed. However, unusually short Dy2—S14 (2.399 (5) Å) and Dy3—S14 (2.508 (7) Å) distances and a large value for the displacement parameter of S14 were observed. To complete the refinement, a statistical mixture (S and O) was assumed at the site of S14. Refinement of this model reduced the unusual displacement parameter to a physically reasonable value. The final composition was Dy8SnS13S1 - xOx (x = 0.39 (4)). The values of the Dy2—S14 (2.399 (5) Å) and Dy3—S14 (2.508 (7) Å) distances are intermediate between the Dy—O (2.220–2.264 Å) and Dy–S (2.704–2.742 Å) distances in Dy2OS2 (Schleid, 1991). A similar substitution of S by O in one position has also been observed in the structure of the La10S14S1 - xOx (x 1/2) compound (Besançon et al., 1973).

The unit cell and coordination polyhedra of the Dy and Sn atoms in the structure of the Dy8SnS14 - xOx (x = 0.39 (4)) compound are shown in Fig. 1. Sulfur and oxygen atoms surround each of eight symmetrically non-equivalent dysprosium atoms. However, only one mono-capped trigonal prism is evident (Dy1) along with seven bi-capped trigonal prisms around the remaining Dy atoms. The Sn atoms are located in tetrahedral surroundings of sulfur atoms. Trigonal prisms and tetrahedra are connected to each other by edges.

Related literature top

For previous structures with a statistical mixture of sulfur and oxygen, see: Besançon et al. (1973); cShleid (1991).

Experimental top

Single crystals of the title compound were grown by fusion of the elemental constituents (Alfa Aesar; purity > 99.9%wt) in evacuated silica ampoules. The ampoule was heated in a tube furnace with a heating rate of 30 K/h to 1420 K and kept at this temperature for 4 h. It was then cooled down slowly (10 K/h) to 870 K and annealed at this temperature for further 240 h and finally quenched in cold water. The product was a brown-coloured compact alloy containing red crystals with a prismatic habit and maximal lengths of 0.2 mm. An EDAX PV9800 microanalyser was used for the confirmation of the composition of the Dy, Sn and S in the crystal. The content of oxygen (<2%) was out of the limit of the microanalyser.

Refinement top

A statistical mixture of the sulfur and oxygen was assumed in the refinement with the same anisotropic displacement parameters for the S14 and O14 atoms. The space group Cmc21 was confirmed with PLATON (Spek, 2003).

Structure description top

An attempt to synthesize Dy2SnS5, a compound with the La2SnS5 type structure was unsuccessful, resulting in a multiphase product. However, the formation of the new compound, Dy8SnS13S1 - xOx (x = 0.39 (4)) was achieved. The structure of this compound was investigated by means of single-crystal X-ray diffraction. In the initial stage of refinement, the composition Dy8SnS14 was assumed. However, unusually short Dy2—S14 (2.399 (5) Å) and Dy3—S14 (2.508 (7) Å) distances and a large value for the displacement parameter of S14 were observed. To complete the refinement, a statistical mixture (S and O) was assumed at the site of S14. Refinement of this model reduced the unusual displacement parameter to a physically reasonable value. The final composition was Dy8SnS13S1 - xOx (x = 0.39 (4)). The values of the Dy2—S14 (2.399 (5) Å) and Dy3—S14 (2.508 (7) Å) distances are intermediate between the Dy—O (2.220–2.264 Å) and Dy–S (2.704–2.742 Å) distances in Dy2OS2 (Schleid, 1991). A similar substitution of S by O in one position has also been observed in the structure of the La10S14S1 - xOx (x 1/2) compound (Besançon et al., 1973).

The unit cell and coordination polyhedra of the Dy and Sn atoms in the structure of the Dy8SnS14 - xOx (x = 0.39 (4)) compound are shown in Fig. 1. Sulfur and oxygen atoms surround each of eight symmetrically non-equivalent dysprosium atoms. However, only one mono-capped trigonal prism is evident (Dy1) along with seven bi-capped trigonal prisms around the remaining Dy atoms. The Sn atoms are located in tetrahedral surroundings of sulfur atoms. Trigonal prisms and tetrahedra are connected to each other by edges.

For previous structures with a statistical mixture of sulfur and oxygen, see: Besançon et al. (1973); cShleid (1991).

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2007); cell refinement: CrysAlis RED (Oxford Diffraction, 2007); data reduction: CrysAlis RED (Oxford Diffraction, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 2005); software used to prepare material for publication: publCIF (Westrip, 2007) and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The structure of Dy8SnS13.61O0.39 viewed down the a axis. Displacement ellipsoids are shown at the 50% probability level.
Dysprosium tin sulfide oxide top
Crystal data top
Dy8SnS13.61O0.39F(000) = 3196
Mr = 1861.27Dx = 6.506 Mg m3
Orthorhombic, Cmc21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: C 2c -2Cell parameters from 1910 reflections
a = 3.7822 (8) Åθ = 2.6–26.7°
b = 23.620 (5) ŵ = 33.80 mm1
c = 21.271 (4) ÅT = 293 K
V = 1900.3 (7) Å3Needle, red
Z = 40.14 × 0.01 × 0.01 mm
Data collection top
KUMA KM-4 with CCD area-detector
diffractometer
2287 independent reflections
Radiation source: fine-focus sealed tube1910 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.049
Detector resolution: 1024x1024 with blocks 2x2, 33.133pixel/mm pixels mm-1θmax = 26.7°, θmin = 2.6°
ω–scanh = 44
Absorption correction: numerical
(CrysAlis; Oxford Diffraction, 2007)
k = 2929
Tmin = 0.104, Tmax = 0.716l = 2626
11655 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.026 w = 1/[σ2(Fo2) + (0.0128P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.038(Δ/σ)max = 0.001
S = 0.89Δρmax = 3.05 e Å3
2287 reflectionsΔρmin = 1.56 e Å3
141 parametersAbsolute structure: Flack (1983), 1089 Friedel pairs
1 restraintAbsolute structure parameter: 0.0 (2)
Crystal data top
Dy8SnS13.61O0.39V = 1900.3 (7) Å3
Mr = 1861.27Z = 4
Orthorhombic, Cmc21Mo Kα radiation
a = 3.7822 (8) ŵ = 33.80 mm1
b = 23.620 (5) ÅT = 293 K
c = 21.271 (4) Å0.14 × 0.01 × 0.01 mm
Data collection top
KUMA KM-4 with CCD area-detector
diffractometer
2287 independent reflections
Absorption correction: numerical
(CrysAlis; Oxford Diffraction, 2007)
1910 reflections with I > 2σ(I)
Tmin = 0.104, Tmax = 0.716Rint = 0.049
11655 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0261 restraint
wR(F2) = 0.038Δρmax = 3.05 e Å3
S = 0.89Δρmin = 1.56 e Å3
2287 reflectionsAbsolute structure: Flack (1983), 1089 Friedel pairs
141 parametersAbsolute structure parameter: 0.0 (2)
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 > 2σ(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*/UeqOcc. (<1)
Dy10.00000.69122 (4)0.08524 (3)0.0086 (2)
Dy20.00000.44849 (4)0.24158 (5)0.0242 (3)
Dy30.00000.10373 (4)0.23391 (4)0.0132 (2)
Dy40.00000.04543 (4)0.40541 (5)0.0125 (2)
Dy50.00000.85422 (4)0.07459 (5)0.0106 (2)
Dy60.00000.27636 (4)0.24724 (4)0.0100 (2)
Dy70.00000.37415 (4)0.41648 (5)0.0109 (2)
Dy80.50000.52208 (3)0.07589 (4)0.01244 (19)
Sn10.00000.70904 (6)0.40908 (8)0.0076 (2)
S10.00000.85740 (18)0.2105 (2)0.0088 (11)
S20.50000.43628 (19)0.3487 (2)0.0100 (10)
S30.50000.7734 (2)0.1121 (2)0.0089 (10)
S40.00000.48205 (18)0.4751 (2)0.0086 (9)
S50.00000.55462 (18)0.3115 (2)0.0100 (10)
S60.50000.63430 (18)0.0139 (2)0.0084 (10)
S70.00000.4362 (2)0.1072 (2)0.0121 (11)
S80.00000.58602 (18)0.13619 (19)0.0105 (9)
S90.50000.7460 (2)0.4772 (2)0.0141 (10)
S100.00000.1733 (2)0.3409 (2)0.0169 (10)
S110.00000.69522 (18)0.21604 (19)0.0079 (9)
S120.00000.6207 (2)0.4722 (2)0.0112 (10)
S130.00000.80025 (18)0.3496 (2)0.0096 (9)
O140.00000.0010 (3)0.2040 (4)0.034 (3)0.39 (4)
S140.00000.0010 (3)0.2040 (4)0.034 (3)0.61 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Dy10.0068 (4)0.0089 (5)0.0101 (5)0.0000.0000.0003 (4)
Dy20.0243 (5)0.0308 (6)0.0174 (7)0.0000.0000.0128 (5)
Dy30.0077 (4)0.0231 (5)0.0089 (5)0.0000.0000.0020 (4)
Dy40.0095 (5)0.0173 (5)0.0106 (5)0.0000.0000.0007 (4)
Dy50.0062 (4)0.0107 (4)0.0149 (5)0.0000.0000.0034 (4)
Dy60.0069 (4)0.0122 (4)0.0110 (5)0.0000.0000.0010 (4)
Dy70.0083 (4)0.0162 (5)0.0083 (5)0.0000.0000.0014 (4)
Dy80.0062 (4)0.0104 (4)0.0207 (5)0.0000.0000.0021 (4)
Sn10.0069 (4)0.0080 (5)0.0079 (5)0.0000.0000.0016 (4)
S10.012 (3)0.010 (2)0.005 (3)0.0000.0000.0009 (18)
S20.007 (2)0.013 (2)0.010 (2)0.0000.0000.004 (2)
S30.006 (2)0.010 (2)0.010 (3)0.0000.0000.002 (2)
S40.008 (2)0.008 (2)0.010 (2)0.0000.0000.0019 (18)
S50.009 (2)0.014 (2)0.006 (2)0.0000.0000.0020 (17)
S60.008 (2)0.009 (2)0.008 (2)0.0000.0000.0006 (16)
S70.008 (2)0.014 (2)0.014 (3)0.0000.0000.006 (2)
S80.011 (2)0.012 (2)0.009 (2)0.0000.0000.0014 (16)
S90.009 (2)0.021 (3)0.013 (2)0.0000.0000.0090 (18)
S100.009 (2)0.029 (3)0.012 (2)0.0000.0000.011 (2)
S110.010 (2)0.007 (2)0.007 (2)0.0000.0000.0045 (17)
S120.013 (2)0.012 (2)0.009 (2)0.0000.0000.001 (2)
S130.013 (2)0.008 (2)0.008 (2)0.0000.0000.0007 (18)
O140.023 (4)0.022 (5)0.056 (6)0.0000.0000.004 (4)
S140.023 (4)0.022 (5)0.056 (6)0.0000.0000.004 (4)
Geometric parameters (Å, º) top
Dy1—S82.711 (4)Dy7—S13vii2.940 (3)
Dy1—S9i2.735 (5)Dy7—S13viii2.940 (3)
Dy1—S32.769 (3)Dy7—Dy7ii3.7822 (8)
Dy1—S3ii2.769 (3)Dy7—Dy7iii3.7822 (8)
Dy1—S6ii2.772 (3)Dy7—Dy1xii3.9078 (15)
Dy1—S62.772 (3)Dy8—S8iii2.739 (3)
Dy1—S112.784 (4)Dy8—S82.739 (3)
Dy1—Dy1ii3.7822 (8)Dy8—S14v2.770 (8)
Dy1—Dy1iii3.7822 (8)Dy8—O14v2.770 (8)
Dy1—Dy53.8567 (14)Dy8—S72.852 (4)
Dy1—Dy7iv3.9078 (15)Dy8—S7iii2.852 (4)
Dy2—S14v2.399 (5)Dy8—S4iv2.861 (3)
Dy2—O14v2.399 (5)Dy8—S4xiii2.861 (3)
Dy2—S14vi2.399 (5)Dy8—S62.960 (4)
Dy2—O14vi2.399 (5)Dy8—Dy8ii3.7822 (8)
Dy2—S72.873 (5)Dy8—Dy8iii3.7822 (8)
Dy2—S52.914 (5)Dy8—Dy3v3.8753 (14)
Dy2—S1vii2.940 (3)Sn1—S122.481 (5)
Dy2—S1viii2.940 (3)Sn1—S132.498 (5)
Dy2—S22.976 (4)Sn1—S10vi2.529 (3)
Dy2—S2ii2.976 (4)Sn1—S10v2.529 (3)
Dy2—Dy2ii3.7822 (8)Sn1—S92.537 (3)
Dy2—Dy2iii3.7822 (8)Sn1—S9ii2.537 (3)
Dy3—O142.508 (7)S1—Dy6vi2.802 (3)
Dy3—S5viii2.765 (3)S1—Dy6v2.802 (3)
Dy3—S5vii2.765 (3)S1—Dy2v2.940 (3)
Dy3—S102.807 (5)S1—Dy2vi2.940 (3)
Dy3—S8vii2.841 (3)S2—Dy7iii2.794 (4)
Dy3—S8viii2.841 (3)S2—Dy4v2.846 (5)
Dy3—S11viii2.897 (3)S2—Dy2iii2.976 (4)
Dy3—S11vii2.897 (3)S3—Dy1iii2.769 (3)
Dy3—Dy3ii3.7822 (8)S3—Dy5iii2.803 (4)
Dy3—Dy3iii3.7822 (8)S3—Dy6v2.876 (5)
Dy3—Dy8vii3.8753 (14)S4—Dy4v2.831 (3)
Dy4—S5vii2.760 (3)S4—Dy4vi2.831 (3)
Dy4—S5viii2.760 (3)S4—Dy8xi2.861 (3)
Dy4—S4viii2.831 (3)S4—Dy8xii2.861 (3)
Dy4—S4vii2.831 (3)S5—Dy4v2.760 (3)
Dy4—S2vii2.846 (5)S5—Dy4vi2.760 (3)
Dy4—S12viii2.960 (4)S5—Dy3vi2.765 (3)
Dy4—S12vii2.960 (4)S5—Dy3v2.765 (3)
Dy4—Dy4iii3.7822 (8)S6—Dy1iii2.772 (3)
Dy4—Dy4ii3.7822 (8)S6—Dy7iv2.813 (3)
Dy4—Dy8ix3.9612 (17)S6—Dy7xiii2.813 (3)
Dy5—S7v2.794 (4)S7—Dy5vii2.794 (4)
Dy5—S7vi2.794 (4)S7—Dy5viii2.794 (4)
Dy5—S32.803 (4)S7—Dy8ii2.852 (4)
Dy5—S3ii2.803 (4)S8—Dy8ii2.739 (3)
Dy5—S12.892 (5)S8—Dy3v2.841 (3)
Dy5—S12x2.944 (4)S8—Dy3vi2.841 (3)
Dy5—S12i2.944 (4)S9—Sn1iii2.537 (3)
Dy5—S9i3.145 (5)S9—Dy1xiv2.735 (5)
Dy5—Dy5ii3.7822 (8)S9—Dy5xiv3.145 (5)
Dy5—Dy5iii3.7822 (8)S10—Sn1viii2.529 (3)
Dy5—Dy8vi3.9649 (15)S10—Sn1vii2.529 (3)
Dy6—S11vii2.773 (3)S11—Dy6v2.773 (3)
Dy6—S11viii2.773 (3)S11—Dy6vi2.773 (3)
Dy6—S1viii2.802 (3)S11—Dy3vi2.897 (3)
Dy6—S1vii2.802 (3)S11—Dy3v2.897 (3)
Dy6—S3vii2.876 (5)S12—Dy5xiv2.944 (4)
Dy6—S13viii2.939 (3)S12—Dy5xv2.944 (4)
Dy6—S13vii2.939 (3)S12—Dy4vi2.960 (4)
Dy6—S103.145 (5)S12—Dy4v2.960 (4)
Dy6—Dy6iii3.7822 (8)S13—Dy6vi2.939 (3)
Dy6—Dy6ii3.7822 (8)S13—Dy6v2.939 (3)
Dy7—S22.794 (4)S13—Dy7v2.940 (3)
Dy7—S2ii2.794 (4)S13—Dy7vi2.940 (3)
Dy7—S6xi2.813 (3)O14—Dy2vii2.399 (5)
Dy7—S6xii2.813 (3)O14—Dy2viii2.399 (5)
Dy7—S42.837 (5)O14—Dy8vii2.770 (8)
S8—Dy1—S9i146.41 (14)S11vii—Dy6—S1viii149.95 (14)
S8—Dy1—S3124.06 (10)S11viii—Dy6—S1viii86.85 (10)
S9i—Dy1—S378.05 (13)S11vii—Dy6—S1vii86.85 (9)
S8—Dy1—S3ii124.06 (10)S11viii—Dy6—S1vii149.95 (14)
S9i—Dy1—S3ii78.05 (13)S1viii—Dy6—S1vii84.89 (12)
S3—Dy1—S3ii86.14 (13)S11vii—Dy6—S3vii75.16 (11)
S8—Dy1—S6ii76.95 (11)S11viii—Dy6—S3vii75.16 (11)
S9i—Dy1—S6ii78.66 (12)S1viii—Dy6—S3vii74.79 (12)
S3—Dy1—S6ii156.70 (14)S1vii—Dy6—S3vii74.79 (12)
S3ii—Dy1—S6ii89.24 (10)S11vii—Dy6—S13viii138.49 (12)
S8—Dy1—S676.95 (11)S11viii—Dy6—S13viii82.60 (10)
S9i—Dy1—S678.66 (12)S1viii—Dy6—S13viii68.99 (11)
S3—Dy1—S689.24 (10)S1vii—Dy6—S13viii120.66 (12)
S3ii—Dy1—S6156.70 (14)S3vii—Dy6—S13viii138.20 (6)
S6ii—Dy1—S686.02 (13)S11vii—Dy6—S13vii82.60 (10)
S8—Dy1—S1168.38 (12)S11viii—Dy6—S13vii138.49 (12)
S9i—Dy1—S11145.21 (13)S1viii—Dy6—S13vii120.66 (12)
S3—Dy1—S1176.72 (12)S1vii—Dy6—S13vii68.99 (11)
S3ii—Dy1—S1176.72 (12)S3vii—Dy6—S13vii138.20 (6)
S6ii—Dy1—S11124.29 (10)S13viii—Dy6—S13vii80.09 (11)
S6—Dy1—S11124.29 (10)S11vii—Dy6—S1067.46 (10)
S8—Dy1—Dy1ii90.0S11viii—Dy6—S1067.46 (10)
S9i—Dy1—Dy1ii90.0S1viii—Dy6—S10134.86 (8)
S3—Dy1—Dy1ii133.07 (7)S1vii—Dy6—S10134.86 (8)
S3ii—Dy1—Dy1ii46.93 (7)S3vii—Dy6—S10127.89 (13)
S6ii—Dy1—Dy1ii46.99 (6)S13viii—Dy6—S1071.30 (10)
S6—Dy1—Dy1ii133.01 (6)S13vii—Dy6—S1071.30 (10)
S11—Dy1—Dy1ii90.0S11vii—Dy6—Dy6iii133.00 (6)
S8—Dy1—Dy1iii90.0S11viii—Dy6—Dy6iii47.00 (6)
S9i—Dy1—Dy1iii90.0S1viii—Dy6—Dy6iii47.55 (6)
S3—Dy1—Dy1iii46.93 (7)S1vii—Dy6—Dy6iii132.45 (6)
S3ii—Dy1—Dy1iii133.07 (7)S3vii—Dy6—Dy6iii90.0
S6ii—Dy1—Dy1iii133.01 (6)S13viii—Dy6—Dy6iii49.95 (5)
S6—Dy1—Dy1iii46.99 (6)S13vii—Dy6—Dy6iii130.05 (5)
S11—Dy1—Dy1iii90.0S10—Dy6—Dy6iii90.0
Dy1ii—Dy1—Dy1iii180.00 (5)S11vii—Dy6—Dy6ii47.00 (6)
S8—Dy1—Dy5159.81 (9)S11viii—Dy6—Dy6ii133.00 (6)
S9i—Dy1—Dy553.78 (10)S1viii—Dy6—Dy6ii132.45 (6)
S3—Dy1—Dy546.56 (8)S1vii—Dy6—Dy6ii47.55 (6)
S3ii—Dy1—Dy546.56 (8)S3vii—Dy6—Dy6ii90.0
S6ii—Dy1—Dy5116.87 (9)S13viii—Dy6—Dy6ii130.05 (5)
S6—Dy1—Dy5116.87 (9)S13vii—Dy6—Dy6ii49.95 (5)
S11—Dy1—Dy591.43 (9)S10—Dy6—Dy6ii90.0
Dy1ii—Dy1—Dy590.0Dy6iii—Dy6—Dy6ii180.00 (5)
Dy1iii—Dy1—Dy590.0S2—Dy7—S2ii85.20 (14)
S8—Dy1—Dy7iv90.29 (9)S2—Dy7—S6xi87.83 (11)
S9i—Dy1—Dy7iv56.12 (10)S2ii—Dy7—S6xi150.73 (13)
S3—Dy1—Dy7iv117.79 (10)S2—Dy7—S6xii150.73 (13)
S3ii—Dy1—Dy7iv117.79 (10)S2ii—Dy7—S6xii87.83 (11)
S6ii—Dy1—Dy7iv46.02 (7)S6xi—Dy7—S6xii84.49 (13)
S6—Dy1—Dy7iv46.02 (7)S2—Dy7—S475.80 (11)
S11—Dy1—Dy7iv158.67 (9)S2ii—Dy7—S475.80 (11)
Dy1ii—Dy1—Dy7iv90.0S6xi—Dy7—S474.93 (11)
Dy1iii—Dy1—Dy7iv90.0S6xii—Dy7—S474.93 (11)
Dy5—Dy1—Dy7iv109.91 (3)S2—Dy7—S13vii119.86 (13)
S14v—Dy2—O14v0.0 (5)S2ii—Dy7—S13vii68.11 (12)
S14v—Dy2—S14vi104.1 (3)S6xi—Dy7—S13vii138.30 (12)
O14v—Dy2—S14vi104.1 (3)S6xii—Dy7—S13vii83.21 (10)
S14v—Dy2—O14vi104.1 (3)S4—Dy7—S13vii138.23 (6)
O14v—Dy2—O14vi104.1 (3)S2—Dy7—S13viii68.11 (12)
S14vi—Dy2—O14vi0.0 (4)S2ii—Dy7—S13viii119.86 (13)
S14v—Dy2—S773.79 (19)S6xi—Dy7—S13viii83.21 (10)
O14v—Dy2—S773.79 (19)S6xii—Dy7—S13viii138.30 (12)
S14vi—Dy2—S773.79 (19)S4—Dy7—S13viii138.23 (6)
O14vi—Dy2—S773.79 (19)S13vii—Dy7—S13viii80.06 (11)
S14v—Dy2—S574.03 (17)S2—Dy7—Dy7ii132.60 (7)
O14v—Dy2—S574.03 (17)S2ii—Dy7—Dy7ii47.40 (7)
S14vi—Dy2—S574.03 (17)S6xi—Dy7—Dy7ii132.25 (6)
O14vi—Dy2—S574.03 (17)S6xii—Dy7—Dy7ii47.75 (6)
S7—Dy2—S5126.46 (14)S4—Dy7—Dy7ii90.0
S14v—Dy2—S1vii144.2 (2)S13vii—Dy7—Dy7ii49.97 (6)
O14v—Dy2—S1vii144.2 (2)S13viii—Dy7—Dy7ii130.03 (6)
S14vi—Dy2—S1vii78.26 (16)S2—Dy7—Dy7iii47.40 (7)
O14vi—Dy2—S1vii78.26 (16)S2ii—Dy7—Dy7iii132.60 (7)
S7—Dy2—S1vii72.68 (12)S6xi—Dy7—Dy7iii47.75 (6)
S5—Dy2—S1vii138.10 (7)S6xii—Dy7—Dy7iii132.25 (6)
S14v—Dy2—S1viii78.26 (16)S4—Dy7—Dy7iii90.0
O14v—Dy2—S1viii78.26 (16)S13vii—Dy7—Dy7iii130.03 (6)
S14vi—Dy2—S1viii144.2 (2)S13viii—Dy7—Dy7iii49.97 (6)
O14vi—Dy2—S1viii144.2 (2)Dy7ii—Dy7—Dy7iii180.00 (8)
S7—Dy2—S1viii72.68 (12)S2—Dy7—Dy1xii132.94 (8)
S5—Dy2—S1viii138.10 (7)S2ii—Dy7—Dy1xii132.94 (8)
S1vii—Dy2—S1viii80.07 (11)S6xi—Dy7—Dy1xii45.18 (7)
S14v—Dy2—S278.71 (18)S6xii—Dy7—Dy1xii45.18 (7)
O14v—Dy2—S278.71 (18)S4—Dy7—Dy1xii87.21 (9)
S14vi—Dy2—S2143.7 (2)S13vii—Dy7—Dy1xii102.10 (8)
O14vi—Dy2—S2143.7 (2)S13viii—Dy7—Dy1xii102.10 (8)
S7—Dy2—S2138.79 (7)Dy7ii—Dy7—Dy1xii90.0
S5—Dy2—S272.10 (11)Dy7iii—Dy7—Dy1xii90.0
S1vii—Dy2—S2120.68 (12)S8iii—Dy8—S887.33 (13)
S1viii—Dy2—S272.10 (11)S8iii—Dy8—S14v68.79 (14)
S14v—Dy2—S2ii143.7 (2)S8—Dy8—S14v68.79 (14)
O14v—Dy2—S2ii143.7 (2)S8iii—Dy8—O14v68.79 (14)
S14vi—Dy2—S2ii78.71 (18)S8—Dy8—O14v68.79 (14)
O14vi—Dy2—S2ii78.71 (18)S14v—Dy8—O14v0.0 (3)
S7—Dy2—S2ii138.79 (7)S8iii—Dy8—S7137.78 (12)
S5—Dy2—S2ii72.10 (11)S8—Dy8—S779.92 (11)
S1vii—Dy2—S2ii72.10 (11)S14v—Dy8—S769.06 (15)
S1viii—Dy2—S2ii120.68 (12)O14v—Dy8—S769.06 (15)
S2—Dy2—S2ii78.91 (12)S8iii—Dy8—S7iii79.92 (11)
S14v—Dy2—Dy2ii142.03 (14)S8—Dy8—S7iii137.78 (12)
O14v—Dy2—Dy2ii142.03 (14)S14v—Dy8—S7iii69.06 (15)
S14vi—Dy2—Dy2ii37.97 (14)O14v—Dy8—S7iii69.06 (15)
O14vi—Dy2—Dy2ii37.97 (14)S7—Dy8—S7iii83.07 (13)
S7—Dy2—Dy2ii90.0S8iii—Dy8—S4iv145.71 (13)
S5—Dy2—Dy2ii90.0S8—Dy8—S4iv85.03 (10)
S1vii—Dy2—Dy2ii49.97 (6)S14v—Dy8—S4iv136.99 (8)
S1viii—Dy2—Dy2ii130.03 (6)O14v—Dy8—S4iv136.99 (8)
S2—Dy2—Dy2ii129.46 (6)S7—Dy8—S4iv73.29 (12)
S2ii—Dy2—Dy2ii50.54 (6)S7iii—Dy8—S4iv126.09 (13)
S14v—Dy2—Dy2iii37.97 (14)S8iii—Dy8—S4xiii85.03 (10)
O14v—Dy2—Dy2iii37.97 (14)S8—Dy8—S4xiii145.71 (13)
S14vi—Dy2—Dy2iii142.03 (14)S14v—Dy8—S4xiii136.99 (8)
O14vi—Dy2—Dy2iii142.03 (14)O14v—Dy8—S4xiii136.99 (8)
S7—Dy2—Dy2iii90.0S7—Dy8—S4xiii126.09 (13)
S5—Dy2—Dy2iii90.0S7iii—Dy8—S4xiii73.29 (12)
S1vii—Dy2—Dy2iii130.03 (6)S4iv—Dy8—S4xiii82.77 (12)
S1viii—Dy2—Dy2iii49.97 (6)S8iii—Dy8—S673.43 (10)
S2—Dy2—Dy2iii50.54 (6)S8—Dy8—S673.43 (10)
S2ii—Dy2—Dy2iii129.46 (6)S14v—Dy8—S6126.78 (17)
Dy2ii—Dy2—Dy2iii180.00 (6)O14v—Dy8—S6126.78 (17)
O14—Dy3—S5viii75.25 (16)S7—Dy8—S6137.80 (7)
O14—Dy3—S5vii75.25 (16)S7iii—Dy8—S6137.80 (7)
S5viii—Dy3—S5vii86.32 (13)S4iv—Dy8—S672.35 (11)
O14—Dy3—S10140.5 (2)S4xiii—Dy8—S672.35 (11)
S5viii—Dy3—S1076.23 (12)S8iii—Dy8—Dy8ii133.66 (6)
S5vii—Dy3—S1076.23 (12)S8—Dy8—Dy8ii46.34 (6)
O14—Dy3—S8vii70.86 (16)S14v—Dy8—Dy8ii90.0
S5viii—Dy3—S8vii146.11 (13)O14v—Dy8—Dy8ii90.0
S5vii—Dy3—S8vii85.38 (10)S7—Dy8—Dy8ii48.47 (7)
S10—Dy3—S8vii132.79 (8)S7iii—Dy8—Dy8ii131.53 (7)
O14—Dy3—S8viii70.86 (16)S4iv—Dy8—Dy8ii48.62 (6)
S5viii—Dy3—S8viii85.38 (10)S4xiii—Dy8—Dy8ii131.38 (6)
S5vii—Dy3—S8viii146.11 (13)S6—Dy8—Dy8ii90.0
S10—Dy3—S8viii132.79 (8)S8iii—Dy8—Dy8iii46.34 (6)
S8vii—Dy3—S8viii83.46 (11)S8—Dy8—Dy8iii133.66 (6)
O14—Dy3—S11viii133.50 (11)S14v—Dy8—Dy8iii90.0
S5viii—Dy3—S11viii86.83 (9)O14v—Dy8—Dy8iii90.0
S5vii—Dy3—S11viii146.92 (13)S7—Dy8—Dy8iii131.53 (7)
S10—Dy3—S11viii70.70 (11)S7iii—Dy8—Dy8iii48.47 (7)
S8vii—Dy3—S11viii116.65 (11)S4iv—Dy8—Dy8iii131.38 (6)
S8viii—Dy3—S11viii65.12 (11)S4xiii—Dy8—Dy8iii48.62 (6)
O14—Dy3—S11vii133.50 (11)S6—Dy8—Dy8iii90.0
S5viii—Dy3—S11vii146.92 (13)Dy8ii—Dy8—Dy8iii180.0
S5vii—Dy3—S11vii86.83 (9)S8iii—Dy8—Dy3v47.11 (7)
S10—Dy3—S11vii70.70 (11)S8—Dy8—Dy3v47.11 (7)
S8vii—Dy3—S11vii65.12 (11)S14v—Dy8—Dy3v40.19 (15)
S8viii—Dy3—S11vii116.65 (11)O14v—Dy8—Dy3v40.19 (15)
S11viii—Dy3—S11vii81.52 (11)S7—Dy8—Dy3v98.71 (10)
O14—Dy3—Dy3ii90.0S7iii—Dy8—Dy3v98.71 (10)
S5viii—Dy3—Dy3ii133.16 (6)S4iv—Dy8—Dy3v131.84 (7)
S5vii—Dy3—Dy3ii46.84 (6)S4xiii—Dy8—Dy3v131.84 (7)
S10—Dy3—Dy3ii90.0S6—Dy8—Dy3v86.59 (9)
S8vii—Dy3—Dy3ii48.27 (6)Dy8ii—Dy8—Dy3v90.0
S8viii—Dy3—Dy3ii131.73 (6)Dy8iii—Dy8—Dy3v90.0
S11viii—Dy3—Dy3ii130.76 (5)S12—Sn1—S13177.64 (19)
S11vii—Dy3—Dy3ii49.24 (5)S12—Sn1—S10vi91.72 (15)
O14—Dy3—Dy3iii90.0S13—Sn1—S10vi89.85 (14)
S5viii—Dy3—Dy3iii46.84 (6)S12—Sn1—S10v91.72 (15)
S5vii—Dy3—Dy3iii133.16 (6)S13—Sn1—S10v89.85 (14)
S10—Dy3—Dy3iii90.0S10vi—Sn1—S10v96.82 (16)
S8vii—Dy3—Dy3iii131.73 (6)S12—Sn1—S988.85 (14)
S8viii—Dy3—Dy3iii48.27 (6)S13—Sn1—S989.58 (14)
S11viii—Dy3—Dy3iii49.24 (5)S10vi—Sn1—S9179.39 (19)
S11vii—Dy3—Dy3iii130.76 (5)S10v—Sn1—S983.40 (8)
Dy3ii—Dy3—Dy3iii180.00 (3)S12—Sn1—S9ii88.85 (14)
O14—Dy3—Dy8vii45.47 (18)S13—Sn1—S9ii89.58 (13)
S5viii—Dy3—Dy8vii107.98 (9)S10vi—Sn1—S9ii83.40 (8)
S5vii—Dy3—Dy8vii107.98 (9)S10v—Sn1—S9ii179.39 (19)
S10—Dy3—Dy8vii174.01 (11)S9—Sn1—S9ii96.38 (16)
S8vii—Dy3—Dy8vii44.94 (7)Dy6vi—S1—Dy6v84.89 (12)
S8viii—Dy3—Dy8vii44.94 (7)Dy6vi—S1—Dy5105.14 (12)
S11viii—Dy3—Dy8vii104.92 (9)Dy6v—S1—Dy5105.14 (12)
S11vii—Dy3—Dy8vii104.92 (8)Dy6vi—S1—Dy2v150.61 (19)
Dy3ii—Dy3—Dy8vii90.0Dy6v—S1—Dy2v90.17 (6)
Dy3iii—Dy3—Dy8vii90.0Dy5—S1—Dy2v104.12 (12)
S5vii—Dy4—S5viii86.51 (13)Dy6vi—S1—Dy2vi90.17 (6)
S5vii—Dy4—S4viii151.45 (13)Dy6v—S1—Dy2vi150.61 (19)
S5viii—Dy4—S4viii87.87 (10)Dy5—S1—Dy2vi104.12 (12)
S5vii—Dy4—S4vii87.87 (10)Dy2v—S1—Dy2vi80.07 (11)
S5viii—Dy4—S4vii151.45 (13)Dy7—S2—Dy7iii85.20 (14)
S4viii—Dy4—S4vii83.83 (12)Dy7—S2—Dy4v104.92 (13)
S5vii—Dy4—S2vii76.38 (11)Dy7iii—S2—Dy4v104.92 (13)
S5viii—Dy4—S2vii76.38 (11)Dy7—S2—Dy290.90 (5)
S4viii—Dy4—S2vii75.09 (11)Dy7iii—S2—Dy2151.17 (18)
S4vii—Dy4—S2vii75.09 (11)Dy4v—S2—Dy2103.69 (13)
S5vii—Dy4—S12viii137.58 (12)Dy7—S2—Dy2iii151.17 (18)
S5viii—Dy4—S12viii82.10 (11)Dy7iii—S2—Dy2iii90.90 (5)
S4viii—Dy4—S12viii68.88 (12)Dy4v—S2—Dy2iii103.69 (13)
S4vii—Dy4—S12viii119.56 (13)Dy2—S2—Dy2iii78.91 (12)
S2vii—Dy4—S12viii138.40 (7)Dy1—S3—Dy1iii86.14 (13)
S5vii—Dy4—S12vii82.10 (11)Dy1—S3—Dy5iii151.58 (19)
S5viii—Dy4—S12vii137.58 (12)Dy1iii—S3—Dy5iii87.60 (5)
S4viii—Dy4—S12vii119.56 (13)Dy1—S3—Dy587.60 (5)
S4vii—Dy4—S12vii68.88 (12)Dy1iii—S3—Dy5151.58 (19)
S2vii—Dy4—S12vii138.40 (7)Dy5iii—S3—Dy584.86 (13)
S12viii—Dy4—S12vii79.43 (12)Dy1—S3—Dy6v102.89 (13)
S5vii—Dy4—Dy4iii133.25 (7)Dy1iii—S3—Dy6v102.89 (13)
S5viii—Dy4—Dy4iii46.75 (7)Dy5iii—S3—Dy6v105.53 (13)
S4viii—Dy4—Dy4iii48.09 (6)Dy5—S3—Dy6v105.53 (13)
S4vii—Dy4—Dy4iii131.91 (6)Dy4v—S4—Dy4vi83.83 (12)
S2vii—Dy4—Dy4iii90.0Dy4v—S4—Dy7104.18 (12)
S12viii—Dy4—Dy4iii50.28 (6)Dy4vi—S4—Dy7104.18 (12)
S12vii—Dy4—Dy4iii129.72 (6)Dy4v—S4—Dy8xi88.21 (5)
S5vii—Dy4—Dy4ii46.75 (7)Dy4vi—S4—Dy8xi148.43 (17)
S5viii—Dy4—Dy4ii133.25 (7)Dy7—S4—Dy8xi107.38 (12)
S4viii—Dy4—Dy4ii131.91 (6)Dy4v—S4—Dy8xii148.43 (17)
S4vii—Dy4—Dy4ii48.09 (6)Dy4vi—S4—Dy8xii88.21 (5)
S2vii—Dy4—Dy4ii90.0Dy7—S4—Dy8xii107.38 (12)
S12viii—Dy4—Dy4ii129.72 (6)Dy8xi—S4—Dy8xii82.77 (12)
S12vii—Dy4—Dy4ii50.28 (6)Dy4v—S5—Dy4vi86.51 (13)
Dy4iii—Dy4—Dy4ii180.00 (5)Dy4v—S5—Dy3vi159.03 (18)
S5vii—Dy4—Dy345.15 (7)Dy4vi—S5—Dy3vi89.79 (4)
S5viii—Dy4—Dy345.15 (7)Dy4v—S5—Dy3v89.79 (4)
S4viii—Dy4—Dy3132.57 (7)Dy4vi—S5—Dy3v159.03 (18)
S4vii—Dy4—Dy3132.57 (7)Dy3vi—S5—Dy3v86.32 (13)
S2vii—Dy4—Dy385.62 (10)Dy4v—S5—Dy2107.56 (12)
S12viii—Dy4—Dy3103.71 (10)Dy4vi—S5—Dy2107.56 (12)
S12vii—Dy4—Dy3103.71 (10)Dy3vi—S5—Dy293.24 (12)
Dy4iii—Dy4—Dy390.0Dy3v—S5—Dy293.24 (12)
Dy4ii—Dy4—Dy390.0Dy1iii—S6—Dy186.02 (13)
S5vii—Dy4—Dy8ix133.99 (7)Dy1iii—S6—Dy7iv153.67 (17)
S5viii—Dy4—Dy8ix133.99 (7)Dy1—S6—Dy7iv88.80 (5)
S4viii—Dy4—Dy8ix46.20 (7)Dy1iii—S6—Dy7xiii88.80 (5)
S4vii—Dy4—Dy8ix46.20 (7)Dy1—S6—Dy7xiii153.67 (17)
S2vii—Dy4—Dy8ix91.32 (10)Dy7iv—S6—Dy7xiii84.49 (13)
S12viii—Dy4—Dy8ix78.60 (10)Dy1iii—S6—Dy8100.99 (12)
S12vii—Dy4—Dy8ix78.60 (10)Dy1—S6—Dy8100.99 (12)
Dy4iii—Dy4—Dy8ix90.0Dy7iv—S6—Dy8105.34 (11)
Dy4ii—Dy4—Dy8ix90.0Dy7xiii—S6—Dy8105.34 (11)
Dy3—Dy4—Dy8ix176.94 (3)Dy5vii—S7—Dy5viii85.19 (13)
S7v—Dy5—S7vi85.19 (13)Dy5vii—S7—Dy8ii89.21 (5)
S7v—Dy5—S386.84 (11)Dy5viii—S7—Dy8ii152.1 (2)
S7vi—Dy5—S3149.10 (16)Dy5vii—S7—Dy8152.1 (2)
S7v—Dy5—S3ii149.10 (16)Dy5viii—S7—Dy889.21 (5)
S7vi—Dy5—S3ii86.84 (11)Dy8ii—S7—Dy883.07 (13)
S3—Dy5—S3ii84.86 (13)Dy5vii—S7—Dy2108.48 (14)
S7v—Dy5—S174.57 (12)Dy5viii—S7—Dy2108.48 (14)
S7vi—Dy5—S174.57 (12)Dy8ii—S7—Dy299.23 (13)
S3—Dy5—S174.54 (12)Dy8—S7—Dy299.23 (13)
S3ii—Dy5—S174.54 (12)Dy1—S8—Dy8ii108.55 (12)
S7v—Dy5—S12x118.62 (13)Dy1—S8—Dy8108.55 (12)
S7vi—Dy5—S12x67.02 (12)Dy8ii—S8—Dy887.33 (13)
S3—Dy5—S12x141.31 (14)Dy1—S8—Dy3v99.06 (12)
S3ii—Dy5—S12x85.06 (11)Dy8ii—S8—Dy3v152.05 (17)
S1—Dy5—S12x137.24 (8)Dy8—S8—Dy3v87.95 (5)
S7v—Dy5—S12i67.02 (12)Dy1—S8—Dy3vi99.06 (12)
S7vi—Dy5—S12i118.62 (13)Dy8ii—S8—Dy3vi87.95 (5)
S3—Dy5—S12i85.06 (11)Dy8—S8—Dy3vi152.05 (17)
S3ii—Dy5—S12i141.31 (14)Dy3v—S8—Dy3vi83.46 (11)
S1—Dy5—S12i137.24 (8)Sn1—S9—Sn1iii96.38 (16)
S12x—Dy5—S12i79.93 (13)Sn1—S9—Dy1xiv131.79 (8)
S7v—Dy5—S9i133.23 (9)Sn1iii—S9—Dy1xiv131.79 (8)
S7vi—Dy5—S9i133.23 (9)Sn1—S9—Dy5xiv96.74 (13)
S3—Dy5—S9i71.02 (11)Sn1iii—S9—Dy5xiv96.74 (13)
S3ii—Dy5—S9i71.02 (11)Dy1xiv—S9—Dy5xiv81.66 (13)
S1—Dy5—S9i132.68 (13)Sn1viii—S10—Sn1vii96.82 (16)
S12x—Dy5—S9i70.38 (11)Sn1viii—S10—Dy3131.34 (8)
S12i—Dy5—S9i70.38 (11)Sn1vii—S10—Dy3131.34 (8)
S7v—Dy5—Dy5ii132.60 (7)Sn1viii—S10—Dy696.03 (14)
S7vi—Dy5—Dy5ii47.40 (7)Sn1vii—S10—Dy696.03 (14)
S3—Dy5—Dy5ii132.43 (7)Dy3—S10—Dy686.55 (13)
S3ii—Dy5—Dy5ii47.57 (7)Dy6v—S11—Dy6vi85.99 (12)
S1—Dy5—Dy5ii90.0Dy6v—S11—Dy1105.23 (11)
S12x—Dy5—Dy5ii50.03 (6)Dy6vi—S11—Dy1105.23 (11)
S12i—Dy5—Dy5ii129.97 (6)Dy6v—S11—Dy3vi158.35 (16)
S9i—Dy5—Dy5ii90.0Dy6vi—S11—Dy3vi92.23 (4)
S7v—Dy5—Dy5iii47.40 (7)Dy1—S11—Dy3vi96.07 (11)
S7vi—Dy5—Dy5iii132.60 (7)Dy6v—S11—Dy3v92.23 (4)
S3—Dy5—Dy5iii47.57 (7)Dy6vi—S11—Dy3v158.35 (16)
S3ii—Dy5—Dy5iii132.43 (7)Dy1—S11—Dy3v96.07 (11)
S1—Dy5—Dy5iii90.0Dy3vi—S11—Dy3v81.52 (11)
S12x—Dy5—Dy5iii129.97 (6)Sn1—S12—Dy5xiv103.38 (14)
S12i—Dy5—Dy5iii50.03 (6)Sn1—S12—Dy5xv103.38 (14)
S9i—Dy5—Dy5iii90.0Dy5xiv—S12—Dy5xv79.93 (13)
Dy5ii—Dy5—Dy5iii180.0Sn1—S12—Dy4vi104.21 (14)
S7v—Dy5—Dy1132.63 (8)Dy5xiv—S12—Dy4vi152.42 (18)
S7vi—Dy5—Dy1132.63 (8)Dy5xv—S12—Dy4vi93.75 (5)
S3—Dy5—Dy145.84 (7)Sn1—S12—Dy4v104.21 (14)
S3ii—Dy5—Dy145.84 (7)Dy5xiv—S12—Dy4v93.75 (5)
S1—Dy5—Dy188.12 (9)Dy5xv—S12—Dy4v152.42 (18)
S12x—Dy5—Dy1104.13 (10)Dy4vi—S12—Dy4v79.43 (12)
S12i—Dy5—Dy1104.13 (10)Sn1—S13—Dy6vi102.09 (12)
S9i—Dy5—Dy144.56 (9)Sn1—S13—Dy6v102.09 (12)
Dy5ii—Dy5—Dy190.0Dy6vi—S13—Dy6v80.09 (11)
Dy5iii—Dy5—Dy190.0Sn1—S13—Dy7v105.50 (12)
S7v—Dy5—Dy8vi45.99 (8)Dy6vi—S13—Dy7v152.39 (16)
S7vi—Dy5—Dy8vi45.99 (8)Dy6v—S13—Dy7v93.35 (5)
S3—Dy5—Dy8vi132.78 (8)Sn1—S13—Dy7vi105.50 (12)
S3ii—Dy5—Dy8vi132.78 (8)Dy6vi—S13—Dy7vi93.35 (5)
S1—Dy5—Dy8vi88.11 (9)Dy6v—S13—Dy7vi152.39 (16)
S12x—Dy5—Dy8vi78.71 (9)Dy7v—S13—Dy7vi80.06 (11)
S12i—Dy5—Dy8vi78.71 (9)Dy2vii—O14—Dy2viii104.1 (3)
S9i—Dy5—Dy8vi139.21 (9)Dy2vii—O14—Dy3114.6 (2)
Dy5ii—Dy5—Dy8vi90.0Dy2viii—O14—Dy3114.6 (2)
Dy5iii—Dy5—Dy8vi90.0Dy2vii—O14—Dy8vii114.9 (2)
Dy1—Dy5—Dy8vi176.23 (4)Dy2viii—O14—Dy8vii114.9 (2)
S11vii—Dy6—S11viii85.99 (12)Dy3—O14—Dy8vii94.3 (2)
Symmetry codes: (i) x+1/2, y+3/2, z1/2; (ii) x1, y, z; (iii) x+1, y, z; (iv) x, y+1, z1/2; (v) x+1/2, y+1/2, z; (vi) x1/2, y+1/2, z; (vii) x1/2, y1/2, z; (viii) x+1/2, y1/2, z; (ix) x+1/2, y+1/2, z+1/2; (x) x1/2, y+3/2, z1/2; (xi) x+1, y+1, z+1/2; (xii) x, y+1, z+1/2; (xiii) x+1, y+1, z1/2; (xiv) x+1/2, y+3/2, z+1/2; (xv) x1/2, y+3/2, z+1/2.

Experimental details

Crystal data
Chemical formulaDy8SnS13.61O0.39
Mr1861.27
Crystal system, space groupOrthorhombic, Cmc21
Temperature (K)293
a, b, c (Å)3.7822 (8), 23.620 (5), 21.271 (4)
V3)1900.3 (7)
Z4
Radiation typeMo Kα
µ (mm1)33.80
Crystal size (mm)0.14 × 0.01 × 0.01
Data collection
DiffractometerKUMA KM-4 with CCD area-detector
Absorption correctionNumerical
(CrysAlis; Oxford Diffraction, 2007)
Tmin, Tmax0.104, 0.716
No. of measured, independent and
observed [I > 2σ(I)] reflections
11655, 2287, 1910
Rint0.049
(sin θ/λ)max1)0.633
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.026, 0.038, 0.89
No. of reflections2287
No. of parameters141
No. of restraints1
Δρmax, Δρmin (e Å3)3.05, 1.56
Absolute structureFlack (1983), 1089 Friedel pairs
Absolute structure parameter0.0 (2)

Computer programs: CrysAlis CCD (Oxford Diffraction, 2007), CrysAlis RED (Oxford Diffraction, 2007), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), DIAMOND (Brandenburg, 2005), publCIF (Westrip, 2007) and PLATON (Spek, 2003).

 

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