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Tricesium tantalum tetra­sulfide, Cs3TaS4, crystallizes in space group Pnma of the orthorhombic system. It is isostructural with K3VS4. In the asymmetric unit, the site symmetries of one of the Cs atoms, the Ta atom, and two of the S atoms are m. The structure consists of the packing of discrete Cs+ cations and nearly regular tetrahedral TaS43- anions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804029927/wm6040sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536804029927/wm6040Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 153 K
  • Mean [sigma](Ta-S) = 0.001 Å
  • R factor = 0.025
  • wR factor = 0.071
  • Data-to-parameter ratio = 33.7

checkCIF/PLATON results

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Computing details top

Data collection: SMART (Bruker, 2003); cell refinement: SAINT (Bruker, 2003); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2003); program(s) used to refine structure: SHELXL97 in SHELXTL; molecular graphics: XP in SHELXTL; software used to prepare material for publication: SHELXTL.

Tricesium tantalum tetrasulfide top
Crystal data top
Cs3TaS4F(000) = 1208
Mr = 707.92Dx = 4.144 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 5650 reflections
a = 9.9205 (8) Åθ = 2.7–28.8°
b = 11.507 (1) ŵ = 19.83 mm1
c = 9.9406 (9) ÅT = 153 K
V = 1134.77 (17) Å3Flat plate, colorless
Z = 40.43 × 0.12 × 0.05 mm
Data collection top
'Bruker SMART 1000 CCD'
diffractometer
1482 independent reflections
Radiation source: fine-focus sealed tube1462 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.046
0.3° ω scansθmax = 28.8°, θmin = 2.7°
Absorption correction: numerical
face indexed (SHELXTL, Sheldrick, 2003)'
h = 1313
Tmin = 0.037, Tmax = 0.396k = 1515
12415 measured reflectionsl = 1313
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) + (0.0478P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.071(Δ/σ)max = 0.002
S = 1.20Δρmax = 3.16 e Å3
1482 reflectionsΔρmin = 3.04 e Å3
44 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.00075 (13)
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*/Ueq
Cs10.04691 (2)0.540192 (18)0.29120 (2)0.01540 (12)
Cs20.14991 (3)0.25000.08566 (4)0.02268 (13)
Ta0.222204 (19)0.25000.51653 (2)0.01070 (11)
S10.33203 (9)0.08637 (9)0.45161 (11)0.0202 (2)
S20.01011 (13)0.25000.42884 (13)0.0143 (3)
S30.20718 (12)0.25000.74462 (13)0.0141 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cs10.01669 (18)0.01083 (17)0.01869 (18)0.00041 (7)0.00036 (8)0.00079 (8)
Cs20.0172 (2)0.0345 (2)0.0164 (2)0.0000.00236 (12)0.000
Ta0.01025 (16)0.01044 (16)0.01141 (16)0.0000.00022 (6)0.000
S10.0168 (5)0.0201 (5)0.0237 (5)0.0056 (4)0.0010 (4)0.0071 (4)
S20.0112 (5)0.0153 (6)0.0164 (6)0.0000.0014 (4)0.000
S30.0161 (6)0.0143 (6)0.0118 (6)0.0000.0001 (5)0.000
Geometric parameters (Å, º) top
Cs1—S3i3.4632 (9)Ta—S12.2691 (9)
Cs1—S3ii3.5085 (9)Ta—S32.2723 (14)
Cs1—S1iii3.5343 (10)Ta—S22.2775 (13)
Cs1—S1iv3.5588 (10)Ta—Cs1ii4.0754 (3)
Cs1—S1v3.6221 (11)Ta—Cs1x4.0755 (3)
Cs1—S23.6271 (6)Ta—Cs1xi4.3047 (3)
Cs1—S2ii3.7274 (11)Ta—Cs1xii4.3047 (3)
Cs1—Cs24.0459 (4)Ta—Cs2vii4.3628 (5)
Cs1—Taii4.0754 (3)Ta—Cs1iv4.3809 (4)
Cs1—Tai4.3046 (3)S1—Cs1xiii3.5342 (10)
Cs1—Cs1ii4.3537 (6)S1—Cs1iv3.5588 (10)
Cs1—Ta4.3809 (4)S1—Cs1xii3.6222 (11)
Cs2—S3vi3.4374 (14)S1—Cs2vii3.6914 (10)
Cs2—S2vii3.5763 (14)S1—Cs2xiv4.0975 (11)
Cs2—S23.6825 (14)S2—Cs2viii3.5764 (14)
Cs2—S1iii3.6915 (10)S2—Cs1iv3.6271 (6)
Cs2—S1viii3.6915 (10)S2—Cs1ii3.7274 (11)
Cs2—Cs1iv4.0459 (4)S2—Cs1x3.7275 (11)
Cs2—S1v4.0974 (11)S3—Cs2xv3.4374 (14)
Cs2—S1ix4.0975 (11)S3—Cs1xi3.4633 (9)
Cs2—Ta4.3428 (6)S3—Cs1xii3.4633 (9)
Cs2—Taviii4.3629 (5)S3—Cs1ii3.5085 (9)
Cs2—Cs1i4.8418 (4)S3—Cs1x3.5085 (9)
Ta—S1iv2.2690 (9)
S3i—Cs1—S3ii90.736 (8)Ta—S1—Cs1xiii145.67 (4)
S3i—Cs1—S1iii128.38 (3)Ta—S1—Cs1iv94.90 (3)
S3ii—Cs1—S1iii77.34 (2)Cs1xiii—S1—Cs1iv90.27 (2)
S3i—Cs1—S1iv77.60 (2)Ta—S1—Cs1xii90.91 (3)
S3ii—Cs1—S1iv153.91 (3)Cs1xiii—S1—Cs1xii112.09 (3)
S1iii—Cs1—S1iv128.08 (3)Cs1iv—S1—Cs1xii128.40 (3)
S3i—Cs1—S1v62.59 (3)Ta—S1—Cs2vii90.89 (3)
S3ii—Cs1—S1v92.45 (3)Cs1xiii—S1—Cs2vii68.063 (19)
S1iii—Cs1—S1v67.91 (3)Cs1iv—S1—Cs2vii147.43 (3)
S1iv—Cs1—S1v102.363 (15)Cs1xii—S1—Cs2vii83.40 (2)
S3i—Cs1—S2139.74 (3)Ta—S1—Cs2xiv135.43 (4)
S3ii—Cs1—S2126.83 (3)Cs1xiii—S1—Cs2xiv78.840 (19)
S1iii—Cs1—S279.49 (3)Cs1iv—S1—Cs2xiv78.11 (2)
S1iv—Cs1—S262.24 (2)Cs1xii—S1—Cs2xiv62.861 (18)
S1v—Cs1—S2121.33 (3)Cs2vii—S1—Cs2xiv118.50 (2)
S3i—Cs1—S2ii75.83 (3)Ta—S2—Cs2viii159.80 (5)
S3ii—Cs1—S2ii61.38 (3)Ta—S2—Cs192.95 (2)
S1iii—Cs1—S2ii133.26 (3)Cs2viii—S2—Cs194.90 (2)
S1iv—Cs1—S2ii92.93 (3)Ta—S2—Cs1iv92.95 (2)
S1v—Cs1—S2ii130.63 (2)Cs2viii—S2—Cs1iv94.90 (2)
S2—Cs1—S2ii107.420 (11)Cs1—S2—Cs1iv134.04 (4)
S3vi—Cs2—S2vii78.18 (3)Ta—S2—Cs290.38 (4)
S3vi—Cs2—S2167.39 (3)Cs2viii—S2—Cs2109.81 (3)
S2vii—Cs2—S2114.43 (3)Cs1—S2—Cs267.21 (2)
S3vi—Cs2—S1iii92.42 (3)Cs1iv—S2—Cs267.21 (2)
S2vii—Cs2—S1iii148.161 (17)Ta—S2—Cs1ii81.63 (3)
S2—Cs2—S1iii76.78 (2)Cs2viii—S2—Cs1ii83.02 (3)
S3vi—Cs2—S1viii92.42 (3)Cs1—S2—Cs1ii72.580 (10)
S2vii—Cs2—S1viii148.160 (17)Cs1iv—S2—Cs1ii153.28 (3)
S2—Cs2—S1viii76.78 (2)Cs2—S2—Cs1ii138.488 (16)
S1iii—Cs2—S1viii61.34 (3)Ta—S2—Cs1x81.63 (3)
S3vi—Cs2—S1v70.857 (15)Cs2viii—S2—Cs1x83.02 (3)
S2vii—Cs2—S1v86.745 (16)Cs1—S2—Cs1x153.28 (3)
S2—Cs2—S1v108.525 (15)Cs1iv—S2—Cs1x72.579 (10)
S1iii—Cs2—S1v61.50 (2)Cs2—S2—Cs1x138.487 (16)
S1viii—Cs2—S1v119.113 (16)Cs1ii—S2—Cs1x80.74 (3)
Cs1—Cs2—S1v52.815 (16)Ta—S3—Cs2xv174.24 (5)
Cs1iv—Cs2—S1v162.729 (16)Ta—S3—Cs1xi95.00 (3)
S3vi—Cs2—S1ix70.856 (15)Cs2xv—S3—Cs1xi89.12 (3)
S2vii—Cs2—S1ix86.744 (16)Ta—S3—Cs1xii95.00 (3)
S2—Cs2—S1ix108.525 (15)Cs2xv—S3—Cs1xii89.12 (3)
S1iii—Cs2—S1ix119.113 (16)Cs1xi—S3—Cs1xii88.39 (3)
S1viii—Cs2—S1ix61.50 (2)Ta—S3—Cs1ii86.90 (3)
Cs1—Cs2—S1ix162.729 (16)Cs2xv—S3—Cs1ii88.93 (3)
Cs1iv—Cs2—S1ix52.816 (16)Cs1xi—S3—Cs1ii92.291 (9)
S1v—Cs2—S1ix141.69 (3)Cs1xii—S3—Cs1ii177.92 (4)
S1iv—Ta—S1112.16 (5)Ta—S3—Cs1x86.90 (3)
S1iv—Ta—S3108.38 (3)Cs2xv—S3—Cs1x88.93 (3)
S1—Ta—S3108.38 (3)Cs1xi—S3—Cs1x177.92 (4)
S1iv—Ta—S2109.56 (3)Cs1xii—S3—Cs1x92.290 (9)
S1—Ta—S2109.56 (3)Cs1ii—S3—Cs1x86.96 (3)
S3—Ta—S2108.74 (4)
Symmetry codes: (i) x+1/2, y+1, z1/2; (ii) x, y+1, z+1; (iii) x1/2, y+1/2, z+1/2; (iv) x, y+1/2, z; (v) x+1/2, y+1/2, z1/2; (vi) x, y, z1; (vii) x+1/2, y, z+1/2; (viii) x1/2, y, z+1/2; (ix) x+1/2, y, z1/2; (x) x, y1/2, z+1; (xi) x+1/2, y+1, z+1/2; (xii) x+1/2, y1/2, z+1/2; (xiii) x+1/2, y+1/2, z+1/2; (xiv) x+1/2, y, z+1/2; (xv) x, y, z+1.
 

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