Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680702394X/zl2025sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S160053680702394X/zl2025Isup2.hkl |
CCDC reference: 650566
Key indicators
- Single-crystal X-ray study
- T = 293 K
- Mean (C-C) = 0.015 Å
- R factor = 0.025
- wR factor = 0.065
- Data-to-parameter ratio = 12.9
checkCIF/PLATON results
No syntax errors found
Alert level A PLAT112_ALERT_2_A ADDSYM Detects Additional (Pseudo) Symm. Elem... m
Author Response: ... I am sure that there is only pseudosymmetry. I tried a refinement in the centrosymmetric space group but this didn't work. There is strong disorder. |
Alert level B PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT110_ALERT_2_B ADDSYM Detects Potential Lattice Centering or Halving . ? PLAT115_ALERT_5_B ADDSYM Detects Noncrystallographic Inversion ... 80 PerFi
Alert level C PLAT222_ALERT_3_C Large Non-Solvent H Ueq(max)/Ueq(min) ... 3.08 Ratio PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C12 PLAT342_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 15 PLAT360_ALERT_2_C Short C(sp3)-C(sp3) Bond C1 - C2 ... 1.43 Ang.
Alert level G REFLT03_ALERT_4_G WARNING: Large fraction of Friedel related reflns may be needed to determine absolute structure From the CIF: _diffrn_reflns_theta_max 27.01 From the CIF: _reflns_number_total 3571 Count of symmetry unique reflns 3309 Completeness (_total/calc) 107.92% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 262 Fraction of Friedel pairs measured 0.079 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 PLAT794_ALERT_5_G Check Predicted Bond Valency for Sb1 (3) 5.84 PLAT794_ALERT_5_G Check Predicted Bond Valency for Sb2 (3) 6.04 PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
1 ALERT level A = In general: serious problem 38 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 6 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 40 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 3 ALERT type 5 Informative message, check
For structures of related compounds, see: Stähler & Bensch (2002); Graf & Schäfer (1976); Graf et al. (1969); Mereiter et al. (1979); Schimek et al. (1996); Bensch & Dürichen (1996); Schur et al. (1998); Schur & Bensch (2000); Schaefer et al. (2003); Jia et al. (2004); Jia, Zhao et al. (2005); Jia, Zhu et al. (2005); Stähler et al. (2002); Alyea et al. (1995).
A mixture of 0.5 mmol MnSb2S4, 0.5 mmol (NH4)2MoS4, 3 mmol S and 5 ml concentrated tris(2-aminoethyl)amine were heated at 413 K for 7 d followed by cooling to room temperature. The product was identified by X-ray powder diffraction and contained two different phases in approximately equivalent amount: red crystals of [Mn(tren)(trenH)]SbS4 (tren = tris(2-ethyl)amine)(Schaefer et al., 2003), and yellow crystals of the title compound.
All hydrogen atoms were positioned with idealized geometry (amine H atoms allowed to rotate but not to tip) and were refined with fixed isotropic displacement parameters (Uiso(H) = 1.2 Ueq(C)) or 1.5 Ueq(N)) using a riding model with d(C—H) = 0.97 Å and d(N—H) = 0.89 Å. In this structure a pseudo mirror plane and a pseudo center of symmetry are found, but refinement of the structure in the centrosymmetric space group Pnma was not successful and leads to pronounced disorder. The absolue structure was determined on the basis of 544 Friedel pairs.
During the last decade numerous thioantimonate(III) compounds were synthesized under solvothermal conditions. An intriguing observation is that in the overwhelming cases Sb(III)Sx (x = 3 - 6) are observed and the number of compounds containing Sb(V)S4 is comparably low. Some examples for thioantimonate(V) compounds are (C3H10N)[NiSbS4(C6H18N4)] (Stähler & Bensch, 2002), K3SbS4 (Graf & Schäfer, 1976), (NH4)3SbS4 (Graf et al., 1969), Na3SbS4 × 9 H2O (Mereiter et al., 1979), KAg2SbS4 (Schimek et al., 1996), Rb3SbS4 (Bensch & Dürichen, 1996), Cr(en)3SbS4 (Schur et al., 1998), [Ni(en)3]2SbS4NO3 (en = ethylenediamine) (Schur & Bensch, 2000), [Mn(C6H14N2)3]2[Mn(C6H14N2)2(SbS4)2] × 6 H2O and [Mn(tren)(trenH)]SbS4 (tren = tris(2-ethyl)amine)(Schaefer et al., 2003), [Ni(en)3(enH)]SbS4 (Jia et al., 2004), [Sm(en)4]SbS4 × 0.5 en (Jia, Zhu et al., 2005), [Ln(en)3(H2O)x(µ3 - xSbS4)] (Ln = La, x = 0; Ln = Nd, x = 1) and [Ln(en)4]SbS4 × 0.5en (Ln = Eu, Dy, Yb) (Jia, Zhao et al., 2005. There is also one example where Sb(III) and Sb(V) species coexist in a common anion, i.e., in [Ni(dien)2]2Sb4S9 (R. Stähler et al., 2002). During our ongoing work in the field of solvothermal syntheses of new thioantimonates the title compound was prepared. In the crystal structure of (C6H21N4)SbS4, discrete tetrathioantimonate anions and tris(2-ethylammonium)amine cations coexist. There are two crystallographically independent cations and anions in the asymmetric unit, all of them located in general positions (Fig. 1). The tetrathioantimonate anions show slightly distorted tetrahedral geometry (Table 1), but the values are in the range reported for the above mentioned compounds containing this anion. The tetrathioantimonate anions and the organic cations are arranged in layers, which are parallel to the a b plane (Fig. 2). These layers are interconnected by intermolecular N—H···S hydrogen bonding (Table 2). The Sb(1)S4 anion has two such S···H contacts to the first and four contacts to the second crystallographically independent cation, whereas for the Sb(2)S4 anion it is the other way around.
For structures of related compounds, see: Stähler & Bensch (2002); Graf & Schäfer (1976); Graf et al. (1969); Mereiter et al. (1979); Schimek et al. (1996); Bensch & Dürichen (1996); Schur et al. (1998); Schur & Bensch (2000); Schaefer et al. (2003); Jia et al. (2004); Jia, Zhao et al. (2005); Jia, Zhu et al. (2005); Stähler et al. (2002); Alyea et al. (1995).
Data collection: DIF4 (Stoe & Cie, 1992); cell refinement: DIF4; data reduction: REDU4 (Stoe & Cie, 1992); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL (Bruker, 1998) and Diamond (Brandenburg, 1999); software used to prepare material for publication: CIFTAB in SHELXL97.
(C6H21N4)[SbS4] | F(000) = 1600 |
Mr = 399.26 | Dx = 1.828 Mg m−3 |
Orthorhombic, Pca21 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2c -2ac | Cell parameters from 132 reflections |
a = 19.7872 (13) Å | θ = 13–20° |
b = 10.8571 (10) Å | µ = 2.46 mm−1 |
c = 13.5055 (8) Å | T = 293 K |
V = 2901.4 (4) Å3 | Block, orange |
Z = 8 | 0.2 × 0.1 × 0.1 mm |
Stoe AEDII diffractometer | 2898 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.023 |
Graphite monochromator | θmax = 27.0°, θmin = 1.9° |
Phi scans | h = −25→14 |
Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1998) | k = −13→1 |
Tmin = 0.738, Tmax = 0.772 | l = −17→1 |
6750 measured reflections | 4 standard reflections every 2 h min |
3571 independent reflections | intensity decay: none |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.025 | H-atom parameters constrained |
wR(F2) = 0.065 | w = 1/[σ2(Fo2) + (0.0261P)2 + 3.7053P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max = 0.001 |
3571 reflections | Δρmax = 0.88 e Å−3 |
277 parameters | Δρmin = −0.55 e Å−3 |
1 restraint | Absolute structure: Flack (1983), 544 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.04 (5) |
(C6H21N4)[SbS4] | V = 2901.4 (4) Å3 |
Mr = 399.26 | Z = 8 |
Orthorhombic, Pca21 | Mo Kα radiation |
a = 19.7872 (13) Å | µ = 2.46 mm−1 |
b = 10.8571 (10) Å | T = 293 K |
c = 13.5055 (8) Å | 0.2 × 0.1 × 0.1 mm |
Stoe AEDII diffractometer | 2898 reflections with I > 2σ(I) |
Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1998) | Rint = 0.023 |
Tmin = 0.738, Tmax = 0.772 | 4 standard reflections every 2 h min |
6750 measured reflections | intensity decay: none |
3571 independent reflections |
R[F2 > 2σ(F2)] = 0.025 | H-atom parameters constrained |
wR(F2) = 0.065 | Δρmax = 0.88 e Å−3 |
S = 1.03 | Δρmin = −0.55 e Å−3 |
3571 reflections | Absolute structure: Flack (1983), 544 Friedel pairs |
277 parameters | Absolute structure parameter: 0.04 (5) |
1 restraint |
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 > σ(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. |
x | y | z | Uiso*/Ueq | ||
Sb1 | 0.72266 (4) | 0.49351 (4) | 0.64960 (3) | 0.0204 (2) | |
S1 | 0.75959 (10) | 0.6794 (2) | 0.7180 (2) | 0.0305 (5) | |
S2 | 0.7352 (2) | 0.50371 (16) | 0.4781 (4) | 0.0289 (9) | |
S3 | 0.78342 (12) | 0.3293 (3) | 0.7154 (3) | 0.0388 (6) | |
S4 | 0.60811 (12) | 0.4725 (2) | 0.6887 (3) | 0.0318 (5) | |
Sb2 | 0.52627 (4) | 0.00637 (4) | 0.83030 (3) | 0.0196 (2) | |
S5 | 0.48991 (11) | −0.1799 (2) | 0.7655 (3) | 0.0338 (5) | |
S6 | 0.5162 (2) | −0.00107 (17) | 1.0015 (4) | 0.0319 (10) | |
S7 | 0.46215 (11) | 0.1664 (2) | 0.7672 (2) | 0.0366 (6) | |
S8 | 0.64036 (11) | 0.0315 (2) | 0.7919 (3) | 0.0338 (5) | |
N1 | 0.2974 (6) | −0.0028 (5) | 1.0178 (10) | 0.023 (3) | |
C1 | 0.2972 (4) | 0.1250 (6) | 0.9832 (6) | 0.0345 (17) | |
H1A | 0.2898 | 0.1259 | 0.9122 | 0.041* | |
H1B | 0.2599 | 0.1684 | 1.0140 | 0.041* | |
C2 | 0.3586 (5) | 0.1882 (9) | 1.0049 (9) | 0.034 (3) | |
H2A | 0.3548 | 0.2732 | 0.9833 | 0.040* | |
H2B | 0.3954 | 0.1503 | 0.9686 | 0.040* | |
N2 | 0.3745 (4) | 0.1851 (7) | 1.1154 (6) | 0.0354 (18) | |
H1N | 0.3463 | 0.2350 | 1.1475 | 0.053* | |
H2N | 0.4169 | 0.2099 | 1.1252 | 0.053* | |
H3N | 0.3697 | 0.1086 | 1.1379 | 0.053* | |
C3 | 0.3304 (4) | −0.0849 (7) | 0.9525 (7) | 0.0362 (18) | |
H3A | 0.3690 | −0.0425 | 0.9242 | 0.043* | |
H3B | 0.2997 | −0.1038 | 0.8987 | 0.043* | |
C4 | 0.3538 (5) | −0.1994 (9) | 0.9943 (10) | 0.035 (3) | |
H4A | 0.3803 | −0.2422 | 0.9446 | 0.042* | |
H4B | 0.3148 | −0.2502 | 1.0091 | 0.042* | |
N3 | 0.3965 (4) | −0.1871 (7) | 1.0885 (7) | 0.039 (2) | |
H4N | 0.4338 | −0.1444 | 1.0751 | 0.059* | |
H5N | 0.4078 | −0.2617 | 1.1102 | 0.059* | |
H6N | 0.3727 | −0.1482 | 1.1348 | 0.059* | |
C5 | 0.2287 (4) | −0.0471 (7) | 1.0443 (6) | 0.0316 (16) | |
H5A | 0.1979 | −0.0278 | 0.9905 | 0.038* | |
H5B | 0.2299 | −0.1359 | 1.0515 | 0.038* | |
C6 | 0.2022 (8) | 0.0076 (8) | 1.1366 (16) | 0.045 (4) | |
H6A | 0.2329 | −0.0116 | 1.1904 | 0.054* | |
H6B | 0.2010 | 0.0964 | 1.1294 | 0.054* | |
N4 | 0.1343 (4) | −0.0365 (7) | 1.1625 (8) | 0.0404 (17) | |
H7N | 0.1091 | −0.0411 | 1.1080 | 0.061* | |
H8N | 0.1153 | 0.0156 | 1.2051 | 0.061* | |
H9N | 0.1373 | −0.1108 | 1.1901 | 0.061* | |
N11 | 0.5448 (7) | 0.5007 (4) | 0.9564 (11) | 0.024 (3) | |
C11 | 0.4766 (4) | 0.4589 (7) | 0.9377 (6) | 0.0307 (15) | |
H11A | 0.4466 | 0.4905 | 0.9885 | 0.037* | |
H11B | 0.4750 | 0.3696 | 0.9399 | 0.037* | |
C12 | 0.4534 (6) | 0.5041 (5) | 0.8357 (12) | 0.021 (2) | |
H12A | 0.4578 | 0.5930 | 0.8322 | 0.025* | |
H12B | 0.4818 | 0.4683 | 0.7847 | 0.025* | |
N12 | 0.3826 (4) | 0.4685 (7) | 0.8190 (8) | 0.0431 (18) | |
H11N | 0.3811 | 0.3936 | 0.7924 | 0.065* | |
H12N | 0.3632 | 0.5222 | 0.7780 | 0.065* | |
H13N | 0.3605 | 0.4683 | 0.8764 | 0.065* | |
C13 | 0.5806 (4) | 0.4188 (7) | 1.0288 (6) | 0.0324 (17) | |
H13A | 0.5505 | 0.3994 | 1.0833 | 0.039* | |
H13B | 0.6195 | 0.4617 | 1.0555 | 0.039* | |
C14 | 0.6045 (5) | 0.2953 (9) | 0.9772 (11) | 0.037 (3) | |
H14A | 0.6290 | 0.2453 | 1.0248 | 0.044* | |
H14B | 0.5653 | 0.2490 | 0.9556 | 0.044* | |
N13 | 0.6473 (3) | 0.3202 (7) | 0.8936 (6) | 0.0348 (18) | |
H14N | 0.6240 | 0.3614 | 0.8480 | 0.052* | |
H15N | 0.6619 | 0.2495 | 0.8681 | 0.052* | |
H16N | 0.6825 | 0.3653 | 0.9130 | 0.052* | |
C15 | 0.5440 (4) | 0.6289 (6) | 0.9983 (6) | 0.0311 (16) | |
H15A | 0.5366 | 0.6247 | 1.0692 | 0.037* | |
H15B | 0.5069 | 0.6747 | 0.9692 | 0.037* | |
C16 | 0.6113 (4) | 0.6975 (10) | 0.9776 (10) | 0.032 (3) | |
H16A | 0.6069 | 0.7840 | 0.9942 | 0.039* | |
H16B | 0.6474 | 0.6626 | 1.0172 | 0.039* | |
N14 | 0.6263 (4) | 0.6837 (8) | 0.8743 (7) | 0.051 (2) | |
H17N | 0.6168 | 0.6071 | 0.8553 | 0.077* | |
H18N | 0.6699 | 0.6991 | 0.8639 | 0.077* | |
H19N | 0.6014 | 0.7365 | 0.8394 | 0.077* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Sb1 | 0.0172 (4) | 0.0241 (4) | 0.0197 (5) | 0.00031 (15) | 0.0006 (4) | −0.0019 (3) |
S1 | 0.0332 (10) | 0.0250 (9) | 0.0333 (11) | −0.0025 (9) | −0.0050 (12) | −0.0036 (9) |
S2 | 0.0218 (15) | 0.042 (2) | 0.023 (2) | 0.0020 (7) | 0.0040 (17) | 0.0018 (7) |
S3 | 0.0500 (13) | 0.0341 (11) | 0.0321 (12) | 0.0173 (10) | −0.0011 (14) | 0.0031 (10) |
S4 | 0.0169 (10) | 0.0494 (9) | 0.0290 (12) | −0.0009 (10) | 0.0043 (8) | −0.0011 (14) |
Sb2 | 0.0160 (4) | 0.0236 (4) | 0.0192 (5) | −0.00037 (14) | −0.0011 (4) | 0.0003 (3) |
S5 | 0.0403 (12) | 0.0253 (9) | 0.0357 (12) | −0.0075 (10) | −0.0061 (13) | −0.0007 (10) |
S6 | 0.0282 (17) | 0.050 (2) | 0.017 (2) | −0.0088 (8) | −0.0049 (17) | 0.0021 (7) |
S7 | 0.0477 (12) | 0.0282 (10) | 0.0340 (12) | 0.0110 (10) | −0.0064 (15) | −0.0007 (9) |
S8 | 0.0183 (10) | 0.0532 (10) | 0.0298 (12) | −0.0053 (11) | 0.0017 (9) | −0.0123 (14) |
N1 | 0.008 (4) | 0.041 (6) | 0.020 (6) | 0.000 (2) | −0.004 (4) | 0.000 (2) |
C1 | 0.038 (4) | 0.038 (4) | 0.028 (4) | −0.008 (4) | −0.009 (4) | 0.014 (3) |
C2 | 0.045 (5) | 0.019 (4) | 0.036 (6) | 0.004 (4) | 0.021 (5) | 0.011 (4) |
N2 | 0.039 (4) | 0.028 (3) | 0.039 (5) | 0.001 (3) | −0.006 (3) | −0.001 (3) |
C3 | 0.027 (4) | 0.048 (5) | 0.033 (5) | 0.003 (3) | 0.003 (4) | −0.008 (4) |
C4 | 0.041 (5) | 0.029 (5) | 0.034 (6) | 0.001 (4) | 0.002 (5) | −0.008 (4) |
N3 | 0.043 (4) | 0.024 (3) | 0.051 (5) | 0.008 (3) | −0.007 (4) | −0.001 (3) |
C5 | 0.023 (4) | 0.042 (4) | 0.030 (4) | −0.012 (4) | 0.000 (4) | −0.004 (4) |
C6 | 0.020 (6) | 0.069 (9) | 0.047 (10) | −0.004 (4) | −0.001 (7) | −0.006 (5) |
N4 | 0.029 (4) | 0.063 (4) | 0.029 (4) | −0.005 (4) | 0.000 (3) | 0.004 (5) |
N11 | 0.028 (5) | 0.017 (5) | 0.029 (6) | 0.0012 (19) | −0.012 (5) | −0.001 (2) |
C11 | 0.020 (4) | 0.045 (4) | 0.028 (4) | 0.000 (4) | −0.001 (3) | 0.000 (4) |
C12 | 0.018 (5) | 0.025 (4) | 0.019 (5) | −0.005 (2) | −0.007 (5) | 0.006 (3) |
N12 | 0.020 (3) | 0.083 (4) | 0.027 (4) | −0.009 (4) | −0.006 (3) | 0.003 (5) |
C13 | 0.036 (4) | 0.039 (4) | 0.022 (4) | −0.003 (3) | −0.004 (4) | 0.000 (3) |
C14 | 0.037 (5) | 0.023 (5) | 0.051 (7) | 0.001 (4) | −0.003 (5) | 0.006 (4) |
N13 | 0.037 (4) | 0.033 (3) | 0.035 (4) | 0.000 (3) | −0.010 (3) | −0.007 (3) |
C15 | 0.024 (4) | 0.038 (4) | 0.031 (4) | 0.011 (3) | −0.007 (3) | −0.006 (3) |
C16 | 0.018 (4) | 0.037 (5) | 0.042 (7) | 0.000 (4) | −0.005 (4) | −0.001 (5) |
N14 | 0.050 (5) | 0.036 (4) | 0.068 (6) | 0.000 (4) | 0.024 (4) | −0.001 (4) |
Sb1—S3 | 2.326 (3) | C6—H6B | 0.9700 |
Sb1—S2 | 2.333 (5) | N4—H7N | 0.8900 |
Sb1—S1 | 2.337 (3) | N4—H8N | 0.8900 |
Sb1—S4 | 2.338 (3) | N4—H9N | 0.8900 |
Sb2—S7 | 2.314 (3) | N11—C11 | 1.445 (14) |
Sb2—S5 | 2.319 (3) | N11—C13 | 1.499 (13) |
Sb2—S6 | 2.323 (5) | N11—C15 | 1.503 (9) |
Sb2—S8 | 2.332 (3) | C11—C12 | 1.532 (17) |
N1—C3 | 1.414 (13) | C11—H11A | 0.9700 |
N1—C1 | 1.463 (9) | C11—H11B | 0.9700 |
N1—C5 | 1.486 (13) | C12—N12 | 1.472 (13) |
C1—C2 | 1.427 (13) | C12—H12A | 0.9700 |
C1—H1A | 0.9700 | C12—H12B | 0.9700 |
C1—H1B | 0.9700 | N12—H11N | 0.8900 |
C2—N2 | 1.525 (14) | N12—H12N | 0.8900 |
C2—H2A | 0.9700 | N12—H13N | 0.8900 |
C2—H2B | 0.9700 | C13—C14 | 1.583 (12) |
N2—H1N | 0.8900 | C13—H13A | 0.9700 |
N2—H2N | 0.8900 | C13—H13B | 0.9700 |
N2—H3N | 0.8900 | C14—N13 | 1.437 (15) |
C3—C4 | 1.441 (13) | C14—H14A | 0.9700 |
C3—H3A | 0.9700 | C14—H14B | 0.9700 |
C3—H3B | 0.9700 | N13—H14N | 0.8900 |
C4—N3 | 1.534 (15) | N13—H15N | 0.8900 |
C4—H4A | 0.9700 | N13—H16N | 0.8900 |
C4—H4B | 0.9700 | C15—C16 | 1.551 (12) |
N3—H4N | 0.8900 | C15—H15A | 0.9700 |
N3—H5N | 0.8900 | C15—H15B | 0.9700 |
N3—H6N | 0.8900 | C16—N14 | 1.434 (16) |
C5—C6 | 1.48 (2) | C16—H16A | 0.9700 |
C5—H5A | 0.9700 | C16—H16B | 0.9700 |
C5—H5B | 0.9700 | N14—H17N | 0.8900 |
C6—N4 | 1.469 (16) | N14—H18N | 0.8900 |
C6—H6A | 0.9700 | N14—H19N | 0.8900 |
S3—Sb1—S2 | 111.14 (11) | C6—N4—H7N | 109.5 |
S3—Sb1—S1 | 110.43 (13) | C6—N4—H8N | 109.5 |
S2—Sb1—S1 | 108.56 (10) | H7N—N4—H8N | 109.5 |
S3—Sb1—S4 | 109.88 (11) | C6—N4—H9N | 109.5 |
S2—Sb1—S4 | 109.39 (14) | H7N—N4—H9N | 109.5 |
S1—Sb1—S4 | 107.34 (10) | H8N—N4—H9N | 109.5 |
S7—Sb2—S5 | 110.24 (12) | C11—N11—C13 | 111.6 (7) |
S7—Sb2—S6 | 110.23 (12) | C11—N11—C15 | 110.3 (9) |
S5—Sb2—S6 | 108.60 (11) | C13—N11—C15 | 107.9 (9) |
S7—Sb2—S8 | 111.17 (11) | N11—C11—C12 | 109.6 (9) |
S5—Sb2—S8 | 108.58 (10) | N11—C11—H11A | 109.8 |
S6—Sb2—S8 | 107.95 (14) | C12—C11—H11A | 109.8 |
C3—N1—C1 | 113.5 (10) | N11—C11—H11B | 109.8 |
C3—N1—C5 | 111.7 (7) | C12—C11—H11B | 109.8 |
C1—N1—C5 | 112.4 (8) | H11A—C11—H11B | 108.2 |
C2—C1—N1 | 112.9 (8) | N12—C12—C11 | 109.8 (10) |
C2—C1—H1A | 109.0 | N12—C12—H12A | 109.7 |
N1—C1—H1A | 109.0 | C11—C12—H12A | 109.7 |
C2—C1—H1B | 109.0 | N12—C12—H12B | 109.7 |
N1—C1—H1B | 109.0 | C11—C12—H12B | 109.7 |
H1A—C1—H1B | 107.8 | H12A—C12—H12B | 108.2 |
C1—C2—N2 | 111.5 (8) | C12—N12—H11N | 109.5 |
C1—C2—H2A | 109.3 | C12—N12—H12N | 109.5 |
N2—C2—H2A | 109.3 | H11N—N12—H12N | 109.5 |
C1—C2—H2B | 109.3 | C12—N12—H13N | 109.5 |
N2—C2—H2B | 109.3 | H11N—N12—H13N | 109.5 |
H2A—C2—H2B | 108.0 | H12N—N12—H13N | 109.5 |
C2—N2—H1N | 109.5 | N11—C13—C14 | 110.9 (8) |
C2—N2—H2N | 109.5 | N11—C13—H13A | 109.5 |
H1N—N2—H2N | 109.5 | C14—C13—H13A | 109.5 |
C2—N2—H3N | 109.5 | N11—C13—H13B | 109.5 |
H1N—N2—H3N | 109.5 | C14—C13—H13B | 109.5 |
H2N—N2—H3N | 109.5 | H13A—C13—H13B | 108.1 |
N1—C3—C4 | 116.6 (9) | N13—C14—C13 | 111.2 (7) |
N1—C3—H3A | 108.1 | N13—C14—H14A | 109.4 |
C4—C3—H3A | 108.1 | C13—C14—H14A | 109.4 |
N1—C3—H3B | 108.1 | N13—C14—H14B | 109.4 |
C4—C3—H3B | 108.1 | C13—C14—H14B | 109.4 |
H3A—C3—H3B | 107.3 | H14A—C14—H14B | 108.0 |
C3—C4—N3 | 115.2 (8) | C14—N13—H14N | 109.5 |
C3—C4—H4A | 108.5 | C14—N13—H15N | 109.5 |
N3—C4—H4A | 108.5 | H14N—N13—H15N | 109.5 |
C3—C4—H4B | 108.5 | C14—N13—H16N | 109.5 |
N3—C4—H4B | 108.5 | H14N—N13—H16N | 109.5 |
H4A—C4—H4B | 107.5 | H15N—N13—H16N | 109.5 |
C4—N3—H4N | 109.5 | N11—C15—C16 | 111.6 (8) |
C4—N3—H5N | 109.5 | N11—C15—H15A | 109.3 |
H4N—N3—H5N | 109.5 | C16—C15—H15A | 109.3 |
C4—N3—H6N | 109.5 | N11—C15—H15B | 109.3 |
H4N—N3—H6N | 109.5 | C16—C15—H15B | 109.3 |
H5N—N3—H6N | 109.5 | H15A—C15—H15B | 108.0 |
C6—C5—N1 | 113.4 (8) | N14—C16—C15 | 107.6 (9) |
C6—C5—H5A | 108.9 | N14—C16—H16A | 110.2 |
N1—C5—H5A | 108.9 | C15—C16—H16A | 110.2 |
C6—C5—H5B | 108.9 | N14—C16—H16B | 110.2 |
N1—C5—H5B | 108.9 | C15—C16—H16B | 110.2 |
H5A—C5—H5B | 107.7 | H16A—C16—H16B | 108.5 |
N4—C6—C5 | 113.2 (11) | C16—N14—H17N | 109.5 |
N4—C6—H6A | 108.9 | C16—N14—H18N | 109.5 |
C5—C6—H6A | 108.9 | H17N—N14—H18N | 109.5 |
N4—C6—H6B | 108.9 | C16—N14—H19N | 109.5 |
C5—C6—H6B | 108.9 | H17N—N14—H19N | 109.5 |
H6A—C6—H6B | 107.7 | H18N—N14—H19N | 109.5 |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H1N···S1i | 0.89 | 2.48 | 3.336 (7) | 161 |
N3—H4N···S6 | 0.89 | 2.46 | 3.327 (9) | 164 |
N3—H5N···S4ii | 0.89 | 2.54 | 3.383 (8) | 158 |
N3—H6N···S8ii | 0.89 | 2.48 | 3.307 (9) | 154 |
N4—H7N···S6iii | 0.89 | 2.38 | 3.217 (10) | 157 |
N4—H8N···S7iv | 0.89 | 2.39 | 3.240 (9) | 159 |
N12—H12N···S3v | 0.89 | 2.41 | 3.259 (9) | 160 |
N12—H13N···S2i | 0.89 | 2.36 | 3.184 (10) | 154 |
N13—H14N···S4 | 0.89 | 2.49 | 3.316 (8) | 155 |
N13—H15N···S8 | 0.89 | 2.62 | 3.425 (8) | 152 |
N13—H16N···S2vi | 0.89 | 2.38 | 3.267 (8) | 172 |
N14—H19N···S5vii | 0.89 | 2.59 | 3.410 (9) | 155 |
Symmetry codes: (i) −x+1, −y+1, z+1/2; (ii) −x+1, −y, z+1/2; (iii) x−1/2, −y, z; (iv) −x+1/2, y, z+1/2; (v) x−1/2, −y+1, z; (vi) −x+3/2, y, z+1/2; (vii) x, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | (C6H21N4)[SbS4] |
Mr | 399.26 |
Crystal system, space group | Orthorhombic, Pca21 |
Temperature (K) | 293 |
a, b, c (Å) | 19.7872 (13), 10.8571 (10), 13.5055 (8) |
V (Å3) | 2901.4 (4) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 2.46 |
Crystal size (mm) | 0.2 × 0.1 × 0.1 |
Data collection | |
Diffractometer | Stoe AEDII |
Absorption correction | Numerical (X-SHAPE; Stoe & Cie, 1998) |
Tmin, Tmax | 0.738, 0.772 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6750, 3571, 2898 |
Rint | 0.023 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.025, 0.065, 1.03 |
No. of reflections | 3571 |
No. of parameters | 277 |
No. of restraints | 1 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.88, −0.55 |
Absolute structure | Flack (1983), 544 Friedel pairs |
Absolute structure parameter | 0.04 (5) |
Computer programs: DIF4 (Stoe & Cie, 1992), DIF4, REDU4 (Stoe & Cie, 1992), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), XP in SHELXTL (Bruker, 1998) and Diamond (Brandenburg, 1999), CIFTAB in SHELXL97.
Sb1—S3 | 2.326 (3) | Sb2—S7 | 2.314 (3) |
Sb1—S2 | 2.333 (5) | Sb2—S5 | 2.319 (3) |
Sb1—S1 | 2.337 (3) | Sb2—S6 | 2.323 (5) |
Sb1—S4 | 2.338 (3) | Sb2—S8 | 2.332 (3) |
S3—Sb1—S2 | 111.14 (11) | S7—Sb2—S5 | 110.24 (12) |
S3—Sb1—S1 | 110.43 (13) | S7—Sb2—S6 | 110.23 (12) |
S2—Sb1—S1 | 108.56 (10) | S5—Sb2—S6 | 108.60 (11) |
S3—Sb1—S4 | 109.88 (11) | S7—Sb2—S8 | 111.17 (11) |
S2—Sb1—S4 | 109.39 (14) | S5—Sb2—S8 | 108.58 (10) |
S1—Sb1—S4 | 107.34 (10) | S6—Sb2—S8 | 107.95 (14) |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H1N···S1i | 0.89 | 2.48 | 3.336 (7) | 160.7 |
N3—H4N···S6 | 0.89 | 2.46 | 3.327 (9) | 163.8 |
N3—H5N···S4ii | 0.89 | 2.54 | 3.383 (8) | 157.8 |
N3—H6N···S8ii | 0.89 | 2.48 | 3.307 (9) | 153.9 |
N4—H7N···S6iii | 0.89 | 2.38 | 3.217 (10) | 157.2 |
N4—H8N···S7iv | 0.89 | 2.39 | 3.240 (9) | 158.7 |
N12—H12N···S3v | 0.89 | 2.41 | 3.259 (9) | 159.7 |
N12—H13N···S2i | 0.89 | 2.36 | 3.184 (10) | 154.2 |
N13—H14N···S4 | 0.89 | 2.49 | 3.316 (8) | 155.2 |
N13—H15N···S8 | 0.89 | 2.62 | 3.425 (8) | 151.6 |
N13—H16N···S2vi | 0.89 | 2.38 | 3.267 (8) | 171.5 |
N14—H19N···S5vii | 0.89 | 2.59 | 3.410 (9) | 154.5 |
Symmetry codes: (i) −x+1, −y+1, z+1/2; (ii) −x+1, −y, z+1/2; (iii) x−1/2, −y, z; (iv) −x+1/2, y, z+1/2; (v) x−1/2, −y+1, z; (vi) −x+3/2, y, z+1/2; (vii) x, y+1, z. |
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During the last decade numerous thioantimonate(III) compounds were synthesized under solvothermal conditions. An intriguing observation is that in the overwhelming cases Sb(III)Sx (x = 3 - 6) are observed and the number of compounds containing Sb(V)S4 is comparably low. Some examples for thioantimonate(V) compounds are (C3H10N)[NiSbS4(C6H18N4)] (Stähler & Bensch, 2002), K3SbS4 (Graf & Schäfer, 1976), (NH4)3SbS4 (Graf et al., 1969), Na3SbS4 × 9 H2O (Mereiter et al., 1979), KAg2SbS4 (Schimek et al., 1996), Rb3SbS4 (Bensch & Dürichen, 1996), Cr(en)3SbS4 (Schur et al., 1998), [Ni(en)3]2SbS4NO3 (en = ethylenediamine) (Schur & Bensch, 2000), [Mn(C6H14N2)3]2[Mn(C6H14N2)2(SbS4)2] × 6 H2O and [Mn(tren)(trenH)]SbS4 (tren = tris(2-ethyl)amine)(Schaefer et al., 2003), [Ni(en)3(enH)]SbS4 (Jia et al., 2004), [Sm(en)4]SbS4 × 0.5 en (Jia, Zhu et al., 2005), [Ln(en)3(H2O)x(µ3 - xSbS4)] (Ln = La, x = 0; Ln = Nd, x = 1) and [Ln(en)4]SbS4 × 0.5en (Ln = Eu, Dy, Yb) (Jia, Zhao et al., 2005. There is also one example where Sb(III) and Sb(V) species coexist in a common anion, i.e., in [Ni(dien)2]2Sb4S9 (R. Stähler et al., 2002). During our ongoing work in the field of solvothermal syntheses of new thioantimonates the title compound was prepared. In the crystal structure of (C6H21N4)SbS4, discrete tetrathioantimonate anions and tris(2-ethylammonium)amine cations coexist. There are two crystallographically independent cations and anions in the asymmetric unit, all of them located in general positions (Fig. 1). The tetrathioantimonate anions show slightly distorted tetrahedral geometry (Table 1), but the values are in the range reported for the above mentioned compounds containing this anion. The tetrathioantimonate anions and the organic cations are arranged in layers, which are parallel to the a b plane (Fig. 2). These layers are interconnected by intermolecular N—H···S hydrogen bonding (Table 2). The Sb(1)S4 anion has two such S···H contacts to the first and four contacts to the second crystallographically independent cation, whereas for the Sb(2)S4 anion it is the other way around.