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The crystal structure of the title compound, (NH4)3[Sb2I9], which crystallizes in the monoclinic space group P21/n, resembles that of hexagonal Cs3[Sb2I9], which crystallizes in space group P\overline 3m1. The title compound consists of double layers parallel to (001). Each layer is made up of distorted corner-sharing SbI6 octahedra. One-third of the ammonium cations reside within six-membered rings formed by corner-sharing SbI6 octahedra within the layers. The other ammonium cations are situated within three-membered rings built from corner-sharing SbI6 octahedra near the edges of the layers.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805011098/wm6059sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805011098/wm6059Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 223 K
  • Mean [sigma](I-Sb) = 0.001 Å
  • H-atom completeness 1%
  • R factor = 0.041
  • wR factor = 0.089
  • Data-to-parameter ratio = 46.8

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT041_ALERT_1_C Calc. and Rep. SumFormula Strings Differ .... ? PLAT068_ALERT_1_C Reported F000 Differs from Calcd (or Missing)... ? PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for I5
Alert level G FORMU01_ALERT_2_G There is a discrepancy between the atom counts in the _chemical_formula_sum and the formula from the _atom_site* data. Atom count from _chemical_formula_sum:H12 I9 N3 Sb2 Atom count from the _atom_site data: I9 N3 Sb2 CELLZ01_ALERT_1_G Difference between formula and atom_site contents detected. CELLZ01_ALERT_1_G WARNING: H atoms missing from atom site list. Is this intentional? From the CIF: _cell_formula_units_Z 4 From the CIF: _chemical_formula_sum H12 I9 N3 Sb2 TEST: Compare cell contents of formula and atom_site data atom Z*formula cif sites diff H 48.00 0.00 48.00 I 36.00 36.00 0.00 N 12.00 12.00 0.00 Sb 8.00 8.00 0.00
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 3 ALERT level G = General alerts; check 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ATOMS (Dowty, 2002) and DIAMOND (Brandenburg, 2001); software used to prepare material for publication: SHELXL97).

Triammonium nonaiododiantimonate(III) top
Crystal data top
(NH4)3[Sb2I9]F(000) = 2448
Mr = 1439.75Dx = 4.016 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 5949 reflections
a = 14.394 (3) Åθ = 1.7–28.4°
b = 8.0685 (18) ŵ = 13.92 mm1
c = 20.505 (5) ÅT = 223 K
β = 90.530 (4)°Prism, red
V = 2381.4 (9) Å30.15 × 0.12 × 0.10 mm
Z = 4
Data collection top
Bruker SMART Apex CCD
diffractometer
5949 independent reflections
Radiation source: fine-focus sealed tube4013 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.067
ω scanθmax = 28.4°, θmin = 1.7°
Absorption correction: multi-scan
(SADABS; Bruker, 1998)
h = 1919
Tmin = 0.151, Tmax = 0.251k = 1010
31497 measured reflectionsl = 2727
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)] = 0.041H-atom parameters not refined
wR(F2) = 0.089 w = 1/[σ2(Fo2) + (0.0263P)2 + 6.8306P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max < 0.001
5949 reflectionsΔρmax = 1.09 e Å3
127 parametersΔρmin = 0.98 e Å3
0 restraints
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 > 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Sb10.16664 (4)0.00860 (6)0.34432 (3)0.02174 (13)
Sb20.16322 (4)0.00890 (6)0.15384 (3)0.02196 (13)
I10.04655 (4)0.20488 (7)0.42306 (3)0.03198 (15)
I20.12331 (4)0.28781 (7)0.41543 (3)0.03279 (15)
I30.30075 (4)0.17702 (7)0.24474 (3)0.03158 (15)
I50.00464 (4)0.08553 (8)0.24624 (4)0.03950 (16)
I40.32819 (4)0.07776 (8)0.42179 (3)0.03589 (17)
I60.24153 (4)0.19363 (7)0.28128 (3)0.03102 (15)
I70.07208 (4)0.30328 (7)0.11033 (3)0.03199 (15)
I80.08585 (4)0.19324 (7)0.05466 (3)0.03291 (15)
I90.32917 (4)0.06904 (8)0.07921 (3)0.03696 (17)
N10.5345 (5)0.0243 (10)0.2242 (4)0.039 (2)
N20.1488 (6)0.0288 (11)0.1100 (4)0.049 (2)
N30.1876 (6)0.9815 (11)0.5630 (5)0.053 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sb10.0202 (3)0.0235 (3)0.0215 (3)0.0013 (2)0.0011 (2)0.0001 (3)
Sb20.0213 (3)0.0229 (3)0.0217 (3)0.0011 (2)0.0007 (2)0.0005 (3)
I10.0306 (3)0.0321 (3)0.0333 (4)0.0051 (2)0.0076 (3)0.0054 (3)
I20.0361 (3)0.0274 (3)0.0350 (4)0.0012 (2)0.0056 (3)0.0080 (3)
I30.0295 (3)0.0293 (3)0.0360 (4)0.0019 (2)0.0074 (3)0.0083 (3)
I50.0291 (3)0.0475 (4)0.0415 (4)0.0066 (3)0.0151 (3)0.0081 (3)
I40.0266 (3)0.0450 (4)0.0359 (4)0.0034 (3)0.0098 (3)0.0003 (3)
I60.0345 (3)0.0272 (3)0.0315 (4)0.0048 (2)0.0058 (3)0.0055 (2)
I70.0347 (3)0.0265 (3)0.0348 (4)0.0072 (2)0.0046 (3)0.0048 (2)
I80.0380 (3)0.0322 (3)0.0286 (3)0.0032 (3)0.0064 (3)0.0061 (3)
I90.0283 (3)0.0450 (4)0.0373 (4)0.0011 (3)0.0106 (3)0.0056 (3)
N10.034 (4)0.039 (5)0.045 (5)0.000 (4)0.003 (4)0.008 (4)
N20.049 (5)0.056 (6)0.042 (6)0.005 (4)0.003 (4)0.010 (5)
N30.054 (5)0.054 (6)0.050 (6)0.012 (5)0.006 (5)0.014 (5)
Geometric parameters (Å, º) top
Sb1—I12.8556 (8)Sb2—I82.8422 (9)
Sb1—I42.8591 (9)Sb2—I72.8602 (9)
Sb1—I22.8725 (9)Sb2—I92.8664 (9)
Sb1—I53.1579 (10)Sb2—I53.1501 (10)
Sb1—I3i3.1633 (9)Sb2—I6ii3.1865 (9)
Sb1—I33.1956 (9)Sb2—I63.2211 (9)
I1—Sb1—I494.08 (3)I7—Sb2—I994.32 (3)
I1—Sb1—I292.26 (3)I8—Sb2—I589.32 (3)
I4—Sb1—I293.42 (3)I7—Sb2—I592.12 (2)
I1—Sb1—I592.65 (3)I9—Sb2—I5173.14 (3)
I4—Sb1—I5173.12 (3)I8—Sb2—I6ii90.78 (3)
I2—Sb1—I587.74 (2)I7—Sb2—I6ii173.49 (3)
I1—Sb1—I3i88.60 (3)I9—Sb2—I6ii89.90 (2)
I4—Sb1—I3i92.29 (2)I5—Sb2—I6ii83.48 (2)
I2—Sb1—I3i174.15 (3)I8—Sb2—I6171.27 (3)
I5—Sb1—I3i86.44 (2)I7—Sb2—I691.94 (2)
I1—Sb1—I3173.51 (3)I9—Sb2—I693.36 (3)
I4—Sb1—I387.33 (3)I5—Sb2—I684.04 (3)
I2—Sb1—I393.98 (3)I6ii—Sb2—I682.85 (2)
I5—Sb1—I385.83 (3)Sb1iii—I3—Sb1146.98 (2)
I3i—Sb1—I385.02 (2)Sb2—I5—Sb1151.96 (3)
I8—Sb2—I793.98 (3)Sb2iv—I6—Sb2149.68 (2)
I8—Sb2—I992.59 (3)
Symmetry codes: (i) x+1/2, y+1/2, z+1/2; (ii) x1/2, y1/2, z+1/2; (iii) x+1/2, y1/2, z+1/2; (iv) x1/2, y+1/2, z+1/2.
 

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