Literature DB >> 21522307

Two-dimensional polymeric [Hg(4)(μ(2)-I)(6)I(2)(μ(2)-C(4)S(6))](n).

Aurélien Hameau, Fabrice Guyon, Michael Knorr, Victoria P Colquhoun, Carsten Strohmann.   

Abstract

The title compound, poly[(μ(2)-2H,5H-1,3-dithiolo[4,5-d][1,3]di-thiole-2,5-dithione)hexa-μ(2)-iodido-diiodidotetra-mercury(II)], [Hg(4)I(8)(C(4)S(6))](n), represents the first example of a coordination polymer assembled by the α,α-C(4)S(6) dithione ligand. The Hg(II) ions are four-coordinated in a distorted tetra-hedral geometry, the coordination demand being satisfied either by four bridging iodide ligands or by three iodide ligands (one terminal and two bridging) and a thio-carbonyl S atom. Due to the bridging nature of the dithione ligand, the coordination polymer has a two-dimensional structure, built up of undulated layers parallel to (001). There is an inversion center at the mid-point of the central C=C double bond.

Entities:  

Year:  2011        PMID: 21522307      PMCID: PMC3051975          DOI: 10.1107/S1600536811006556

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the synthesis and structure of the α,α-C4S6 ligand, see: Krug et al. (1977 ▶); Beck et al. (2006 ▶). For related studies on polymeric binary carbon sulfides, see: Galloway et al. (1994 ▶). For the synthesis and structures of coordination polymers with sulfur-rich ligands, see: Peindy et al. (2005 ▶); Hameau et al. (2006 ▶); Ndiaye et al. (2007 ▶); Guyon et al. (2008 ▶).

Experimental

Crystal data

[Hg4I8(C4S6)] M = 1028.98 Monoclinic, a = 8.5502 (6) Å b = 11.2156 (8) Å c = 13.4634 (9) Å β = 91.343 (1)° V = 1290.73 (16) Å3 Z = 4 Mo Kα radiation μ = 33.76 mm−1 T = 173 K 0.30 × 0.10 × 0.10 mm

Data collection

Bruker APEX CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 1999 ▶) T min = 0.035, T max = 0.133 24415 measured reflections 2543 independent reflections 2337 reflections with I > 2σ(I) R int = 0.086

Refinement

R[F 2 > 2σ(F 2)] = 0.039 wR(F 2) = 0.114 S = 1.03 2543 reflections 100 parameters Δρmax = 3.56 e Å−3 Δρmin = −3.29 e Å−3 Data collection: SMART (Bruker, 2001 ▶); cell refinement: SAINT-Plus (Bruker, 1999 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811006556/fi2103sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006556/fi2103Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Hg4I8(C4S6)]F(000) = 1728
Mr = 1028.98Dx = 5.295 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 8987 reflections
a = 8.5502 (6) Åθ = 2.4–26°
b = 11.2156 (8) ŵ = 33.76 mm1
c = 13.4634 (9) ÅT = 173 K
β = 91.343 (1)°Needle, dark red
V = 1290.73 (16) Å30.30 × 0.10 × 0.10 mm
Z = 4
Bruker APEX CCD diffractometer2543 independent reflections
Radiation source: fine-focus sealed tube2337 reflections with I > 2σ(I)
graphiteRint = 0.086
ω scansθmax = 26.0°, θmin = 2.4°
Absorption correction: multi-scan (SADABS; Bruker, 1999)h = −10→10
Tmin = 0.035, Tmax = 0.133k = −13→13
24415 measured reflectionsl = −16→16
Refinement on F20 restraints
Least-squares matrix: fullPrimary atom site location: structure-invariant direct methods
R[F2 > 2σ(F2)] = 0.039Secondary atom site location: difference Fourier map
wR(F2) = 0.114w = 1/[σ2(Fo2) + (0.077P)2 + 7.1937P] where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
2543 reflectionsΔρmax = 3.56 e Å3
100 parametersΔρmin = −3.29 e Å3
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.
xyzUiso*/Ueq
C10.0263 (12)0.9542 (9)1.0288 (7)0.029 (2)
C20.2439 (12)0.9942 (9)0.9076 (8)0.033 (2)
Hg10.51629 (6)0.77041 (5)0.83365 (5)0.05585 (19)
Hg20.22624 (7)0.46970 (6)0.97826 (5)0.0672 (2)
I10.82359 (9)0.77867 (6)0.83985 (5)0.0374 (2)
I20.25603 (8)0.64475 (6)0.79810 (5)0.0372 (2)
I30.08558 (9)0.60123 (6)1.11662 (5)0.03616 (19)
I40.45656 (8)0.32667 (6)0.92556 (5)0.03444 (19)
S10.2076 (3)0.8973 (2)1.0033 (2)0.0374 (6)
S20.4123 (3)0.9968 (3)0.8465 (2)0.0427 (6)
S3−0.0987 (3)0.9043 (2)1.1185 (2)0.0363 (6)
U11U22U33U12U13U23
C10.025 (5)0.035 (5)0.028 (5)−0.001 (4)0.003 (4)0.002 (4)
C20.031 (5)0.029 (5)0.039 (5)−0.002 (4)0.003 (4)−0.001 (4)
Hg10.0325 (3)0.0672 (4)0.0682 (4)−0.0029 (2)0.0078 (2)0.0044 (3)
Hg20.0477 (4)0.0668 (4)0.0881 (5)0.0157 (3)0.0243 (3)−0.0110 (3)
I10.0303 (4)0.0452 (4)0.0369 (4)−0.0012 (3)0.0048 (3)−0.0032 (3)
I20.0332 (4)0.0424 (4)0.0359 (4)−0.0019 (3)0.0013 (3)0.0038 (3)
I30.0351 (4)0.0365 (4)0.0369 (4)−0.0014 (3)0.0029 (3)−0.0047 (3)
I40.0305 (4)0.0404 (4)0.0326 (4)0.0048 (3)0.0041 (3)−0.0024 (3)
S10.0310 (14)0.0406 (14)0.0410 (14)0.0074 (11)0.0101 (11)0.0073 (11)
S20.0350 (15)0.0365 (13)0.0576 (17)0.0020 (11)0.0205 (13)0.0038 (12)
S30.0339 (14)0.0372 (13)0.0383 (13)0.0051 (10)0.0128 (11)0.0067 (11)
C1—C1i1.36 (2)Hg1—S22.697 (3)
C1—S11.718 (11)Hg2—I42.6496 (9)
C1—S31.724 (11)Hg2—I32.6828 (9)
C2—S21.675 (11)Hg2—I3ii3.0353 (10)
C2—S3i1.715 (11)Hg2—I23.1357 (10)
C2—S11.720 (11)I3—Hg2ii3.0353 (10)
Hg1—I12.6285 (9)S3—C2i1.715 (11)
Hg1—I22.6678 (9)
C1i—C1—S1117.1 (11)I4—Hg2—I3ii112.31 (3)
C1i—C1—S3116.3 (11)I3—Hg2—I3ii91.87 (3)
S1—C1—S3126.6 (6)I4—Hg2—I295.60 (3)
S2—C2—S3i121.0 (6)I3—Hg2—I2103.81 (3)
S2—C2—S1123.4 (6)I3ii—Hg2—I285.70 (3)
S3i—C2—S1115.5 (6)Hg1—I2—Hg2105.93 (3)
I1—Hg1—I2148.57 (3)Hg2—I3—Hg2ii88.13 (3)
I1—Hg1—S2107.19 (7)C1—S1—C295.4 (5)
I2—Hg1—S2103.53 (7)C2—S2—Hg1107.7 (4)
I4—Hg2—I3150.11 (4)C2i—S3—C195.7 (5)
Qxnearest atomdistancevalue
-Q1Hg10.68-3.29
Q1Hg10.9513.56
Q2Hg20.9941.67
Q3Hg20.7701.49
Q4I30.7971.07
Q5Hg11.2560.92
Q6I30.6880.92
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1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  Syntheses, structures, and photophysical properties of mono- and dinuclear sulfur-rich gold(I) complexes.

Authors:  Fabrice Guyon; Aurélien Hameau; Abderrahim Khatyr; Michael Knorr; Hedi Amrouche; Daniel Fortin; Pierre D Harvey; Carsten Strohmann; Amadou L Ndiaye; Volker Huch; Michael Veith; Narcis Avarvari
Journal:  Inorg Chem       Date:  2008-07-29       Impact factor: 5.165

3.  Isomers among the carbon sulfides C4S6--synthesis and crystal structures of alpha,alpha-C4S6, alpha,beta-C4S6, and of a second polymorph of the diiodine adduct alpha,beta-C4S6.I2.

Authors:  Johannes Beck; Jörg Daniels; Albrecht Roloff; Norbert Wagner
Journal:  Dalton Trans       Date:  2005-11-14       Impact factor: 4.390

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