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The ditopic organic molecule 3-(pyridin-4-yl)acetyl­acetone (HacacPy) acts as a pyridine-type ligand towards HgX2 (X = Cl, Br, I). The nature of the anion and the ligand-to-cation ratio dominate the outcome of the reaction. Two different coordination compounds form with HgCl2, namely a ligand-rich mononuclear complex, HgCl2(HacacPy)2, and a ligand-deficient one-dimensional chain polymer, [Hg(μ-Cl)2(HacacPy)]1, with five-coordinated HgII cations. Two compounds are also observed for HgBr2, a molecular complex isomorphous to the chloride derivative and a chain polymer with the composition [Hg(μ-Br)Br(HacacPy)]1, in which the cations are four-coordinated. The ligand-rich mononuclear and ligand-deficient polymeric chloride and bromide complexes may be interconverted via thermal degradation and mechanochemical synthesis. In contrast to the chloride and bromide compounds, the reaction product with HgI2 does not depend on the ligand-to-cation ratio but corresponds to [Hg(μ-I)I(HacacPy)]1, isomorphous to the bromide derivative. The N-coordinated HacacPy complexes could not be deprotonated and further crosslinked with a second cation. Synthesis of mixed-metal products could be achieved, however, by deprotonation of the acetyl­acetone moiety in HacacPy and formation of tris­-chelated Fe(acacPy)3 and Al(acacPy)3 complexes in the first step. These mononuclear building blocks act as bridging poly(pyridine) ligands towards HgII halides and form two structure types. The first represents a one-dimensional ladder, with the tris­(ligand) complexes acting as triconnected nodes and the HgII halides acting as linkers. In the alternative unprecedented product, both the tris­(ligand) complexes and the [HgX2(μ-X)HgX] groups act as equivalent triconnected nodes. They form a uninodal two-dimensional coordination network with vertex symbol 4.82 and fes topology.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520617011118/bm5094sup1.cif
Contains datablocks global, 1a, 1b, 2, 2b, 3, 6c, 9d

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011118/bm50941asup2.hkl
Contains datablock 1a

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011118/bm50941bsup3.hkl
Contains datablock 1b

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011118/bm50942sup4.hkl
Contains datablock 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011118/bm50942bsup5.hkl
Contains datablock 2b

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011118/bm50943sup6.hkl
Contains datablock 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011118/bm50946csup7.hkl
Contains datablock 6c

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011118/bm50949dsup8.hkl
Contains datablock 9d

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520617011118/bm5094sup9.pdf
Additional figures and tables

CCDC references: 1565220; 1565221; 1565222; 1565223; 1565224; 1565225; 1565226

Computing details top

For all structures, data collection: SMART (Bruker, 2001); cell refinement: SMART (Bruker, 2001); data reduction: SAINT-Plus (Bruker, 2009); program(s) used to solve structure: SHELXS2013 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2015); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL2013 (Sheldrick, 2015).

(1a) top
Crystal data top
C10H11Cl2HgNO2F(000) = 832
Mr = 448.69Dx = 2.479 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 7.0762 (9) ÅCell parameters from 2968 reflections
b = 25.9640 (17) Åθ = 3.1–28.6°
c = 7.4450 (7) ŵ = 13.23 mm1
β = 118.506 (9)°T = 100 K
V = 1202.0 (2) Å3Plate, colourless
Z = 40.20 × 0.10 × 0.04 mm
Data collection top
CCD area detector
diffractometer
2758 independent reflections
Radiation source: microsource2452 reflections with I > 2σ(I)
Multilayer optics monochromatorRint = 0.061
/w scansθmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan
SADABS
h = 99
Tmin = 0.177, Tmax = 0.620k = 3333
15487 measured reflectionsl = 99
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.029H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.062 w = 1/[σ2(Fo2) + (0.0112P)2 + 5.701P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
2758 reflectionsΔρmax = 1.26 e Å3
151 parametersΔρmin = 2.76 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Hg10.28134 (3)0.00484 (2)0.69523 (3)0.01393 (7)
Cl10.0707 (2)0.06125 (5)0.3821 (2)0.0150 (3)
Cl20.3009 (2)0.05003 (5)0.9569 (2)0.0177 (3)
O10.5616 (6)0.22787 (15)0.0030 (6)0.0209 (9)
O20.1666 (7)0.22447 (16)0.1918 (6)0.0224 (9)
H2A0.307 (15)0.231 (4)0.150 (15)0.07 (3)*
N10.3431 (7)0.05981 (17)0.5097 (7)0.0129 (9)
C10.7725 (9)0.1826 (2)0.3108 (9)0.0169 (12)
H1A0.88970.19510.28760.025*
H1B0.78270.14500.32680.025*
H1C0.78350.19840.43500.025*
C20.5614 (9)0.1965 (2)0.1323 (9)0.0158 (11)
C30.3615 (9)0.1751 (2)0.1076 (8)0.0142 (11)
C40.1707 (9)0.1912 (2)0.0568 (8)0.0142 (11)
C50.0487 (9)0.1744 (2)0.0961 (9)0.0195 (12)
H5A0.13940.20470.11770.029*
H5B0.03630.15490.02180.029*
H5C0.11370.15250.21810.029*
C60.3601 (8)0.1354 (2)0.2501 (8)0.0140 (11)
C70.2858 (9)0.0859 (2)0.1805 (9)0.0167 (11)
H70.23870.07730.04150.020*
C80.2800 (8)0.0490 (2)0.3125 (8)0.0144 (11)
H80.23020.01540.26240.017*
C90.4150 (9)0.1078 (2)0.5790 (8)0.0161 (11)
H90.45980.11560.71820.019*
C100.4257 (9)0.1456 (2)0.4553 (9)0.0157 (11)
H100.47800.17880.50990.019*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.01509 (11)0.01440 (11)0.01143 (11)0.00016 (8)0.00563 (8)0.00235 (8)
Cl10.0158 (6)0.0135 (6)0.0143 (6)0.0005 (5)0.0061 (5)0.0008 (5)
Cl20.0189 (7)0.0193 (7)0.0130 (6)0.0030 (5)0.0062 (5)0.0039 (5)
O10.019 (2)0.020 (2)0.023 (2)0.0009 (16)0.0098 (19)0.0089 (17)
O20.023 (2)0.022 (2)0.017 (2)0.0029 (17)0.0057 (19)0.0072 (17)
N10.012 (2)0.017 (2)0.009 (2)0.0002 (17)0.0044 (18)0.0011 (17)
C10.017 (3)0.016 (3)0.017 (3)0.001 (2)0.008 (2)0.005 (2)
C20.018 (3)0.011 (2)0.020 (3)0.002 (2)0.010 (2)0.002 (2)
C30.016 (3)0.015 (3)0.013 (3)0.002 (2)0.008 (2)0.001 (2)
C40.020 (3)0.013 (3)0.012 (3)0.001 (2)0.009 (2)0.003 (2)
C50.014 (3)0.027 (3)0.014 (3)0.005 (2)0.004 (2)0.004 (2)
C60.011 (3)0.019 (3)0.015 (3)0.002 (2)0.008 (2)0.001 (2)
C70.018 (3)0.019 (3)0.016 (3)0.002 (2)0.011 (2)0.000 (2)
C80.014 (3)0.017 (3)0.013 (3)0.002 (2)0.007 (2)0.005 (2)
C90.017 (3)0.018 (3)0.012 (3)0.002 (2)0.006 (2)0.002 (2)
C100.015 (3)0.011 (3)0.018 (3)0.002 (2)0.006 (2)0.001 (2)
Geometric parameters (Å, º) top
Hg1—N12.171 (4)C1—C21.494 (8)
Hg1—Cl22.3636 (13)C2—C31.447 (8)
Hg1—Cl12.6992 (13)C3—C41.385 (7)
Hg1—Cl1i2.7043 (13)C3—C61.483 (7)
Cl1—Hg1i2.7043 (13)C4—C51.501 (8)
O1—C21.261 (7)C6—C71.391 (8)
O2—C41.315 (7)C6—C101.394 (8)
N1—C81.344 (7)C7—C81.387 (8)
N1—C91.351 (7)C9—C101.372 (8)
N1—Hg1—Cl2166.02 (12)C4—C3—C2118.6 (5)
N1—Hg1—Cl193.68 (12)C4—C3—C6120.3 (5)
Cl2—Hg1—Cl196.88 (4)C2—C3—C6121.0 (5)
N1—Hg1—Cl1i87.32 (12)O2—C4—C3122.0 (5)
Cl2—Hg1—Cl1i100.81 (5)O2—C4—C5113.5 (5)
Cl1—Hg1—Cl1i95.03 (4)C3—C4—C5124.5 (5)
Hg1—Cl1—Hg1i84.97 (4)C7—C6—C10116.8 (5)
C8—N1—C9118.5 (5)C7—C6—C3120.4 (5)
C8—N1—Hg1119.7 (4)C10—C6—C3122.7 (5)
C9—N1—Hg1121.1 (4)C8—C7—C6120.5 (5)
O1—C2—C3120.5 (5)N1—C8—C7121.5 (5)
O1—C2—C1118.1 (5)N1—C9—C10122.3 (5)
C3—C2—C1121.4 (5)C9—C10—C6120.3 (5)
Symmetry code: (i) x, y, z+1.
(1b) top
Crystal data top
C20H22Cl2HgN2O4F(000) = 1208
Mr = 625.88Dx = 1.911 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 26.0002 (19) ÅCell parameters from 9048 reflections
b = 6.4821 (10) Åθ = 2.5–31.6°
c = 16.1960 (16) ŵ = 7.35 mm1
β = 127.176 (1)°T = 100 K
V = 2174.9 (4) Å3Block, colourless
Z = 40.23 × 0.22 × 0.19 mm
Data collection top
CCD area detector
diffractometer
3390 independent reflections
Radiation source: microsource3285 reflections with I > 2σ(I)
Multilayer optics monochromatorRint = 0.032
/w scansθmax = 31.6°, θmin = 2.5°
Absorption correction: multi-scan
SADABS
h = 3731
Tmin = 0.283, Tmax = 0.336k = 99
10383 measured reflectionsl = 2022
Refinement top
Refinement on F21 restraint
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.022H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.050 w = 1/[σ2(Fo2) + (0.0225P)2 + 1.7235P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
3390 reflectionsΔρmax = 2.22 e Å3
138 parametersΔρmin = 1.88 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Hg10.50000.11012 (2)0.75000.01382 (4)
Cl10.54198 (3)0.23528 (10)0.66363 (5)0.02135 (12)
O10.29780 (10)0.8914 (3)0.29668 (15)0.0210 (4)
H1O0.2631 (18)0.894 (6)0.301 (4)0.061 (16)*
O20.21635 (8)0.8183 (3)0.32362 (14)0.0212 (4)
N10.43412 (10)0.1561 (3)0.62895 (15)0.0155 (4)
C10.39497 (12)0.7066 (4)0.3749 (2)0.0201 (5)
H1A0.38810.60380.32470.030*
H1B0.42820.65710.44530.030*
H1C0.40900.83680.36350.030*
C20.33345 (11)0.7402 (4)0.36120 (17)0.0154 (4)
C30.31278 (11)0.6263 (3)0.40829 (17)0.0132 (4)
C40.24913 (11)0.6650 (4)0.37945 (17)0.0158 (4)
C50.21865 (12)0.5199 (4)0.4110 (2)0.0202 (5)
H5A0.23840.54000.48450.030*
H5B0.22540.37730.39950.030*
H5C0.17220.54810.36940.030*
C60.35397 (10)0.4605 (3)0.48360 (17)0.0127 (4)
C70.37578 (11)0.2937 (4)0.45726 (17)0.0156 (4)
H70.36310.28070.38880.019*
C80.41602 (12)0.1479 (4)0.53191 (18)0.0164 (4)
H80.43140.03760.51360.020*
C90.41322 (11)0.3141 (4)0.65505 (17)0.0166 (4)
H90.42600.32080.72370.020*
C100.37349 (11)0.4687 (4)0.58511 (17)0.0150 (4)
H100.35970.57890.60620.018*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.01446 (6)0.01299 (6)0.01239 (6)0.0000.00726 (5)0.000
Cl10.0236 (3)0.0234 (3)0.0206 (3)0.0070 (2)0.0153 (2)0.0022 (2)
O10.0253 (9)0.0170 (9)0.0172 (9)0.0037 (7)0.0110 (8)0.0064 (6)
O20.0175 (8)0.0186 (8)0.0192 (8)0.0059 (7)0.0067 (7)0.0022 (7)
N10.0169 (9)0.0150 (9)0.0124 (8)0.0024 (7)0.0076 (7)0.0012 (7)
C10.0241 (11)0.0173 (12)0.0240 (12)0.0012 (9)0.0172 (10)0.0005 (9)
C20.0199 (10)0.0124 (10)0.0108 (9)0.0007 (8)0.0078 (8)0.0012 (7)
C30.0145 (9)0.0107 (10)0.0106 (9)0.0012 (7)0.0056 (8)0.0010 (7)
C40.0154 (9)0.0135 (10)0.0139 (10)0.0006 (8)0.0065 (8)0.0022 (8)
C50.0171 (10)0.0216 (12)0.0223 (11)0.0008 (9)0.0122 (9)0.0022 (9)
C60.0129 (9)0.0115 (9)0.0129 (9)0.0007 (7)0.0073 (8)0.0001 (7)
C70.0198 (10)0.0146 (11)0.0121 (9)0.0025 (8)0.0095 (8)0.0005 (8)
C80.0197 (10)0.0133 (10)0.0153 (10)0.0038 (8)0.0100 (9)0.0004 (8)
C90.0203 (10)0.0166 (11)0.0134 (10)0.0039 (9)0.0105 (9)0.0026 (8)
C100.0179 (10)0.0136 (10)0.0133 (10)0.0025 (8)0.0093 (8)0.0003 (8)
Geometric parameters (Å, º) top
Hg1—Cl12.3773 (6)C3—C41.444 (3)
Hg1—Cl1i2.3773 (6)C3—C61.487 (3)
Hg1—N1i2.387 (2)C4—C51.504 (4)
Hg1—N12.387 (2)C5—H5A0.9800
O1—C21.319 (3)C5—H5B0.9800
O1—H1O0.949 (19)C5—H5C0.9800
O2—C41.265 (3)C6—C101.398 (3)
N1—C81.342 (3)C6—C71.402 (3)
N1—C91.342 (3)C7—C81.386 (3)
C1—C21.493 (3)C7—H70.9500
C1—H1A0.9800C8—H80.9500
C1—H1B0.9800C9—C101.393 (3)
C1—H1C0.9800C9—H90.9500
C2—C31.382 (3)C10—H100.9500
Cl1—Hg1—Cl1i140.09 (3)O2—C4—C5117.9 (2)
Cl1—Hg1—N1i111.92 (5)C3—C4—C5121.2 (2)
Cl1i—Hg1—N1i96.90 (5)C4—C5—H5A109.5
Cl1—Hg1—N196.90 (5)C4—C5—H5B109.5
Cl1i—Hg1—N1111.92 (5)H5A—C5—H5B109.5
N1i—Hg1—N187.40 (10)C4—C5—H5C109.5
C2—O1—H1O101 (3)H5A—C5—H5C109.5
C8—N1—C9118.5 (2)H5B—C5—H5C109.5
C8—N1—Hg1120.21 (16)C10—C6—C7117.5 (2)
C9—N1—Hg1121.29 (15)C10—C6—C3120.5 (2)
C2—C1—H1A109.5C7—C6—C3122.1 (2)
C2—C1—H1B109.5C8—C7—C6119.4 (2)
H1A—C1—H1B109.5C8—C7—H7120.3
C2—C1—H1C109.5C6—C7—H7120.3
H1A—C1—H1C109.5N1—C8—C7122.7 (2)
H1B—C1—H1C109.5N1—C8—H8118.6
O1—C2—C3120.8 (2)C7—C8—H8118.6
O1—C2—C1113.8 (2)N1—C9—C10122.4 (2)
C3—C2—C1125.4 (2)N1—C9—H9118.8
C2—C3—C4118.7 (2)C10—C9—H9118.8
C2—C3—C6120.7 (2)C9—C10—C6119.5 (2)
C4—C3—C6120.5 (2)C9—C10—H10120.2
O2—C4—C3120.9 (2)C6—C10—H10120.2
Symmetry code: (i) x+1, y, z+3/2.
(2) top
Crystal data top
C10H11Br2HgNO2Dx = 2.796 Mg m3
Mr = 537.61Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 3321 reflections
a = 6.8597 (5) Åθ = 2.9–26.2°
b = 13.9425 (10) ŵ = 18.29 mm1
c = 26.7054 (19) ÅT = 100 K
V = 2554.1 (3) Å3Plate, colourless
Z = 80.10 × 0.10 × 0.03 mm
F(000) = 1952
Data collection top
CCD area detector
diffractometer
3800 independent reflections
Radiation source: microsource3154 reflections with I > 2σ(I)
Multilayer optics monochromatorRint = 0.076
/w scansθmax = 30.4°, θmin = 2.9°
Absorption correction: multi-scan
SADABS
h = 99
Tmin = 0.262, Tmax = 0.610k = 1919
35990 measured reflectionsl = 3737
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.029H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.051 w = 1/[σ2(Fo2) + (0.013P)2 + 0.1177P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
3800 reflectionsΔρmax = 1.17 e Å3
151 parametersΔρmin = 0.83 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Hg11.23641 (2)0.52333 (2)0.20950 (2)0.01584 (5)
Br11.07768 (6)0.45573 (3)0.29989 (2)0.01673 (9)
Br21.04071 (6)0.67071 (3)0.19690 (2)0.02201 (10)
O10.4768 (5)0.1583 (2)0.02973 (12)0.0257 (7)
H1O0.662 (7)0.076 (4)0.022 (2)0.040 (19)*
O20.7592 (5)0.0528 (2)0.03017 (13)0.0234 (7)
N11.0653 (5)0.4059 (2)0.16406 (13)0.0137 (7)
C10.4562 (7)0.3069 (3)0.07225 (18)0.0253 (11)
H1A0.49900.36100.05160.038*
H1B0.48250.32100.10760.038*
H1C0.31610.29670.06750.038*
C20.5645 (6)0.2188 (3)0.05719 (16)0.0181 (9)
C30.7610 (6)0.1996 (3)0.07382 (15)0.0161 (9)
C40.8498 (6)0.1149 (3)0.05929 (16)0.0169 (9)
C51.0506 (7)0.0849 (3)0.07293 (17)0.0231 (10)
H5A1.04440.03390.09820.035*
H5B1.12190.13990.08650.035*
H5C1.11780.06090.04310.035*
C60.8647 (6)0.2708 (3)0.10596 (15)0.0134 (8)
C70.9319 (6)0.2485 (3)0.15347 (16)0.0162 (9)
H70.90940.18670.16730.019*
C81.0325 (6)0.3173 (3)0.18068 (15)0.0146 (8)
H81.08050.30040.21290.017*
C90.9967 (6)0.4288 (3)0.11799 (15)0.0151 (8)
H91.01630.49210.10570.018*
C100.8994 (6)0.3638 (3)0.08825 (16)0.0157 (9)
H100.85590.38200.05580.019*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.01448 (8)0.01707 (9)0.01598 (8)0.00085 (6)0.00035 (6)0.00112 (7)
Br10.01370 (19)0.0223 (2)0.0142 (2)0.00241 (16)0.00067 (15)0.00363 (17)
Br20.0204 (2)0.0176 (2)0.0281 (3)0.00368 (17)0.00235 (18)0.00065 (19)
O10.0256 (18)0.0313 (19)0.0203 (17)0.0071 (15)0.0071 (14)0.0063 (15)
O20.033 (2)0.0150 (16)0.0218 (18)0.0047 (15)0.0036 (16)0.0051 (13)
N10.0123 (16)0.0137 (17)0.0152 (18)0.0009 (14)0.0006 (14)0.0018 (14)
C10.024 (2)0.025 (3)0.027 (3)0.000 (2)0.007 (2)0.000 (2)
C20.020 (2)0.020 (2)0.015 (2)0.0021 (18)0.0010 (18)0.0006 (18)
C30.022 (2)0.014 (2)0.012 (2)0.0051 (17)0.0002 (17)0.0005 (16)
C40.023 (2)0.012 (2)0.015 (2)0.0067 (17)0.0025 (17)0.0002 (17)
C50.031 (3)0.019 (2)0.019 (2)0.003 (2)0.006 (2)0.0031 (19)
C60.0149 (19)0.012 (2)0.014 (2)0.0002 (16)0.0053 (16)0.0032 (16)
C70.015 (2)0.013 (2)0.020 (2)0.0026 (16)0.0021 (17)0.0028 (17)
C80.017 (2)0.014 (2)0.013 (2)0.0023 (16)0.0025 (16)0.0016 (17)
C90.015 (2)0.012 (2)0.018 (2)0.0023 (16)0.0022 (16)0.0020 (17)
C100.018 (2)0.018 (2)0.011 (2)0.0022 (17)0.0013 (16)0.0015 (17)
Geometric parameters (Å, º) top
Hg1—N12.351 (3)C1—C21.491 (6)
Hg1—Br22.4775 (5)C2—C31.444 (6)
Hg1—Br1i2.5361 (5)C3—C41.384 (6)
Hg1—Br12.8107 (5)C3—C61.492 (6)
Br1—Hg1ii2.5361 (5)C4—C51.485 (6)
O1—C21.269 (5)C6—C71.385 (6)
O2—C41.319 (5)C6—C101.401 (5)
N1—C81.332 (5)C7—C81.388 (5)
N1—C91.355 (5)C9—C101.378 (5)
N1—Hg1—Br2103.70 (8)C4—C3—C2118.8 (4)
N1—Hg1—Br1i98.68 (8)C4—C3—C6121.2 (4)
Br2—Hg1—Br1i142.653 (16)C2—C3—C6119.9 (4)
N1—Hg1—Br190.95 (8)O2—C4—C3121.2 (4)
Br2—Hg1—Br1100.656 (15)O2—C4—C5113.3 (4)
Br1i—Hg1—Br1108.536 (14)C3—C4—C5125.5 (4)
Hg1ii—Br1—Hg198.511 (14)C7—C6—C10117.4 (4)
C8—N1—C9117.5 (3)C7—C6—C3122.4 (4)
C8—N1—Hg1123.9 (3)C10—C6—C3120.2 (4)
C9—N1—Hg1118.6 (3)C6—C7—C8119.3 (4)
O1—C2—C3119.8 (4)N1—C8—C7123.5 (4)
O1—C2—C1117.9 (4)N1—C9—C10122.5 (4)
C3—C2—C1122.3 (4)C9—C10—C6119.8 (4)
Symmetry codes: (i) x+1/2, y, z+1/2; (ii) x1/2, y, z+1/2.
(2b) top
Crystal data top
C20H22Br2HgN2O4F(000) = 1352
Mr = 714.80Dx = 2.123 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 26.6909 (15) ÅCell parameters from 5553 reflections
b = 6.5248 (4) Åθ = 2.5–30.1°
c = 16.0700 (9) ŵ = 10.48 mm1
β = 126.946 (1)°T = 100 K
V = 2236.7 (2) Å3Block, colourless
Z = 40.17 × 0.14 × 0.07 mm
Data collection top
CCD area detector
diffractometer
3296 independent reflections
Radiation source: microsource3121 reflections with I > 2σ(I)
Multilayer optics monochromatorRint = 0.040
/w scansθmax = 30.8°, θmin = 2.5°
Absorption correction: multi-scan
SADABS
h = 3738
Tmin = 0.269, Tmax = 0.527k = 88
16192 measured reflectionsl = 2223
Refinement top
Refinement on F21 restraint
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.021H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.045 w = 1/[σ2(Fo2) + (0.0195P)2 + 0.8744P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.002
3296 reflectionsΔρmax = 1.21 e Å3
137 parametersΔρmin = 0.71 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Hg10.50000.09885 (2)0.75000.01415 (4)
Br10.54016 (2)0.23349 (4)0.65486 (2)0.02086 (6)
O10.29282 (10)0.8850 (3)0.29413 (15)0.0215 (4)
O20.21572 (8)0.8077 (3)0.32646 (14)0.0212 (4)
H2O0.2625 (17)0.887 (5)0.297 (3)0.032*
N10.43243 (10)0.1602 (3)0.62897 (16)0.0156 (4)
C10.38662 (12)0.7014 (4)0.3676 (2)0.0213 (5)
H1A0.37850.60000.31580.032*
H1B0.41990.65110.43760.032*
H1C0.39970.83090.35520.032*
C20.32829 (12)0.7353 (4)0.35891 (19)0.0159 (5)
C30.30970 (11)0.6216 (3)0.40841 (19)0.0144 (5)
C40.24846 (11)0.6574 (4)0.38243 (19)0.0160 (5)
C50.22071 (12)0.5111 (4)0.4161 (2)0.0213 (5)
H5A0.24090.52970.49050.032*
H5B0.22740.37020.40350.032*
H5C0.17560.53730.37640.032*
C60.35094 (11)0.4586 (4)0.48357 (18)0.0137 (4)
C70.37045 (11)0.2921 (4)0.45512 (19)0.0166 (5)
H70.35600.27680.38510.020*
C80.41109 (12)0.1496 (4)0.52966 (19)0.0173 (5)
H80.42450.03860.50920.021*
C90.41338 (12)0.3184 (4)0.65705 (19)0.0174 (5)
H90.42790.32750.72730.021*
C100.37325 (11)0.4691 (4)0.58726 (19)0.0156 (5)
H100.36100.57920.61020.019*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.01455 (7)0.01443 (7)0.01243 (7)0.0000.00756 (5)0.000
Br10.02286 (13)0.02393 (13)0.01991 (13)0.00666 (10)0.01504 (11)0.00232 (10)
O10.0260 (10)0.0171 (9)0.0191 (9)0.0033 (7)0.0123 (9)0.0062 (7)
O20.0185 (9)0.0205 (9)0.0192 (9)0.0050 (7)0.0084 (8)0.0019 (7)
N10.0166 (10)0.0151 (10)0.0132 (10)0.0022 (8)0.0080 (8)0.0005 (8)
C10.0245 (13)0.0199 (13)0.0240 (14)0.0020 (10)0.0169 (12)0.0001 (10)
C20.0193 (12)0.0130 (11)0.0117 (11)0.0005 (9)0.0074 (10)0.0015 (9)
C30.0154 (11)0.0134 (11)0.0121 (11)0.0000 (8)0.0071 (9)0.0020 (8)
C40.0153 (11)0.0168 (11)0.0124 (11)0.0006 (9)0.0064 (10)0.0030 (9)
C50.0189 (12)0.0241 (13)0.0207 (13)0.0010 (10)0.0118 (11)0.0003 (10)
C60.0128 (10)0.0151 (11)0.0127 (10)0.0000 (9)0.0074 (9)0.0000 (9)
C70.0185 (12)0.0161 (12)0.0124 (11)0.0030 (9)0.0077 (10)0.0009 (9)
C80.0184 (12)0.0168 (12)0.0142 (11)0.0042 (9)0.0085 (10)0.0005 (9)
C90.0199 (12)0.0195 (12)0.0125 (11)0.0001 (10)0.0095 (10)0.0011 (9)
C100.0188 (11)0.0145 (11)0.0152 (11)0.0018 (9)0.0111 (10)0.0019 (9)
Geometric parameters (Å, º) top
Hg1—N1i2.382 (2)C2—C31.380 (3)
Hg1—N12.382 (2)C3—C41.442 (3)
Hg1—Br12.4958 (3)C3—C61.484 (3)
Hg1—Br1i2.4958 (3)C4—C51.495 (4)
O1—C21.323 (3)C6—C101.394 (3)
O2—C41.260 (3)C6—C71.395 (3)
N1—C81.335 (3)C7—C81.383 (3)
N1—C91.343 (3)C9—C101.388 (3)
C1—C21.493 (4)
N1i—Hg1—N189.61 (10)C2—C3—C6120.4 (2)
N1i—Hg1—Br1110.90 (5)C4—C3—C6120.6 (2)
N1—Hg1—Br198.21 (5)O2—C4—C3120.8 (2)
N1i—Hg1—Br1i98.21 (5)O2—C4—C5118.3 (2)
N1—Hg1—Br1i110.90 (5)C3—C4—C5120.9 (2)
Br1—Hg1—Br1i138.781 (14)C10—C6—C7117.0 (2)
C8—N1—C9117.7 (2)C10—C6—C3120.8 (2)
C8—N1—Hg1120.58 (16)C7—C6—C3122.1 (2)
C9—N1—Hg1121.65 (16)C8—C7—C6119.5 (2)
O1—C2—C3121.0 (2)N1—C8—C7123.3 (2)
O1—C2—C1113.3 (2)N1—C9—C10122.5 (2)
C3—C2—C1125.6 (2)C9—C10—C6119.9 (2)
C2—C3—C4118.9 (2)
Symmetry code: (i) x+1, y, z+3/2.
(3) top
Crystal data top
C10H11HgI2NO2Dx = 3.039 Mg m3
Mr = 631.59Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 2232 reflections
a = 7.0546 (14) Åθ = 2.9–25.8°
b = 14.2685 (16) ŵ = 15.61 mm1
c = 27.4248 (19) ÅT = 293 K
V = 2760.5 (7) Å3Plate, colourless
Z = 80.21 × 0.11 × 0.02 mm
F(000) = 2240
Data collection top
CCD area detector
diffractometer
2654 independent reflections
Radiation source: microsource2206 reflections with I > 2σ(I)
Multilayer optics monochromatorRint = 0.086
/w scansθmax = 25.8°, θmin = 2.9°
Absorption correction: multi-scan
SADABS
h = 88
Tmin = 0.138, Tmax = 0.745k = 1617
21367 measured reflectionsl = 3333
Refinement top
Refinement on F28 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.044H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.099 w = 1/[σ2(Fo2) + (0.0358P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
2654 reflectionsΔρmax = 1.93 e Å3
150 parametersΔρmin = 2.18 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Hg10.27702 (6)0.50806 (3)0.20842 (2)0.01910 (14)
I10.08445 (10)0.44490 (5)0.19734 (3)0.01832 (19)
I20.45739 (11)0.66690 (5)0.19110 (3)0.0233 (2)
O10.7287 (11)0.0469 (6)0.0326 (3)0.0254 (19)
H1D0.860 (6)0.065 (9)0.038 (5)0.038*
O21.0044 (13)0.1507 (6)0.0303 (3)0.033 (2)
N10.4369 (12)0.3948 (6)0.1603 (3)0.016 (2)
C10.4434 (17)0.0820 (8)0.0711 (4)0.026 (3)
H1A0.38430.05410.04220.039*
H1B0.37110.13740.08110.039*
H1C0.44440.03620.09770.039*
C20.6380 (17)0.1095 (8)0.0595 (4)0.021 (3)
C30.7252 (16)0.1949 (8)0.0716 (4)0.019 (2)
C40.9117 (17)0.2107 (9)0.0554 (4)0.025 (3)
C51.0153 (17)0.3008 (8)0.0661 (5)0.029 (3)
H5A1.15220.29050.06320.044*
H5B0.98540.32160.09920.044*
H5C0.97570.34900.04270.044*
C60.6224 (16)0.2628 (8)0.1021 (4)0.020 (2)
C70.5647 (14)0.2418 (8)0.1486 (4)0.019 (2)
H70.58900.18130.16170.023*
C80.4724 (17)0.3070 (7)0.1762 (4)0.023 (3)
H80.43130.28990.20800.027*
C90.4942 (16)0.4171 (8)0.1154 (4)0.021 (3)
H90.47090.47870.10370.025*
C100.5861 (15)0.3541 (8)0.0855 (4)0.021 (2)
H100.62460.37240.05370.026*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.0177 (3)0.0113 (2)0.0283 (3)0.00123 (17)0.00099 (18)0.00103 (17)
I10.0144 (4)0.0155 (4)0.0250 (4)0.0009 (3)0.0002 (3)0.0026 (3)
I20.0204 (4)0.0122 (4)0.0373 (5)0.0020 (3)0.0011 (3)0.0028 (3)
O10.028 (5)0.019 (5)0.029 (5)0.008 (4)0.006 (4)0.005 (4)
O20.038 (6)0.030 (5)0.030 (5)0.007 (4)0.004 (4)0.008 (4)
N10.008 (5)0.013 (5)0.027 (5)0.000 (4)0.000 (4)0.001 (4)
C10.037 (8)0.013 (6)0.029 (7)0.003 (5)0.004 (6)0.003 (5)
C20.030 (7)0.009 (6)0.025 (6)0.005 (5)0.009 (5)0.006 (5)
C30.025 (7)0.011 (6)0.021 (6)0.003 (5)0.003 (5)0.002 (4)
C40.032 (7)0.026 (7)0.018 (6)0.005 (6)0.001 (5)0.001 (5)
C50.030 (7)0.022 (7)0.036 (8)0.000 (6)0.003 (6)0.002 (6)
C60.018 (6)0.014 (5)0.028 (6)0.001 (5)0.004 (5)0.006 (5)
C70.007 (6)0.013 (6)0.038 (6)0.004 (4)0.002 (5)0.001 (4)
C80.037 (7)0.007 (6)0.024 (6)0.007 (5)0.002 (5)0.002 (4)
C90.026 (7)0.018 (6)0.020 (6)0.008 (5)0.001 (5)0.000 (5)
C100.023 (7)0.023 (6)0.018 (6)0.001 (5)0.005 (5)0.000 (4)
Geometric parameters (Å, º) top
Hg1—N12.371 (9)C3—C41.407 (16)
Hg1—I22.6423 (9)C3—C61.471 (15)
Hg1—I12.7215 (9)C4—C51.508 (17)
Hg1—I1i2.9062 (9)C5—H5A0.9800
I1—Hg1ii2.9062 (9)C5—H5B0.9800
O1—C21.324 (13)C5—H5C0.9800
O1—H1D0.97 (2)C6—C71.371 (16)
O2—C41.278 (14)C6—C101.404 (15)
N1—C91.334 (14)C7—C81.365 (15)
N1—C81.350 (14)C7—H70.9500
C1—C21.463 (16)C8—H80.9500
C1—H1A0.9800C9—C101.380 (15)
C1—H1B0.9800C9—H90.9500
C1—H1C0.9800C10—H100.9500
C2—C31.405 (15)
N1—Hg1—I2104.8 (2)O2—C4—C5115.3 (11)
N1—Hg1—I199.1 (2)C3—C4—C5121.9 (11)
I2—Hg1—I1135.66 (3)C4—C5—H5A109.5
N1—Hg1—I1i97.1 (2)C4—C5—H5B109.5
I2—Hg1—I1i105.30 (3)H5A—C5—H5B109.5
I1—Hg1—I1i108.16 (3)C4—C5—H5C109.5
Hg1—I1—Hg1ii96.50 (2)H5A—C5—H5C109.5
C2—O1—H1D101 (8)H5B—C5—H5C109.5
C9—N1—C8117.6 (10)C7—C6—C10116.9 (10)
C9—N1—Hg1119.7 (7)C7—C6—C3122.0 (10)
C8—N1—Hg1122.7 (7)C10—C6—C3121.0 (11)
C2—C1—H1A109.5C8—C7—C6120.5 (11)
C2—C1—H1B109.5C8—C7—H7119.7
H1A—C1—H1B109.5C6—C7—H7119.7
C2—C1—H1C109.5N1—C8—C7122.8 (11)
H1A—C1—H1C109.5N1—C8—H8118.6
H1B—C1—H1C109.5C7—C8—H8118.6
O1—C2—C3120.4 (11)N1—C9—C10122.4 (11)
O1—C2—C1113.2 (10)N1—C9—H9118.8
C3—C2—C1126.3 (10)C10—C9—H9118.8
C2—C3—C4118.3 (10)C9—C10—C6119.7 (11)
C2—C3—C6119.4 (10)C9—C10—H10120.1
C4—C3—C6122.3 (10)C6—C10—H10120.1
O2—C4—C3122.8 (12)
O1—C2—C3—C41.6 (17)C4—C3—C6—C1060.5 (16)
C1—C2—C3—C4177.1 (11)C10—C6—C7—C81.5 (17)
O1—C2—C3—C6179.2 (10)C3—C6—C7—C8178.9 (11)
C1—C2—C3—C65.3 (18)C9—N1—C8—C70.6 (17)
C2—C3—C4—O20.0 (18)Hg1—N1—C8—C7179.9 (8)
C6—C3—C4—O2177.6 (11)C6—C7—C8—N11.5 (18)
C2—C3—C4—C5179.1 (11)C8—N1—C9—C100.2 (17)
C6—C3—C4—C53.3 (18)Hg1—N1—C9—C10179.3 (8)
C2—C3—C6—C760.8 (16)N1—C9—C10—C60.2 (18)
C4—C3—C6—C7116.8 (13)C7—C6—C10—C90.7 (17)
C2—C3—C6—C10121.9 (12)C3—C6—C10—C9178.1 (11)
Symmetry codes: (i) x+1/2, y, z+1/2; (ii) x1/2, y, z+1/2.
(6c) top
Crystal data top
2(C30H30AlBr4Hg2N3O6)·4(C6H5Cl)·2(O0.50)·2(O0.50)·2(O0.50)·2(O0.50)·2(O0.50)'F(000) = 2912
Mr = 3082.94Dx = 1.879 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 16.7982 (18) ÅCell parameters from 1903 reflections
b = 24.3995 (19) Åθ = 2.3–19.5°
c = 13.9346 (15) ŵ = 8.72 mm1
β = 107.435 (4)°T = 100 K
V = 5448.9 (9) Å3Rod, colourless
Z = 20.26 × 0.14 × 0.13 mm
Data collection top
CCD area detector
diffractometer
11349 independent reflections
Radiation source: microsource6418 reflections with I > 2σ(I)
Multilayer optics monochromatorRint = 0.156
/w scansθmax = 26.6°, θmin = 1.9°
Absorption correction: multi-scan
SADABS
h = 2121
Tmin = 0.443, Tmax = 0.745k = 3030
66382 measured reflectionsl = 1717
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.072 w = 1/[σ2(Fo2) + (0.0983P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.203(Δ/σ)max = 0.004
S = 1.07Δρmax = 5.01 e Å3
11349 reflectionsΔρmin = 2.99 e Å3
305 parametersExtinction correction: SHELXL-2014/7 (Sheldrick 2014, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.00138 (11)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Hg10.25690 (3)0.81790 (2)1.02371 (4)0.02894 (18)
Hg21.13932 (4)0.82469 (3)0.47212 (4)0.0381 (2)
Br10.13734 (9)0.77870 (6)0.87564 (10)0.0349 (4)
Br20.25274 (11)0.85272 (7)1.18815 (10)0.0444 (4)
Br31.26553 (9)0.80989 (6)0.62097 (11)0.0352 (4)
Br41.08381 (11)0.88955 (7)0.33206 (11)0.0466 (4)
Al10.6971 (2)0.68817 (15)0.7478 (3)0.0192 (8)*
Cl20.4906 (3)0.5820 (2)0.8528 (4)0.0653 (13)
Cl10.5869 (3)0.5864 (2)0.3574 (4)0.0739 (15)
O10.6861 (6)0.6859 (3)0.8775 (6)0.0231 (19)*
O20.6147 (5)0.7419 (3)0.7118 (5)0.0184 (18)*
O30.7087 (5)0.6901 (3)0.6179 (6)0.0203 (19)*
O40.7821 (5)0.7411 (3)0.7879 (6)0.024 (2)*
O50.7784 (5)0.6339 (3)0.7850 (6)0.0215 (19)*
O60.6145 (6)0.6344 (3)0.7011 (6)0.024 (2)*
O7A0.989 (2)0.6069 (13)0.538 (3)0.093 (5)*0.5
O7B0.970 (2)0.5832 (13)0.515 (2)0.093 (5)*0.5
O8A1.009 (2)0.4434 (13)0.751 (2)0.093 (5)*0.5
O8B0.959 (2)0.4097 (13)0.762 (2)0.093 (5)*0.5
O91.0211 (12)0.4841 (7)0.9685 (13)0.034 (5)*0.5
N10.3662 (7)0.7852 (4)0.9736 (7)0.023 (2)*
N21.0315 (7)0.7943 (4)0.5337 (7)0.023 (2)*
N30.7241 (7)0.4045 (4)0.5552 (8)0.029 (3)*
C10.6270 (9)0.6848 (5)1.0109 (9)0.027 (3)*
H1A0.57750.66251.00600.040*
H1B0.62720.71681.05350.040*
H1C0.67730.66291.04060.040*
C20.6257 (8)0.7034 (5)0.9087 (8)0.020 (3)*
C30.5627 (8)0.7392 (5)0.8534 (9)0.023 (3)*
C40.5629 (8)0.7568 (5)0.7576 (9)0.024 (3)*
C50.4956 (9)0.7982 (6)0.6986 (10)0.034 (3)*
H5A0.51730.81910.65190.051*
H5B0.48160.82330.74600.051*
H5C0.44540.77820.66070.051*
C60.4963 (8)0.7545 (5)0.8958 (8)0.022 (3)*
C70.4153 (9)0.7324 (5)0.8565 (9)0.027 (3)*
H70.40340.70700.80240.032*
C80.3514 (9)0.7488 (5)0.8989 (9)0.030 (3)*
H80.29720.73350.87320.036*
C90.4416 (8)0.8049 (5)1.0131 (9)0.024 (3)*
H90.45130.82911.06880.029*
C100.5095 (9)0.7914 (6)0.9762 (9)0.031 (3)*
H100.56290.80721.00560.037*
C110.7721 (9)0.6854 (5)0.4902 (9)0.025 (3)*
H11A0.82130.66220.49790.037*
H11B0.77360.71630.44590.037*
H11C0.72150.66380.46080.037*
C120.7720 (8)0.7065 (5)0.5909 (9)0.021 (3)*
C130.8353 (8)0.7377 (5)0.6496 (8)0.018 (3)*
C140.8369 (8)0.7559 (5)0.7464 (8)0.017 (3)*
C150.9030 (8)0.7937 (5)0.8072 (9)0.025 (3)*
H15A0.87920.81760.84810.038*
H15B0.92450.81610.76210.038*
H15C0.94870.77220.85140.038*
C160.9035 (8)0.7582 (5)0.6070 (8)0.019 (3)*
C170.9825 (8)0.7357 (5)0.6413 (9)0.027 (3)*
H170.99460.70680.68920.032*
C181.0447 (9)0.7572 (5)0.6027 (9)0.025 (3)*
H181.09980.74340.62920.030*
C190.9511 (8)0.8149 (5)0.4958 (9)0.023 (3)*
H190.93980.84150.44360.027*
C200.8872 (8)0.7977 (5)0.5323 (8)0.022 (3)*
H200.83280.81280.50640.026*
C210.8576 (11)0.5578 (7)0.7675 (12)0.052 (4)*
H21A0.90030.57990.81520.078*
H21B0.87310.55280.70560.078*
H21C0.85340.52190.79720.078*
C220.7747 (9)0.5867 (5)0.7434 (9)0.027 (3)*
C230.7022 (9)0.5620 (6)0.6860 (9)0.029 (3)*
C240.6258 (8)0.5868 (5)0.6697 (9)0.023 (3)*
C250.5443 (9)0.5563 (6)0.6175 (10)0.032 (3)*
H25A0.49900.57110.64060.048*
H25B0.55130.51720.63400.048*
H25C0.53060.56100.54450.048*
C260.7082 (9)0.5065 (5)0.6390 (9)0.027 (3)*
C270.6923 (10)0.4589 (6)0.6819 (11)0.039 (4)*
H270.67380.45970.73990.047*
C280.7037 (11)0.4099 (7)0.6394 (12)0.050 (4)*
H280.69620.37730.67300.060*
C290.7398 (10)0.4518 (6)0.5141 (11)0.038 (4)*
H290.75650.44980.45470.045*
C300.7331 (10)0.5031 (6)0.5532 (11)0.042 (4)*
H300.74520.53530.52190.050*
C310.6586 (11)0.5694 (7)0.2915 (12)0.052 (4)*
C320.6986 (11)0.6085 (8)0.2578 (11)0.052 (4)*
H320.68980.64600.26950.062*
C330.7529 (12)0.5934 (8)0.2057 (13)0.062 (5)*
H330.78270.62050.18140.074*
C340.7635 (14)0.5386 (9)0.1891 (15)0.078 (6)*
H340.79960.52790.15140.094*
C350.7244 (15)0.5013 (10)0.2249 (16)0.085 (7)*
H350.73410.46390.21310.103*
C360.6698 (13)0.5133 (8)0.2788 (14)0.070 (6)*
H360.64220.48590.30520.083*
C370.5700 (11)0.5320 (7)0.8920 (12)0.048 (4)*
C380.5449 (13)0.4770 (8)0.9063 (14)0.065 (5)*
H380.48830.46640.89360.078*
C390.6119 (13)0.4405 (8)0.9408 (13)0.064 (5)*
H390.59860.40350.95130.077*
C400.6920 (14)0.4527 (8)0.9601 (13)0.068 (6)*
H400.73400.42570.98350.082*
C410.7127 (14)0.5069 (8)0.9451 (14)0.068 (5)*
H410.76970.51700.95930.082*
C420.6494 (11)0.5469 (7)0.9087 (12)0.054 (5)*
H420.66340.58350.89660.064*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.0223 (3)0.0381 (3)0.0321 (3)0.0034 (3)0.0168 (2)0.0033 (2)
Hg20.0138 (3)0.0614 (5)0.0395 (3)0.0050 (3)0.0090 (2)0.0151 (3)
Br10.0125 (7)0.0587 (10)0.0322 (7)0.0002 (7)0.0048 (6)0.0096 (7)
Br20.0602 (12)0.0450 (10)0.0310 (8)0.0108 (8)0.0184 (8)0.0047 (7)
Br30.0141 (7)0.0471 (10)0.0406 (8)0.0032 (7)0.0026 (6)0.0032 (7)
Br40.0384 (10)0.0600 (11)0.0420 (9)0.0028 (8)0.0132 (7)0.0127 (8)
Cl20.061 (3)0.064 (3)0.073 (3)0.001 (3)0.024 (3)0.008 (2)
Cl10.069 (4)0.078 (4)0.067 (3)0.009 (3)0.011 (3)0.010 (3)
Geometric parameters (Å, º) top
Hg1—N12.295 (10)C13—C161.524 (16)
Hg1—N3i2.448 (11)C14—C151.497 (17)
Hg1—Br22.4645 (15)C15—H15A0.9800
Hg1—Br12.5927 (15)C15—H15B0.9800
Hg2—N22.345 (10)C15—H15C0.9800
Hg2—Br42.4683 (16)C16—C171.382 (18)
Hg2—Br32.5085 (15)C16—C201.386 (16)
Hg2—Br1ii2.8542 (16)C17—C181.411 (17)
Br1—Hg2iii2.8542 (16)C17—H170.9500
Al1—O51.861 (9)C18—H180.9500
Al1—O21.862 (9)C19—C201.384 (17)
Al1—O11.872 (8)C19—H190.9500
Al1—O31.878 (8)C20—H200.9500
Al1—O61.879 (9)C21—C221.51 (2)
Al1—O41.882 (9)C21—H21A0.9800
Cl2—C371.767 (18)C21—H21B0.9800
Cl1—C311.769 (18)C21—H21C0.9800
O1—C21.291 (14)C22—C231.381 (19)
O2—C41.277 (14)C23—C241.376 (18)
O3—C121.294 (14)C23—C261.521 (18)
O4—C141.277 (14)C24—C251.537 (18)
O5—C221.282 (15)C25—H25A0.9800
O6—C241.274 (14)C25—H25B0.9800
N1—C91.311 (16)C25—H25C0.9800
N1—C81.333 (16)C26—C271.369 (19)
N2—C181.291 (15)C26—C301.381 (18)
N2—C191.388 (16)C27—C281.37 (2)
N3—C281.324 (17)C27—H270.9500
N3—C291.349 (17)C28—H280.9500
N3—Hg1iv2.448 (11)C29—C301.38 (2)
C1—C21.488 (16)C29—H290.9500
C1—H1A0.9800C30—H300.9500
C1—H1B0.9800C31—C321.33 (2)
C1—H1C0.9800C31—C361.40 (2)
C2—C31.410 (17)C32—C331.38 (2)
C3—C41.404 (16)C32—H320.9500
C3—C61.458 (17)C33—C341.38 (3)
C4—C51.554 (18)C33—H330.9500
C5—H5A0.9800C34—C351.31 (3)
C5—H5B0.9800C34—H340.9500
C5—H5C0.9800C35—C361.38 (3)
C6—C101.403 (17)C35—H350.9500
C6—C71.412 (18)C36—H360.9500
C7—C81.428 (18)C37—C421.33 (2)
C7—H70.9500C37—C381.44 (2)
C8—H80.9500C38—C391.40 (3)
C9—C101.423 (18)C38—H380.9500
C9—H90.9500C39—C401.33 (3)
C10—H100.9500C39—H390.9500
C11—C121.495 (16)C40—C411.40 (2)
C11—H11A0.9800C40—H400.9500
C11—H11B0.9800C41—C421.42 (2)
C11—H11C0.9800C41—H410.9500
C12—C131.363 (17)C42—H420.9500
C13—C141.412 (15)
N1—Hg1—N3i86.6 (4)C14—C15—H15A109.5
N1—Hg1—Br2130.6 (3)C14—C15—H15B109.5
N3i—Hg1—Br299.4 (2)H15A—C15—H15B109.5
N1—Hg1—Br197.4 (3)C14—C15—H15C109.5
N3i—Hg1—Br197.8 (3)H15A—C15—H15C109.5
Br2—Hg1—Br1129.50 (6)H15B—C15—H15C109.5
N2—Hg2—Br4110.0 (3)C17—C16—C20119.3 (11)
N2—Hg2—Br3101.9 (3)C17—C16—C13119.4 (11)
Br4—Hg2—Br3140.50 (6)C20—C16—C13121.2 (11)
N2—Hg2—Br1ii89.5 (2)C16—C17—C18117.6 (12)
Br4—Hg2—Br1ii104.24 (5)C16—C17—H17121.2
Br3—Hg2—Br1ii98.62 (5)C18—C17—H17121.2
Hg1—Br1—Hg2iii93.11 (4)N2—C18—C17124.3 (13)
O5—Al1—O2179.0 (4)N2—C18—H18117.8
O5—Al1—O189.2 (4)C17—C18—H18117.8
O2—Al1—O190.1 (4)C20—C19—N2121.6 (11)
O5—Al1—O390.4 (4)C20—C19—H19119.2
O2—Al1—O390.3 (4)N2—C19—H19119.2
O1—Al1—O3179.6 (5)C19—C20—C16119.1 (12)
O5—Al1—O690.2 (4)C19—C20—H20120.4
O2—Al1—O689.2 (4)C16—C20—H20120.4
O1—Al1—O692.1 (4)C22—C21—H21A109.5
O3—Al1—O687.9 (4)C22—C21—H21B109.5
O5—Al1—O488.7 (4)H21A—C21—H21B109.5
O2—Al1—O491.9 (4)C22—C21—H21C109.5
O1—Al1—O491.1 (4)H21A—C21—H21C109.5
O3—Al1—O488.9 (4)H21B—C21—H21C109.5
O6—Al1—O4176.6 (4)O5—C22—C23124.7 (13)
C2—O1—Al1129.1 (8)O5—C22—C21113.8 (13)
C4—O2—Al1129.0 (8)C23—C22—C21121.4 (13)
C12—O3—Al1128.3 (8)C24—C23—C22121.4 (12)
C14—O4—Al1130.2 (8)C24—C23—C26120.1 (12)
C22—O5—Al1125.5 (8)C22—C23—C26118.5 (13)
C24—O6—Al1125.7 (9)O6—C24—C23124.9 (12)
C9—N1—C8120.2 (11)O6—C24—C25113.7 (12)
C9—N1—Hg1120.3 (8)C23—C24—C25121.2 (12)
C8—N1—Hg1119.4 (9)C24—C25—H25A109.5
C18—N2—C19117.9 (11)C24—C25—H25B109.5
C18—N2—Hg2121.0 (9)H25A—C25—H25B109.5
C19—N2—Hg2121.1 (8)C24—C25—H25C109.5
C28—N3—C29115.4 (13)H25A—C25—H25C109.5
C28—N3—Hg1iv125.9 (10)H25B—C25—H25C109.5
C29—N3—Hg1iv118.6 (9)C27—C26—C30118.5 (13)
C2—C1—H1A109.5C27—C26—C23121.4 (12)
C2—C1—H1B109.5C30—C26—C23120.1 (12)
H1A—C1—H1B109.5C26—C27—C28118.7 (14)
C2—C1—H1C109.5C26—C27—H27120.7
H1A—C1—H1C109.5C28—C27—H27120.7
H1B—C1—H1C109.5N3—C28—C27125.0 (15)
O1—C2—C3123.9 (10)N3—C28—H28117.5
O1—C2—C1115.7 (11)C27—C28—H28117.5
C3—C2—C1120.3 (11)N3—C29—C30123.8 (13)
C4—C3—C2119.5 (11)N3—C29—H29118.1
C4—C3—C6121.9 (12)C30—C29—H29118.1
C2—C3—C6118.5 (11)C26—C30—C29118.5 (14)
O2—C4—C3125.8 (12)C26—C30—H30120.8
O2—C4—C5114.7 (10)C29—C30—H30120.8
C3—C4—C5119.5 (11)C32—C31—C36123.7 (18)
C4—C5—H5A109.5C32—C31—Cl1120.7 (14)
C4—C5—H5B109.5C36—C31—Cl1115.7 (14)
H5A—C5—H5B109.5C31—C32—C33118.7 (18)
C4—C5—H5C109.5C31—C32—H32120.6
H5A—C5—H5C109.5C33—C32—H32120.6
H5B—C5—H5C109.5C34—C33—C32119 (2)
C10—C6—C7117.3 (12)C34—C33—H33120.4
C10—C6—C3122.0 (12)C32—C33—H33120.4
C7—C6—C3120.7 (11)C35—C34—C33121 (2)
C6—C7—C8119.3 (12)C35—C34—H34119.7
C6—C7—H7120.4C33—C34—H34119.7
C8—C7—H7120.4C34—C35—C36123 (2)
N1—C8—C7121.5 (13)C34—C35—H35118.3
N1—C8—H8119.3C36—C35—H35118.3
C7—C8—H8119.3C35—C36—C31114.4 (19)
N1—C9—C10122.8 (12)C35—C36—H36122.8
N1—C9—H9118.6C31—C36—H36122.8
C10—C9—H9118.6C42—C37—C38123.3 (17)
C6—C10—C9119.0 (13)C42—C37—Cl2119.3 (14)
C6—C10—H10120.5C38—C37—Cl2117.4 (14)
C9—C10—H10120.5C39—C38—C37113.7 (19)
C12—C11—H11A109.5C39—C38—H38123.1
C12—C11—H11B109.5C37—C38—H38123.1
H11A—C11—H11B109.5C40—C39—C38126 (2)
C12—C11—H11C109.5C40—C39—H39117.0
H11A—C11—H11C109.5C38—C39—H39117.0
H11B—C11—H11C109.5C39—C40—C41118 (2)
O3—C12—C13124.0 (11)C39—C40—H40121.1
O3—C12—C11113.5 (11)C41—C40—H40121.1
C13—C12—C11122.4 (11)C40—C41—C42121 (2)
C12—C13—C14122.5 (11)C40—C41—H41119.7
C12—C13—C16119.4 (10)C42—C41—H41119.7
C14—C13—C16117.8 (10)C37—C42—C41118.5 (18)
O4—C14—C13122.2 (11)C37—C42—H42120.8
O4—C14—C15115.5 (10)C41—C42—H42120.8
C13—C14—C15122.3 (11)
Symmetry codes: (i) x+1, y+1/2, z+3/2; (ii) x+1, y+3/2, z1/2; (iii) x1, y+3/2, z+1/2; (iv) x+1, y1/2, z+3/2.
(9d) top
Crystal data top
C60H60Al2Hg3I6N6O12·CH2Cl2·4(C2H6O)·7.178(O)F(000) = 5382
Mr = 2858.30Dx = 1.885 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 32.1651 (19) ÅCell parameters from 7144 reflections
b = 13.8294 (12) Åθ = 2.4–24.1°
c = 27.6145 (16) ŵ = 6.53 mm1
β = 124.917 (3)°T = 100 K
V = 10072.3 (12) Å3Block, colourless
Z = 40.28 × 0.20 × 0.07 mm
Data collection top
CCD area detector
diffractometer
6621 reflections with I > 2σ(I)
Radiation source: microsourceRint = 0.126
/w scansθmax = 25.4°, θmin = 2.1°
Absorption correction: multi-scan
SADABS
h = 3838
Tmin = 0.318, Tmax = 0.745k = 1616
51862 measured reflectionsl = 3333
9165 independent reflections
Refinement top
Refinement on F269 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.056H-atom parameters constrained
wR(F2) = 0.172 w = 1/[σ2(Fo2) + (0.0766P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
9165 reflectionsΔρmax = 3.26 e Å3
469 parametersΔρmin = 2.05 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Hg10.00000.71458 (4)0.75000.02641 (18)
Hg20.35862 (2)0.66607 (3)0.67590 (2)0.02869 (15)
Al10.06409 (13)0.2544 (2)0.52542 (14)0.0225 (7)
I10.09049 (4)0.78902 (6)0.67202 (4)0.0426 (2)
I20.39442 (3)0.60390 (7)0.61491 (4)0.0416 (2)
I30.31951 (4)0.83034 (6)0.68087 (4)0.0512 (3)
O10.0620 (3)0.3896 (5)0.5313 (3)0.0232 (16)
O20.0257 (3)0.2417 (5)0.5570 (3)0.0275 (18)
O30.1233 (3)0.2464 (5)0.6019 (3)0.0252 (17)
O40.1045 (3)0.2751 (5)0.4968 (3)0.0272 (18)
O50.0660 (3)0.1204 (5)0.5192 (3)0.0243 (17)
O60.0060 (3)0.2604 (5)0.4485 (3)0.0252 (17)
N10.0092 (4)0.5952 (6)0.6960 (4)0.026 (2)
N20.2973 (4)0.5462 (7)0.6554 (4)0.031 (2)
N30.0860 (4)0.0913 (6)0.2688 (4)0.028 (2)
C10.0230 (4)0.5921 (7)0.6373 (5)0.024 (2)
H10.05200.63310.61850.029*
C20.0159 (4)0.5317 (8)0.6031 (5)0.028 (3)
H20.03860.53440.56120.034*
C30.0246 (4)0.4664 (7)0.6296 (5)0.022 (2)
C40.0564 (5)0.4681 (8)0.6898 (5)0.033 (3)
H40.08480.42600.70980.039*
C50.0473 (5)0.5308 (8)0.7217 (5)0.034 (3)
H50.06880.52830.76360.041*
C60.0327 (4)0.4001 (7)0.5922 (5)0.022 (2)
C70.0536 (4)0.4387 (7)0.5636 (5)0.021 (2)
C80.0691 (4)0.5451 (7)0.5705 (5)0.023 (2)
H8A0.07970.55970.54440.035*
H8B0.09720.55760.61160.035*
H8C0.04020.58610.56000.035*
C90.0192 (5)0.3030 (8)0.5860 (5)0.028 (3)
C100.0068 (5)0.2644 (9)0.6137 (6)0.039 (3)
H10A0.04290.28100.58860.059*
H10B0.00870.29330.65280.059*
H10C0.00300.19390.61750.059*
C110.2549 (5)0.5660 (9)0.6500 (6)0.040 (3)
H110.25090.62870.66090.048*
C120.2156 (5)0.5002 (9)0.6291 (6)0.040 (3)
H120.18600.51840.62670.048*
C130.2190 (4)0.4094 (8)0.6120 (5)0.028 (3)
C140.2639 (5)0.3889 (9)0.6182 (6)0.044 (3)
H140.26890.32710.60740.053*
C150.3018 (5)0.4586 (9)0.6403 (7)0.047 (4)
H150.33250.44210.64480.056*
C160.1760 (4)0.3408 (8)0.5858 (5)0.025 (2)
C170.1633 (5)0.2969 (8)0.6205 (5)0.033 (3)
C180.1997 (5)0.3018 (10)0.6887 (5)0.044 (3)
H18A0.19430.36260.70250.066*
H18B0.23480.29840.70080.066*
H18C0.19280.24730.70590.066*
C190.1458 (5)0.3251 (8)0.5241 (5)0.030 (3)
C200.1600 (6)0.3634 (12)0.4844 (6)0.052 (4)
H20A0.13030.36170.44330.078*
H20B0.18700.32320.48850.078*
H20C0.17210.43010.49550.078*
C210.0495 (4)0.0325 (8)0.2767 (4)0.025 (2)
H210.04280.03210.24740.030*
C220.0211 (4)0.0277 (7)0.3250 (5)0.024 (2)
H220.00430.06820.32840.029*
C230.0303 (4)0.0279 (7)0.3679 (4)0.023 (2)
C240.0658 (5)0.0363 (8)0.3616 (5)0.033 (3)
H240.07080.04180.39220.040*
C250.0939 (5)0.0924 (8)0.3122 (5)0.034 (3)
H250.11960.13300.30800.041*
C260.0022 (4)0.0976 (7)0.4193 (4)0.021 (2)
C270.0386 (4)0.0652 (8)0.4746 (5)0.025 (2)
C280.0535 (4)0.0397 (7)0.4847 (5)0.025 (3)
H28A0.08120.04980.52630.038*
H28B0.06460.05860.45970.038*
H28C0.02420.07910.47470.038*
C290.0166 (4)0.1953 (8)0.4090 (5)0.027 (2)
C300.0612 (5)0.2287 (8)0.3508 (5)0.034 (3)
H30A0.07180.29260.35520.051*
H30B0.08920.18270.33620.051*
H30C0.05210.23260.32250.051*
Cl10.2042 (4)0.1790 (7)1.0248 (5)0.0826 (19)*0.5
Cl20.2668 (4)0.1177 (8)0.9932 (4)0.0826 (19)*0.5
C350.2597 (10)0.213 (2)1.0302 (15)0.0826 (19)*0.5
H35A0.25530.27571.01060.099*0.5
H35B0.28930.21711.07200.099*0.5
O70.2013 (8)0.6076 (15)0.7243 (9)0.156 (7)*
H70.19260.66170.70740.234*
C310.1822 (8)0.5964 (14)0.7528 (9)0.085 (6)*
H31A0.19220.53110.77060.102*
H31B0.14500.59510.72360.102*
C320.1923 (9)0.6609 (16)0.7983 (10)0.111 (8)*
H32A0.19030.72770.78530.166*
H32B0.22630.64840.83390.166*
H32C0.16720.65110.80730.166*
O80.3231 (5)0.5697 (10)0.9116 (6)0.090 (4)*
H80.35030.60000.93450.135*
C330.3074 (8)0.5273 (15)0.9439 (9)0.085 (6)*
H33A0.33360.48070.97220.102*
H33B0.27580.49060.91680.102*
C340.2976 (10)0.604 (2)0.9792 (11)0.132 (9)*
H34A0.31730.66230.98580.199*
H34B0.30810.57601.01730.199*
H34C0.26150.61970.95630.199*
O9A0.2924 (6)0.5245 (11)0.7964 (7)0.051 (3)*0.607 (14)
O9B0.2651 (9)0.4819 (18)0.8231 (10)0.051 (3)*0.393 (14)
O10A0.3559 (7)0.2503 (15)0.9449 (9)0.065 (3)*0.589 (11)
O10B0.3553 (10)0.207 (2)0.9736 (13)0.065 (3)*0.411 (11)
O110.3656 (7)0.1070 (13)1.0356 (8)0.065 (3)*0.589 (11)
O12A0.3189 (7)0.3297 (13)0.8274 (9)0.065 (3)*0.589 (11)
O12B0.3275 (10)0.3303 (19)0.8697 (13)0.065 (3)*0.411 (11)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.0496 (4)0.0137 (3)0.0270 (3)0.0000.0284 (3)0.000
Hg20.0327 (3)0.0246 (3)0.0260 (3)0.00181 (18)0.0151 (2)0.00260 (18)
Al10.0333 (18)0.0134 (15)0.0265 (17)0.0028 (13)0.0205 (15)0.0061 (13)
I10.0545 (5)0.0325 (5)0.0397 (5)0.0137 (4)0.0262 (4)0.0011 (4)
I20.0474 (5)0.0504 (6)0.0377 (5)0.0063 (4)0.0307 (4)0.0115 (4)
I30.0520 (6)0.0303 (5)0.0512 (6)0.0036 (4)0.0179 (5)0.0103 (4)
O10.037 (4)0.012 (4)0.024 (4)0.003 (3)0.020 (4)0.006 (3)
O20.039 (5)0.010 (4)0.044 (5)0.005 (3)0.030 (4)0.009 (3)
O30.032 (4)0.018 (4)0.026 (4)0.000 (3)0.017 (4)0.007 (3)
O40.036 (5)0.025 (4)0.031 (4)0.000 (3)0.026 (4)0.007 (3)
O50.034 (4)0.015 (4)0.025 (4)0.001 (3)0.018 (4)0.006 (3)
O60.035 (4)0.009 (4)0.034 (4)0.004 (3)0.021 (4)0.008 (3)
N10.046 (5)0.009 (4)0.026 (4)0.000 (4)0.022 (4)0.004 (3)
N20.029 (5)0.031 (6)0.031 (5)0.006 (4)0.016 (5)0.003 (4)
N30.043 (5)0.017 (4)0.018 (4)0.001 (4)0.014 (4)0.000 (4)
C10.040 (6)0.012 (5)0.026 (4)0.000 (4)0.021 (4)0.004 (4)
C20.031 (6)0.034 (7)0.022 (6)0.001 (5)0.016 (5)0.002 (5)
C30.037 (6)0.011 (5)0.024 (5)0.005 (4)0.021 (5)0.006 (4)
C40.044 (7)0.025 (6)0.031 (6)0.003 (5)0.023 (6)0.005 (5)
C50.047 (6)0.033 (6)0.023 (5)0.009 (5)0.021 (5)0.002 (5)
C60.036 (6)0.009 (4)0.027 (5)0.001 (4)0.020 (5)0.005 (4)
C70.028 (6)0.012 (5)0.024 (5)0.001 (4)0.015 (5)0.004 (4)
C80.028 (6)0.011 (5)0.035 (6)0.006 (4)0.020 (5)0.011 (5)
C90.046 (7)0.017 (5)0.034 (6)0.000 (4)0.032 (6)0.008 (4)
C100.059 (9)0.024 (7)0.055 (8)0.012 (6)0.045 (7)0.000 (6)
C110.041 (8)0.024 (7)0.054 (8)0.009 (6)0.027 (7)0.009 (6)
C120.037 (7)0.035 (7)0.054 (8)0.007 (6)0.029 (7)0.018 (6)
C130.032 (6)0.023 (6)0.027 (6)0.004 (5)0.016 (5)0.000 (5)
C140.045 (8)0.023 (7)0.065 (9)0.003 (6)0.031 (7)0.006 (6)
C150.038 (7)0.026 (7)0.076 (10)0.002 (6)0.032 (7)0.004 (7)
C160.034 (6)0.021 (6)0.028 (6)0.007 (5)0.022 (5)0.009 (4)
C170.047 (7)0.023 (6)0.032 (6)0.003 (5)0.025 (6)0.009 (5)
C180.045 (8)0.049 (9)0.033 (7)0.018 (6)0.020 (6)0.004 (6)
C190.040 (7)0.026 (6)0.037 (7)0.004 (5)0.030 (6)0.009 (5)
C200.055 (9)0.079 (11)0.029 (7)0.022 (8)0.028 (7)0.008 (7)
C210.039 (6)0.024 (5)0.018 (5)0.000 (4)0.019 (4)0.004 (4)
C220.032 (6)0.018 (5)0.025 (5)0.001 (4)0.018 (4)0.002 (4)
C230.028 (5)0.016 (5)0.019 (5)0.003 (4)0.011 (4)0.003 (4)
C240.049 (8)0.030 (7)0.029 (6)0.016 (6)0.027 (6)0.009 (5)
C250.054 (8)0.026 (6)0.031 (7)0.012 (6)0.030 (6)0.004 (5)
C260.036 (5)0.011 (4)0.024 (4)0.010 (4)0.022 (4)0.003 (4)
C270.039 (5)0.018 (5)0.028 (5)0.004 (4)0.025 (4)0.001 (4)
C280.044 (7)0.008 (5)0.024 (6)0.002 (5)0.019 (5)0.003 (4)
C290.039 (6)0.019 (5)0.032 (6)0.005 (4)0.027 (5)0.004 (4)
C300.048 (8)0.014 (6)0.031 (7)0.004 (5)0.018 (6)0.005 (5)
Geometric parameters (Å, º) top
Hg1—N12.355 (8)C6—C91.391 (14)
Hg1—N1i2.355 (8)C6—C71.402 (15)
Hg1—I1i2.6444 (9)C7—C81.530 (13)
Hg1—I12.6444 (9)C9—C101.518 (15)
Hg2—N3ii2.366 (9)C11—C121.386 (17)
Hg2—N22.384 (9)C12—C131.368 (16)
Hg2—I32.6380 (10)C13—C141.382 (17)
Hg2—I22.6687 (10)C13—C161.483 (15)
Al1—O61.862 (8)C14—C151.391 (17)
Al1—O51.865 (7)C16—C171.378 (16)
Al1—O31.870 (8)C16—C191.413 (16)
Al1—O11.881 (7)C17—C181.548 (17)
Al1—O21.882 (8)C19—C201.506 (16)
Al1—O41.889 (8)C21—C221.381 (15)
O1—C71.268 (12)C22—C231.378 (15)
O2—C91.265 (12)C23—C241.375 (15)
O3—C171.284 (14)C23—C261.512 (14)
O4—C191.290 (14)C24—C251.367 (16)
O5—C271.278 (13)C26—C271.401 (15)
O6—C291.273 (13)C26—C291.404 (15)
N1—C11.335 (13)C27—C281.503 (14)
N1—C51.341 (14)C29—C301.490 (16)
N2—C111.313 (15)Cl1—C351.768 (18)
N2—C151.315 (15)Cl2—C351.761 (18)
N3—C211.339 (14)O7—C311.25 (2)
N3—C251.358 (14)C31—C321.420 (16)
N3—Hg2iii2.366 (9)O8—C331.38 (2)
C1—C21.375 (15)C33—C341.58 (3)
C2—C31.400 (15)O9A—O9B1.55 (3)
C3—C41.366 (15)O10A—O10B1.00 (3)
C3—C61.510 (14)O12A—O12B1.03 (3)
C4—C51.383 (15)
N1—Hg1—N1i91.0 (4)C3—C4—C5120.2 (11)
N1—Hg1—I1i108.0 (2)N1—C5—C4122.8 (11)
N1i—Hg1—I1i103.7 (2)C9—C6—C7120.9 (9)
N1—Hg1—I1103.7 (2)C9—C6—C3120.4 (9)
N1i—Hg1—I1108.0 (2)C7—C6—C3118.6 (9)
I1i—Hg1—I1134.18 (5)O1—C7—C6123.8 (9)
N3ii—Hg2—N287.7 (3)O1—C7—C8114.6 (9)
N3ii—Hg2—I3113.9 (2)C6—C7—C8121.5 (9)
N2—Hg2—I3104.9 (2)O2—C9—C6124.9 (10)
N3ii—Hg2—I2102.4 (2)O2—C9—C10115.0 (10)
N2—Hg2—I2102.9 (2)C6—C9—C10120.0 (9)
I3—Hg2—I2134.51 (3)N2—C11—C12123.4 (12)
O6—Al1—O590.2 (3)C13—C12—C11120.8 (12)
O6—Al1—O3178.4 (4)C12—C13—C14115.5 (11)
O5—Al1—O388.8 (3)C12—C13—C16121.3 (11)
O6—Al1—O189.6 (3)C14—C13—C16123.2 (10)
O5—Al1—O1179.7 (3)C13—C14—C15120.2 (12)
O3—Al1—O191.4 (3)N2—C15—C14123.3 (13)
O6—Al1—O292.1 (4)C17—C16—C19119.9 (10)
O5—Al1—O290.9 (3)C17—C16—C13120.5 (10)
O3—Al1—O289.2 (4)C19—C16—C13119.5 (10)
O1—Al1—O289.3 (3)O3—C17—C16126.0 (11)
O6—Al1—O489.8 (3)O3—C17—C18113.3 (10)
O5—Al1—O492.5 (3)C16—C17—C18120.6 (11)
O3—Al1—O488.9 (4)O4—C19—C16123.6 (10)
O1—Al1—O487.3 (3)O4—C19—C20113.8 (10)
O2—Al1—O4176.1 (4)C16—C19—C20122.6 (11)
C7—O1—Al1128.7 (7)N3—C21—C22123.8 (10)
C9—O2—Al1128.4 (7)C23—C22—C21118.9 (10)
C17—O3—Al1124.1 (8)C24—C23—C22117.4 (10)
C19—O4—Al1124.2 (7)C24—C23—C26122.6 (10)
C27—O5—Al1129.9 (7)C22—C23—C26120.1 (10)
C29—O6—Al1130.8 (7)C25—C24—C23121.4 (11)
C1—N1—C5117.5 (9)N3—C25—C24121.5 (11)
C1—N1—Hg1120.0 (7)C27—C26—C29121.5 (9)
C5—N1—Hg1122.5 (7)C27—C26—C23120.2 (9)
C11—N2—C15116.9 (11)C29—C26—C23118.2 (9)
C11—N2—Hg2123.1 (8)O5—C27—C26124.0 (10)
C15—N2—Hg2119.3 (8)O5—C27—C28115.3 (9)
C21—N3—C25116.9 (9)C26—C27—C28120.7 (9)
C21—N3—Hg2iii119.2 (7)O6—C29—C26123.3 (10)
C25—N3—Hg2iii123.1 (8)O6—C29—C30115.5 (10)
N1—C1—C2122.3 (10)C26—C29—C30121.2 (10)
C1—C2—C3120.3 (10)Cl2—C35—Cl1102.3 (12)
C4—C3—C2116.7 (10)O7—C31—C32122 (2)
C4—C3—C6122.7 (10)O8—C33—C34112.8 (18)
C2—C3—C6120.5 (9)
Symmetry codes: (i) x, y, z+3/2; (ii) x+1/2, y+1/2, z+1/2; (iii) x1/2, y+1/2, z1/2.
 

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