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Tricarbon­yl[9-(triphenyl­phospho­nio)fluorenyl­idene]ruthenium, [Ru(C31H21P)(CO)3], (I), is mononuclear, consisting of a single Ru centre, to which three carbonyl units and a chelating μ3-9-(triphenyl­phospho­nio)fluorenide ylide bind to generate a distorted octa­hedral RuC6 core. Nonacarbonyl-μ3-fluorenyl­idene-μ2-hydrido-triangulo-triosmium(III), [Os3H(C13H7)(CO)9], (II), is trinuclear and presents a triangular triosmium core, nine carbonyl ligands and one fluorenyl­idene ligand. Two of the OsIII centres present a highly distorted hexa­coordinated Os(Os2C4) core and are in turn bridged by a hydride ligand. The remaining OsIII cation is octa­coordinated, with an Os(Os2C6) nucleus. The crystal structures of both compounds are the result of nondirectional forces, much resembling the packing of weakly inter­acting quasi-spherical units, viz. the mol­ecules themselves in (I) and centrosymmetric π–π-bonded dimers in (II).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270113005489/dt3019sup1.cif
Contains datablocks global, I, II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113005489/dt3019Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113005489/dt3019IIsup3.hkl
Contains datablock II

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Portable Document Format (PDF) file https://doi.org/10.1107/S0108270113005489/dt3019sup4.pdf
Supplementary material

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S0108270113005489/dt3019sup5.pdf
Supplementary material

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S0108270113005489/dt3019sup6.pdf
Supplementary material

CCDC references: 934600; 934601

Computing details top

For both compounds, data collection: P3/P4-PC (Siemens, 1991); cell refinement: P3/P4-PC (Siemens, 1991); data reduction: P3/P4-PC (Siemens, 1991); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL-NT (Sheldrick, 2008); software used to prepare material for publication: SHELXTL-NT (Sheldrick, 2008) and PLATON (Spek, 2009).

(I) Tricarbonyl[9-(triphenylphosphonio)fluorenylidene]ruthenium top
Crystal data top
[Ru(C31H21P)(CO)3]F(000) = 1232
Mr = 609.55Dx = 1.481 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 25 reflections
a = 10.029 (7) Åθ = 5–12.5°
b = 15.242 (5) ŵ = 0.67 mm1
c = 17.922 (5) ÅT = 295 K
β = 93.50 (5)°Needle, colourless
V = 2735 (2) Å30.28 × 0.10 × 0.08 mm
Z = 4
Data collection top
Siemens R3m
diffractometer
2864 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.060
Graphite monochromatorθmax = 25.0°, θmin = 1.8°
ω/2θ scansh = 1111
Absorption correction: ψ scan
(XEMP in SHELXTL-NT; Sheldrick, 2008)
k = 118
Tmin = 0.90, Tmax = 0.94l = 121
4957 measured reflections2 standard reflections every 98 reflections
4799 independent reflections intensity decay: 1%
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)] = 0.065Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.081H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2))2 + 4.5949P]
where P = (Fo2 + 2Fc2)/3
4799 reflections(Δ/σ)max < 0.001
352 parametersΔρmax = 0.44 e Å3
124 restraintsΔρmin = 0.46 e Å3
Special details top

Experimental. Spectroscopic data for (I): IR data [cyclohexane, ν(CO), cm-1]: 2080m, 2024s, 2000ms; 1H NMR (acetone-d6, δ, p.p.m.): 8.10d (2H), 7.99d (2H), 7.23dd (2H), 6.93dd (2H), 6.38d (2H), 7.38dd (2H), 7.31dd (2H), 7.59dd (2H), 7.14dd (2H), 7.50dd (2H), 7.65dd (1H); 31P NMR data for (I) (δ, p.p.m.): 11.9.

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Ru10.16017 (5)0.51744 (3)0.16295 (3)0.03182 (13)
P10.03200 (18)0.43142 (11)0.28827 (9)0.0347 (4)
C10.2871 (7)0.6082 (5)0.1520 (3)0.0480 (18)
O10.3668 (5)0.6595 (3)0.1462 (3)0.0682 (15)
C20.0413 (7)0.5667 (4)0.0845 (3)0.0477 (17)
O20.0304 (5)0.6020 (3)0.0412 (2)0.0630 (15)
C30.2557 (7)0.4350 (5)0.0998 (3)0.0437 (17)
O30.3083 (5)0.3909 (3)0.0638 (3)0.0613 (15)
C110.0641 (7)0.3669 (4)0.3508 (4)0.0381 (16)
C210.1521 (7)0.3057 (4)0.3215 (3)0.0398 (16)
H210.15950.29680.27010.048*
C310.2296 (7)0.2572 (4)0.3666 (4)0.058 (2)
H310.28690.21420.34640.070*
C410.2207 (7)0.2735 (4)0.4433 (4)0.0546 (19)
H410.27610.24320.47420.066*
C510.1319 (7)0.3332 (5)0.4738 (4)0.066 (2)
H510.12230.34120.52530.079*
C610.0566 (6)0.3818 (4)0.4267 (3)0.0476 (18)
H610.00010.42520.44660.057*
C40.0064 (6)0.4105 (4)0.1911 (3)0.0339 (14)
C120.1288 (6)0.4287 (4)0.1550 (3)0.0349 (14)
C220.2191 (5)0.4997 (4)0.1589 (3)0.0424 (16)
H220.20180.54470.19310.051*
C320.3338 (6)0.5017 (4)0.1114 (3)0.0558 (19)
H320.39160.54930.11320.067*
C420.3637 (6)0.4342 (5)0.0614 (4)0.055 (2)
H420.44180.43590.03060.066*
C520.2777 (6)0.3653 (4)0.0578 (3)0.0381 (15)
H520.29750.32000.02410.046*
C620.1637 (5)0.3614 (4)0.1024 (3)0.0311 (14)
C130.0362 (5)0.3228 (3)0.1633 (3)0.0242 (13)
C230.1451 (6)0.2648 (3)0.1809 (3)0.0311 (15)
H230.21340.28220.21510.037*
C330.1506 (8)0.1825 (4)0.1475 (3)0.0531 (19)
H330.22040.14420.16030.064*
C430.0504 (7)0.1588 (4)0.0950 (3)0.0525 (19)
H430.05530.10410.07230.063*
C530.0558 (6)0.2119 (4)0.0749 (3)0.0381 (16)
H530.12090.19440.03880.046*
C630.0634 (5)0.2940 (4)0.1106 (3)0.0269 (13)
C140.0030 (6)0.5449 (3)0.2964 (3)0.0315 (14)
C240.0612 (5)0.5927 (3)0.2403 (3)0.0243 (12)
C340.0368 (6)0.6837 (4)0.2427 (3)0.0405 (17)
H340.07450.71910.20730.049*
C440.0414 (6)0.7241 (4)0.2955 (3)0.0406 (16)
H440.05490.78440.29460.049*
C540.0980 (7)0.6724 (4)0.3488 (3)0.049 (2)
H540.14680.69880.38510.059*
C640.0831 (7)0.5830 (5)0.3486 (4)0.0504 (19)
H640.12560.54840.38270.060*
C150.2087 (6)0.4214 (4)0.3090 (3)0.0305 (14)
C250.2783 (5)0.4651 (4)0.2556 (3)0.0314 (14)
C350.4162 (6)0.4629 (4)0.2661 (3)0.0398 (16)
H350.46730.48940.23080.048*
C450.4795 (7)0.4228 (4)0.3267 (4)0.0504 (18)
H450.57230.42380.33240.060*
C550.4081 (7)0.3812 (4)0.3791 (3)0.0488 (19)
H550.45260.35370.41960.059*
C650.2699 (7)0.3801 (4)0.3718 (3)0.0439 (17)
H650.21980.35300.40730.053*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ru10.0310 (3)0.0318 (2)0.0328 (2)0.0008 (3)0.00334 (19)0.0045 (3)
P10.0393 (11)0.0309 (10)0.0343 (10)0.0036 (8)0.0050 (8)0.0004 (8)
C10.055 (5)0.061 (5)0.029 (4)0.006 (4)0.009 (3)0.013 (3)
O10.062 (4)0.049 (3)0.093 (4)0.022 (3)0.008 (3)0.003 (3)
C20.053 (5)0.049 (4)0.041 (4)0.012 (3)0.003 (3)0.004 (3)
O20.051 (4)0.073 (4)0.062 (3)0.006 (3)0.011 (3)0.015 (3)
C30.045 (4)0.062 (5)0.025 (3)0.017 (3)0.009 (3)0.001 (3)
O30.064 (4)0.052 (3)0.068 (4)0.012 (3)0.010 (3)0.025 (3)
C110.048 (4)0.023 (4)0.044 (4)0.003 (3)0.013 (3)0.001 (3)
C210.052 (4)0.039 (4)0.028 (4)0.001 (3)0.001 (3)0.005 (3)
C310.073 (6)0.047 (5)0.057 (4)0.020 (4)0.028 (4)0.003 (4)
C410.047 (5)0.057 (5)0.063 (4)0.003 (4)0.024 (4)0.017 (4)
C510.068 (6)0.087 (6)0.043 (4)0.017 (5)0.002 (4)0.018 (4)
C610.048 (4)0.056 (5)0.037 (3)0.020 (4)0.009 (3)0.005 (3)
C40.030 (3)0.032 (3)0.038 (3)0.012 (3)0.010 (3)0.009 (3)
C120.029 (3)0.040 (4)0.036 (3)0.007 (3)0.001 (3)0.012 (3)
C220.036 (4)0.038 (5)0.053 (4)0.012 (3)0.001 (3)0.011 (3)
C320.050 (4)0.043 (5)0.073 (5)0.009 (4)0.004 (3)0.024 (3)
C420.025 (4)0.066 (5)0.072 (5)0.006 (4)0.014 (4)0.021 (4)
C520.035 (4)0.050 (4)0.030 (3)0.023 (3)0.006 (3)0.019 (3)
C620.021 (3)0.037 (3)0.035 (3)0.012 (3)0.005 (3)0.020 (3)
C130.028 (3)0.030 (3)0.014 (3)0.001 (2)0.006 (2)0.009 (2)
C230.024 (3)0.025 (3)0.044 (4)0.003 (3)0.002 (3)0.003 (3)
C330.074 (5)0.035 (4)0.049 (5)0.012 (4)0.004 (4)0.001 (3)
C430.070 (5)0.048 (4)0.040 (4)0.004 (4)0.006 (4)0.007 (3)
C530.038 (4)0.053 (4)0.023 (3)0.000 (3)0.002 (3)0.021 (3)
C630.019 (3)0.039 (3)0.023 (3)0.005 (3)0.001 (2)0.008 (3)
C140.032 (4)0.025 (3)0.036 (3)0.001 (3)0.010 (3)0.005 (2)
C240.017 (3)0.025 (3)0.031 (3)0.005 (2)0.000 (2)0.003 (2)
C340.058 (5)0.029 (3)0.034 (4)0.014 (3)0.001 (3)0.008 (3)
C440.041 (4)0.039 (4)0.042 (4)0.015 (3)0.002 (3)0.008 (3)
C540.066 (6)0.055 (4)0.027 (4)0.003 (4)0.001 (3)0.019 (3)
C640.044 (5)0.050 (4)0.058 (5)0.001 (4)0.008 (4)0.001 (4)
C150.032 (3)0.032 (4)0.026 (3)0.008 (3)0.009 (3)0.004 (3)
C250.028 (3)0.035 (4)0.032 (3)0.007 (3)0.010 (2)0.001 (3)
C350.036 (3)0.024 (4)0.060 (4)0.004 (3)0.008 (3)0.009 (3)
C450.032 (4)0.064 (5)0.053 (4)0.008 (4)0.012 (3)0.007 (4)
C550.064 (5)0.060 (5)0.020 (4)0.005 (4)0.014 (3)0.001 (3)
C650.052 (4)0.047 (4)0.034 (4)0.005 (4)0.010 (3)0.009 (3)
Geometric parameters (Å, º) top
Ru1—C11.898 (7)C52—C621.355 (7)
Ru1—C21.938 (7)C52—H520.9300
Ru1—C31.977 (7)C62—C631.439 (7)
Ru1—C242.095 (5)C13—C631.402 (7)
Ru1—C252.134 (5)C13—C231.426 (7)
Ru1—C42.320 (6)C23—C331.393 (7)
P1—C141.772 (5)C23—H230.9300
P1—C41.774 (6)C33—C431.382 (8)
P1—C151.795 (6)C33—H330.9300
P1—C111.812 (6)C43—C531.369 (8)
C1—O11.128 (7)C43—H430.9300
C2—O21.158 (7)C53—C631.409 (7)
C3—O31.091 (7)C53—H530.9300
C11—C211.367 (8)C14—C641.397 (8)
C11—C611.376 (7)C14—C241.427 (7)
C21—C311.371 (8)C24—C341.410 (7)
C21—H210.9300C34—C441.406 (7)
C31—C411.396 (8)C34—H340.9300
C31—H310.9300C44—C541.386 (8)
C41—C511.364 (9)C44—H440.9300
C41—H410.9300C54—C641.371 (8)
C51—C611.381 (8)C54—H540.9300
C51—H510.9300C64—H640.9300
C61—H610.9300C15—C251.390 (7)
C4—C131.463 (7)C15—C651.398 (7)
C4—C121.492 (8)C25—C351.385 (7)
C12—C221.415 (8)C35—C451.368 (8)
C12—C621.422 (7)C35—H350.9300
C22—C321.390 (7)C45—C551.371 (8)
C22—H220.9300C45—H450.9300
C32—C421.384 (8)C55—C651.384 (9)
C32—H320.9300C55—H550.9300
C42—C521.364 (8)C65—H650.9300
C42—H420.9300
C1—Ru1—C291.7 (3)C62—C52—C42121.2 (6)
C1—Ru1—C393.0 (3)C62—C52—H52119.4
C2—Ru1—C397.4 (3)C42—C52—H52119.4
C1—Ru1—C2491.0 (2)C52—C62—C12121.7 (6)
C2—Ru1—C2488.4 (2)C52—C62—C63130.5 (6)
C3—Ru1—C24172.8 (2)C12—C62—C63107.7 (5)
C1—Ru1—C2590.5 (2)C63—C13—C23117.4 (5)
C2—Ru1—C25175.2 (2)C63—C13—C4111.3 (5)
C3—Ru1—C2586.7 (2)C23—C13—C4131.3 (5)
C24—Ru1—C2587.3 (2)C33—C23—C13120.9 (6)
C1—Ru1—C4173.3 (2)C33—C23—H23119.5
C2—Ru1—C492.4 (3)C13—C23—H23119.5
C3—Ru1—C491.7 (2)C43—C33—C23118.8 (7)
C24—Ru1—C483.9 (2)C43—C33—H33120.6
C25—Ru1—C485.0 (2)C23—C33—H33120.6
C14—P1—C4103.8 (3)C53—C43—C33123.1 (6)
C14—P1—C15105.3 (3)C53—C43—H43118.5
C4—P1—C15105.7 (3)C33—C43—H43118.5
C14—P1—C11111.3 (3)C43—C53—C63118.0 (6)
C4—P1—C11117.4 (3)C43—C53—H53121.0
C15—P1—C11112.4 (3)C63—C53—H53121.0
O1—C1—Ru1177.0 (7)C13—C63—C53121.8 (5)
O2—C2—Ru1174.6 (6)C13—C63—C62108.1 (5)
O3—C3—Ru1178.4 (6)C53—C63—C62130.1 (5)
C21—C11—C61119.2 (6)C64—C14—C24124.2 (5)
C21—C11—P1119.2 (5)C64—C14—P1125.9 (5)
C61—C11—P1121.5 (5)C24—C14—P1109.9 (4)
C11—C21—C31121.2 (6)C34—C24—C14113.2 (5)
C11—C21—H21119.4C34—C24—Ru1130.5 (4)
C31—C21—H21119.4C14—C24—Ru1116.0 (4)
C21—C31—C41118.7 (7)C44—C34—C24123.8 (6)
C21—C31—H31120.7C44—C34—H34118.1
C41—C31—H31120.7C24—C34—H34118.1
C51—C41—C31120.9 (6)C54—C44—C34118.9 (6)
C51—C41—H41119.5C54—C44—H44120.5
C31—C41—H41119.5C34—C44—H44120.5
C41—C51—C61118.8 (7)C64—C54—C44121.0 (6)
C41—C51—H51120.6C64—C54—H54119.5
C61—C51—H51120.6C44—C54—H54119.5
C11—C61—C51121.1 (6)C54—C64—C14118.8 (6)
C11—C61—H61119.4C54—C64—H64120.6
C51—C61—H61119.4C14—C64—H64120.6
C13—C4—C12102.8 (5)C25—C15—C65123.8 (6)
C13—C4—P1118.6 (4)C25—C15—P1110.3 (4)
C12—C4—P1117.7 (4)C65—C15—P1125.8 (5)
C13—C4—Ru1114.5 (4)C35—C25—C15115.7 (5)
C12—C4—Ru1112.0 (4)C35—C25—Ru1128.1 (4)
P1—C4—Ru191.6 (2)C15—C25—Ru1115.9 (4)
C22—C12—C62116.8 (5)C45—C35—C25122.0 (6)
C22—C12—C4133.5 (6)C45—C35—H35119.0
C62—C12—C4109.5 (5)C25—C35—H35119.0
C32—C22—C12119.7 (6)C35—C45—C55120.9 (6)
C32—C22—H22120.2C35—C45—H45119.5
C12—C22—H22120.2C55—C45—H45119.5
C42—C32—C22121.2 (6)C45—C55—C65120.2 (6)
C42—C32—H32119.4C45—C55—H55119.9
C22—C32—H32119.4C65—C55—H55119.9
C52—C42—C32119.4 (6)C55—C65—C15117.2 (6)
C52—C42—H42120.3C55—C65—H65121.4
C32—C42—H42120.3C15—C65—H65121.4
Hydrogen-bond geometry (Å, º) top
Cg1 and Cg2 are the centroids of the C12/C62/C63/C13/C4 and C14/C24/C34/C44/C54/C64 rings, respectively.
D—H···AD—HH···AD···AD—H···A
C21—H21···Cg10.932.713.470 (10)140
C22—H22···Cg20.932.833.665 (9)149
(II) Nonacarbonyl-µ3-fluorenylidene-µ2-hydrido-triangulo-triosmium(III) top
Crystal data top
[Os3H(C13H7)(CO)9]F(000) = 1760
Mr = 986.88Dx = 2.900 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 25 reflections
a = 9.3325 (13) Åθ = 5–12.5°
b = 13.960 (2) ŵ = 16.87 mm1
c = 17.865 (3) ÅT = 295 K
β = 103.771 (13)°Needle, orange
V = 2260.6 (6) Å30.12 × 0.08 × 0.06 mm
Z = 4
Data collection top
Siemens R3m
diffractometer
2892 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.051
Graphite monochromatorθmax = 25.0°, θmin = 1.9°
ω/2θ scansh = 111
Absorption correction: ψ scan
(XEMP in SHELXTL-NT; Sheldrick, 2008)
k = 116
Tmin = 0.22, Tmax = 0.38l = 2120
4675 measured reflections2 standard reflections every 98 reflections
3975 independent reflections intensity decay: 1%
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)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0364P)2]
where P = (Fo2 + 2Fc2)/3
3975 reflections(Δ/σ)max = 0.001
311 parametersΔρmax = 1.17 e Å3
143 restraintsΔρmin = 1.30 e Å3
Special details top

Experimental. Spectroscopic data for (II): IR data [cyclohexane, n(CO), cm-1]: 2095m, 2067ms, 2050ms, 2032mw, 2016w, 2001w, 1990mw; 1H NMR (acetone-d6, δ, p.p.m.): 8.38dd (1H), 8,28td (1H), 8.06dd (1H), 8.01m (1H), 7.65dd (1H), 7.62dt (1H), 7.53dt (1H), -18.3s (Os-H).

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Os10.64687 (6)0.80258 (4)0.05241 (3)0.03423 (16)
Os20.69732 (6)0.62514 (4)0.14762 (3)0.02987 (15)
H120.625 (13)0.668 (5)0.046 (5)0.036*
Os30.91348 (6)0.77009 (4)0.16136 (3)0.03143 (15)
C10.4904 (18)0.8402 (11)0.1037 (9)0.050 (3)
O10.4048 (17)0.8640 (10)0.1326 (8)0.093 (5)
C20.6806 (17)0.9340 (10)0.0394 (8)0.046 (3)
O20.7042 (15)1.0131 (8)0.0302 (8)0.079 (4)
C30.5173 (17)0.7918 (10)0.0467 (8)0.043 (3)
O30.4422 (15)0.7833 (8)0.1060 (6)0.072 (4)
C40.5293 (18)0.6580 (11)0.1903 (10)0.051 (4)
O40.4360 (17)0.6751 (10)0.2168 (10)0.106 (5)
C50.7890 (16)0.5708 (11)0.2447 (9)0.045 (3)
O50.8381 (14)0.5395 (7)0.3042 (6)0.065 (3)
C60.6158 (16)0.5086 (10)0.1035 (8)0.035 (3)
O60.5766 (11)0.4365 (7)0.0750 (6)0.048 (3)
C71.005 (2)0.8914 (11)0.1556 (10)0.064 (4)
O71.0633 (17)0.9620 (9)0.1490 (9)0.106 (5)
C81.0765 (17)0.7181 (10)0.2352 (8)0.041 (3)
O81.1673 (12)0.6855 (8)0.2820 (6)0.063 (3)
C90.8105 (18)0.8140 (10)0.2324 (8)0.047 (3)
O90.7459 (12)0.8417 (8)0.2752 (6)0.060 (3)
C100.8903 (14)0.6179 (9)0.1107 (7)0.029 (2)
C110.9271 (14)0.6832 (9)0.0526 (7)0.028 (2)
C210.8445 (16)0.7666 (10)0.0228 (8)0.036 (2)
C310.9179 (19)0.8207 (12)0.0267 (8)0.053 (4)
H310.87740.87890.04650.064*
C411.039 (2)0.7910 (11)0.0447 (9)0.055 (4)
H411.07590.82840.07900.067*
C511.1177 (18)0.7082 (11)0.0168 (9)0.050 (4)
H511.20240.69050.03230.061*
C611.0639 (14)0.6542 (10)0.0344 (7)0.032 (3)
C121.0087 (15)0.5455 (9)0.1233 (7)0.031 (3)
C221.0293 (17)0.4653 (10)0.1685 (8)0.044 (4)
H220.96350.45060.19850.053*
C321.1501 (16)0.4054 (11)0.1692 (9)0.050 (4)
H321.16360.35100.20020.059*
C421.2497 (16)0.4249 (10)0.1251 (9)0.045 (3)
H421.33030.38500.12700.054*
C521.2276 (17)0.5047 (10)0.0781 (9)0.046 (4)
H521.29120.51710.04620.055*
C621.1110 (15)0.5668 (10)0.0780 (8)0.037 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Os10.0419 (3)0.0272 (3)0.0301 (3)0.0056 (3)0.0017 (2)0.0003 (2)
Os20.0345 (3)0.0259 (3)0.0306 (3)0.0005 (2)0.0105 (2)0.0005 (2)
Os30.0391 (3)0.0244 (3)0.0280 (3)0.0026 (2)0.0026 (2)0.0023 (2)
C10.054 (7)0.049 (8)0.042 (8)0.018 (7)0.003 (6)0.002 (7)
O10.115 (12)0.097 (11)0.081 (10)0.051 (9)0.050 (9)0.002 (8)
C20.060 (10)0.033 (5)0.034 (8)0.008 (5)0.014 (6)0.002 (5)
O20.097 (10)0.025 (5)0.105 (11)0.009 (6)0.003 (8)0.010 (6)
C30.058 (8)0.027 (7)0.035 (6)0.016 (7)0.007 (5)0.000 (5)
O30.102 (10)0.068 (8)0.031 (6)0.010 (7)0.013 (6)0.003 (6)
C40.052 (8)0.046 (9)0.062 (10)0.003 (6)0.030 (7)0.000 (7)
O40.105 (12)0.088 (11)0.156 (15)0.013 (9)0.093 (11)0.014 (10)
C50.043 (8)0.049 (9)0.042 (6)0.016 (6)0.007 (6)0.008 (6)
O50.110 (10)0.041 (6)0.035 (5)0.011 (7)0.001 (6)0.007 (5)
C60.041 (8)0.033 (6)0.039 (7)0.008 (5)0.025 (6)0.001 (5)
O60.058 (7)0.036 (5)0.048 (6)0.012 (5)0.011 (5)0.000 (5)
C70.090 (11)0.031 (6)0.059 (10)0.023 (7)0.008 (8)0.005 (6)
O70.122 (13)0.056 (8)0.120 (13)0.053 (8)0.007 (10)0.013 (8)
C80.043 (6)0.036 (8)0.038 (7)0.006 (5)0.003 (5)0.004 (5)
O80.050 (7)0.075 (8)0.054 (7)0.014 (6)0.006 (5)0.003 (6)
C90.070 (10)0.039 (7)0.031 (6)0.019 (7)0.005 (6)0.006 (6)
O90.061 (7)0.078 (8)0.038 (6)0.030 (6)0.004 (5)0.016 (6)
C100.032 (5)0.020 (4)0.034 (6)0.003 (4)0.006 (5)0.002 (3)
C110.029 (6)0.027 (6)0.030 (5)0.005 (4)0.010 (5)0.006 (4)
C210.048 (6)0.033 (6)0.028 (4)0.002 (5)0.010 (5)0.005 (4)
C310.073 (10)0.052 (9)0.038 (7)0.001 (7)0.020 (8)0.013 (7)
C410.086 (12)0.042 (9)0.049 (10)0.016 (7)0.035 (9)0.006 (7)
C510.067 (10)0.046 (9)0.048 (9)0.007 (7)0.031 (8)0.003 (6)
C610.028 (6)0.039 (7)0.029 (7)0.006 (5)0.005 (5)0.009 (5)
C120.036 (7)0.024 (5)0.033 (7)0.002 (5)0.005 (5)0.012 (4)
C220.051 (9)0.041 (8)0.045 (9)0.013 (6)0.017 (7)0.005 (6)
C320.039 (8)0.038 (8)0.069 (11)0.002 (6)0.007 (7)0.006 (7)
C420.037 (8)0.038 (8)0.059 (10)0.006 (6)0.009 (7)0.007 (6)
C520.044 (9)0.047 (8)0.051 (9)0.003 (6)0.023 (7)0.002 (6)
C620.044 (8)0.033 (7)0.034 (8)0.004 (5)0.011 (6)0.008 (5)
Geometric parameters (Å, º) top
Os1—C21.885 (15)C7—O71.144 (18)
Os1—C31.898 (14)C8—O81.135 (16)
Os1—C11.971 (17)C9—O91.148 (16)
Os1—C212.097 (14)C10—C111.482 (17)
Os1—H121.89 (7)C10—C121.475 (18)
Os2—C61.886 (14)C11—C211.427 (18)
Os2—C51.900 (15)C11—C611.448 (18)
Os2—C41.954 (16)C21—C311.454 (19)
Os2—C102.062 (13)C31—C411.32 (2)
Os2—H121.88 (7)C31—H310.9300
Os3—C91.868 (15)C41—C511.40 (2)
Os3—C81.904 (15)C41—H410.9300
Os3—C71.912 (16)C51—C611.369 (19)
Os3—C102.299 (12)C51—H510.9300
Os3—C112.319 (12)C61—C621.458 (19)
Os3—C212.405 (13)C12—C221.367 (19)
Os1—Os22.9782 (8)C12—C621.422 (19)
Os1—Os32.8070 (9)C22—C321.402 (19)
Os2—Os32.8264 (8)C22—H220.9300
C1—O11.101 (18)C32—C421.38 (2)
C2—O21.146 (17)C32—H320.9300
C3—O31.129 (16)C42—C521.38 (2)
C4—O41.112 (17)C42—H420.9300
C5—O51.139 (16)C52—C621.391 (19)
C6—O61.149 (15)C52—H520.9300
C2—Os1—C392.9 (6)C8—Os3—Os2102.9 (4)
C2—Os1—C187.8 (7)C7—Os3—Os2161.6 (6)
C3—Os1—C194.4 (6)C10—Os3—Os246.0 (3)
C2—Os1—C2191.1 (6)C11—Os3—Os274.5 (3)
C3—Os1—C2198.6 (6)C21—Os3—Os283.4 (3)
C1—Os1—C21167.0 (6)Os1—Os3—Os263.83 (2)
C2—Os1—Os395.5 (4)O1—C1—Os1177.7 (17)
C3—Os1—Os3153.8 (4)O2—C2—Os1177.9 (16)
C1—Os1—Os3110.7 (4)O3—C3—Os1178.2 (14)
C21—Os1—Os356.5 (4)O4—C4—Os2177.6 (17)
C2—Os1—Os2150.6 (4)O5—C5—Os2176.7 (15)
C3—Os1—Os2116.5 (4)O6—C6—Os2174.5 (12)
C1—Os1—Os289.4 (5)O7—C7—Os3176.3 (19)
C21—Os1—Os285.2 (4)O8—C8—Os3175.5 (14)
Os3—Os1—Os258.402 (19)O9—C9—Os3179.0 (13)
C2—Os1—H12168 (3)C11—C10—C12103.8 (11)
C3—Os1—H1280 (3)C11—C10—Os2124.0 (9)
C1—Os1—H12102 (3)C12—C10—Os2131.6 (9)
C21—Os1—H1280 (4)C11—C10—Os372.0 (7)
Os3—Os1—H1287 (3)C12—C10—Os3125.2 (9)
Os2—Os1—H1238 (3)Os2—C10—Os380.6 (4)
C6—Os2—C594.9 (6)C21—C11—C61124.8 (12)
C6—Os2—C494.8 (6)C21—C11—C10124.6 (12)
C5—Os2—C488.1 (7)C61—C11—C10110.5 (11)
C6—Os2—C1096.9 (5)C21—C11—Os375.7 (7)
C5—Os2—C1092.0 (6)C61—C11—Os3124.2 (9)
C4—Os2—C10168.2 (6)C10—C11—Os370.6 (7)
C6—Os2—Os3149.5 (4)C11—C21—C31111.1 (13)
C5—Os2—Os392.9 (4)C11—C21—Os1122.1 (9)
C4—Os2—Os3114.9 (5)C31—C21—Os1126.8 (11)
C10—Os2—Os353.4 (3)C11—C21—Os369.2 (7)
C6—Os2—Os1119.0 (4)C31—C21—Os3124.5 (10)
C5—Os2—Os1146.0 (4)Os1—C21—Os376.8 (4)
C4—Os2—Os189.7 (5)C41—C31—C21122.9 (15)
C10—Os2—Os183.6 (3)C41—C31—H31118.6
Os3—Os2—Os157.77 (2)C21—C31—H31118.6
C6—Os2—H1282 (3)C31—C41—C51125.7 (15)
C5—Os2—H12172 (3)C31—C41—H41117.2
C4—Os2—H12100 (3)C51—C41—H41117.2
C10—Os2—H1281 (4)C61—C51—C41116.7 (15)
Os3—Os2—H1286 (3)C61—C51—H51121.7
Os1—Os2—H1238 (3)C41—C51—H51121.7
C9—Os3—C896.3 (6)C51—C61—C11118.7 (13)
C9—Os3—C793.2 (8)C51—C61—C62134.8 (14)
C8—Os3—C794.7 (7)C11—C61—C62106.4 (11)
C9—Os3—C10123.7 (6)C22—C12—C62119.2 (13)
C8—Os3—C1084.6 (5)C22—C12—C10130.3 (13)
C7—Os3—C10143.0 (7)C62—C12—C10110.5 (12)
C9—Os3—C11151.7 (6)C12—C22—C32119.6 (14)
C8—Os3—C11100.8 (5)C12—C22—H22120.2
C7—Os3—C11107.7 (6)C32—C22—H22120.2
C10—Os3—C1137.4 (4)C42—C32—C22121.7 (14)
C9—Os3—C21130.6 (6)C42—C32—H32119.1
C8—Os3—C21132.8 (6)C22—C32—H32119.1
C7—Os3—C2188.6 (6)C52—C42—C32118.9 (14)
C10—Os3—C2166.4 (5)C52—C42—H42120.5
C11—Os3—C2135.1 (4)C32—C42—H42120.5
C9—Os3—Os184.5 (5)C42—C52—C62120.5 (14)
C8—Os3—Os1166.4 (4)C42—C52—H52119.8
C7—Os3—Os198.8 (5)C62—C52—H52119.8
C10—Os3—Os183.8 (3)C52—C62—C12120.0 (13)
C11—Os3—Os173.7 (3)C52—C62—C61131.2 (13)
C21—Os3—Os146.7 (3)C12—C62—C61108.7 (12)
C9—Os3—Os279.7 (5)
ππ contacts (Å, °) for (II) top
Group 1···Group 2CCD (Å)IPD (Å)IPA (°)SA (°)
Cg1···Cg3i3.808 (8)3.526 (6)2.3 (7)22.15 (16)
Cg2···Cg3i3.850 (8)3.520 (6)2.6 (7)23.9 (2)
Symmetry code: (i) -x+2, -y+1, -z.

Cg1, Cg2 and Cg3 are the centroids of the C10/C11/C61/C62/C12, C11/C21/C31/C41/C51/C61 and C12/C22/C32/C42/C52/C62 rings, respectively. CCD is the centroid-to-centroid distance, IPD is the mean interplanar distance, IPA is the interplanar angle and SA is the mean slippage angle. For details, see Janiak (2000).
 

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