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In the two ruthenium(II)-porphyrin-carbene complexes ­(di­benzoyl­carbenyl-[kappa]C)(pyridine-[kappa]N)(5,10,15,20-tetra-p-tolyl­porphyrinato-[kappa]4N)­ruthenium(II), [Ru(C15H10O2)(C5H5N)(C48H36N4)], (I), and (pyridine-[kappa]N)(5,10,15,20-tetra-p-tolyl­porphyrinato-[kappa]4N)[bis(3-tri­fluoro­methyl­phenyl)­carbenyl-[kappa]C]­ruthenium(II), [Ru(C15H8F6)(C5H5N)(C48H36N4)], (II), the pyridine ligand coordinates to the octahedral Ru atom trans with respect to the carbene ligand. The C(carbene)-Ru-N(pyridine) bonds in (I) coincide with a crystallographic twofold axis. The Ru-C bond lengths of 1.877 (8) and 1.868 (3) Å in (I) and (II), respectively, are slightly longer than those of other ruthenium(II)-porphyrin-carbene complexes, owing to the trans influence of the pyridine ligands.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102022461/tr1046sup1.cif
Contains datablocks I, II, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102022461/tr1046Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102022461/tr1046IIsup3.hkl
Contains datablock II

CCDC references: 205289; 205290

Comment top

Ruthenium(II) porphyrin carbene complexes have been reported as effective catalysts for the production of olefins or cyclopropanes from diazo compounds (Che & Huang, 2002). Assuming that the catalytic reaction would take place at the position trans to the carbene ligand, the ligand-exchange reaction should play an important role in the study of such catalytic reactions. A large amount of Lewis base, PPh3, pyridine or CO, causes dissociation of the carbene ligand, and the exchange reaction of the axial ligand trans to carbene has been examined using UV-vis spectroscopy in CH2Cl2 solution (Galardon et al., 1998). We have synthesized two (porphyrinato)ruthenium(II) carbene complexes coordinated by a pyridine ligand, [Ru(ttp){C(COPh)2}(py)], (I) and [Ru(ttp){C(3—C6H4CF3)2}(py)], (II) (where H2ttp is 5,10,15,20-tetra-p-tolylporphyrin and py is pyridine), and have investigated the trans influence of the axial ligands on the molecular structures in the crystalline state. \sch

The molecular structures of (I) and (II) are shown in Figs. 1 and 2, respectively. The geometry about the Ru atoms is distorted octahedral in both complexes, and the equatorial Ru—N(porphyrin) bond lengths in (I) and (II) are as expected for ruthenium(II) porphyrin complexes. The Ru—C bond length in (II) is longer than that in the five-coordinate derivative [Ru(ttp){C(3—C6H4CF3)2}] [1.842 (6) Å; Wada et al., 2002]. Compared with analogous ruthenium(II) tetra-p-tolylporphyrin and tetraphenylporphyrin (H2tpp) carbene complexes, the Ru—C bond trans to the N-donor ligand in (I) and (II) is obviously longer than that trans to an O-donor; an Ru—C bond length of 1.829 (9) Å was observed in [Ru(tpp){C(CO2Et)2}(CH3OH)]·H2O (Galardon et al., 1998), and a value of 1.845 (3) Å was observed in [Ru(ttp)(CPh2)(CH3OH)]·CH3OH (Kawai et al., 2002). Thus, the N-donor ligand seems to have a larger trans influence than the O-donor ligand in ruthenium(II) porphyrin carbene complexes. In addition, the Ru—N bond trans to the carbene in (I) and (II) is much longer than that trans to a carbonyl group; an Ru—N distance of 2.193 (4) Å was observed in [Ru(tpp)(CO)(py)].1.5(toluene) (Little & Ibers, 1973). Therefore, the trans influence of the carbene ligand is apparently stronger than that of the carbonyl ligand for (porphyrinato)ruthenium(II) complexes. The Ru—C—C angle about the carbene C atom in (I) is closer to 120° than in (II). The pairs of benzoyl [(I)] and 3-trifluoromethylphenyl [(II)] groups assume a face-to-face arrangement in an anti conformation.

The porphyrin rings in these two compounds are slightly distorted into saddle conformations. The largest deviations from the C20N4 least-squares planes are −0.235 (6) and 0.194 (6) Å at C3 and C8, respectively, for (I), and 0.148 (3) and −0.107 (3) Å at C10 and C13, respectively, for (II). The Ru atoms are displaced out of the least-squares planes toward the carbene ligands by 0.1460 (17) and 0.0603 (6) Å for (I) and (II), respectively. The Ru displacement in (II) is the smallest among ruthenium(II) porphyrin carbene complexes reported to date.

Experimental top

For (I), a solution of [Ru(ttp)(CO)(EtOH)] in tetrahydrofuran was irradiated with a 100 W high-pressure mercury lamp under N2 for 6 h. An equimolar quantity of N2C(COPh)2 was added and the resulting solution refluxed for 6 h. After removal of the solvent in vacuo, the residue was purified by column chromatography on silica gel and eluted with CH2Cl2/hexane (2:1), to afford [Ru(ttp){C(COPh)2}], (I'). Addition of an excess amount of pyridine to a CH2Cl2 solution of (I') and evaporation gave compound (I) as a dark-red solid. Compound (II) was prepared according to a procedure similar to that of Kawai et al. (2002). The detailed procedure will be published elsewhere (Wada et al., 2002). Crystals of (I) and (II) were prepared by recrystallization from CH2Cl2/cyclohexane (1:1) and CH2Cl2/pyridine (1:1) solutions, respectively.

Refinement top

All H atoms were placed in geometrically idealized positions, with Csp2—H = 0.93 Å or Csp3—H = 0.96 Å, and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C).

Computing details top

For both compounds, data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: CrystalStructure (Molecular Structure Corporation & Rigaku Corporation, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing displacement ellipsoids at the 30% probability level. H atoms and p-tolyl groups have been omitted for clarity.
[Figure 2] Fig. 2. The molecular structure of (II), showing displacement ellipsoids at the 30% probability level. H atoms and p-tolyl groups have been omitted for clarity.
(I) (dibenzoylcarbenyl-κC)(pyridine-κN)(5,10,15,20-tetra-p-tolylporphyrinato- κ4N)ruthenium(II) top
Crystal data top
[Ru(C48H36N4)(C15H10O2)(C5H5N)]F(000) = 2216
Mr = 1071.21Dx = 1.319 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71069 Å
Hall symbol: -C 2ycCell parameters from 25 reflections
a = 15.806 (2) Åθ = 10.8–13.7°
b = 16.6172 (18) ŵ = 0.34 mm1
c = 20.644 (2) ÅT = 296 K
β = 95.872 (10)°Needle, dark red
V = 5393.7 (10) Å30.20 × 0.12 × 0.10 mm
Z = 4
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.048
Radiation source: rotating Mo anticathodeθmax = 27.5°, θmin = 2.6°
Graphite monochromatorh = 020
ω/2θ scansk = 021
6419 measured reflectionsl = 2626
6197 independent reflections3 standard reflections every 150 reflections
2792 reflections with I > 2σ(I) intensity decay: 1.5%
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)] = 0.061Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.182H-atom parameters constrained
S = 0.97 w = 1/[σ2(Fo2) + (0.0752P)2]
where P = (Fo2 + 2Fc2)/3
6197 reflections(Δ/σ)max < 0.001
345 parametersΔρmax = 0.64 e Å3
0 restraintsΔρmin = 0.51 e Å3
Crystal data top
[Ru(C48H36N4)(C15H10O2)(C5H5N)]V = 5393.7 (10) Å3
Mr = 1071.21Z = 4
Monoclinic, C2/cMo Kα radiation
a = 15.806 (2) ŵ = 0.34 mm1
b = 16.6172 (18) ÅT = 296 K
c = 20.644 (2) Å0.20 × 0.12 × 0.10 mm
β = 95.872 (10)°
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.048
6419 measured reflections3 standard reflections every 150 reflections
6197 independent reflections intensity decay: 1.5%
2792 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0610 restraints
wR(F2) = 0.182H-atom parameters constrained
S = 0.97Δρmax = 0.64 e Å3
6197 reflectionsΔρmin = 0.51 e Å3
345 parameters
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
Ru0.50000.63899 (4)0.25000.0426 (2)
O0.5512 (3)0.8122 (3)0.15859 (19)0.0658 (11)
N10.3831 (3)0.6273 (3)0.28244 (19)0.0447 (10)
N20.4442 (3)0.6359 (3)0.15594 (19)0.0461 (10)
N30.50000.4988 (4)0.25000.0548 (17)
C10.3664 (3)0.6281 (3)0.3473 (3)0.0502 (14)
C20.2762 (4)0.6202 (4)0.3491 (3)0.0620 (18)
H10.24770.61830.38630.074*
C30.2402 (4)0.6161 (4)0.2871 (3)0.0627 (17)
H20.18250.61040.27410.075*
C40.3058 (3)0.6219 (3)0.2452 (3)0.0504 (14)
C50.2946 (3)0.6247 (3)0.1767 (3)0.0521 (14)
C60.3586 (3)0.6339 (3)0.1358 (2)0.0476 (12)
C70.3464 (4)0.6390 (4)0.0660 (3)0.0621 (15)
H30.29450.64000.04030.074*
C80.4237 (4)0.6419 (4)0.0447 (3)0.0585 (14)
H40.43490.64540.00140.070*
C90.4866 (3)0.6387 (4)0.1003 (2)0.0503 (12)
C100.5739 (3)0.6348 (3)0.0990 (2)0.0491 (12)
C110.2044 (4)0.6154 (3)0.1448 (3)0.0529 (15)
C120.1617 (4)0.6767 (4)0.1099 (3)0.0675 (17)
H50.18840.72600.10550.081*
C130.0796 (4)0.6652 (4)0.0814 (4)0.083 (2)
H60.05210.70690.05780.100*
C140.0377 (4)0.5932 (4)0.0871 (4)0.078 (2)
C150.0797 (5)0.5337 (4)0.1224 (4)0.092 (2)
H70.05220.48500.12740.110*
C160.1611 (4)0.5433 (4)0.1506 (3)0.0741 (19)
H80.18790.50110.17390.089*
C170.0516 (5)0.5811 (5)0.0537 (5)0.121 (3)
H90.07070.62980.03180.145*
H100.08940.56750.08560.145*
H110.05120.53820.02250.145*
C180.6085 (3)0.6388 (4)0.0340 (3)0.0529 (13)
C190.6268 (5)0.7110 (4)0.0080 (3)0.084 (2)
H120.61630.75820.03000.101*
C200.6611 (5)0.7148 (4)0.0512 (4)0.095 (3)
H130.67330.76510.06780.114*
C210.6774 (4)0.6491 (5)0.0856 (3)0.0698 (18)
C220.6562 (6)0.5782 (5)0.0601 (4)0.103 (3)
H140.66490.53140.08320.123*
C230.6218 (6)0.5715 (4)0.0012 (3)0.095 (3)
H150.60780.52120.01420.114*
C240.7157 (5)0.6553 (5)0.1496 (3)0.099 (3)
H160.72240.60230.16700.118*
H170.77020.68110.14270.118*
H180.67870.68630.17980.118*
C250.50000.7519 (5)0.25000.0441 (18)
C260.4888 (4)0.7992 (3)0.1879 (2)0.0493 (14)
C270.4045 (4)0.8323 (3)0.1641 (3)0.0513 (14)
C280.3933 (4)0.8643 (4)0.1022 (3)0.0746 (18)
H190.43730.86290.07550.089*
C290.3153 (6)0.8989 (5)0.0800 (4)0.101 (3)
H200.30760.92160.03860.121*
C300.2501 (6)0.8996 (5)0.1184 (5)0.094 (3)
H210.19850.92330.10330.112*
C310.2601 (5)0.8661 (5)0.1785 (4)0.085 (2)
H220.21530.86650.20450.102*
C320.3371 (4)0.8311 (4)0.2014 (3)0.0652 (17)
H230.34330.80680.24220.078*
C330.5149 (4)0.4568 (4)0.1979 (3)0.0721 (19)
H240.52530.48490.16060.087*
C340.5160 (5)0.3752 (4)0.1958 (4)0.096 (2)
H250.52740.34850.15800.115*
C350.50000.3327 (7)0.25000.100 (4)
H260.50000.27670.25000.120*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ru0.0424 (4)0.0448 (4)0.0412 (3)0.0000.0076 (3)0.000
O0.069 (3)0.070 (3)0.061 (3)0.010 (2)0.018 (2)0.010 (2)
N10.046 (2)0.053 (3)0.035 (2)0.001 (2)0.0068 (19)0.004 (2)
N20.046 (2)0.048 (2)0.044 (2)0.003 (2)0.0068 (19)0.007 (2)
N30.048 (4)0.052 (4)0.065 (5)0.0000.007 (3)0.000
C10.048 (3)0.042 (3)0.062 (3)0.002 (3)0.017 (3)0.003 (3)
C20.057 (4)0.075 (5)0.058 (4)0.001 (3)0.020 (3)0.002 (3)
C30.042 (3)0.078 (5)0.069 (4)0.001 (3)0.012 (3)0.002 (3)
C40.044 (3)0.050 (4)0.058 (3)0.000 (2)0.007 (3)0.001 (3)
C50.045 (3)0.050 (4)0.061 (3)0.005 (3)0.001 (3)0.003 (3)
C60.047 (3)0.046 (3)0.047 (3)0.002 (3)0.003 (2)0.004 (3)
C70.055 (3)0.080 (4)0.049 (3)0.009 (4)0.004 (3)0.001 (4)
C80.069 (4)0.064 (4)0.041 (3)0.011 (4)0.003 (3)0.013 (3)
C90.060 (3)0.046 (3)0.045 (3)0.007 (3)0.009 (2)0.003 (3)
C100.058 (3)0.046 (3)0.045 (3)0.005 (3)0.012 (2)0.003 (3)
C110.047 (3)0.054 (4)0.057 (3)0.003 (3)0.000 (3)0.008 (3)
C120.062 (4)0.061 (4)0.076 (4)0.014 (3)0.007 (3)0.004 (3)
C130.064 (4)0.067 (5)0.113 (6)0.000 (4)0.020 (4)0.008 (4)
C140.053 (4)0.070 (5)0.106 (6)0.011 (4)0.010 (4)0.002 (4)
C150.066 (5)0.060 (5)0.143 (7)0.017 (4)0.020 (5)0.015 (5)
C160.055 (4)0.060 (4)0.101 (5)0.009 (3)0.019 (4)0.007 (4)
C170.060 (5)0.105 (7)0.187 (10)0.020 (5)0.033 (5)0.012 (7)
C180.053 (3)0.053 (3)0.055 (3)0.001 (3)0.014 (3)0.001 (3)
C190.134 (7)0.052 (4)0.075 (5)0.000 (4)0.057 (5)0.006 (3)
C200.149 (8)0.051 (4)0.098 (6)0.005 (4)0.074 (6)0.005 (4)
C210.086 (5)0.079 (5)0.049 (3)0.009 (4)0.026 (3)0.002 (4)
C220.183 (9)0.069 (5)0.066 (5)0.012 (5)0.058 (5)0.009 (4)
C230.167 (8)0.057 (4)0.069 (5)0.009 (5)0.056 (5)0.005 (4)
C240.132 (7)0.103 (6)0.070 (4)0.006 (5)0.056 (5)0.007 (4)
C250.036 (4)0.055 (5)0.041 (4)0.0000.001 (3)0.000
C260.066 (4)0.041 (3)0.041 (3)0.007 (3)0.010 (3)0.002 (2)
C270.059 (4)0.042 (3)0.051 (3)0.001 (3)0.004 (3)0.008 (2)
C280.084 (5)0.085 (5)0.052 (3)0.022 (4)0.012 (3)0.008 (4)
C290.110 (7)0.093 (6)0.089 (6)0.033 (5)0.043 (5)0.037 (5)
C300.082 (6)0.080 (5)0.109 (7)0.013 (5)0.036 (5)0.012 (5)
C310.075 (5)0.096 (6)0.080 (5)0.023 (5)0.008 (4)0.007 (5)
C320.064 (4)0.076 (4)0.055 (4)0.014 (3)0.001 (3)0.001 (3)
C330.076 (5)0.061 (4)0.081 (5)0.001 (4)0.012 (4)0.013 (4)
C340.111 (6)0.064 (6)0.112 (7)0.002 (4)0.010 (5)0.021 (4)
C350.114 (10)0.051 (6)0.132 (11)0.0000.004 (9)0.000
Geometric parameters (Å, º) top
Ru—N12.038 (4)C25—C261.498 (6)
Ru—N22.049 (4)C26—C271.479 (8)
Ru—N32.329 (7)C27—C321.377 (8)
Ru—C251.877 (8)C27—C281.378 (8)
O—C261.228 (6)C28—C291.394 (11)
N1—C11.392 (6)C29—C301.362 (12)
N1—C41.379 (7)C30—C311.354 (10)
N2—C61.374 (6)C31—C321.388 (9)
N2—C91.387 (6)C33—C341.358 (9)
N3—C331.323 (7)C34—C351.369 (9)
C1—C21.436 (8)C2—H10.9300
C2—C31.347 (8)C3—H20.9300
C3—C41.420 (8)C7—H30.9300
C4—C51.407 (8)C8—H40.9300
C5—C61.391 (7)C12—H50.9300
C6—C71.437 (7)C13—H60.9300
C7—C81.342 (8)C15—H70.9300
C8—C91.440 (7)C16—H80.9300
C9—C101.385 (7)C17—H90.9600
C10—C1i1.384 (7)C17—H100.9600
C5—C111.515 (8)C17—H110.9600
C11—C121.383 (8)C19—H120.9300
C12—C131.382 (9)C20—H130.9300
C13—C141.378 (9)C22—H140.9300
C14—C151.360 (9)C23—H150.9300
C15—C161.366 (9)C24—H160.9600
C16—C111.390 (8)C24—H170.9600
C14—C171.520 (9)C24—H180.9600
C10—C181.501 (7)C28—H190.9300
C18—C191.357 (8)C29—H200.9300
C19—C201.388 (8)C30—H210.9300
C20—C211.342 (9)C31—H220.9300
C21—C221.347 (9)C32—H230.9300
C22—C231.386 (9)C33—H240.9300
C23—C181.361 (8)C34—H250.9300
C21—C241.512 (8)C35—H260.9300
N1—Ru—N1i169.1 (2)C27—C26—C25120.2 (4)
N1—Ru—N289.57 (15)C32—C27—C28119.4 (6)
N1—Ru—N2i90.16 (15)C32—C27—C26122.0 (5)
N1—Ru—N384.55 (12)C28—C27—C26118.6 (6)
N2i—Ru—N2177.1 (3)C27—C28—C29119.3 (7)
N2—Ru—N388.57 (13)C30—C29—C28120.5 (7)
N1—Ru—C2595.45 (12)C31—C30—C29120.4 (7)
N2—Ru—C2591.43 (13)C30—C31—C32120.0 (7)
N3—Ru—C25180C27—C32—C31120.4 (6)
C4—N1—C1107.1 (4)N3—C33—C34123.9 (8)
C4—N1—Ru127.2 (3)C33—C34—C35119.0 (9)
C1—N1—Ru125.6 (3)C34—C35—C34i117.9 (11)
C6—N2—C9107.1 (4)C3—C2—H1126.1
C6—N2—Ru127.0 (3)C1—C2—H1126.1
C9—N2—Ru125.9 (3)C2—C3—H2125.9
C33—N3—C33i116.4 (9)C4—C3—H2125.9
C33—N3—Ru121.8 (4)C8—C7—H3126.4
C33i—N3—Ru121.8 (4)C6—C7—H3126.4
C10i—C1—N1126.3 (5)C7—C8—H4125.8
C10i—C1—C2125.7 (5)C9—C8—H4125.8
N1—C1—C2108.0 (5)C13—C12—H5119.8
C3—C2—C1107.7 (5)C11—C12—H5119.8
C2—C3—C4108.2 (5)C14—C13—H6119.3
N1—C4—C5124.9 (5)C12—C13—H6119.3
N1—C4—C3108.9 (5)C14—C15—H7119.0
C5—C4—C3126.2 (5)C16—C15—H7119.0
C6—C5—C4126.0 (5)C15—C16—H8119.5
C6—C5—C11117.3 (5)C11—C16—H8119.5
C4—C5—C11116.7 (5)C14—C17—H9109.5
N2—C6—C5125.1 (5)C14—C17—H10109.5
N2—C6—C7109.2 (5)H9—C17—H10109.5
C5—C6—C7125.6 (5)C14—C17—H11109.5
C8—C7—C6107.2 (5)H9—C17—H11109.5
C7—C8—C9108.4 (5)H10—C17—H11109.5
C10—C9—N2125.5 (5)C18—C19—H12119.8
C10—C9—C8126.4 (5)C20—C19—H12119.8
N2—C9—C8108.0 (5)C21—C20—H13118.6
C1i—C10—C9125.9 (5)C19—C20—H13118.6
C1i—C10—C18116.0 (5)C21—C22—H14118.4
C9—C10—C18118.1 (5)C23—C22—H14118.4
C12—C11—C16117.4 (6)C18—C23—H15120.1
C12—C11—C5122.6 (5)C22—C23—H15120.1
C16—C11—C5120.0 (5)C21—C24—H16109.5
C13—C12—C11120.5 (6)C21—C24—H17109.5
C14—C13—C12121.5 (7)H16—C24—H17109.5
C15—C14—C13117.7 (6)C21—C24—H18109.5
C15—C14—C17121.7 (7)H16—C24—H18109.5
C13—C14—C17120.6 (7)H17—C24—H18109.5
C14—C15—C16122.0 (7)C27—C28—H19120.4
C15—C16—C11121.0 (6)C29—C28—H19120.4
C19—C18—C23117.6 (5)C30—C29—H20119.7
C19—C18—C10120.3 (5)C28—C29—H20119.7
C23—C18—C10122.0 (6)C31—C30—H21119.8
C18—C19—C20120.5 (6)C29—C30—H21119.8
C21—C20—C19122.8 (6)C30—C31—H22120.0
C20—C21—C22115.8 (5)C32—C31—H22120.0
C20—C21—C24121.5 (7)C27—C32—H23119.8
C22—C21—C24122.6 (7)C31—C32—H23119.8
C21—C22—C23123.3 (6)N3—C33—H24118.1
C18—C23—C22119.9 (6)C34—C33—H24118.1
C26—C25—C26i116.8 (6)C33—C34—H25120.5
Ru—C25—C26121.6 (3)C35—C34—H25120.5
O—C26—C27120.8 (5)C34—C35—H26121.1
O—C26—C25118.9 (5)
N1—Ru—N3—C33127.1 (4)C26i—C25—C26—C2781.6 (5)
N2—Ru—N3—C3337.4 (4)Ru—C25—C26—C2798.4 (5)
N1—Ru—C25—C26107.1 (3)O—C26—C27—C32168.2 (5)
N2—Ru—C25—C2617.4 (3)C25—C26—C27—C329.3 (8)
C26i—C25—C26—O95.9 (5)O—C26—C27—C2812.6 (8)
Ru—C25—C26—O84.1 (5)C25—C26—C27—C28170.0 (6)
Symmetry code: (i) x+1, y, z+1/2.
(II) (pyridine-κN)(5,10,15,20-tetra-p-tolylporphyrinato-κ4N)[bis(3- trifluoromethylphenyl)carbenyl-κC]ruthenium(II) top
Crystal data top
[Ru(C48H36N4)(C15H8F6)(C5H5N)]F(000) = 2360
Mr = 1151.19Dx = 1.424 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71069 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 12.4428 (17) Åθ = 14.9–15.0°
b = 17.3768 (19) ŵ = 0.36 mm1
c = 25.1794 (17) ÅT = 296 K
β = 99.436 (9)°Prism, dark red
V = 5370.5 (10) Å30.50 × 0.40 × 0.20 mm
Z = 4
Data collection top
Rigaku AFC-7R
diffractometer
8702 reflections with I > 2σ(I)
Radiation source: rotating Mo anticathodeRint = 0.018
Graphite monochromatorθmax = 27.5°, θmin = 2.5°
ω scansh = 016
Absorption correction: ψ scan
(North et al., 1968)
k = 220
Tmin = 0.840, Tmax = 0.930l = 3232
12882 measured reflections3 standard reflections every 150 reflections
12323 independent reflections intensity decay: 0.5%
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)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.108H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0488P)2 + 1.7405P]
where P = (Fo2 + 2Fc2)/3
12323 reflections(Δ/σ)max = 0.001
721 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.30 e Å3
Crystal data top
[Ru(C48H36N4)(C15H8F6)(C5H5N)]V = 5370.5 (10) Å3
Mr = 1151.19Z = 4
Monoclinic, P21/cMo Kα radiation
a = 12.4428 (17) ŵ = 0.36 mm1
b = 17.3768 (19) ÅT = 296 K
c = 25.1794 (17) Å0.50 × 0.40 × 0.20 mm
β = 99.436 (9)°
Data collection top
Rigaku AFC-7R
diffractometer
8702 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.018
Tmin = 0.840, Tmax = 0.9303 standard reflections every 150 reflections
12882 measured reflections intensity decay: 0.5%
12323 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0380 restraints
wR(F2) = 0.108H-atom parameters constrained
S = 1.02Δρmax = 0.32 e Å3
12323 reflectionsΔρmin = 0.30 e Å3
721 parameters
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
Ru0.099529 (15)0.276037 (12)0.112533 (8)0.03681 (6)
F10.1755 (3)0.02171 (17)0.32508 (10)0.1254 (10)
F20.3033 (2)0.0438 (2)0.30258 (10)0.1422 (13)
F30.1773 (3)0.09841 (19)0.33376 (10)0.1470 (13)
F40.3295 (2)0.01272 (15)0.04399 (10)0.1109 (8)
F50.1622 (2)0.00427 (17)0.03831 (10)0.1122 (9)
F60.2485 (3)0.09030 (15)0.07310 (9)0.1177 (9)
N10.05825 (16)0.24049 (13)0.08965 (8)0.0410 (5)
N20.07158 (16)0.28449 (12)0.19014 (8)0.0407 (5)
N30.25141 (16)0.32371 (12)0.13378 (8)0.0400 (5)
N40.12282 (16)0.27647 (12)0.03356 (8)0.0402 (4)
N50.03744 (18)0.40103 (13)0.09832 (9)0.0470 (5)
C10.1032 (2)0.21636 (15)0.03845 (10)0.0434 (6)
C20.2102 (2)0.18622 (17)0.04027 (11)0.0495 (6)
H10.25840.16670.01120.059*
C30.2281 (2)0.19124 (18)0.09123 (11)0.0511 (7)
H20.29070.17540.10390.061*
C40.1332 (2)0.22545 (16)0.12274 (10)0.0435 (6)
C50.1176 (2)0.23684 (16)0.17851 (10)0.0437 (6)
C60.0225 (2)0.26538 (16)0.20932 (10)0.0433 (6)
C70.0056 (2)0.27736 (18)0.26690 (11)0.0541 (7)
H30.05670.26970.28950.065*
C80.0976 (2)0.30171 (18)0.28176 (11)0.0520 (7)
H40.13090.31360.31660.062*
C90.1472 (2)0.30601 (16)0.23391 (10)0.0433 (6)
C100.2538 (2)0.32930 (15)0.23234 (10)0.0422 (6)
C110.3008 (2)0.33989 (15)0.18582 (10)0.0431 (6)
C120.4076 (2)0.37039 (17)0.18433 (11)0.0514 (7)
H50.45820.38550.21390.062*
C130.4212 (2)0.37315 (17)0.13228 (11)0.0517 (7)
H60.48220.39180.11950.062*
C140.3247 (2)0.34220 (15)0.10003 (10)0.0436 (6)
C150.3093 (2)0.32987 (15)0.04438 (10)0.0439 (6)
C160.2162 (2)0.29682 (15)0.01416 (10)0.0424 (6)
C170.2036 (2)0.27733 (16)0.04219 (11)0.0490 (6)
H70.25520.28450.06460.059*
C180.1038 (2)0.24695 (17)0.05628 (11)0.0488 (6)
H80.07350.22930.09030.059*
C190.0521 (2)0.24668 (15)0.00914 (10)0.0423 (6)
C200.0525 (2)0.21902 (15)0.00729 (10)0.0423 (6)
C210.2073 (2)0.20829 (16)0.20679 (10)0.0461 (6)
C220.1905 (2)0.14399 (18)0.23965 (11)0.0513 (7)
H90.12110.12260.24740.062*
C230.2751 (2)0.11093 (18)0.26127 (12)0.0560 (7)
H100.26160.06760.28300.067*
C240.3792 (2)0.14130 (19)0.25103 (12)0.0568 (7)
C250.3950 (2)0.2070 (2)0.21953 (12)0.0584 (8)
H110.46370.22950.21290.070*
C260.3106 (2)0.24026 (18)0.19759 (12)0.0522 (7)
H120.32360.28430.17660.063*
C270.4726 (3)0.1042 (2)0.27239 (16)0.0828 (11)
H130.52050.08030.24330.099*
H140.51190.14270.28880.099*
H150.44500.06600.29870.099*
C280.3276 (2)0.33959 (16)0.28545 (10)0.0450 (6)
C290.3615 (3)0.27619 (18)0.31649 (12)0.0594 (8)
H160.33520.22790.30490.071*
C300.4333 (3)0.2822 (2)0.36432 (13)0.0651 (8)
H170.45520.23820.38420.078*
C310.4728 (2)0.3529 (2)0.38276 (11)0.0583 (8)
C320.4381 (3)0.4163 (2)0.35279 (12)0.0642 (8)
H180.46380.46460.36470.077*
C330.3647 (3)0.41023 (18)0.30450 (12)0.0591 (8)
H190.34090.45440.28520.071*
C340.5538 (3)0.3587 (3)0.43448 (13)0.0837 (12)
H200.54420.31590.45730.100*
H210.54200.40590.45260.100*
H220.62650.35810.42630.100*
C350.3998 (2)0.35308 (16)0.01488 (11)0.0463 (6)
C360.5029 (2)0.32118 (19)0.02690 (13)0.0598 (8)
H230.51670.28370.05350.072*
C370.5858 (2)0.34432 (19)0.00010 (14)0.0631 (8)
H240.65460.32260.00920.076*
C380.5690 (2)0.39871 (19)0.04031 (12)0.0568 (7)
C390.4658 (3)0.42957 (18)0.05300 (12)0.0582 (7)
H250.45170.46590.08040.070*
C400.3825 (2)0.40745 (17)0.02564 (12)0.0536 (7)
H260.31400.42960.03480.064*
C410.6594 (3)0.4239 (2)0.06927 (16)0.0825 (11)
H270.63750.41690.10730.099*
H280.72330.39370.05710.099*
H290.67530.47730.06180.099*
C420.1179 (2)0.18966 (16)0.05901 (10)0.0428 (6)
C430.1274 (3)0.11240 (18)0.06961 (12)0.0599 (8)
H300.09150.07750.04490.072*
C440.1897 (3)0.08560 (18)0.11658 (12)0.0616 (8)
H310.19540.03290.12270.074*
C450.2432 (2)0.13562 (18)0.15431 (10)0.0502 (7)
C460.2329 (3)0.21277 (18)0.14392 (11)0.0585 (8)
H320.26840.24770.16880.070*
C470.1705 (2)0.23992 (17)0.09700 (11)0.0531 (7)
H330.16400.29270.09110.064*
C480.3125 (3)0.1058 (2)0.20524 (13)0.0747 (10)
H340.38160.08880.19730.090*
H350.27600.06350.21910.090*
H360.32390.14620.23160.090*
C490.15061 (19)0.17531 (15)0.12378 (9)0.0399 (5)
C500.1107 (2)0.11845 (15)0.16059 (11)0.0448 (6)
C510.1672 (2)0.10765 (17)0.21242 (11)0.0527 (7)
H370.22750.13820.22480.063*
C520.1348 (3)0.05184 (19)0.24593 (12)0.0604 (8)
C530.0457 (3)0.00593 (19)0.22824 (15)0.0685 (9)
H380.02450.03190.25050.082*
C540.0116 (3)0.01678 (19)0.17714 (16)0.0692 (9)
H390.07180.01400.16500.083*
C550.0195 (2)0.07307 (17)0.14366 (13)0.0568 (7)
H400.02100.08050.10960.068*
C560.1981 (4)0.0427 (3)0.30129 (15)0.0860 (12)
C570.2377 (2)0.14355 (15)0.09600 (11)0.0432 (6)
C580.2099 (2)0.10557 (16)0.04724 (11)0.0499 (6)
H410.13690.09980.03220.060*
C590.2903 (3)0.07613 (17)0.02087 (13)0.0585 (8)
C600.3989 (3)0.0830 (2)0.04397 (16)0.0719 (10)
H420.45300.06280.02660.086*
C610.4264 (3)0.1196 (2)0.09246 (16)0.0736 (10)
H430.49930.12390.10800.088*
C620.3474 (2)0.14995 (18)0.11813 (13)0.0583 (7)
H440.36720.17520.15080.070*
C630.2578 (4)0.0400 (2)0.03295 (16)0.0779 (10)
C640.0862 (3)0.45997 (19)0.12564 (15)0.0674 (9)
H450.14480.44990.15270.081*
C650.0549 (3)0.5351 (2)0.11612 (18)0.0832 (11)
H460.09110.57460.13670.100*
C660.0297 (3)0.5511 (2)0.07625 (16)0.0786 (10)
H470.05200.60160.06870.094*
C670.0806 (3)0.4918 (2)0.04790 (15)0.0812 (11)
H480.13870.50100.02040.097*
C680.0458 (3)0.41744 (19)0.05997 (13)0.0663 (9)
H490.08220.37720.04040.080*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ru0.03286 (10)0.04300 (11)0.03268 (10)0.00014 (9)0.00027 (7)0.00060 (9)
F10.165 (3)0.125 (2)0.0840 (16)0.0253 (19)0.0128 (16)0.0513 (16)
F20.0933 (19)0.254 (4)0.0722 (16)0.027 (2)0.0091 (14)0.057 (2)
F30.241 (4)0.133 (2)0.0640 (15)0.002 (2)0.018 (2)0.0082 (16)
F40.137 (2)0.0966 (18)0.1071 (18)0.0351 (16)0.0434 (16)0.0270 (14)
F50.119 (2)0.136 (2)0.0863 (16)0.0295 (18)0.0292 (14)0.0496 (15)
F60.191 (3)0.1004 (19)0.0668 (14)0.0263 (19)0.0363 (16)0.0059 (13)
N10.0351 (10)0.0504 (13)0.0355 (10)0.0015 (9)0.0007 (8)0.0008 (9)
N20.0354 (10)0.0503 (13)0.0343 (10)0.0004 (9)0.0008 (8)0.0030 (9)
N30.0356 (10)0.0452 (12)0.0372 (10)0.0014 (9)0.0001 (8)0.0021 (9)
N40.0382 (10)0.0450 (11)0.0362 (10)0.0005 (9)0.0023 (8)0.0018 (9)
N50.0448 (12)0.0497 (13)0.0452 (12)0.0057 (10)0.0033 (10)0.0024 (10)
C10.0373 (12)0.0529 (16)0.0366 (12)0.0013 (11)0.0041 (10)0.0013 (11)
C20.0378 (13)0.0641 (18)0.0428 (14)0.0042 (12)0.0046 (11)0.0045 (13)
C30.0362 (13)0.0687 (18)0.0461 (15)0.0051 (13)0.0002 (11)0.0031 (14)
C40.0339 (12)0.0541 (15)0.0413 (13)0.0015 (11)0.0026 (10)0.0019 (12)
C50.0350 (12)0.0529 (16)0.0424 (13)0.0026 (11)0.0039 (10)0.0029 (11)
C60.0364 (12)0.0533 (16)0.0398 (13)0.0022 (11)0.0052 (10)0.0031 (11)
C70.0460 (15)0.077 (2)0.0394 (14)0.0039 (14)0.0071 (11)0.0070 (14)
C80.0468 (15)0.0727 (19)0.0347 (13)0.0021 (13)0.0013 (11)0.0075 (13)
C90.0417 (13)0.0507 (15)0.0348 (12)0.0004 (11)0.0015 (10)0.0033 (11)
C100.0387 (12)0.0455 (14)0.0389 (13)0.0003 (11)0.0034 (10)0.0028 (11)
C110.0376 (12)0.0467 (15)0.0415 (13)0.0005 (11)0.0033 (10)0.0029 (11)
C120.0410 (14)0.0594 (17)0.0494 (15)0.0081 (12)0.0055 (12)0.0011 (13)
C130.0420 (14)0.0581 (17)0.0524 (16)0.0089 (13)0.0000 (12)0.0057 (13)
C140.0385 (13)0.0455 (15)0.0447 (14)0.0029 (11)0.0004 (10)0.0046 (11)
C150.0404 (13)0.0439 (14)0.0462 (14)0.0027 (11)0.0037 (11)0.0083 (11)
C160.0427 (13)0.0423 (14)0.0413 (13)0.0022 (11)0.0045 (11)0.0044 (11)
C170.0518 (15)0.0555 (16)0.0408 (14)0.0010 (13)0.0105 (11)0.0043 (12)
C180.0546 (16)0.0548 (16)0.0359 (13)0.0013 (13)0.0042 (12)0.0001 (12)
C190.0441 (14)0.0446 (14)0.0359 (12)0.0033 (11)0.0010 (10)0.0020 (10)
C200.0430 (13)0.0463 (14)0.0345 (12)0.0033 (11)0.0027 (10)0.0021 (11)
C210.0373 (13)0.0614 (18)0.0387 (13)0.0013 (12)0.0040 (10)0.0054 (12)
C220.0400 (14)0.0650 (19)0.0488 (15)0.0061 (13)0.0071 (12)0.0011 (13)
C230.0579 (17)0.0563 (18)0.0535 (17)0.0002 (14)0.0083 (14)0.0011 (14)
C240.0481 (16)0.069 (2)0.0545 (17)0.0120 (14)0.0114 (13)0.0113 (15)
C250.0353 (14)0.080 (2)0.0587 (17)0.0032 (14)0.0050 (12)0.0100 (16)
C260.0425 (14)0.0620 (18)0.0509 (16)0.0032 (13)0.0037 (12)0.0004 (13)
C270.061 (2)0.099 (3)0.092 (3)0.014 (2)0.0233 (19)0.005 (2)
C280.0378 (13)0.0569 (16)0.0378 (13)0.0028 (12)0.0014 (10)0.0013 (12)
C290.0632 (18)0.0551 (17)0.0525 (16)0.0013 (15)0.0123 (14)0.0001 (14)
C300.0636 (19)0.073 (2)0.0519 (17)0.0071 (17)0.0120 (14)0.0051 (16)
C310.0438 (15)0.090 (2)0.0385 (14)0.0006 (15)0.0002 (12)0.0071 (15)
C320.068 (2)0.068 (2)0.0523 (17)0.0153 (16)0.0038 (15)0.0139 (15)
C330.0686 (19)0.0535 (18)0.0507 (16)0.0047 (15)0.0037 (14)0.0001 (14)
C340.060 (2)0.139 (4)0.0456 (18)0.006 (2)0.0105 (15)0.010 (2)
C350.0424 (14)0.0509 (16)0.0454 (14)0.0022 (12)0.0062 (11)0.0043 (12)
C360.0511 (16)0.063 (2)0.0654 (19)0.0079 (14)0.0114 (14)0.0171 (16)
C370.0437 (15)0.070 (2)0.077 (2)0.0100 (15)0.0147 (15)0.0049 (17)
C380.0519 (17)0.0621 (19)0.0594 (18)0.0056 (14)0.0177 (14)0.0032 (15)
C390.0605 (18)0.0587 (18)0.0562 (17)0.0047 (15)0.0115 (14)0.0128 (14)
C400.0466 (15)0.0564 (17)0.0576 (17)0.0058 (13)0.0084 (13)0.0114 (14)
C410.068 (2)0.094 (3)0.092 (3)0.010 (2)0.034 (2)0.003 (2)
C420.0395 (13)0.0535 (15)0.0332 (12)0.0001 (11)0.0007 (10)0.0007 (11)
C430.0683 (19)0.0545 (18)0.0495 (16)0.0107 (15)0.0117 (14)0.0004 (13)
C440.074 (2)0.0494 (17)0.0550 (17)0.0077 (15)0.0074 (15)0.0110 (14)
C450.0458 (14)0.0672 (19)0.0360 (13)0.0027 (13)0.0018 (11)0.0051 (12)
C460.0634 (18)0.064 (2)0.0416 (15)0.0024 (15)0.0093 (13)0.0121 (13)
C470.0638 (18)0.0452 (16)0.0462 (15)0.0008 (13)0.0032 (13)0.0056 (12)
C480.077 (2)0.092 (3)0.0481 (17)0.005 (2)0.0081 (16)0.0104 (17)
C490.0361 (12)0.0438 (14)0.0370 (12)0.0012 (11)0.0021 (10)0.0008 (10)
C500.0439 (14)0.0434 (14)0.0479 (14)0.0006 (11)0.0095 (11)0.0011 (11)
C510.0538 (16)0.0574 (17)0.0471 (15)0.0079 (13)0.0090 (13)0.0024 (13)
C520.0663 (19)0.064 (2)0.0546 (17)0.0023 (16)0.0203 (15)0.0112 (15)
C530.072 (2)0.0575 (19)0.083 (2)0.0083 (16)0.0317 (19)0.0135 (17)
C540.0554 (18)0.0569 (19)0.096 (3)0.0153 (15)0.0159 (18)0.0043 (18)
C550.0470 (16)0.0545 (18)0.0679 (19)0.0045 (13)0.0063 (14)0.0008 (15)
C560.108 (3)0.099 (3)0.054 (2)0.012 (3)0.022 (2)0.015 (2)
C570.0422 (13)0.0390 (13)0.0485 (14)0.0013 (11)0.0078 (11)0.0070 (11)
C580.0486 (15)0.0481 (16)0.0536 (16)0.0021 (12)0.0104 (12)0.0040 (13)
C590.069 (2)0.0481 (17)0.0644 (19)0.0068 (14)0.0272 (16)0.0036 (14)
C600.060 (2)0.064 (2)0.101 (3)0.0096 (16)0.039 (2)0.006 (2)
C610.0420 (16)0.074 (2)0.105 (3)0.0040 (15)0.0127 (18)0.002 (2)
C620.0431 (15)0.0601 (19)0.0693 (19)0.0021 (13)0.0023 (14)0.0007 (15)
C630.101 (3)0.065 (2)0.076 (2)0.005 (2)0.038 (2)0.0052 (19)
C640.0604 (19)0.0540 (19)0.081 (2)0.0046 (15)0.0078 (16)0.0046 (16)
C650.082 (3)0.052 (2)0.110 (3)0.0036 (18)0.000 (2)0.006 (2)
C660.095 (3)0.052 (2)0.089 (3)0.0221 (19)0.015 (2)0.0097 (19)
C670.086 (3)0.077 (3)0.073 (2)0.029 (2)0.0115 (19)0.0038 (19)
C680.071 (2)0.061 (2)0.0607 (19)0.0152 (16)0.0086 (16)0.0021 (15)
Geometric parameters (Å, º) top
Ru—N12.049 (2)C47—C421.379 (4)
Ru—N22.046 (2)C45—C481.514 (4)
Ru—N32.052 (2)C49—C501.494 (4)
Ru—N42.056 (2)C49—C571.489 (3)
Ru—N52.313 (2)C50—C511.390 (4)
Ru—C491.868 (3)C51—C521.388 (4)
F1—C561.321 (4)C52—C531.379 (5)
F2—C561.304 (5)C53—C541.378 (5)
F3—C561.321 (5)C54—C551.387 (4)
F4—C631.340 (4)C55—C501.390 (4)
F5—C631.329 (4)C52—C561.493 (5)
F6—C631.327 (4)C57—C581.387 (4)
N1—C11.383 (3)C58—C591.386 (4)
N1—C41.374 (3)C59—C601.387 (5)
N2—C61.378 (3)C60—C611.369 (5)
N2—C91.378 (3)C61—C621.368 (4)
N3—C111.382 (3)C62—C571.391 (4)
N3—C141.383 (3)C59—C631.488 (5)
N4—C161.378 (3)C64—C651.373 (5)
N4—C191.374 (3)C65—C661.359 (5)
N5—C641.324 (4)C66—C671.351 (5)
N5—C681.326 (3)C67—C681.380 (5)
C1—C21.439 (4)C2—H10.9300
C2—C31.341 (4)C3—H20.9300
C3—C41.439 (3)C7—H30.9300
C4—C51.400 (3)C8—H40.9300
C5—C61.395 (3)C12—H50.9300
C6—C71.446 (4)C13—H60.9300
C7—C81.345 (4)C17—H70.9300
C8—C91.443 (4)C18—H80.9300
C9—C101.394 (3)C22—H90.9300
C10—C111.404 (4)C23—H100.9300
C11—C121.437 (4)C25—H110.9300
C12—C131.350 (4)C26—H120.9300
C13—C141.439 (3)C27—H130.9600
C14—C151.399 (4)C27—H140.9600
C15—C161.401 (4)C27—H150.9600
C16—C171.442 (4)C29—H160.9300
C17—C181.343 (4)C30—H170.9300
C18—C191.440 (4)C32—H180.9300
C19—C201.396 (4)C33—H190.9300
C20—C11.401 (4)C34—H200.9600
C5—C211.504 (4)C34—H210.9600
C21—C221.386 (4)C34—H220.9600
C22—C231.387 (4)C36—H230.9300
C23—C241.384 (4)C37—H240.9300
C24—C251.386 (4)C39—H250.9300
C25—C261.389 (4)C40—H260.9300
C26—C211.384 (4)C41—H270.9600
C24—C271.503 (4)C41—H280.9600
C10—C281.504 (3)C41—H290.9600
C28—C291.376 (4)C43—H300.9300
C29—C301.381 (4)C44—H310.9300
C30—C311.375 (5)C46—H320.9300
C31—C321.365 (5)C47—H330.9300
C32—C331.400 (4)C48—H340.9600
C33—C281.370 (4)C48—H350.9600
C31—C341.514 (4)C48—H360.9600
C15—C351.502 (4)C51—H370.9300
C35—C361.385 (4)C53—H380.9300
C36—C371.385 (4)C54—H390.9300
C37—C381.376 (4)C55—H400.9300
C38—C391.380 (4)C58—H410.9300
C39—C401.389 (4)C60—H420.9300
C40—C351.381 (4)C61—H430.9300
C38—C411.503 (4)C62—H440.9300
C20—C421.507 (3)C64—H450.9300
C42—C431.370 (4)C65—H460.9300
C43—C441.384 (4)C66—H470.9300
C44—C451.376 (4)C67—H480.9300
C45—C461.368 (4)C68—H490.9300
C46—C471.386 (4)
N1—Ru—N289.15 (8)C54—C55—C50120.6 (3)
N1—Ru—N3173.72 (8)F2—C56—F3105.8 (4)
N1—Ru—N490.55 (8)F2—C56—F1106.8 (4)
N2—Ru—N390.89 (8)F3—C56—F1105.2 (3)
N2—Ru—N4175.36 (8)F2—C56—C52113.3 (3)
N3—Ru—N488.90 (8)F3—C56—C52111.9 (4)
N1—Ru—N587.66 (8)F1—C56—C52113.3 (4)
N2—Ru—N588.60 (8)C58—C57—C62118.6 (3)
N3—Ru—N586.06 (8)C58—C57—C49119.8 (2)
N4—Ru—N586.75 (8)C62—C57—C49121.6 (2)
C49—Ru—N192.68 (10)C59—C58—C57120.3 (3)
C49—Ru—N291.69 (10)C58—C59—C60119.9 (3)
C49—Ru—N393.60 (9)C58—C59—C63118.8 (3)
C49—Ru—N492.96 (10)C60—C59—C63121.3 (3)
C49—Ru—N5179.56 (10)C61—C60—C59119.9 (3)
C4—N1—C1107.3 (2)C62—C61—C60120.4 (3)
C4—N1—Ru126.97 (16)C61—C62—C57120.9 (3)
C1—N1—Ru125.14 (17)F6—C63—F5105.4 (4)
C6—N2—C9107.0 (2)F6—C63—F4105.7 (3)
C6—N2—Ru127.21 (16)F5—C63—F4105.9 (3)
C9—N2—Ru125.65 (17)F6—C63—C59113.2 (3)
C11—N3—C14107.5 (2)F5—C63—C59113.3 (3)
C11—N3—Ru125.21 (16)F4—C63—C59112.7 (3)
C14—N3—Ru127.28 (16)N5—C64—C65123.5 (3)
C19—N4—C16106.8 (2)C66—C65—C64119.1 (4)
C19—N4—Ru125.58 (17)C67—C66—C65118.2 (3)
C16—N4—Ru127.18 (16)C66—C67—C68119.7 (3)
C64—N5—C68116.7 (3)N5—C68—C67122.7 (3)
C64—N5—Ru122.20 (19)C1—C2—H1126.1
C68—N5—Ru121.0 (2)C3—C2—H1126.1
N1—C1—C20126.1 (2)C2—C3—H2126.1
N1—C1—C2108.4 (2)C4—C3—H2126.1
C20—C1—C2125.6 (2)C8—C7—H3126.3
C3—C2—C1107.9 (2)C6—C7—H3126.3
C2—C3—C4107.7 (2)C7—C8—H4126.2
N1—C4—C5125.8 (2)C9—C8—H4126.2
N1—C4—C3108.8 (2)C13—C12—H5126.2
C5—C4—C3125.4 (2)C11—C12—H5126.2
C6—C5—C4125.0 (2)C12—C13—H6126.0
C6—C5—C21118.8 (2)C14—C13—H6126.0
C4—C5—C21115.9 (2)C18—C17—H7126.3
N2—C6—C5125.6 (2)C16—C17—H7126.3
N2—C6—C7108.9 (2)C17—C18—H8126.2
C5—C6—C7125.4 (2)C19—C18—H8126.2
C8—C7—C6107.4 (2)C21—C22—H9119.4
C7—C8—C9107.6 (2)C23—C22—H9119.4
N2—C9—C10125.7 (2)C24—C23—H10119.4
N2—C9—C8108.9 (2)C22—C23—H10119.4
C10—C9—C8125.3 (2)C24—C25—H11119.2
C9—C10—C11126.2 (2)C26—C25—H11119.2
C9—C10—C28117.1 (2)C21—C26—H12119.7
C11—C10—C28116.7 (2)C25—C26—H12119.7
N3—C11—C10125.7 (2)C24—C27—H13109.5
N3—C11—C12108.6 (2)C24—C27—H14109.5
C10—C11—C12125.7 (2)H13—C27—H14109.5
C13—C12—C11107.6 (2)C24—C27—H15109.5
C12—C13—C14108.0 (2)H13—C27—H15109.5
N3—C14—C15125.7 (2)H14—C27—H15109.5
N3—C14—C13108.3 (2)C28—C29—H16119.1
C15—C14—C13125.9 (2)C30—C29—H16119.1
C14—C15—C16124.9 (2)C31—C30—H17119.8
C14—C15—C35117.6 (2)C29—C30—H17119.8
C16—C15—C35117.5 (2)C31—C32—H18119.3
N4—C16—C15125.7 (2)C33—C32—H18119.3
N4—C16—C17109.1 (2)C28—C33—H19119.8
C15—C16—C17125.3 (2)C32—C33—H19119.8
C18—C17—C16107.4 (2)C31—C34—H20109.5
C17—C18—C19107.6 (2)C31—C34—H21109.5
N4—C19—C20125.8 (2)H20—C34—H21109.5
N4—C19—C18109.2 (2)C31—C34—H22109.5
C20—C19—C18125.0 (2)H20—C34—H22109.5
C19—C20—C1125.9 (2)H21—C34—H22109.5
C19—C20—C42117.5 (2)C37—C36—H23119.5
C1—C20—C42116.6 (2)C35—C36—H23119.5
C26—C21—C22118.0 (3)C38—C37—H24119.2
C26—C21—C5122.0 (3)C36—C37—H24119.2
C22—C21—C5119.8 (2)C38—C39—H25119.4
C21—C22—C23121.2 (3)C40—C39—H25119.4
C24—C23—C22121.1 (3)C35—C40—H26119.4
C23—C24—C25117.5 (3)C39—C40—H26119.4
C23—C24—C27121.7 (3)C38—C41—H27109.5
C25—C24—C27120.9 (3)C38—C41—H28109.5
C24—C25—C26121.6 (3)H27—C41—H28109.5
C21—C26—C25120.5 (3)C38—C41—H29109.5
C33—C28—C29117.7 (2)H27—C41—H29109.5
C33—C28—C10122.6 (3)H28—C41—H29109.5
C29—C28—C10119.7 (2)C42—C43—H30119.5
C28—C29—C30121.9 (3)C44—C43—H30119.5
C31—C30—C29120.5 (3)C45—C44—H31119.4
C32—C31—C30118.1 (3)C43—C44—H31119.4
C32—C31—C34121.8 (3)C45—C46—H32119.4
C30—C31—C34120.0 (3)C47—C46—H32119.4
C31—C32—C33121.4 (3)C42—C47—H33119.6
C28—C33—C32120.4 (3)C46—C47—H33119.6
C40—C35—C36117.5 (3)C45—C48—H34109.5
C40—C35—C15120.7 (2)C45—C48—H35109.5
C36—C35—C15121.8 (2)H34—C48—H35109.5
C37—C36—C35121.0 (3)C45—C48—H36109.5
C38—C37—C36121.7 (3)H34—C48—H36109.5
C37—C38—C39117.5 (3)H35—C48—H36109.5
C37—C38—C41121.4 (3)C52—C51—H37119.6
C39—C38—C41121.1 (3)C50—C51—H37119.6
C38—C39—C40121.3 (3)C54—C53—H38120.4
C35—C40—C39121.2 (3)C52—C53—H38120.4
C43—C42—C47118.0 (2)C53—C54—H39119.6
C43—C42—C20121.1 (2)C55—C54—H39119.6
C47—C42—C20120.8 (3)C54—C55—H40119.7
C42—C43—C44121.0 (3)C50—C55—H40119.7
C45—C44—C43121.2 (3)C59—C58—H41119.8
C46—C45—C44117.8 (3)C57—C58—H41119.8
C46—C45—C48121.3 (3)C61—C60—H42120.1
C44—C45—C48120.8 (3)C59—C60—H42120.1
C45—C46—C47121.3 (3)C62—C61—H43119.8
C42—C47—C46120.8 (3)C60—C61—H43119.8
C50—C49—C57112.8 (2)C61—C62—H44119.5
Ru—C49—C50125.04 (18)C57—C62—H44119.5
Ru—C49—C57122.13 (18)N5—C64—H45118.2
C55—C50—C51118.2 (3)C65—C64—H45118.2
C55—C50—C49121.5 (2)C66—C65—H46120.4
C51—C50—C49120.2 (2)C64—C65—H46120.4
C52—C51—C50120.8 (3)C67—C66—H47120.9
C53—C52—C51120.4 (3)C65—C66—H47120.9
C53—C52—C56120.9 (3)C66—C67—H48120.2
C51—C52—C56118.7 (3)C68—C67—H48120.2
C54—C53—C52119.2 (3)N5—C68—H49118.6
C53—C54—C55120.7 (3)C67—C68—H49118.6
C49—Ru—N1—C486.4 (2)C14—C15—C35—C40119.7 (3)
N5—Ru—N1—C493.9 (2)C16—C15—C35—C4060.9 (4)
C49—Ru—N1—C183.4 (2)C19—C20—C42—C43100.9 (3)
N5—Ru—N1—C196.3 (2)C1—C20—C42—C4379.5 (3)
C49—Ru—N2—C689.3 (2)C19—C20—C42—C4779.5 (3)
N5—Ru—N2—C691.0 (2)C1—C20—C42—C47100.2 (3)
C49—Ru—N2—C986.1 (2)N1—Ru—C49—C57123.7 (2)
N5—Ru—N2—C993.5 (2)N2—Ru—C49—C57147.1 (2)
C49—Ru—N3—C1184.6 (2)N3—Ru—C49—C5756.1 (2)
N5—Ru—N3—C1195.7 (2)N4—Ru—C49—C5733.0 (2)
C49—Ru—N3—C1492.2 (2)N1—Ru—C49—C5056.4 (2)
N5—Ru—N3—C1487.5 (2)N2—Ru—C49—C5032.8 (2)
C49—Ru—N4—C1688.4 (2)N3—Ru—C49—C50123.8 (2)
N5—Ru—N4—C1691.3 (2)N4—Ru—C49—C50147.1 (2)
C49—Ru—N4—C1982.5 (2)C57—C49—C50—C5182.8 (3)
N5—Ru—N4—C1997.9 (2)Ru—C49—C50—C5197.1 (3)
N1—Ru—N5—C64150.7 (3)C57—C49—C50—C5594.6 (3)
N2—Ru—N5—C6461.5 (3)Ru—C49—C50—C5585.5 (3)
N3—Ru—N5—C6429.5 (3)C51—C52—C56—F1166.2 (3)
N4—Ru—N5—C64118.6 (3)C53—C52—C56—F113.9 (6)
N1—Ru—N5—C6833.1 (2)C51—C52—C56—F244.3 (5)
N2—Ru—N5—C68122.3 (2)C53—C52—C56—F2135.7 (4)
N3—Ru—N5—C68146.7 (2)C51—C52—C56—F375.1 (5)
N4—Ru—N5—C6857.6 (2)C53—C52—C56—F3104.8 (4)
C4—C5—C21—C22108.7 (3)C50—C49—C57—C5888.7 (3)
C6—C5—C21—C2265.4 (4)Ru—C49—C57—C5891.4 (3)
C4—C5—C21—C2665.6 (4)C50—C49—C57—C6290.4 (3)
C6—C5—C21—C26120.3 (3)Ru—C49—C57—C6289.5 (3)
C5—C21—C22—C23172.4 (3)C58—C59—C63—F4153.5 (3)
C5—C21—C26—C25172.6 (3)C60—C59—C63—F428.7 (5)
C9—C10—C28—C2969.6 (4)C58—C59—C63—F533.3 (5)
C11—C10—C28—C29106.9 (3)C60—C59—C63—F5149.0 (3)
C9—C10—C28—C33111.2 (3)C58—C59—C63—F686.7 (4)
C11—C10—C28—C3372.2 (4)C60—C59—C63—F691.1 (4)
C14—C15—C35—C3660.4 (4)Ru—N5—C64—C65176.4 (3)
C16—C15—C35—C36119.0 (3)Ru—N5—C68—C67175.6 (3)

Experimental details

(I)(II)
Crystal data
Chemical formula[Ru(C48H36N4)(C15H10O2)(C5H5N)][Ru(C48H36N4)(C15H8F6)(C5H5N)]
Mr1071.211151.19
Crystal system, space groupMonoclinic, C2/cMonoclinic, P21/c
Temperature (K)296296
a, b, c (Å)15.806 (2), 16.6172 (18), 20.644 (2)12.4428 (17), 17.3768 (19), 25.1794 (17)
β (°) 95.872 (10) 99.436 (9)
V3)5393.7 (10)5370.5 (10)
Z44
Radiation typeMo KαMo Kα
µ (mm1)0.340.36
Crystal size (mm)0.20 × 0.12 × 0.100.50 × 0.40 × 0.20
Data collection
DiffractometerRigaku AFC-7R
diffractometer
Rigaku AFC-7R
diffractometer
Absorption correctionψ scan
(North et al., 1968)
Tmin, Tmax0.840, 0.930
No. of measured, independent and
observed [I > 2σ(I)] reflections
6419, 6197, 2792 12882, 12323, 8702
Rint0.0480.018
(sin θ/λ)max1)0.6500.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.061, 0.182, 0.97 0.038, 0.108, 1.02
No. of reflections619712323
No. of parameters345721
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.64, 0.510.32, 0.30

Computer programs: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1993), MSC/AFC Diffractometer Control Software, CrystalStructure (Molecular Structure Corporation & Rigaku Corporation, 2001), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), SHELXL97.

Selected geometric parameters (Å, º) for (I) top
Ru—N12.038 (4)O—C261.228 (6)
Ru—N22.049 (4)C25—C261.498 (6)
Ru—N32.329 (7)C26—C271.479 (8)
Ru—C251.877 (8)
N1—Ru—N1i169.1 (2)N1—Ru—C2595.45 (12)
N1—Ru—N289.57 (15)N2—Ru—C2591.43 (13)
N1—Ru—N2i90.16 (15)N3—Ru—C25180
N1—Ru—N384.55 (12)C26—C25—C26i116.8 (6)
N2i—Ru—N2177.1 (3)Ru—C25—C26121.6 (3)
N2—Ru—N388.57 (13)
Symmetry code: (i) x+1, y, z+1/2.
Selected geometric parameters (Å, º) for (II) top
Ru—N12.049 (2)Ru—N42.056 (2)
Ru—N22.046 (2)Ru—N52.313 (2)
Ru—N32.052 (2)Ru—C491.868 (3)
N1—Ru—N289.15 (8)N4—Ru—N586.75 (8)
N1—Ru—N3173.72 (8)C49—Ru—N192.68 (10)
N1—Ru—N490.55 (8)C49—Ru—N291.69 (10)
N2—Ru—N390.89 (8)C49—Ru—N393.60 (9)
N2—Ru—N4175.36 (8)C49—Ru—N492.96 (10)
N3—Ru—N488.90 (8)C49—Ru—N5179.56 (10)
N1—Ru—N587.66 (8)C50—C49—C57112.8 (2)
N2—Ru—N588.60 (8)Ru—C49—C50125.04 (18)
N3—Ru—N586.06 (8)Ru—C49—C57122.13 (18)
 

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