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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Dec 16;66(Pt 1):m66–m67. doi: 10.1107/S1600536809052726

mer-Bis[3,5-difluoro-2-(2-pyrid­yl)phenyl-κ2 C 1,N]{5-(2-pyridyl-κN)-3-[3-(4-vinyl­benz­yloxy)phen­yl]-1,2,4-triazol-1-ido}iridium(III) methanol solvate

Peter G Jones a,*, Marc Debeaux b, Andreas Weinkauf a, Henning Hopf c, Wolfgang Kowalsky b, Hans-Hermann Johannes b
PMCID: PMC2980050  PMID: 21579961

Abstract

In the title compound, [Ir(C11H6F2N)2(C22H17N4O)]·CH3OH, the coordination at iridium is essentially octa­hedral, but with distortions associated with the bite angles of the ligands [76.25 (9)–80.71 (12)°] and the differing trans influences of C and N ligands [Ir—N = 2.04 Å (average) trans to N but 2.14 Å trans to C]. All three bidentate ligands have coordinating ring systems that are almost coplanar [inter­planar angles = 1.7 (1)–3.8 (2)°]. The vinyl­benzyl group is disordered over two positions with occupations of 0.653 (4) and 0.347 (4). The methanol solvent mol­ecule is involved in a classical O—H⋯N hydrogen bond to a triazole N atom.

Related literature

For background to organic light-emitting diodes (OLEDs), see: Adachi et al. (2001); Baldo et al. (1998); Burroughes et al. (1990); Chang et al. (2007); Coppo et al. (2004); Dedeian et al. (1991); Dixon et al. (2000); Gong et al. (2002); Grushin et al. (2001); Lamansky et al. (2001); Schütz et al. (2008); Suzuki et al. (2005); Tang & VanSlyke (1987); You & Park (2005). graphic file with name e-66-00m66-scheme1.jpg

Experimental

Crystal data

  • [Ir(C11H6F2N)2(C22H17N4O)]·CH4O

  • M r = 957.97

  • Triclinic, Inline graphic

  • a = 9.8934 (1) Å

  • b = 12.3039 (2) Å

  • c = 16.8933 (3) Å

  • α = 81.7429 (14)°

  • β = 83.2858 (11)°

  • γ = 69.9647 (14)°

  • V = 1906.82 (5) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 3.57 mm−1

  • T = 100 K

  • 0.20 × 0.15 × 0.10 mm

Data collection

  • Oxford Diffraction Xcalibur E diffractometer

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008) T min = 0.848, T max = 1.000

  • 53102 measured reflections

  • 10448 independent reflections

  • 8442 reflections with I > 2σ(I)

  • R int = 0.034

Refinement

  • R[F 2 > 2σ(F 2)] = 0.029

  • wR(F 2) = 0.064

  • S = 0.93

  • 10448 reflections

  • 538 parameters

  • 69 restraints

  • H-atom parameters constrained

  • Δρmax = 2.18 e Å−3

  • Δρmin = −0.84 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2008); cell refinement: CrysAlis RED (Oxford Diffraction, 2008); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP (Siemens, 1994); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809052726/tk2595sup1.cif

e-66-00m66-sup1.cif (41.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809052726/tk2595Isup2.hkl

e-66-00m66-Isup2.hkl (510.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

Ir—C11 2.010 (3)
Ir—C22 2.012 (3)
Ir—N1 2.033 (2)
Ir—N2 2.049 (2)
Ir—N4 2.118 (2)
Ir—N3 2.158 (2)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O99—H99⋯N6 0.84 2.04 2.853 (3) 164
C24—H24⋯O99 0.95 2.49 3.368 (4) 154
C31—H31⋯O99 0.95 2.66 3.587 (4) 164

Acknowledgments

The authors thank the Bundesministerium für Bildung und Forschung (BMBF 01 BD 0687) for financial support.

supplementary crystallographic information

Comment

Since Tang and VanSlyke (1987) reported on the first organic light-emitting diode (OLED) based on the electroluminescence of tris(8-hydroxyquinoline)aluminium, and Burroughes et al. (1990) discovered a device with an electroluminescent organic polymer (PLED), OLEDs have attracted much attention because of their application in flat-panel and large-area displays (Burroughes et al., 1990; Tang & VanSlyke, 1987). By incorporation of phosphorescent organometallic complexes of transition metals with a strong spin-orbit coupling, electroluminescent quantum efficiencies up to 100% can be achieved (Baldo et al., 1998; Gong et al., 2002). Among these heavy metals, iridium(III)-based complexes are especially attractive because of their highly tunable emission colors and relatively short phosphorescence lifetimes (Dixon et al., 2000; Lamansky et al., 2001).

Homo- and heteroleptic iridium(III) complexes are versatile and readily available. The emission colour of heteroleptic complexes can be tuned by varying the two monoanionic cyclometalating ligands (Dedeian et al., 1991; Grushin et al., 2001) and/or the third ligand (Chang et al., 2007; You et al., 2005). For example, the replacement of the picolinate by a triazolylpyridine ligand in the well known "blue" emitting FIrpic leads to a hypsochromically shifted phosphorescence (Adachi et al., 2001; Coppo et al., 2004).

In terms of large scale fabrication, the easiness and inexpensiveness of wet processes such as spin coating, dip coating or ink-jet printing of PLEDs represent important advantages over vacuum techniques. Chemically attaching emitter moieties to the polymer matrix can prevent degradation processes clearly caused by phase separation (Suzuki et al., 2005). Furthermore, the covalent attachment also prevents cascading energy transfer through steric shielding (Schütz et al., 2008).

In this contribution, we report the structure of a styrene-functionalized, cyan-emitting complex that can be incorporated in an ambipolar polymer approach (Suzuki et al., 2005). The structure of the title complex, which crystallizes as a methanol solvate, is shown in Fig. 1. The vinylbenzyl group is disordered over two positions with occupations 0.653 (4), 0.347 (4); this is shown in Fig. 2. The coordination at iridium is essentially octahedral, but with some distortions associated with the restricted bite of the bidentate ligands; C11—Ir—N1 80.20 (11), C22—Ir —N2 80.71 (12), and N4—Ir—N3 76.25 (9)°. All five-membered chelate rings are planar (max. r.m.s.d. 0.019 Å) and mutually perpendicular (max. deviation 3°). Interplanar angles between the coordinating rings of each ligand are small: 3.8 (2)° in the ligand based on N1/C11, 3.4 (2)° for N2/C22, and 1.7 (1)° for N3/N4.

The bond lengths, Table 1, at Ir reflect the different trans influences of C and N ligands, although the significant difference between the two Ir—N bond lengths trans to C has no obvious explanation.

Hydrogen bonds are listed in Table 2. The methanol molecule is linked to an N atom of the triazole ring via a classical H bond. The contacts H24···O99 and H31···O99 may also be interpreted as weak H bonds within the asymmetric unit, but are not drawn explicitly in Fig. 1.

Experimental

A suspension of bis[3,5-difluoro-2-(pyridin-2-yl-κN)phenyl]-[3-(3-hydroxyphenyl)-5-(pyridin-2-yl-κN)-1,2,4-triazol-1-yl]-iridium(III) (400 mg, 494 µmol) in dry DMF (5 ml) was treated with sodium hydride (60% dispersion in mineral oil, 40 mg, 988 µmol) and stirred for 30 min at room temperature. 1-(Chloromethyl)-4-vinylbenzene (151 mg, 988 µmol) was added and stirred for 1 d at room temperature. The solvent was removed under reduced pressure at 373 K. The product was isolated from the residue by flash chromatography on silica gel (dichloromethane/acetone 4:1; Rf = 0.40) as a yellow solid (255 mg, 56%). Single crystals were grown from dichloromethane/methanol solution. Elemental analysis: calculated for C44H29F4IrN6O: C 57.07, H 3.16, N 9.08%; found: C 57.06, H 3.04, N 8.82%.

Refinement

Methyl- and hydroxyl-H atoms were identified in a difference synthesis and refined as idealized rigid groups allowed to rotate but not tip (C—H 0.98, O—H 0.84 Å, H—C—H and C—O—H angles 109.5°). These U(H) values were fixed at 1.5 × Ueq(C) of the parent C or O atom. Other hydrogen atoms were included at calculated positions using a riding model with C—H distances in Å as follows; aromatic C—H and C═CH2 0.95, methylene 0.99. These U(H) values were fixed at 1.2 × Ueq(C) of the parent C atom.

The atoms C36–C44 (the vinylbenzyl group) are disordered over two positions rotated about the O—C32 bond, with refined occupancies 0.653 (4) and 0.347 (4). The less occupied group was refined isotropically. For the disordered group, rigid idealized aromatic rings (C—C 1.395, C—H 0.95 Å and all angles 120°), similarity restraints and and a system of restraints to U values were employed to improve refinement stability, but nevertheless the dimensions of the disordered group should be interpreted with caution.

There are several peaks of 1.5–2.2 e Å-3ca 0.8 Å from the Ir atom; these may reasonably be attributed to residual absorption errors.

Figures

Fig. 1.

Fig. 1.

Structure of the title complex. Displacement ellipsoids represent 50% probability levels. The dashed line represents the classical H bond H99···N6. The minor disorder component is omitted.

Fig. 2.

Fig. 2.

Detail of the structure, showing both disorder components of the vinylbenzyl group. Atoms C32 and O are ordered. The minor component is shown as dashed bonds/atoms. Only the major component is labelled.

Crystal data

[Ir(C11H6F2N)2(C22H17N4O)]·CH4O Z = 2
Mr = 957.97 F(000) = 948
Triclinic, P1 Dx = 1.668 Mg m3
Hall symbol: -P 1 Melting point: 560 K
a = 9.8934 (1) Å Mo Kα radiation, λ = 0.71073 Å
b = 12.3039 (2) Å Cell parameters from 25891 reflections
c = 16.8933 (3) Å θ = 2.0–30.7°
α = 81.7429 (14)° µ = 3.57 mm1
β = 83.2858 (11)° T = 100 K
γ = 69.9647 (14)° Prism, yellow
V = 1906.82 (5) Å3 0.20 × 0.15 × 0.10 mm

Data collection

Oxford Diffraction Xcalibur E diffractometer 10448 independent reflections
Radiation source: Enhance (Mo) X-ray Source 8442 reflections with I > 2σ(I)
graphite Rint = 0.034
Detector resolution: 16.1419 pixels mm-1 θmax = 29.6°, θmin = 2.0°
ω scan h = −13→13
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008) k = −17→17
Tmin = 0.848, Tmax = 1.000 l = −23→23
53102 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.029 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.064 H-atom parameters constrained
S = 0.93 w = 1/[σ2(Fo2) + (0.0374P)2] where P = (Fo2 + 2Fc2)/3
10448 reflections (Δ/σ)max = 0.028
538 parameters Δρmax = 2.18 e Å3
69 restraints Δρmin = −0.84 e Å3

Special details

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.Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)3.2255 (0.0106) x + 5.5173 (0.0081) y + 15.8973 (0.0047) z = 8.4546 (0.0089)* -0.0191 (0.0010) Ir * 0.0215 (0.0015) N3 * 0.0244 (0.0015) N4 * -0.0109 (0.0018) C23 * -0.0159 (0.0018) C28Rms deviation of fitted atoms = 0.0190- 5.0032 (0.0075) x + 7.5842 (0.0079) y - 2.6742 (0.0193) z = 0.8875 (0.0113)Angle to previous plane (with approximate e.s.d.) = 88.07 (0.08)* -0.0017 (0.0011) Ir * -0.0003 (0.0016) N1 * 0.0030 (0.0019) C1 * -0.0050 (0.0018) C6 * 0.0041 (0.0015) C11Rms deviation of fitted atoms = 0.00338.0059 (0.0047) x + 7.0413 (0.0123) y - 6.0961 (0.0152) z = 9.2723 (0.0097)Angle to previous plane (with approximate e.s.d.) = 87.21 (0.07)* -0.0001 (0.0011) Ir * 0.0052 (0.0015) N2 * -0.0092 (0.0018) C12 * 0.0091 (0.0019) C17 * -0.0051 (0.0016) C22Rms deviation of fitted atoms = 0.0066- 4.9239 (0.0124) x + 7.5102 (0.0143) y - 3.5667 (0.0238) z = 0.6667 (0.0227)Angle to previous plane (with approximate e.s.d.) = 88.93 (0.09)* -0.0051 (0.0020) N1 * 0.0097 (0.0022) C1 * -0.0065 (0.0026) C2 * -0.0011 (0.0029) C3 * 0.0057 (0.0026) C4 * -0.0027 (0.0022) C5Rms deviation of fitted atoms = 0.0058- 5.0855 (0.0105) x + 7.5155 (0.0121) y - 2.5377 (0.0215) z = 0.7805 (0.0195)Angle to previous plane (with approximate e.s.d.) = 3.74 (0.23)* -0.0030 (0.0020) C6 * -0.0032 (0.0024) C7 * 0.0061 (0.0024) C8 * -0.0028 (0.0023) C9 * -0.0034 (0.0021) C10 * 0.0063 (0.0019) C11Rms deviation of fitted atoms = 0.00447.8608 (0.0075) x + 6.9324 (0.0128) y - 6.5592 (0.0188) z = 9.0941 (0.0078)Angle to previous plane (with approximate e.s.d.) = 87.00 (0.09)* -0.0057 (0.0019) N2 * 0.0051 (0.0020) C12 * -0.0006 (0.0023) C13 * -0.0035 (0.0023) C14 * 0.0030 (0.0022) C15 * 0.0016 (0.0021) C16Rms deviation of fitted atoms = 0.00378.1881 (0.0069) x + 6.6251 (0.0132) y - 6.0523 (0.0203) z = 9.0428 (0.0130)Angle to previous plane (with approximate e.s.d.) = 3.41 (0.18)* 0.0009 (0.0020) C17 * 0.0004 (0.0022) C18 * -0.0039 (0.0023) C19 * 0.0060 (0.0024) C20 * -0.0045 (0.0022) C21 * 0.0010 (0.0021) C22Rms deviation of fitted atoms = 0.00353.1752 (0.0118) x + 5.2258 (0.0137) y + 16.0284 (0.0067) z = 8.3218 (0.0125)Angle to previous plane (with approximate e.s.d.) = 85.49 (0.09)* -0.0036 (0.0019) N3 * -0.0039 (0.0020) C23 * 0.0076 (0.0022) C24 * -0.0040 (0.0023) C25 * -0.0033 (0.0022) C26 * 0.0073 (0.0020) C27Rms deviation of fitted atoms = 0.00533.4499 (0.0143) x + 5.2695 (0.0146) y + 15.9354 (0.0080) z = 8.4866 (0.0099)Angle to previous plane (with approximate e.s.d.) = 1.70 (0.14)* -0.0012 (0.0016) N4 * -0.0019 (0.0016) N5 * -0.0046 (0.0016) N6 * 0.0036 (0.0016) C28 * 0.0040 (0.0017) C29Rms deviation of fitted atoms = 0.0033
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)

x y z Uiso*/Ueq Occ. (<1)
Ir 0.714159 (11) 0.644989 (9) 0.161874 (7) 0.02659 (4)
N1 0.7504 (3) 0.7041 (2) 0.26105 (15) 0.0309 (5)
N2 0.6692 (2) 0.6055 (2) 0.05631 (14) 0.0297 (5)
N3 0.8732 (2) 0.4767 (2) 0.19058 (14) 0.0278 (5)
N4 0.5913 (2) 0.5443 (2) 0.22449 (14) 0.0290 (5)
N5 0.4497 (3) 0.5607 (2) 0.24969 (15) 0.0313 (5)
N6 0.5827 (3) 0.3722 (2) 0.28304 (14) 0.0305 (5)
F1 1.0571 (2) 0.8804 (2) 0.19271 (14) 0.0637 (6)
F2 1.0605 (2) 0.7954 (2) −0.06767 (12) 0.0556 (5)
F3 0.3418 (2) 0.9040 (2) −0.04453 (13) 0.0608 (6)
F4 0.3587 (2) 1.08740 (17) 0.17490 (17) 0.0701 (7)
O 0.2211 (3) 0.1772 (2) 0.41368 (14) 0.0503 (6)
C1 0.8454 (3) 0.7639 (3) 0.25172 (19) 0.0363 (7)
C2 0.8715 (4) 0.8095 (3) 0.3164 (2) 0.0513 (9)
H2 0.9397 0.8494 0.3101 0.062*
C3 0.7979 (5) 0.7970 (4) 0.3901 (2) 0.0625 (11)
H3 0.8147 0.8290 0.4344 0.075*
C4 0.7006 (4) 0.7383 (3) 0.3989 (2) 0.0521 (10)
H4 0.6489 0.7296 0.4491 0.063*
C5 0.6797 (3) 0.6927 (3) 0.33407 (19) 0.0386 (7)
H5 0.6130 0.6514 0.3403 0.046*
C6 0.9075 (3) 0.7745 (2) 0.16876 (18) 0.0319 (6)
C7 1.0059 (4) 0.8317 (3) 0.1408 (2) 0.0425 (8)
C8 1.0578 (4) 0.8414 (3) 0.0622 (2) 0.0434 (8)
H8 1.1240 0.8819 0.0445 0.052*
C9 1.0087 (3) 0.7895 (3) 0.0103 (2) 0.0400 (8)
C10 0.9111 (3) 0.7311 (3) 0.03312 (18) 0.0323 (7)
H10 0.8807 0.6967 −0.0052 0.039*
C11 0.8574 (3) 0.7232 (2) 0.11339 (18) 0.0280 (6)
C12 0.5624 (3) 0.6896 (3) 0.01559 (19) 0.0351 (7)
C13 0.5223 (4) 0.6677 (3) −0.0547 (2) 0.0455 (9)
H13 0.4475 0.7260 −0.0825 0.055*
C14 0.5895 (4) 0.5627 (4) −0.0848 (2) 0.0479 (9)
H14 0.5614 0.5480 −0.1330 0.058*
C15 0.6979 (4) 0.4792 (3) −0.04409 (19) 0.0416 (8)
H15 0.7464 0.4062 −0.0639 0.050*
C16 0.7347 (3) 0.5033 (3) 0.02574 (18) 0.0347 (7)
H16 0.8096 0.4455 0.0537 0.042*
C17 0.5012 (3) 0.7966 (3) 0.05579 (19) 0.0356 (7)
C18 0.3976 (3) 0.8979 (3) 0.0267 (2) 0.0442 (9)
C19 0.3463 (3) 0.9952 (3) 0.0644 (3) 0.0518 (10)
H19 0.2743 1.0633 0.0431 0.062*
C20 0.4042 (4) 0.9899 (3) 0.1353 (3) 0.0510 (10)
C21 0.5066 (3) 0.8936 (3) 0.1702 (2) 0.0406 (8)
H21 0.5415 0.8944 0.2201 0.049*
C22 0.5573 (3) 0.7946 (2) 0.12954 (19) 0.0329 (7)
C23 0.8215 (3) 0.3924 (2) 0.22827 (16) 0.0276 (6)
C24 0.9108 (3) 0.2797 (3) 0.24803 (19) 0.0346 (7)
H24 0.8722 0.2226 0.2753 0.042*
C25 1.0571 (3) 0.2515 (3) 0.2275 (2) 0.0390 (8)
H25 1.1201 0.1742 0.2397 0.047*
C26 1.1106 (3) 0.3365 (3) 0.18928 (19) 0.0354 (7)
H26 1.2109 0.3185 0.1748 0.042*
C27 1.0169 (3) 0.4480 (3) 0.17215 (17) 0.0314 (6)
H27 1.0547 0.5065 0.1465 0.038*
C28 0.6655 (3) 0.4329 (2) 0.24554 (16) 0.0273 (6)
C29 0.4508 (3) 0.4553 (3) 0.28467 (17) 0.0308 (6)
C30 0.3195 (3) 0.4309 (3) 0.32093 (18) 0.0336 (7)
C31 0.3315 (4) 0.3168 (3) 0.35168 (18) 0.0379 (7)
H31 0.4226 0.2569 0.3486 0.045*
C32 0.2111 (4) 0.2905 (3) 0.38664 (19) 0.0432 (8)
C33 0.0807 (4) 0.3776 (3) 0.3946 (2) 0.0469 (9)
H33 −0.0007 0.3605 0.4215 0.056*
C34 0.0688 (4) 0.4897 (3) 0.3636 (2) 0.0487 (9)
H34 −0.0219 0.5496 0.3684 0.058*
C35 0.1860 (3) 0.5171 (3) 0.3254 (2) 0.0429 (8)
H35 0.1751 0.5945 0.3023 0.052*
C36 0.3592 (7) 0.0866 (5) 0.4007 (4) 0.071 (2) 0.653 (4)
H36A 0.4299 0.0918 0.4357 0.085* 0.653 (4)
H36B 0.3973 0.0954 0.3442 0.085* 0.653 (4)
C37 0.3348 (5) −0.0286 (3) 0.4204 (2) 0.0622 (19) 0.653 (4)
C38 0.3438 (5) −0.0840 (3) 0.49835 (19) 0.072 (2) 0.653 (4)
H38 0.3633 −0.0482 0.5399 0.086* 0.653 (4)
C39 0.3242 (6) −0.1918 (3) 0.51547 (16) 0.0604 (19) 0.653 (4)
H39 0.3303 −0.2296 0.5687 0.072* 0.653 (4)
C40 0.2956 (6) −0.2442 (3) 0.4547 (2) 0.0362 (13) 0.653 (4)
C41 0.2867 (6) −0.1888 (3) 0.37680 (19) 0.0527 (18) 0.653 (4)
H41 0.2672 −0.2246 0.3353 0.063* 0.653 (4)
C42 0.3063 (5) −0.0810 (3) 0.35967 (17) 0.0585 (16) 0.653 (4)
H42 0.3002 −0.0432 0.3064 0.070* 0.653 (4)
C43 0.2863 (11) −0.3593 (5) 0.4678 (4) 0.0501 (18) 0.653 (4)
H43 0.2594 −0.3860 0.4240 0.060* 0.653 (4)
C44 0.311 (2) −0.4304 (10) 0.5326 (6) 0.080 (4) 0.653 (4)
H44A 0.3378 −0.4082 0.5782 0.096* 0.653 (4)
H44B 0.3011 −0.5051 0.5346 0.096* 0.653 (4)
C36' 0.0909 (11) 0.1407 (8) 0.4352 (7) 0.049 (3)* 0.347 (4)
H36C 0.0432 0.1676 0.4871 0.059* 0.347 (4)
H36D 0.0210 0.1747 0.3936 0.059* 0.347 (4)
C37' 0.1405 (9) 0.0112 (6) 0.4411 (5) 0.049 (3)* 0.347 (4)
C38' 0.1309 (12) −0.0504 (9) 0.5161 (5) 0.143 (8)* 0.347 (4)
H38' 0.0859 −0.0099 0.5611 0.172* 0.347 (4)
C39' 0.1870 (14) −0.1713 (9) 0.5251 (6) 0.103 (6)* 0.347 (4)
H39' 0.1804 −0.2134 0.5763 0.124* 0.347 (4)
C40' 0.2528 (13) −0.2305 (6) 0.4592 (8) 0.073 (5)* 0.347 (4)
C41' 0.2625 (12) −0.1689 (8) 0.3843 (6) 0.076 (5)* 0.347 (4)
H41' 0.3074 −0.2094 0.3393 0.091* 0.347 (4)
C42' 0.2063 (10) −0.0480 (8) 0.3753 (4) 0.078 (4)* 0.347 (4)
H42' 0.2129 −0.0059 0.3240 0.093* 0.347 (4)
C43' 0.325 (3) −0.3545 (13) 0.4677 (15) 0.087 (7)* 0.347 (4)
H43' 0.3818 −0.3868 0.4220 0.105* 0.347 (4)
C44' 0.321 (5) −0.427 (3) 0.5311 (19) 0.115 (11)* 0.347 (4)
H44C 0.2657 −0.3991 0.5785 0.137* 0.347 (4)
H44D 0.3729 −0.5074 0.5302 0.137* 0.347 (4)
O99 0.6874 (3) 0.1238 (2) 0.30300 (14) 0.0464 (6)
H99 0.6500 0.1956 0.3065 0.070*
C99 0.6872 (4) 0.1023 (3) 0.2235 (2) 0.0543 (10)
H99A 0.5892 0.1373 0.2057 0.081*
H99B 0.7200 0.0181 0.2207 0.081*
H99C 0.7521 0.1363 0.1887 0.081*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ir 0.02141 (6) 0.02302 (6) 0.02931 (6) −0.00108 (4) 0.00057 (4) −0.00128 (4)
N1 0.0286 (13) 0.0270 (12) 0.0314 (13) −0.0031 (10) 0.0062 (10) −0.0068 (10)
N2 0.0231 (12) 0.0330 (13) 0.0301 (13) −0.0088 (10) −0.0002 (10) 0.0029 (10)
N3 0.0265 (12) 0.0274 (12) 0.0243 (12) −0.0014 (10) −0.0016 (10) −0.0058 (10)
N4 0.0239 (12) 0.0281 (12) 0.0303 (13) −0.0033 (10) 0.0020 (10) −0.0047 (10)
N5 0.0249 (12) 0.0309 (13) 0.0327 (13) −0.0040 (10) 0.0049 (10) −0.0045 (11)
N6 0.0328 (13) 0.0285 (13) 0.0276 (13) −0.0063 (11) 0.0008 (10) −0.0063 (10)
F1 0.0689 (15) 0.0842 (17) 0.0595 (14) −0.0496 (13) 0.0101 (11) −0.0284 (12)
F2 0.0598 (13) 0.0782 (15) 0.0380 (11) −0.0407 (12) 0.0111 (9) −0.0034 (10)
F3 0.0347 (11) 0.0685 (15) 0.0649 (14) −0.0097 (10) −0.0156 (10) 0.0293 (12)
F4 0.0377 (12) 0.0281 (10) 0.130 (2) 0.0050 (9) 0.0069 (12) −0.0134 (12)
O 0.0573 (16) 0.0502 (15) 0.0440 (14) −0.0271 (13) 0.0128 (12) 0.0028 (12)
C1 0.0388 (17) 0.0300 (16) 0.0372 (17) −0.0073 (14) 0.0014 (14) −0.0077 (13)
C2 0.069 (3) 0.048 (2) 0.044 (2) −0.0274 (19) 0.0065 (18) −0.0164 (17)
C3 0.096 (3) 0.057 (2) 0.043 (2) −0.033 (2) 0.010 (2) −0.0255 (19)
C4 0.071 (3) 0.042 (2) 0.0359 (19) −0.0122 (19) 0.0165 (18) −0.0122 (16)
C5 0.0410 (18) 0.0311 (16) 0.0369 (18) −0.0055 (14) 0.0063 (14) −0.0054 (14)
C6 0.0295 (15) 0.0282 (15) 0.0336 (16) −0.0035 (12) −0.0008 (12) −0.0059 (12)
C7 0.0404 (18) 0.0448 (19) 0.047 (2) −0.0172 (15) 0.0001 (15) −0.0161 (16)
C8 0.0368 (18) 0.048 (2) 0.050 (2) −0.0239 (16) 0.0080 (15) −0.0068 (16)
C9 0.0335 (17) 0.0463 (19) 0.0365 (18) −0.0123 (15) 0.0043 (14) −0.0009 (15)
C10 0.0277 (15) 0.0326 (16) 0.0318 (16) −0.0048 (13) −0.0027 (12) −0.0010 (13)
C11 0.0180 (13) 0.0250 (14) 0.0345 (16) 0.0005 (11) −0.0019 (11) −0.0009 (12)
C12 0.0235 (14) 0.0431 (18) 0.0361 (17) −0.0141 (13) 0.0002 (12) 0.0097 (14)
C13 0.0363 (18) 0.066 (2) 0.0328 (18) −0.0220 (17) −0.0084 (14) 0.0149 (17)
C14 0.046 (2) 0.078 (3) 0.0270 (17) −0.032 (2) 0.0020 (15) −0.0029 (17)
C15 0.0393 (18) 0.057 (2) 0.0326 (17) −0.0235 (17) 0.0059 (14) −0.0073 (15)
C16 0.0341 (16) 0.0377 (17) 0.0314 (16) −0.0122 (14) 0.0007 (13) −0.0031 (13)
C17 0.0204 (14) 0.0355 (16) 0.0441 (18) −0.0086 (12) −0.0003 (13) 0.0146 (14)
C18 0.0219 (15) 0.046 (2) 0.056 (2) −0.0112 (14) −0.0027 (14) 0.0210 (17)
C19 0.0171 (15) 0.0383 (19) 0.085 (3) −0.0022 (14) −0.0017 (17) 0.0209 (19)
C20 0.0277 (17) 0.0284 (17) 0.088 (3) −0.0052 (14) 0.0141 (18) −0.0027 (18)
C21 0.0200 (14) 0.0293 (16) 0.065 (2) −0.0011 (12) 0.0024 (14) −0.0042 (15)
C22 0.0217 (14) 0.0242 (14) 0.0462 (18) −0.0054 (12) 0.0058 (13) 0.0048 (13)
C23 0.0273 (14) 0.0277 (14) 0.0245 (14) −0.0049 (12) 0.0012 (11) −0.0055 (11)
C24 0.0350 (17) 0.0254 (15) 0.0373 (17) −0.0033 (13) 0.0004 (13) −0.0032 (13)
C25 0.0361 (17) 0.0276 (15) 0.0423 (19) 0.0033 (13) −0.0005 (14) −0.0056 (14)
C26 0.0261 (15) 0.0337 (16) 0.0366 (17) 0.0019 (13) 0.0016 (13) −0.0057 (13)
C27 0.0278 (15) 0.0331 (16) 0.0302 (16) −0.0060 (13) 0.0006 (12) −0.0056 (12)
C28 0.0309 (15) 0.0255 (14) 0.0230 (14) −0.0057 (12) 0.0013 (11) −0.0063 (11)
C29 0.0295 (15) 0.0316 (15) 0.0279 (15) −0.0062 (13) 0.0018 (12) −0.0056 (12)
C30 0.0331 (16) 0.0379 (17) 0.0293 (16) −0.0115 (14) 0.0016 (13) −0.0059 (13)
C31 0.0436 (18) 0.0378 (17) 0.0288 (16) −0.0116 (14) 0.0020 (13) −0.0011 (13)
C32 0.056 (2) 0.046 (2) 0.0288 (17) −0.0224 (18) 0.0034 (15) −0.0023 (15)
C33 0.050 (2) 0.058 (2) 0.0375 (19) −0.0283 (19) 0.0085 (16) −0.0067 (17)
C34 0.0362 (19) 0.049 (2) 0.056 (2) −0.0108 (16) 0.0059 (16) −0.0080 (18)
C35 0.0360 (18) 0.0375 (18) 0.052 (2) −0.0119 (15) 0.0064 (15) −0.0042 (16)
C36 0.102 (5) 0.037 (3) 0.062 (4) −0.024 (3) 0.041 (4) −0.008 (3)
C37 0.099 (5) 0.034 (3) 0.046 (3) −0.021 (3) 0.027 (3) −0.008 (2)
C38 0.141 (7) 0.052 (4) 0.034 (3) −0.052 (4) 0.011 (4) −0.011 (3)
C39 0.122 (6) 0.042 (3) 0.022 (3) −0.035 (3) −0.007 (3) 0.002 (2)
C40 0.053 (4) 0.033 (3) 0.025 (3) −0.017 (2) 0.000 (2) −0.0018 (18)
C41 0.072 (4) 0.045 (3) 0.029 (3) −0.005 (3) 0.000 (3) −0.004 (2)
C42 0.070 (4) 0.040 (3) 0.046 (3) 0.003 (3) 0.005 (3) −0.001 (2)
C43 0.077 (6) 0.050 (3) 0.035 (3) −0.031 (3) −0.011 (3) −0.009 (2)
C44 0.170 (11) 0.059 (5) 0.039 (4) −0.079 (6) −0.002 (4) 0.002 (3)
O99 0.0594 (16) 0.0366 (13) 0.0406 (13) −0.0142 (12) −0.0046 (11) 0.0005 (10)
C99 0.073 (3) 0.044 (2) 0.050 (2) −0.0206 (19) −0.0161 (19) −0.0038 (17)

Geometric parameters (Å, °)

Ir—C11 2.010 (3) C24—C25 1.381 (4)
Ir—C22 2.012 (3) C24—H24 0.9500
Ir—N1 2.033 (2) C25—C26 1.377 (5)
Ir—N2 2.049 (2) C25—H25 0.9500
Ir—N4 2.118 (2) C26—C27 1.379 (4)
Ir—N3 2.158 (2) C26—H26 0.9500
N1—C5 1.359 (4) C27—H27 0.9500
N1—C1 1.361 (4) C29—C30 1.476 (4)
N2—C16 1.348 (4) C30—C35 1.384 (4)
N2—C12 1.370 (4) C30—C31 1.395 (4)
N3—C27 1.352 (4) C31—C32 1.385 (5)
N3—C23 1.356 (4) C31—H31 0.9500
N4—C28 1.332 (3) C32—C33 1.373 (5)
N4—N5 1.370 (3) C33—C34 1.373 (5)
N5—C29 1.342 (4) C33—H33 0.9500
N6—C28 1.339 (4) C34—C35 1.380 (5)
N6—C29 1.355 (4) C34—H34 0.9500
F1—C7 1.359 (4) C35—H35 0.9500
F2—C9 1.357 (4) C36—C37 1.503 (6)
F3—C18 1.363 (4) C36—H36A 0.9900
F4—C20 1.371 (4) C36—H36B 0.9900
O—C32 1.375 (4) C37—C38 1.3900
O—C36 1.454 (6) C37—C42 1.3900
O—C36' 1.495 (11) C38—C39 1.3900
C1—C2 1.385 (5) C38—H38 0.9500
C1—C6 1.469 (4) C39—C40 1.3900
C2—C3 1.383 (5) C39—H39 0.9500
C2—H2 0.9500 C40—C41 1.3900
C3—C4 1.372 (6) C40—C43 1.435 (6)
C3—H3 0.9500 C41—C42 1.3900
C4—C5 1.367 (5) C41—H41 0.9500
C4—H4 0.9500 C42—H42 0.9500
C5—H5 0.9500 C43—C44 1.290 (9)
C6—C7 1.390 (4) C43—H43 0.9500
C6—C11 1.418 (4) C44—H44A 0.9500
C7—C8 1.371 (5) C44—H44B 0.9500
C8—C9 1.373 (5) C36'—C37' 1.490 (10)
C8—H8 0.9500 C36'—H36C 0.9900
C9—C10 1.381 (4) C36'—H36D 0.9900
C10—C11 1.400 (4) C37'—C38' 1.3900
C10—H10 0.9500 C37'—C42' 1.3900
C12—C13 1.383 (5) C38'—C39' 1.3900
C12—C17 1.475 (5) C38'—H38' 0.9500
C13—C14 1.376 (5) C39'—C40' 1.3900
C13—H13 0.9500 C39'—H39' 0.9500
C14—C15 1.376 (5) C40'—C41' 1.3900
C14—H14 0.9500 C40'—C43' 1.439 (14)
C15—C16 1.374 (4) C41'—C42' 1.3900
C15—H15 0.9500 C41'—H41' 0.9500
C16—H16 0.9500 C42'—H42' 0.9500
C17—C18 1.382 (4) C43'—C44' 1.296 (16)
C17—C22 1.416 (5) C43'—H43' 0.9500
C18—C19 1.351 (5) C44'—H44C 0.9500
C19—C20 1.370 (6) C44'—H44D 0.9500
C19—H19 0.9500 O99—C99 1.406 (4)
C20—C21 1.377 (5) O99—H99 0.8400
C21—C22 1.395 (4) C99—H99A 0.9800
C21—H21 0.9500 C99—H99B 0.9800
C23—C24 1.382 (4) C99—H99C 0.9800
C23—C28 1.457 (4)
C11—Ir—C22 87.62 (11) C25—C24—H24 120.5
C11—Ir—N1 80.20 (11) C23—C24—H24 120.5
C22—Ir—N1 93.29 (12) C26—C25—C24 119.3 (3)
C11—Ir—N2 96.44 (11) C26—C25—H25 120.3
C22—Ir—N2 80.71 (12) C24—C25—H25 120.3
N1—Ir—N2 173.28 (9) C25—C26—C27 119.3 (3)
C11—Ir—N4 170.49 (10) C25—C26—H26 120.3
C22—Ir—N4 101.08 (10) C27—C26—H26 120.3
N1—Ir—N4 95.35 (10) N3—C27—C26 122.2 (3)
N2—Ir—N4 88.81 (9) N3—C27—H27 118.9
C11—Ir—N3 95.37 (10) C26—C27—H27 118.9
C22—Ir—N3 174.78 (11) N4—C28—N6 113.2 (2)
N1—Ir—N3 91.44 (9) N4—C28—C23 118.7 (3)
N2—Ir—N3 94.68 (9) N6—C28—C23 128.1 (3)
N4—Ir—N3 76.25 (9) N5—C29—N6 114.3 (3)
C5—N1—C1 118.9 (3) N5—C29—C30 123.2 (3)
C5—N1—Ir 123.7 (2) N6—C29—C30 122.5 (3)
C1—N1—Ir 117.3 (2) C35—C30—C31 119.2 (3)
C16—N2—C12 118.7 (3) C35—C30—C29 122.3 (3)
C16—N2—Ir 124.8 (2) C31—C30—C29 118.5 (3)
C12—N2—Ir 116.5 (2) C32—C31—C30 120.2 (3)
C27—N3—C23 118.1 (2) C32—C31—H31 119.9
C27—N3—Ir 125.9 (2) C30—C31—H31 119.9
C23—N3—Ir 115.98 (18) C33—C32—O 119.6 (3)
C28—N4—N5 107.2 (2) C33—C32—C31 120.0 (3)
C28—N4—Ir 115.38 (18) O—C32—C31 120.4 (3)
N5—N4—Ir 137.37 (18) C32—C33—C34 119.6 (3)
C29—N5—N4 103.8 (2) C32—C33—H33 120.2
C28—N6—C29 101.5 (2) C34—C33—H33 120.2
C32—O—C36 118.1 (3) C33—C34—C35 121.3 (3)
C32—O—C36' 122.2 (4) C33—C34—H34 119.3
C36—O—C36' 117.7 (5) C35—C34—H34 119.3
N1—C1—C2 120.2 (3) C30—C35—C34 119.5 (3)
N1—C1—C6 112.8 (3) C30—C35—H35 120.3
C2—C1—C6 127.0 (3) C34—C35—H35 120.3
C3—C2—C1 119.8 (4) O—C36—C37 107.5 (4)
C3—C2—H2 120.1 O—C36—H36A 110.2
C1—C2—H2 120.1 C37—C36—H36A 110.2
C4—C3—C2 119.8 (4) O—C36—H36B 110.2
C4—C3—H3 120.1 C37—C36—H36B 110.2
C2—C3—H3 120.1 H36A—C36—H36B 108.5
C5—C4—C3 118.6 (3) C38—C37—C42 120.0
C5—C4—H4 120.7 C38—C37—C36 120.6 (4)
C3—C4—H4 120.7 C42—C37—C36 119.4 (4)
N1—C5—C4 122.6 (3) C37—C38—C39 120.0
N1—C5—H5 118.7 C37—C38—H38 120.0
C4—C5—H5 118.7 C39—C38—H38 120.0
C7—C6—C11 118.7 (3) C40—C39—C38 120.0
C7—C6—C1 126.0 (3) C40—C39—H39 120.0
C11—C6—C1 115.4 (3) C38—C39—H39 120.0
F1—C7—C8 116.5 (3) C39—C40—C41 120.0
F1—C7—C6 120.0 (3) C39—C40—C43 122.2 (3)
C8—C7—C6 123.5 (3) C41—C40—C43 117.6 (3)
C7—C8—C9 116.4 (3) C42—C41—C40 120.0
C7—C8—H8 121.8 C42—C41—H41 120.0
C9—C8—H8 121.8 C40—C41—H41 120.0
F2—C9—C8 117.8 (3) C41—C42—C37 120.0
F2—C9—C10 118.5 (3) C41—C42—H42 120.0
C8—C9—C10 123.7 (3) C37—C42—H42 120.0
C9—C10—C11 119.4 (3) C44—C43—C40 127.1 (7)
C9—C10—H10 120.3 C44—C43—H43 116.5
C11—C10—H10 120.3 C40—C43—H43 116.5
C10—C11—C6 118.3 (3) C43—C44—H44A 120.0
C10—C11—Ir 127.3 (2) C43—C44—H44B 120.0
C6—C11—Ir 114.3 (2) H44A—C44—H44B 120.0
N2—C12—C13 119.8 (3) C37'—C36'—O 107.3 (7)
N2—C12—C17 112.7 (3) C37'—C36'—H36C 110.2
C13—C12—C17 127.5 (3) O—C36'—H36C 110.2
C14—C13—C12 120.8 (3) C37'—C36'—H36D 110.2
C14—C13—H13 119.6 O—C36'—H36D 110.2
C12—C13—H13 119.6 H36C—C36'—H36D 108.5
C15—C14—C13 119.0 (3) C38'—C37'—C42' 120.0
C15—C14—H14 120.5 C38'—C37'—C36' 118.3 (7)
C13—C14—H14 120.5 C42'—C37'—C36' 121.4 (7)
C16—C15—C14 118.8 (3) C37'—C38'—C39' 120.0
C16—C15—H15 120.6 C37'—C38'—H38' 120.0
C14—C15—H15 120.6 C39'—C38'—H38' 120.0
N2—C16—C15 122.9 (3) C40'—C39'—C38' 120.0
N2—C16—H16 118.6 C40'—C39'—H39' 120.0
C15—C16—H16 118.6 C38'—C39'—H39' 120.0
C18—C17—C22 118.1 (3) C39'—C40'—C41' 120.0
C18—C17—C12 125.6 (3) C39'—C40'—C43' 121.5 (11)
C22—C17—C12 116.2 (3) C41'—C40'—C43' 118.2 (11)
C19—C18—F3 115.9 (3) C42'—C41'—C40' 120.0
C19—C18—C17 124.0 (4) C42'—C41'—H41' 120.0
F3—C18—C17 120.1 (3) C40'—C41'—H41' 120.0
C18—C19—C20 116.0 (3) C41'—C42'—C37' 120.0
C18—C19—H19 122.0 C41'—C42'—H42' 120.0
C20—C19—H19 122.0 C37'—C42'—H42' 120.0
C19—C20—F4 118.3 (3) C44'—C43'—C40' 127 (3)
C19—C20—C21 125.0 (4) C44'—C43'—H43' 116.5
F4—C20—C21 116.7 (4) C40'—C43'—H43' 116.6
C20—C21—C22 117.5 (4) C43'—C44'—H44C 119.9
C20—C21—H21 121.2 C43'—C44'—H44D 120.1
C22—C21—H21 121.2 H44C—C44'—H44D 120.0
C21—C22—C17 119.4 (3) C99—O99—H99 109.5
C21—C22—Ir 126.6 (3) O99—C99—H99A 109.5
C17—C22—Ir 113.9 (2) O99—C99—H99B 109.5
N3—C23—C24 122.1 (3) H99A—C99—H99B 109.5
N3—C23—C28 113.5 (2) O99—C99—H99C 109.5
C24—C23—C28 124.4 (3) H99A—C99—H99C 109.5
C25—C24—C23 119.0 (3) H99B—C99—H99C 109.5
C11—Ir—N1—C5 176.2 (2) C18—C19—C20—F4 178.2 (3)
C22—Ir—N1—C5 89.2 (2) C18—C19—C20—C21 −1.2 (5)
N4—Ir—N1—C5 −12.3 (2) C19—C20—C21—C22 1.3 (5)
N3—Ir—N1—C5 −88.6 (2) F4—C20—C21—C22 −178.2 (3)
C11—Ir—N1—C1 0.0 (2) C20—C21—C22—C17 −0.7 (4)
C22—Ir—N1—C1 −87.0 (2) C20—C21—C22—Ir 176.1 (2)
N4—Ir—N1—C1 171.5 (2) C18—C17—C22—C21 0.2 (4)
N3—Ir—N1—C1 95.2 (2) C12—C17—C22—C21 178.7 (3)
C11—Ir—N2—C16 94.2 (2) C18—C17—C22—Ir −177.0 (2)
C22—Ir—N2—C16 −179.3 (2) C12—C17—C22—Ir 1.5 (3)
N4—Ir—N2—C16 −77.9 (2) C11—Ir—C22—C21 −80.6 (3)
N3—Ir—N2—C16 −1.8 (2) N1—Ir—C22—C21 −0.6 (3)
C11—Ir—N2—C12 −87.1 (2) N2—Ir—C22—C21 −177.5 (3)
C22—Ir—N2—C12 −0.6 (2) N4—Ir—C22—C21 95.6 (3)
N4—Ir—N2—C12 100.8 (2) C11—Ir—C22—C17 96.4 (2)
N3—Ir—N2—C12 176.9 (2) N1—Ir—C22—C17 176.4 (2)
C11—Ir—N3—C27 −3.8 (2) N2—Ir—C22—C17 −0.5 (2)
N1—Ir—N3—C27 −84.0 (2) N4—Ir—C22—C17 −87.5 (2)
N2—Ir—N3—C27 93.2 (2) C27—N3—C23—C24 0.1 (4)
N4—Ir—N3—C27 −179.2 (2) Ir—N3—C23—C24 178.0 (2)
C11—Ir—N3—C23 178.4 (2) C27—N3—C23—C28 179.8 (2)
N1—Ir—N3—C23 98.2 (2) Ir—N3—C23—C28 −2.3 (3)
N2—Ir—N3—C23 −84.6 (2) N3—C23—C24—C25 −1.1 (5)
N4—Ir—N3—C23 3.00 (19) C28—C23—C24—C25 179.2 (3)
C22—Ir—N4—C28 172.1 (2) C23—C24—C25—C26 1.1 (5)
N1—Ir—N4—C28 −93.5 (2) C24—C25—C26—C27 −0.1 (5)
N2—Ir—N4—C28 91.8 (2) C23—N3—C27—C26 1.0 (4)
N3—Ir—N4—C28 −3.30 (19) Ir—N3—C27—C26 −176.7 (2)
C22—Ir—N4—N5 −6.3 (3) C25—C26—C27—N3 −1.0 (5)
N1—Ir—N4—N5 88.2 (3) N5—N4—C28—N6 0.5 (3)
N2—Ir—N4—N5 −86.5 (3) Ir—N4—C28—N6 −178.33 (18)
N3—Ir—N4—N5 178.3 (3) N5—N4—C28—C23 −177.9 (2)
C28—N4—N5—C29 0.1 (3) Ir—N4—C28—C23 3.3 (3)
Ir—N4—N5—C29 178.5 (2) C29—N6—C28—N4 −0.8 (3)
C5—N1—C1—C2 1.6 (4) C29—N6—C28—C23 177.4 (3)
Ir—N1—C1—C2 178.0 (2) N3—C23—C28—N4 −0.7 (4)
C5—N1—C1—C6 −176.8 (2) C24—C23—C28—N4 179.0 (3)
Ir—N1—C1—C6 −0.4 (3) N3—C23—C28—N6 −178.8 (3)
N1—C1—C2—C3 −1.7 (5) C24—C23—C28—N6 0.9 (5)
C6—C1—C2—C3 176.4 (3) N4—N5—C29—N6 −0.6 (3)
C1—C2—C3—C4 0.7 (6) N4—N5—C29—C30 −179.8 (3)
C2—C3—C4—C5 0.5 (6) C28—N6—C29—N5 0.9 (3)
C1—N1—C5—C4 −0.4 (5) C28—N6—C29—C30 −180.0 (3)
Ir—N1—C5—C4 −176.6 (2) N5—C29—C30—C35 −3.6 (5)
C3—C4—C5—N1 −0.6 (5) N6—C29—C30—C35 177.3 (3)
N1—C1—C6—C7 179.3 (3) N5—C29—C30—C31 176.4 (3)
C2—C1—C6—C7 1.0 (5) N6—C29—C30—C31 −2.7 (4)
N1—C1—C6—C11 0.8 (4) C35—C30—C31—C32 −0.4 (5)
C2—C1—C6—C11 −177.5 (3) C29—C30—C31—C32 179.6 (3)
C11—C6—C7—F1 −179.2 (3) C36—O—C32—C33 177.1 (4)
C1—C6—C7—F1 2.5 (5) C36'—O—C32—C33 13.7 (7)
C11—C6—C7—C8 0.1 (5) C36—O—C32—C31 −3.1 (6)
C1—C6—C7—C8 −178.3 (3) C36'—O—C32—C31 −166.5 (5)
F1—C7—C8—C9 178.4 (3) C30—C31—C32—C33 −3.2 (5)
C6—C7—C8—C9 −0.9 (5) C30—C31—C32—O 177.0 (3)
C7—C8—C9—F2 −178.5 (3) O—C32—C33—C34 −176.3 (3)
C7—C8—C9—C10 0.8 (5) C31—C32—C33—C34 3.9 (5)
F2—C9—C10—C11 179.4 (3) C32—C33—C34—C35 −1.0 (6)
C8—C9—C10—C11 0.0 (5) C31—C30—C35—C34 3.2 (5)
C9—C10—C11—C6 −0.9 (4) C29—C30—C35—C34 −176.8 (3)
C9—C10—C11—Ir 179.4 (2) C33—C34—C35—C30 −2.5 (6)
C7—C6—C11—C10 0.8 (4) C32—O—C36—C37 −169.1 (3)
C1—C6—C11—C10 179.4 (3) C36'—O—C36—C37 −5.0 (8)
C7—C6—C11—Ir −179.4 (2) O—C36—C37—C38 −88.2 (5)
C1—C6—C11—Ir −0.9 (3) O—C36—C37—C42 93.2 (5)
C22—Ir—C11—C10 −86.0 (3) C42—C37—C38—C39 0.0
N1—Ir—C11—C10 −179.8 (3) C36—C37—C38—C39 −178.6 (4)
N2—Ir—C11—C10 −5.7 (3) C37—C38—C39—C40 0.0
N3—Ir—C11—C10 89.7 (2) C38—C39—C40—C41 0.0
C22—Ir—C11—C6 94.2 (2) C38—C39—C40—C43 174.8 (7)
N1—Ir—C11—C6 0.49 (19) C39—C40—C41—C42 0.0
N2—Ir—C11—C6 174.6 (2) C43—C40—C41—C42 −175.0 (6)
N3—Ir—C11—C6 −90.0 (2) C40—C41—C42—C37 0.0
C16—N2—C12—C13 1.1 (4) C38—C37—C42—C41 0.0
Ir—N2—C12—C13 −177.7 (2) C36—C37—C42—C41 178.6 (4)
C16—N2—C12—C17 −179.7 (2) C39—C40—C43—C44 −4.5 (17)
Ir—N2—C12—C17 1.5 (3) C41—C40—C43—C44 170.4 (13)
N2—C12—C13—C14 −0.7 (5) C32—O—C36'—C37' 165.6 (5)
C17—C12—C13—C14 −179.7 (3) C36—O—C36'—C37' 2.1 (9)
C12—C13—C14—C15 −0.2 (5) O—C36'—C37'—C38' 112.4 (7)
C13—C14—C15—C16 0.5 (5) O—C36'—C37'—C42' −62.2 (10)
C12—N2—C16—C15 −0.8 (4) C42'—C37'—C38'—C39' 0.0
Ir—N2—C16—C15 177.9 (2) C36'—C37'—C38'—C39' −174.7 (9)
C14—C15—C16—N2 0.0 (5) C37'—C38'—C39'—C40' 0.0
N2—C12—C17—C18 176.4 (3) C38'—C39'—C40'—C41' 0.0
C13—C12—C17—C18 −4.5 (5) C38'—C39'—C40'—C43' 173.5 (15)
N2—C12—C17—C22 −1.9 (4) C39'—C40'—C41'—C42' 0.0
C13—C12—C17—C22 177.1 (3) C43'—C40'—C41'—C42' −173.8 (14)
C22—C17—C18—C19 −0.2 (5) C40'—C41'—C42'—C37' 0.0
C12—C17—C18—C19 −178.5 (3) C38'—C37'—C42'—C41' 0.0
C22—C17—C18—F3 179.3 (3) C36'—C37'—C42'—C41' 174.5 (9)
C12—C17—C18—F3 1.0 (5) C39'—C40'—C43'—C44' 11 (4)
F3—C18—C19—C20 −178.9 (3) C41'—C40'—C43'—C44' −175 (3)
C17—C18—C19—C20 0.7 (5)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O99—H99···N6 0.84 2.04 2.853 (3) 164
C24—H24···O99 0.95 2.49 3.368 (4) 154
C31—H31···O99 0.95 2.66 3.587 (4) 164
C8—H8···F3i 0.95 2.55 3.412 (4) 151
C25—H25···F4ii 0.95 2.43 3.088 (4) 126
C3—H3···Oiii 0.95 2.54 3.353 (5) 143
C14—H14···N5iv 0.95 2.57 3.475 (5) 160
C39—H39···O99v 0.95 2.64 3.272 (4) 124

Symmetry codes: (i) x+1, y, z; (ii) x+1, y−1, z; (iii) −x+1, −y+1, −z+1; (iv) −x+1, −y+1, −z; (v) −x+1, −y, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: TK2595).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809052726/tk2595sup1.cif

e-66-00m66-sup1.cif (41.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809052726/tk2595Isup2.hkl

e-66-00m66-Isup2.hkl (510.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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