Literature DB >> 21588839

mer-[3-Phenyl-5-(2-pyridyl-κN)-1,2,4-triazol-1-ido-κN]bis-(2-quinolylphenyl-κC,N)iridium(III) deuterochloro-form disolvate.

Peter G Jones, Andreas Freund, Marc Debeaux, Wolfgang Kowalsky, Hans-Hermann Johannes.   

Abstract

In the title compound, [Ir(C(13)H(9)N(4))(C(15)H(10)N)(2)]·2CDCl(3), the coordination at iridium is octa-hedral, but with narrow ligand bite angles ranging from 74.85 (8) to 83.99 (8)°. The bond lengths at iridium show the expected trans influence, with Ir-N trans to C being appreciably longer than trans to N. The chelate rings are mutually perpendicular to a reasonable approximation [interplanar angles ranging from 77.79 (6) to 83.93 (7)°]. All ligands are approximately planar; the maximum inter-planar angles within ligands are ca 12°. One CDCl(3) solvent molecule is severly disordered and was excluded from the refinement.

Entities:  

Year:  2010        PMID: 21588839      PMCID: PMC3009293          DOI: 10.1107/S1600536810038596

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


Related literature

For the preparation of iridium complexes, see: Lamansky et al. (2001 ▶); Coppo et al. (2004 ▶). For the photoluminescent properties and color tuning of cyclo­metalated iridium complexes, see: Grushin et al. (2001 ▶); You & Park (2005 ▶); Stagni et al. (2008 ▶). For general background to organic light-emitting diodes (OLEDs), see: Hertel et al. (2005 ▶); Holder et al. (2005 ▶). For two recent related publications from our groups, see: Jones et al. (2010a ▶,b ▶).

Experimental

Crystal data

[Ir(C13H9N4)(C15H10N)2]·2CDCl3 M = 1062.67 Triclinic, a = 9.1399 (3) Å b = 12.4430 (5) Å c = 17.6762 (6) Å α = 81.493 (4)° β = 81.509 (4)° γ = 85.193 (4)° V = 1962.41 (12) Å3 Z = 2 Mo Kα radiation μ = 3.86 mm−1 T = 100 K 0.25 × 0.20 × 0.05 mm

Data collection

Oxford Diffraction Xcalibur Eos diffractometer Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010 ▶) T min = 0.739, T max = 1.000 78670 measured reflections 9739 independent reflections 8125 reflections with I > 2σ(I) R int = 0.062

Refinement

R[F 2 > 2σ(F 2)] = 0.025 wR(F 2) = 0.048 S = 0.93 9739 reflections 487 parameters 134 restraints H-atom parameters constrained Δρmax = 1.03 e Å−3 Δρmin = −1.08 e Å−3 Data collection: CrysAlis PRO (Oxford Diffraction, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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 and PLATON (Spek, 2009 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810038596/bt5363sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810038596/bt5363Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Ir(C13H9N4)(C15H10N)2]·2CDCl3Z = 2
Mr = 1062.67F(000) = 1044
Triclinic, P1Dx = 1.798 Mg m3
a = 9.1399 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.4430 (5) ÅCell parameters from 26610 reflections
c = 17.6762 (6) Åθ = 2.2–30.8°
α = 81.493 (4)°µ = 3.86 mm1
β = 81.509 (4)°T = 100 K
γ = 85.193 (4)°Tablet, orange
V = 1962.41 (12) Å30.25 × 0.20 × 0.05 mm
Oxford Diffraction Xcalibur Eos diffractometer9739 independent reflections
Radiation source: Enhance (Mo) X-ray Source8125 reflections with I > 2σ(I)
graphiteRint = 0.062
Detector resolution: 16.1419 pixels mm-1θmax = 28.3°, θmin = 2.2°
ω–scanh = −12→12
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010)k = −16→16
Tmin = 0.739, Tmax = 1.000l = −23→23
78670 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.025Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.048H-atom parameters constrained
S = 0.93w = 1/[σ2(Fo2) + (0.019P)2] where P = (Fo2 + 2Fc2)/3
9739 reflections(Δ/σ)max = 0.003
487 parametersΔρmax = 1.03 e Å3
134 restraintsΔρmin = −1.07 e Å3
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)8.0107 (0.0039) x - 5.0559 (0.0100) y + 1.0694 (0.0169) z = 0.3793 (0.0119)* 0.0612 (0.0010) Ir * -0.0747 (0.0014) N1 * 0.0495 (0.0016) C2 * 0.0270 (0.0017) C11 * -0.0630 (0.0014) C12Rms deviation of fitted atoms = 0.05743.5166 (0.0086) x + 11.8000 (0.0045) y + 4.6463 (0.0182) z = 11.4217 (0.0048)Angle to previous plane (with approximate e.s.d.) = 83.93 (0.07)* -0.0639 (0.0011) Ir * 0.0668 (0.0016) C28 * -0.0280 (0.0019) C27 * -0.0526 (0.0019) C18 * 0.0777 (0.0015) N17Rms deviation of fitted atoms = 0.06022.1808 (0.0086) x + 0.5392 (0.0092) y + 17.4903 (0.0021) z = 5.6802 (0.0088)Angle to previous plane (with approximate e.s.d.) = 78.84 (0.08)* -0.0035 (0.0009) Ir * 0.0040 (0.0013) N33 * -0.0019 (0.0016) C37 * -0.0031 (0.0016) C38 * 0.0045 (0.0014) N39Rms deviation of fitted atoms = 0.00358.0107 (0.0039) x - 5.0559 (0.0100) y + 1.0694 (0.0169) z = 0.3793 (0.0119)Angle to previous plane (with approximate e.s.d.) = 78.79 (0.08)* 0.0612 (0.0010) Ir * -0.0747 (0.0014) N1 * 0.0495 (0.0016) C2 * 0.0270 (0.0017) C11 * -0.0630 (0.0014) C12Rms deviation of fitted atoms = 0.05748.1366 (0.0044) x - 4.6169 (0.0120) y + 2.7467 (0.0185) z = 1.1577 (0.0155)Angle to previous plane (with approximate e.s.d.) = 5.58 (0.11)* -0.0062 (0.0018) C11 * 0.0042 (0.0018) C12 * 0.0004 (0.0019) C13 * -0.0031 (0.0020) C14 * 0.0011 (0.0020) C15 * 0.0036 (0.0019) C16Rms deviation of fitted atoms = 0.0036- 7.1556 (0.0029) x + 6.8670 (0.0050) y - 1.5139 (0.0120) z = 1.5526 (0.0051)Angle to previous plane (with approximate e.s.d.) = 11.79 (0.10)* -0.0880 (0.0018) N1 * 0.0273 (0.0020) C2 * 0.0689 (0.0021) C3 * 0.0094 (0.0021) C4 * -0.0354 (0.0024) C5 * -0.0377 (0.0021) C6 * -0.0110 (0.0022) C7 * 0.0624 (0.0021) C8 * 0.0474 (0.0020) C9 * -0.0432 (0.0022) C10Rms deviation of fitted atoms = 0.04913.8481 (0.0098) x + 11.4658 (0.0058) y + 6.3281 (0.0208) z = 11.7536 (0.0044)Angle to previous plane (with approximate e.s.d.) = 77.79 (0.06)* -0.0067 (0.0020) C28 * 0.0001 (0.0020) C29 * 0.0072 (0.0023) C30 * -0.0080 (0.0025) C31 * 0.0013 (0.0023) C32 * 0.0060 (0.0021) C27Rms deviation of fitted atoms = 0.00582.0501 (0.0054) x + 12.1910 (0.0019) y + 5.3371 (0.0154) z = 11.4565 (0.0058)Angle to previous plane (with approximate e.s.d.) = 12.28 (0.08)* -0.0704 (0.0021) N17 * 0.0393 (0.0024) C18 * 0.0498 (0.0028) C19 * -0.0036 (0.0029) C20 * -0.0280 (0.0030) C21 * -0.0253 (0.0030) C22 * 0.0012 (0.0029) C23 * 0.0474 (0.0026) C24 * 0.0300 (0.0024) C25 * -0.0404 (0.0026) C26Rms deviation of fitted atoms = 0.03902.0139 (0.0103) x + 0.5046 (0.0150) y + 17.5147 (0.0030) z = 5.5443 (0.0128)Angle to previous plane (with approximate e.s.d.) = 78.01 (0.09)* 0.0047 (0.0018) C38 * 0.0079 (0.0017) N39 * -0.0141 (0.0019) C40 * 0.0073 (0.0022) C41 * 0.0051 (0.0023) C42 * -0.0109 (0.0020) C43Rms deviation of fitted atoms = 0.00902.2942 (0.0112) x + 0.5668 (0.0154) y + 17.4708 (0.0033) z = 5.7456 (0.0097)Angle to previous plane (with approximate e.s.d.) = 1.81 (0.06)* -0.0023 (0.0014) N33 * 0.0007 (0.0014) N34 * 0.0010 (0.0015) C35 * -0.0024 (0.0015) N36 * 0.0029 (0.0015) C37Rms deviation of fitted atoms = 0.00203.5283 (0.0116) x - 0.8562 (0.0173) y + 16.6404 (0.0084) z = 5.4129 (0.0060)Angle to previous plane (with approximate e.s.d.) = 11.00 (0.10)* -0.0031 (0.0021) C44 * 0.0013 (0.0022) C45 * -0.0006 (0.0025) C46 * 0.0019 (0.0027) C47 * -0.0038 (0.0027) C48 * 0.0044 (0.0024) C49Rms deviation of fitted atoms = 0.0029
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
Ir0.479659 (11)0.724128 (9)0.242431 (7)0.01435 (3)
N10.5063 (2)0.76795 (18)0.12298 (13)0.0164 (5)
C20.5821 (3)0.8582 (2)0.09770 (16)0.0183 (6)
C30.6254 (3)0.8918 (2)0.01826 (17)0.0241 (7)
H30.67970.95500.00220.029*
C40.5898 (3)0.8342 (2)−0.03560 (17)0.0250 (7)
H40.62270.8551−0.08890.030*
C50.5035 (3)0.7430 (2)−0.01136 (16)0.0224 (6)
C60.4578 (3)0.6834 (3)−0.06484 (17)0.0274 (7)
H60.48970.7018−0.11850.033*
C70.3680 (3)0.5992 (3)−0.03966 (18)0.0283 (7)
H70.34030.5578−0.07570.034*
C80.3166 (3)0.5737 (2)0.03924 (17)0.0253 (7)
H80.25040.51730.05590.030*
C90.3608 (3)0.6295 (2)0.09300 (16)0.0198 (6)
H90.32510.61140.14630.024*
C100.4586 (3)0.7129 (2)0.06896 (16)0.0184 (6)
C110.6096 (3)0.9190 (2)0.15802 (16)0.0189 (6)
C120.5580 (3)0.8711 (2)0.23424 (17)0.0190 (6)
C130.5710 (3)0.9308 (2)0.29458 (17)0.0226 (6)
H130.53710.90190.34640.027*
C140.6325 (3)1.0308 (2)0.27935 (19)0.0284 (7)
H140.63971.06950.32100.034*
C150.6835 (3)1.0757 (2)0.20527 (19)0.0293 (7)
H150.72571.14440.19610.035*
C160.6729 (3)1.0201 (2)0.14405 (18)0.0261 (7)
H160.70851.05040.09280.031*
N170.4354 (3)0.70179 (19)0.36314 (13)0.0239 (6)
C180.2901 (3)0.7236 (3)0.38966 (19)0.0348 (8)
C190.2355 (5)0.6990 (3)0.4688 (2)0.0534 (11)
H190.13300.71260.48570.064*
C200.3248 (5)0.6572 (3)0.5199 (2)0.0562 (11)
H200.28550.63900.57270.067*
C210.4788 (5)0.6398 (3)0.49591 (18)0.0439 (9)
C220.5786 (5)0.6009 (3)0.5471 (2)0.0589 (11)
H220.54230.58230.60020.071*
C230.7259 (5)0.5885 (3)0.5236 (2)0.0557 (11)
H230.79160.56070.55980.067*
C240.7820 (4)0.6177 (3)0.4441 (2)0.0431 (9)
H240.88570.61110.42750.052*
C250.6862 (3)0.6555 (2)0.39132 (17)0.0298 (7)
H250.72370.67530.33850.036*
C260.5336 (4)0.6647 (2)0.41575 (17)0.0290 (7)
C270.1995 (3)0.7753 (3)0.3323 (2)0.0338 (8)
C280.2731 (3)0.7910 (2)0.25696 (19)0.0266 (7)
C290.1941 (3)0.8497 (2)0.1998 (2)0.0354 (8)
H290.24120.86250.14800.043*
C300.0488 (4)0.8890 (3)0.2181 (3)0.0552 (12)
H30−0.00210.92910.17880.066*
C31−0.0228 (4)0.8707 (3)0.2923 (3)0.0645 (14)
H31−0.12320.89650.30390.077*
C320.0508 (4)0.8153 (3)0.3494 (3)0.0541 (11)
H320.00190.80360.40100.065*
N330.4299 (2)0.55788 (18)0.25419 (12)0.0145 (5)
N340.3042 (2)0.50125 (18)0.27271 (13)0.0185 (5)
C350.3547 (3)0.3969 (2)0.26948 (14)0.0169 (6)
N360.5032 (2)0.38198 (18)0.25027 (12)0.0169 (5)
C370.5433 (3)0.4844 (2)0.24198 (14)0.0148 (5)
C380.6914 (3)0.5248 (2)0.22220 (15)0.0167 (6)
N390.6947 (2)0.63400 (18)0.21885 (12)0.0153 (5)
C400.8272 (3)0.6779 (2)0.20110 (16)0.0205 (6)
H400.83000.75470.19680.025*
C410.9589 (3)0.6165 (3)0.18894 (19)0.0317 (8)
H411.05070.65000.17830.038*
C420.9549 (3)0.5056 (3)0.19247 (19)0.0334 (8)
H421.04430.46160.18400.040*
C430.8196 (3)0.4583 (2)0.20849 (17)0.0254 (7)
H430.81470.38200.21000.030*
C440.2545 (3)0.3068 (2)0.28691 (16)0.0215 (6)
C450.3072 (3)0.2027 (2)0.27066 (17)0.0258 (7)
H450.40760.19040.24900.031*
C460.2140 (4)0.1174 (3)0.2859 (2)0.0387 (8)
H460.25040.04700.27440.046*
C470.0680 (4)0.1350 (3)0.3179 (2)0.0477 (10)
H470.00400.07670.32880.057*
C480.0154 (4)0.2382 (3)0.3340 (2)0.0472 (10)
H48−0.08520.25030.35540.057*
C490.1075 (3)0.3236 (3)0.31940 (18)0.0330 (8)
H490.07060.39360.33150.040*
C980.9808 (4)1.2544 (3)0.0450 (2)0.0480 (10)
H980.87701.28660.05520.058*
Cl11.03734 (9)1.19846 (8)0.13387 (6)0.0509 (2)
Cl20.98185 (9)1.15510 (8)−0.01637 (6)0.0519 (3)
Cl31.09404 (12)1.35913 (7)0.00000 (6)0.0619 (3)
U11U22U33U12U13U23
Ir0.01027 (5)0.01557 (6)0.01753 (5)−0.00124 (4)0.00080 (4)−0.00580 (4)
N10.0137 (11)0.0170 (12)0.0190 (12)0.0011 (9)−0.0057 (9)−0.0016 (10)
C20.0145 (14)0.0177 (15)0.0219 (15)0.0030 (11)−0.0063 (11)0.0011 (12)
C30.0183 (15)0.0236 (17)0.0286 (17)0.0005 (12)−0.0045 (12)0.0029 (13)
C40.0206 (15)0.0322 (18)0.0177 (15)0.0092 (13)−0.0024 (12)0.0046 (13)
C50.0157 (14)0.0289 (17)0.0224 (15)0.0077 (12)−0.0059 (12)−0.0047 (13)
C60.0237 (16)0.0372 (19)0.0218 (16)0.0120 (14)−0.0072 (12)−0.0090 (14)
C70.0260 (16)0.0340 (19)0.0292 (17)0.0109 (14)−0.0132 (13)−0.0161 (15)
C80.0193 (15)0.0284 (17)0.0321 (17)0.0038 (13)−0.0108 (13)−0.0130 (14)
C90.0155 (14)0.0219 (16)0.0228 (15)0.0031 (11)−0.0061 (11)−0.0044 (12)
C100.0130 (13)0.0232 (16)0.0199 (15)0.0075 (11)−0.0074 (11)−0.0057 (12)
C110.0114 (13)0.0179 (15)0.0274 (16)0.0023 (11)−0.0055 (11)−0.0018 (12)
C120.0089 (13)0.0183 (15)0.0309 (17)0.0003 (11)−0.0028 (11)−0.0075 (13)
C130.0194 (15)0.0226 (16)0.0266 (16)−0.0023 (12)−0.0029 (12)−0.0053 (13)
C140.0262 (16)0.0241 (17)0.0389 (19)−0.0049 (13)−0.0101 (14)−0.0099 (15)
C150.0266 (16)0.0153 (16)0.048 (2)−0.0090 (13)−0.0103 (15)−0.0008 (14)
C160.0210 (15)0.0228 (16)0.0330 (18)−0.0039 (13)−0.0059 (13)0.0048 (13)
N170.0315 (14)0.0215 (14)0.0196 (13)−0.0124 (11)0.0068 (10)−0.0094 (11)
C180.0363 (18)0.0285 (19)0.0391 (19)−0.0156 (14)0.0231 (15)−0.0230 (15)
C190.065 (3)0.047 (2)0.046 (2)−0.025 (2)0.0348 (19)−0.027 (2)
C200.090 (3)0.044 (2)0.031 (2)−0.031 (2)0.036 (2)−0.0190 (18)
C210.090 (3)0.029 (2)0.0147 (16)−0.0232 (19)0.0005 (17)−0.0069 (15)
C220.118 (3)0.043 (2)0.0192 (19)−0.027 (3)−0.008 (2)−0.0038 (17)
C230.118 (3)0.031 (2)0.029 (2)−0.013 (2)−0.045 (2)0.0019 (17)
C240.065 (2)0.036 (2)0.036 (2)−0.0128 (18)−0.0306 (18)0.0001 (16)
C250.049 (2)0.0257 (17)0.0184 (16)−0.0096 (15)−0.0127 (14)−0.0035 (13)
C260.051 (2)0.0201 (17)0.0175 (15)−0.0127 (15)0.0003 (14)−0.0084 (13)
C270.0210 (16)0.0265 (18)0.057 (2)−0.0097 (13)0.0094 (15)−0.0267 (16)
C280.0155 (14)0.0172 (16)0.051 (2)−0.0057 (12)0.0017 (13)−0.0216 (15)
C290.0188 (15)0.0224 (17)0.073 (3)0.0013 (13)−0.0158 (16)−0.0240 (17)
C300.0200 (18)0.036 (2)0.124 (4)0.0090 (16)−0.026 (2)−0.047 (2)
C310.0127 (18)0.047 (3)0.145 (4)0.0018 (16)−0.002 (2)−0.062 (3)
C320.0250 (18)0.042 (2)0.099 (3)−0.0172 (16)0.0256 (19)−0.050 (2)
N330.0144 (11)0.0160 (12)0.0132 (12)−0.0018 (9)0.0017 (9)−0.0056 (9)
N340.0170 (12)0.0172 (12)0.0210 (13)−0.0051 (10)0.0037 (10)−0.0062 (10)
C350.0227 (14)0.0170 (14)0.0109 (13)−0.0033 (11)0.0006 (11)−0.0035 (11)
N360.0207 (12)0.0162 (12)0.0146 (12)−0.0002 (9)−0.0048 (9)−0.0029 (10)
C370.0161 (13)0.0180 (14)0.0109 (13)0.0006 (11)−0.0036 (10)−0.0029 (11)
C380.0171 (13)0.0203 (15)0.0147 (14)−0.0013 (11)−0.0057 (11)−0.0057 (11)
N390.0111 (11)0.0204 (13)0.0156 (12)−0.0015 (9)−0.0023 (9)−0.0055 (10)
C400.0149 (14)0.0237 (16)0.0245 (16)−0.0026 (12)−0.0010 (12)−0.0093 (13)
C410.0124 (14)0.0341 (19)0.051 (2)−0.0007 (13)−0.0025 (14)−0.0148 (17)
C420.0149 (15)0.035 (2)0.053 (2)0.0089 (13)−0.0069 (14)−0.0177 (17)
C430.0198 (15)0.0235 (17)0.0356 (18)0.0044 (12)−0.0091 (13)−0.0111 (14)
C440.0268 (15)0.0195 (15)0.0182 (15)−0.0054 (12)−0.0002 (12)−0.0035 (12)
C450.0299 (16)0.0197 (16)0.0274 (17)−0.0029 (13)−0.0007 (13)−0.0049 (13)
C460.048 (2)0.0209 (18)0.046 (2)−0.0094 (15)0.0068 (17)−0.0090 (16)
C470.052 (2)0.029 (2)0.060 (3)−0.0240 (17)0.0233 (19)−0.0152 (18)
C480.045 (2)0.037 (2)0.057 (2)−0.0215 (17)0.0272 (18)−0.0181 (19)
C490.0357 (18)0.0235 (17)0.038 (2)−0.0119 (14)0.0150 (15)−0.0113 (15)
C980.0281 (19)0.041 (2)0.079 (3)0.0085 (16)−0.0137 (19)−0.021 (2)
Cl10.0316 (5)0.0592 (6)0.0578 (6)−0.0033 (4)0.0045 (4)−0.0049 (5)
Cl20.0398 (5)0.0402 (6)0.0808 (8)−0.0097 (4)−0.0109 (5)−0.0188 (5)
Cl30.0956 (8)0.0249 (5)0.0750 (8)−0.0077 (5)−0.0487 (6)0.0000 (5)
Ir—C281.995 (3)N36—C371.336 (3)
Ir—C121.997 (3)C37—C381.460 (3)
Ir—N12.084 (2)C38—N391.354 (3)
Ir—N172.093 (2)C38—C431.389 (4)
Ir—N332.129 (2)N39—C401.346 (3)
Ir—N392.196 (2)C40—C411.378 (4)
N1—C21.353 (3)C41—C421.375 (4)
N1—C101.392 (3)C42—C431.388 (4)
C2—C31.412 (4)C44—C491.393 (4)
C2—C111.457 (4)C44—C451.398 (4)
C3—C41.363 (4)C45—C461.387 (4)
C4—C51.414 (4)C46—C471.384 (4)
C5—C61.413 (4)C47—C481.387 (4)
C5—C101.421 (4)C48—C491.381 (4)
C6—C71.367 (4)C98—Cl11.753 (4)
C7—C81.403 (4)C98—Cl31.755 (4)
C8—C91.380 (4)C98—Cl21.760 (3)
C9—C101.403 (4)C3—H30.9500
C11—C161.402 (4)C4—H40.9500
C11—C121.419 (4)C6—H60.9500
C12—C131.411 (4)C7—H70.9500
C13—C141.382 (4)C8—H80.9500
C14—C151.375 (4)C9—H90.9500
C15—C161.387 (4)C13—H130.9500
N17—C181.361 (4)C14—H140.9500
N17—C261.391 (4)C15—H150.9500
C18—C191.411 (5)C16—H160.9500
C18—C271.447 (5)C19—H190.9500
C19—C201.328 (5)C20—H200.9500
C20—C211.417 (5)C22—H220.9500
C21—C221.387 (5)C23—H230.9500
C21—C261.429 (4)C24—H240.9500
C22—C231.352 (5)C25—H250.9500
C23—C241.428 (5)C29—H290.9500
C24—C251.379 (4)C30—H300.9500
C25—C261.398 (4)C31—H310.9500
C27—C281.394 (4)C32—H320.9500
C27—C321.413 (4)C40—H400.9500
C28—C291.408 (4)C41—H410.9500
C29—C301.386 (4)C42—H420.9500
C30—C311.372 (6)C43—H430.9500
C31—C321.365 (6)C45—H450.9500
N33—C371.339 (3)C46—H460.9500
N33—N341.371 (3)C47—H470.9500
N34—C351.347 (3)C48—H480.9500
C35—N361.354 (3)C49—H490.9500
C35—C441.476 (4)C98—H981.0000
C28—Ir—C1289.81 (10)N39—C38—C43122.0 (2)
C28—Ir—N193.57 (11)N39—C38—C37114.3 (2)
C12—Ir—N179.82 (10)C43—C38—C37123.7 (3)
C28—Ir—N1779.82 (12)C40—N39—C38118.0 (2)
C12—Ir—N1795.05 (10)C40—N39—Ir125.77 (18)
N1—Ir—N17171.70 (9)C38—N39—Ir116.20 (16)
C28—Ir—N3398.69 (10)N39—C40—C41123.0 (3)
C12—Ir—N33171.11 (9)C42—C41—C40118.7 (3)
N1—Ir—N33102.08 (8)C41—C42—C43119.6 (3)
N17—Ir—N3383.99 (8)C42—C43—C38118.6 (3)
C28—Ir—N39172.20 (9)C49—C44—C45119.2 (3)
C12—Ir—N3996.86 (9)C49—C44—C35121.0 (3)
N1—Ir—N3983.69 (8)C45—C44—C35119.9 (3)
N17—Ir—N39103.50 (9)C46—C45—C44120.6 (3)
N33—Ir—N3974.85 (8)C47—C46—C45119.8 (3)
C2—N1—C10118.8 (2)C46—C47—C48119.7 (3)
C2—N1—Ir114.28 (18)C49—C48—C47120.9 (3)
C10—N1—Ir126.87 (19)C48—C49—C44119.9 (3)
N1—C2—C3121.6 (3)Cl1—C98—Cl3110.20 (18)
N1—C2—C11115.0 (2)Cl1—C98—Cl2111.88 (19)
C3—C2—C11123.3 (3)Cl3—C98—Cl2110.3 (2)
C4—C3—C2120.4 (3)C4—C3—H3119.8
C3—C4—C5119.4 (3)C2—C3—H3119.8
C6—C5—C4121.7 (3)C3—C4—H4120.3
C6—C5—C10119.5 (3)C5—C4—H4120.3
C4—C5—C10118.8 (3)C7—C6—H6119.9
C7—C6—C5120.2 (3)C5—C6—H6119.9
C6—C7—C8120.2 (3)C6—C7—H7119.9
C9—C8—C7120.9 (3)C8—C7—H7119.9
C8—C9—C10120.0 (3)C9—C8—H8119.6
N1—C10—C9120.3 (2)C7—C8—H8119.6
N1—C10—C5120.6 (3)C8—C9—H9120.0
C9—C10—C5119.0 (3)C10—C9—H9120.0
C16—C11—C12121.1 (3)C14—C13—H13119.5
C16—C11—C2124.3 (3)C12—C13—H13119.5
C12—C11—C2114.5 (2)C15—C14—H14119.2
C13—C12—C11116.9 (3)C13—C14—H14119.2
C13—C12—Ir128.0 (2)C14—C15—H15120.2
C11—C12—Ir115.1 (2)C16—C15—H15120.2
C14—C13—C12120.9 (3)C15—C16—H16120.1
C15—C14—C13121.5 (3)C11—C16—H16120.1
C14—C15—C16119.7 (3)C20—C19—H19119.4
C15—C16—C11119.9 (3)C18—C19—H19119.4
C18—N17—C26119.3 (3)C19—C20—H20120.0
C18—N17—Ir112.8 (2)C21—C20—H20120.0
C26—N17—Ir127.88 (19)C23—C22—H22119.0
N17—C18—C19120.8 (3)C21—C22—H22119.0
N17—C18—C27115.7 (3)C22—C23—H23120.2
C19—C18—C27123.5 (3)C24—C23—H23120.2
C20—C19—C18121.2 (4)C25—C24—H24119.9
C19—C20—C21120.0 (3)C23—C24—H24119.9
C22—C21—C20122.7 (4)C24—C25—H25120.1
C22—C21—C26118.7 (4)C26—C25—H25120.1
C20—C21—C26118.6 (3)C30—C29—H29119.5
C23—C22—C21122.0 (4)C28—C29—H29119.5
C22—C23—C24119.5 (3)C31—C30—H30119.6
C25—C24—C23120.2 (4)C29—C30—H30119.6
C24—C25—C26119.9 (3)C32—C31—H31120.1
N17—C26—C25120.6 (3)C30—C31—H31120.1
N17—C26—C21119.8 (3)C31—C32—H32119.9
C25—C26—C21119.6 (3)C27—C32—H32119.9
C28—C27—C32120.7 (3)N39—C40—H40118.5
C28—C27—C18114.9 (3)C41—C40—H40118.5
C32—C27—C18124.2 (3)C42—C41—H41120.7
C27—C28—C29117.3 (3)C40—C41—H41120.7
C27—C28—Ir115.4 (2)C41—C42—H42120.2
C29—C28—Ir127.3 (2)C43—C42—H42120.2
C30—C29—C28120.9 (4)C42—C43—H43120.7
C31—C30—C29120.9 (4)C38—C43—H43120.7
C32—C31—C30119.8 (3)C46—C45—H45119.7
C31—C32—C27120.3 (4)C44—C45—H45119.7
C37—N33—N34106.6 (2)C47—C46—H46120.1
C37—N33—Ir117.48 (17)C45—C46—H46120.1
N34—N33—Ir135.89 (16)C46—C47—H47120.1
C35—N34—N33103.7 (2)C48—C47—H47120.1
N34—C35—N36114.8 (2)C49—C48—H48119.6
N34—C35—C44121.9 (2)C47—C48—H48119.6
N36—C35—C44123.3 (2)C48—C49—H49120.1
C37—N36—C35100.9 (2)C44—C49—H49120.1
N36—C37—N33113.9 (2)Cl1—C98—H98108.1
N36—C37—C38128.8 (2)Cl3—C98—H98108.1
N33—C37—C38117.2 (2)Cl2—C98—H98108.1
  7 in total

1.  Inter-ligand energy transfer and related emission change in the cyclometalated heteroleptic iridium complex: facile and efficient color tuning over the whole visible range by the ancillary ligand structure.

Authors:  Youngmin You; Soo Young Park
Journal:  J Am Chem Soc       Date:  2005-09-14       Impact factor: 15.419

2.  A short history of SHELX.

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

3.  Synthesis and characterization of phosphorescent cyclometalated iridium complexes.

Authors:  S Lamansky; P Djurovich; D Murphy; F Abdel-Razzaq; R Kwong; I Tsyba; M Bortz; B Mui; R Bau; M E Thompson
Journal:  Inorg Chem       Date:  2001-03-26       Impact factor: 5.165

4.  Tuning iridium(III) phenylpyridine complexes in the "almost blue" region.

Authors:  Paolo Coppo; Edward A Plummer; Luisa De Cola
Journal:  Chem Commun (Camb)       Date:  2004-06-30       Impact factor: 6.222

5.  Essential role of the ancillary ligand in the color tuning of iridium tetrazolate complexes.

Authors:  Stefano Stagni; Silvia Colella; Antonio Palazzi; Giovanni Valenti; Stefano Zacchini; Francesco Paolucci; Massimo Marcaccio; Rodrigo Q Albuquerque; Luisa De Cola
Journal:  Inorg Chem       Date:  2008-10-22       Impact factor: 5.165

6.  mer-Bis[2-(1,3-benzothiazol-2-yl)phenyl-κC,N][3-phenyl-5-(2-pyridyl)-1,2,4-triazol-1-ido-κN,N]iridium(III) deuterochloro-form 3.5-solvate.

Authors:  Peter G Jones; Andreas Freund; Andreas Weinkauf; Wolfgang Kowalsky; Hans-Hermann Johannes
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2010-08-11

7.  Structure validation in chemical crystallography.

Authors:  Anthony L Spek
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2009-01-20
  7 in total

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