Abstract
In the title compound, [Rh(C8H12)(C7H12N2)2]BF4, the square-planar Rh complex cation and the BF4 − anion are both bisected by a crystallographic twofold rotation axis. The Rh and B atoms lie on this axis and all others are in general positions. In the crystal, two unique C—H⋯F hydrogen-bonding interactions are present, which involve both imidazolin-2-ylidene H atoms. They form two separate C(5) motifs, the combination of which is a rippled hydrogen-bonded sheet structure in the ab plane.
Related literature
For the structure and dynamics of related N-heterocyclic carbene rhodium and iridium complexes, see: Chianese et al. (2003 ▶); Köcher & Herrmann (1997 ▶); Leung et al. (2006 ▶); Nichol et al. (2009 ▶, 2010 ▶); Herrmann et al. (2006 ▶). For the catalytic properties of these complexes, see: Albrecht et al. (2002 ▶); Frey et al. (2006 ▶); Gnanamgari et al. (2007 ▶); Voutchkova et al. (2008 ▶).
Experimental
Crystal data
[Rh(C8H12)(C7H12N2)2]BF4
M r = 546.27
Orthorhombic,
a = 11.7508 (6) Å
b = 11.9283 (6) Å
c = 17.3129 (9) Å
V = 2426.7 (2) Å3
Z = 4
Mo Kα radiation
μ = 0.75 mm−1
T = 100 K
0.38 × 0.37 × 0.37 mm
Data collection
Bruker Kappa APEXII DUO CCD diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.763, T max = 0.771
234794 measured reflections
14018 independent reflections
10241 reflections with I > 2σ(I)
R int = 0.033
Refinement
R[F 2 > 2σ(F 2)] = 0.020
wR(F 2) = 0.059
S = 1.13
14018 reflections
218 parameters
All H-atom parameters refined
Δρmax = 1.55 e Å−3
Δρmin = −0.92 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXTL and publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811049890/fj2478sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811049890/fj2478Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811049890/fj2478Isup3.cdx
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C2—H2⋯F1i | 0.909 (11) | 2.496 (11) | 3.3975 (8) | 171.4 (10) |
| C3—H3⋯F2ii | 0.877 (12) | 2.478 (12) | 3.2415 (8) | 145.9 (11) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
JR and DPW thank the Department of Chemistry, Millersville University, for project funding. The diffractometer was purchased with funding from NSF grant CHE-0741837.
supplementary crystallographic information
Comment
We are interested in rhodium and iridium complexes with N-heterocyclic carbene ligands, in particular ligands derived from 1,2,4-triazole-derived compounds (Nichol et al., 2009, 2010). The title compound, (I), was prepared as part of this study (Figure 1). The Rh center has an expected square planar geometry and bond distances are unexceptional. Both the Rh and B atoms lie on a crystallographic twofold rotation axis, which bisects the complex and BF4- counterion. C–H···F hydrogen bonding interactions, which involve both imidazolin-2-ylidene H atoms and all four F atoms, form a thick two-dimensional sheet structure in the ab plane (Figure 2).
Experimental
The title compound was synthesized by transmetallation. 1-Isopropyl-3-methylimidazolium bromide (268 mg, 1.31 mmol) was mixed with Ag2O (152 mg, 0.654 mmol), and was stirred under dark at room temperature for 90 minutes in 10 ml of CH2Cl2. The resulting mixture was filtered through Celite into a new flask containing the neutral compound [(cod)Rh(NHC)Cl](585 mg, 1.31 mmol), and AgBF4(254 mg, 1.31 mmol)and stirred for an additional 90 minutes under dark. The mixture was filtered once more through Celite to remove silver bromide and silver chloride, and the solvent was removed under pressure to give a yellow solid (93%). Crystals of the resulting solid of the title compound, (I), were obtained by slow diffusion of pentane into dichloromethane solution of the compound. 1H NMR (400 MHz, CDCl3): δ (p.p.m.) = 7.15 (s, 2 H, NCH), 6.93 (s, 2 H, NCH), 5.03 (m, 3JH—H = 6.8 Hz, 2 H, CH of iPr), 4.63 (br, 2 H, CH of COD), 4.21 (s, 6 H, N—CH3), 3.92 (m, 2 H, CH of COD), 2.63 (m, 2 H, CH2 of COD), 2.42 – 1.92 (m, 6 H, CH2 of COD), 1.46 (d, 3JH—H = 6.8 Hz, 6 H, CH3 of iPr), 1.00 (d, 3JH—H = 6.8 Hz, 6 H, CH3 of iPr). 13C NMR: δ = 178.76, 178.22 (Ir—C), 124, 117 (N—CH—N), 91.34, 91.25 (N-CHMe3), 86.36, 86.28 (N—CH3), 52.60 (CH of COD), 38.10, 33.75, 27.99, (CH2 of COD), 23.5, 22.90 (CH3 of iPr).
Refinement
H atoms were located from a difference Fourier map and are freely refined.
Figures
Fig. 1.
Twice the asymmetric unit of (I), with H atoms omitted. Displacement ellipsoids are at the 50% probability level. Unlabeled atoms are related to labeled atoms by twofold rotation symmetry.
Fig. 2.
A c-axis projection showing C–H···F interactions (blue dotted lines) in (I). Red dotted lines indicate H bond continuation.
Crystal data
| [Rh(C8H12)(C7H12N2)2]BF4 | F(000) = 1128 |
| Mr = 546.27 | Dx = 1.495 Mg m−3 |
| Orthorhombic, Pccn | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ab 2ac | Cell parameters from 9624 reflections |
| a = 11.7508 (6) Å | θ = 4.2–51.7° |
| b = 11.9283 (6) Å | µ = 0.75 mm−1 |
| c = 17.3129 (9) Å | T = 100 K |
| V = 2426.7 (2) Å3 | Block, yellow |
| Z = 4 | 0.38 × 0.37 × 0.37 mm |
Data collection
| Bruker Kappa APEXII DUO CCD diffractometer | 14018 independent reflections |
| Radiation source: fine-focus sealed tube with Miracol optics | 10241 reflections with I > 2σ(I) |
| graphite | Rint = 0.033 |
| φ and ω scans | θmax = 52.3°, θmin = 2.9° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −26→25 |
| Tmin = 0.763, Tmax = 0.771 | k = −26→26 |
| 234794 measured reflections | l = −37→38 |
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)] = 0.020 | Hydrogen site location: difference Fourier map |
| wR(F2) = 0.059 | All H-atom parameters refined |
| S = 1.13 | w = 1/[σ2(Fo2) + (0.0182P)2 + 0.6772P] where P = (Fo2 + 2Fc2)/3 |
| 14018 reflections | (Δ/σ)max = 0.002 |
| 218 parameters | Δρmax = 1.55 e Å−3 |
| 0 restraints | Δρmin = −0.92 e Å−3 |
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. |
| 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 | ||
| Rh1 | 0.7500 | 0.2500 | 0.507678 (3) | 0.01052 (1) | |
| N1 | 0.56243 (4) | 0.20105 (4) | 0.38873 (3) | 0.01399 (6) | |
| N2 | 0.66738 (4) | 0.05648 (4) | 0.40496 (3) | 0.01512 (6) | |
| C1 | 0.65651 (4) | 0.16534 (4) | 0.42664 (3) | 0.01295 (6) | |
| C2 | 0.51512 (5) | 0.11598 (5) | 0.34425 (4) | 0.01757 (8) | |
| H2 | 0.4526 (10) | 0.1269 (10) | 0.3143 (7) | 0.022 (3)* | |
| C3 | 0.58158 (5) | 0.02502 (5) | 0.35458 (4) | 0.01811 (8) | |
| H3 | 0.5769 (10) | −0.0434 (10) | 0.3364 (7) | 0.028 (3)* | |
| C4 | 0.51719 (5) | 0.31568 (5) | 0.39338 (3) | 0.01602 (7) | |
| H4 | 0.5633 (9) | 0.3517 (9) | 0.4313 (6) | 0.019 (3)* | |
| C5 | 0.53212 (7) | 0.37474 (6) | 0.31623 (4) | 0.02376 (11) | |
| H5A | 0.4910 (11) | 0.3362 (11) | 0.2772 (7) | 0.030 (3)* | |
| H5B | 0.6089 (11) | 0.3778 (11) | 0.3028 (8) | 0.031 (3)* | |
| H5C | 0.5034 (11) | 0.4517 (11) | 0.3183 (8) | 0.035 (3)* | |
| C6 | 0.39373 (6) | 0.31435 (7) | 0.41936 (5) | 0.02579 (12) | |
| H6A | 0.3478 (11) | 0.2754 (11) | 0.3834 (8) | 0.028 (3)* | |
| H6B | 0.3635 (11) | 0.3876 (11) | 0.4230 (8) | 0.035 (3)* | |
| H6C | 0.3844 (12) | 0.2775 (12) | 0.4678 (9) | 0.033 (3)* | |
| C7 | 0.75478 (6) | −0.02030 (5) | 0.43195 (4) | 0.02033 (9) | |
| H7A | 0.8005 (10) | 0.0166 (10) | 0.4689 (7) | 0.024 (3)* | |
| H7B | 0.7196 (11) | −0.0845 (12) | 0.4540 (8) | 0.031 (3)* | |
| H7C | 0.8014 (11) | −0.0430 (11) | 0.3906 (8) | 0.032 (3)* | |
| C8 | 0.61291 (5) | 0.22486 (5) | 0.59096 (3) | 0.01603 (7) | |
| H8 | 0.5433 (10) | 0.2098 (10) | 0.5610 (7) | 0.021 (3)* | |
| C9 | 0.68830 (5) | 0.13645 (5) | 0.60051 (3) | 0.01646 (8) | |
| H9 | 0.6691 (10) | 0.0669 (10) | 0.5751 (7) | 0.025 (3)* | |
| C10 | 0.77717 (6) | 0.12488 (6) | 0.66365 (4) | 0.01943 (9) | |
| H10A | 0.7517 (9) | 0.1609 (11) | 0.7107 (8) | 0.023 (3)* | |
| H10B | 0.7852 (10) | 0.0442 (11) | 0.6775 (7) | 0.026 (3)* | |
| C11 | 0.89369 (5) | 0.16926 (6) | 0.63829 (4) | 0.01888 (9) | |
| H11A | 0.9440 (9) | 0.1813 (9) | 0.6833 (7) | 0.020 (2)* | |
| H11B | 0.9335 (10) | 0.1111 (10) | 0.6049 (7) | 0.023 (3)* | |
| B1 | 0.7500 | 0.7500 | 0.29593 (6) | 0.01705 (12) | |
| F1 | 0.76439 (5) | 0.84479 (5) | 0.24966 (3) | 0.03003 (10) | |
| F2 | 0.65419 (4) | 0.76347 (4) | 0.34218 (3) | 0.02659 (9) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Rh1 | 0.01063 (2) | 0.00980 (2) | 0.01114 (2) | −0.00124 (1) | 0.000 | 0.000 |
| N1 | 0.01412 (14) | 0.01361 (14) | 0.01424 (15) | 0.00070 (11) | −0.00193 (11) | −0.00109 (12) |
| N2 | 0.01684 (16) | 0.01164 (14) | 0.01689 (16) | 0.00010 (12) | −0.00365 (13) | −0.00144 (12) |
| C1 | 0.01345 (15) | 0.01194 (15) | 0.01347 (16) | −0.00035 (12) | −0.00093 (12) | −0.00044 (12) |
| C2 | 0.01794 (19) | 0.01713 (19) | 0.0176 (2) | −0.00031 (15) | −0.00510 (16) | −0.00262 (15) |
| C3 | 0.0211 (2) | 0.01475 (18) | 0.0185 (2) | −0.00131 (16) | −0.00536 (17) | −0.00293 (15) |
| C4 | 0.01615 (18) | 0.01608 (18) | 0.01583 (18) | 0.00398 (14) | −0.00011 (14) | −0.00123 (14) |
| C5 | 0.0321 (3) | 0.0195 (2) | 0.0197 (2) | 0.0075 (2) | 0.0032 (2) | 0.00306 (19) |
| C6 | 0.0185 (2) | 0.0318 (3) | 0.0270 (3) | 0.0065 (2) | 0.0043 (2) | −0.0023 (2) |
| C7 | 0.0218 (2) | 0.01268 (16) | 0.0265 (3) | 0.00234 (17) | −0.0073 (2) | −0.00142 (16) |
| C8 | 0.01421 (17) | 0.01788 (18) | 0.01599 (18) | −0.00244 (14) | 0.00177 (14) | −0.00026 (15) |
| C9 | 0.01790 (19) | 0.01465 (17) | 0.01685 (19) | −0.00334 (15) | 0.00120 (15) | 0.00176 (14) |
| C10 | 0.0215 (2) | 0.0200 (2) | 0.0168 (2) | −0.00095 (18) | −0.00002 (17) | 0.00507 (17) |
| C11 | 0.0179 (2) | 0.0210 (2) | 0.0178 (2) | 0.00064 (17) | −0.00287 (16) | 0.00310 (17) |
| B1 | 0.0149 (3) | 0.0145 (3) | 0.0218 (3) | 0.0006 (2) | 0.000 | 0.000 |
| F1 | 0.0346 (3) | 0.0235 (2) | 0.0320 (2) | 0.00074 (18) | 0.00329 (18) | 0.01073 (17) |
| F2 | 0.01926 (17) | 0.02301 (19) | 0.0375 (3) | 0.00023 (13) | 0.00938 (16) | −0.00171 (16) |
Geometric parameters (Å, °)
| Rh1—C1 | 2.0482 (5) | C6—H6A | 0.946 (13) |
| Rh1—C1i | 2.0482 (5) | C6—H6B | 0.946 (14) |
| Rh1—C8 | 2.1826 (6) | C6—H6C | 0.952 (15) |
| Rh1—C8i | 2.1826 (6) | C7—H7A | 0.944 (12) |
| Rh1—C9 | 2.2233 (6) | C7—H7B | 0.950 (14) |
| Rh1—C9i | 2.2233 (6) | C7—H7C | 0.941 (13) |
| N1—C1 | 1.3544 (7) | C8—H8 | 0.985 (12) |
| N1—C2 | 1.3899 (7) | C8—C9 | 1.3872 (9) |
| N1—C4 | 1.4692 (7) | C8—C11i | 1.5074 (9) |
| N2—C1 | 1.3577 (7) | C9—H9 | 0.965 (12) |
| N2—C3 | 1.3850 (7) | C9—C10 | 1.5181 (9) |
| N2—C7 | 1.4532 (8) | C10—H10A | 0.968 (13) |
| C2—H2 | 0.909 (11) | C10—H10B | 0.997 (13) |
| C2—C3 | 1.3487 (9) | C10—C11 | 1.5322 (9) |
| C3—H3 | 0.877 (12) | C11—C8i | 1.5075 (9) |
| C4—H4 | 0.954 (11) | C11—H11A | 0.989 (11) |
| C4—C5 | 1.5202 (9) | C11—H11B | 1.017 (12) |
| C4—C6 | 1.5190 (9) | B1—F1 | 1.3960 (8) |
| C5—H5A | 0.950 (13) | B1—F1ii | 1.3960 (8) |
| C5—H5B | 0.933 (13) | B1—F2 | 1.3908 (8) |
| C5—H5C | 0.979 (14) | B1—F2ii | 1.3909 (8) |
| C1—Rh1—C1i | 93.53 (3) | C4—C6—H6A | 110.8 (8) |
| C1—Rh1—C8 | 89.36 (2) | C4—C6—H6B | 111.7 (8) |
| C1i—Rh1—C8i | 89.36 (2) | C4—C6—H6C | 112.0 (8) |
| C1—Rh1—C8i | 156.36 (2) | H6A—C6—H6B | 106.4 (11) |
| C1i—Rh1—C8 | 156.36 (2) | H6A—C6—H6C | 106.7 (11) |
| C1—Rh1—C9 | 91.14 (2) | H6B—C6—H6C | 108.9 (11) |
| C1i—Rh1—C9 | 166.03 (2) | N2—C7—H7A | 109.0 (7) |
| C1i—Rh1—C9i | 91.14 (2) | N2—C7—H7B | 109.3 (8) |
| C1—Rh1—C9i | 166.03 (2) | N2—C7—H7C | 110.4 (8) |
| C8—Rh1—C8i | 97.31 (3) | H7A—C7—H7B | 110.6 (11) |
| C8—Rh1—C9 | 36.69 (2) | H7A—C7—H7C | 108.6 (11) |
| C8i—Rh1—C9 | 81.19 (2) | H7B—C7—H7C | 109.0 (11) |
| C8i—Rh1—C9i | 36.69 (2) | Rh1—C8—H8 | 106.8 (7) |
| C8—Rh1—C9i | 81.19 (2) | Rh1—C8—C9 | 73.25 (3) |
| C9—Rh1—C9i | 87.42 (3) | Rh1—C8—C11i | 106.38 (4) |
| C1—N1—C2 | 111.43 (5) | H8—C8—C9 | 117.0 (7) |
| C1—N1—C4 | 124.16 (5) | H8—C8—C11i | 113.3 (7) |
| C2—N1—C4 | 124.41 (5) | C9—C8—C11i | 127.23 (5) |
| C1—N2—C3 | 111.39 (5) | Rh1—C9—C8 | 70.06 (3) |
| C1—N2—C7 | 125.48 (5) | Rh1—C9—H9 | 105.7 (7) |
| C3—N2—C7 | 123.10 (5) | Rh1—C9—C10 | 110.59 (4) |
| Rh1—C1—N1 | 127.93 (4) | C8—C9—H9 | 116.7 (7) |
| Rh1—C1—N2 | 127.62 (4) | C8—C9—C10 | 126.46 (6) |
| N1—C1—N2 | 104.10 (4) | H9—C9—C10 | 114.2 (7) |
| N1—C2—H2 | 122.4 (7) | C9—C10—H10A | 110.7 (7) |
| N1—C2—C3 | 106.40 (5) | C9—C10—H10B | 109.0 (7) |
| H2—C2—C3 | 131.2 (7) | C9—C10—C11 | 112.14 (5) |
| N2—C3—C2 | 106.68 (5) | H10A—C10—H10B | 104.8 (11) |
| N2—C3—H3 | 121.6 (8) | H10A—C10—C11 | 111.3 (7) |
| C2—C3—H3 | 131.7 (8) | H10B—C10—C11 | 108.6 (7) |
| N1—C4—H4 | 104.6 (7) | C8i—C11—C10 | 113.53 (5) |
| N1—C4—C5 | 109.96 (5) | C8i—C11—H11A | 109.7 (7) |
| N1—C4—C6 | 110.61 (5) | C8i—C11—H11B | 106.6 (7) |
| H4—C4—C5 | 109.3 (7) | C10—C11—H11A | 111.0 (7) |
| H4—C4—C6 | 110.0 (7) | C10—C11—H11B | 109.8 (7) |
| C5—C4—C6 | 112.04 (6) | H11A—C11—H11B | 105.8 (9) |
| C4—C5—H5A | 110.0 (8) | F1—B1—F1ii | 109.97 (9) |
| C4—C5—H5B | 110.4 (8) | F1—B1—F2 | 109.56 (3) |
| C4—C5—H5C | 111.2 (8) | F1ii—B1—F2 | 109.02 (3) |
| H5A—C5—H5B | 109.5 (11) | F1ii—B1—F2ii | 109.56 (3) |
| H5A—C5—H5C | 107.7 (11) | F1—B1—F2ii | 109.02 (3) |
| H5B—C5—H5C | 107.9 (11) | F2—B1—F2ii | 109.70 (9) |
| C2—N1—C1—Rh1 | −173.45 (4) | C2—N1—C4—C6 | 56.65 (8) |
| C2—N1—C1—N2 | 0.13 (6) | C1—Rh1—C8—C9 | 92.76 (4) |
| C4—N1—C1—Rh1 | 7.28 (8) | C1i—Rh1—C8—C9 | −169.87 (5) |
| C4—N1—C1—N2 | −179.14 (5) | C1i—Rh1—C8—C11i | −45.11 (7) |
| C3—N2—C1—Rh1 | 173.54 (4) | C1—Rh1—C8—C11i | −142.49 (4) |
| C3—N2—C1—N1 | −0.07 (6) | C8i—Rh1—C8—C9 | −64.50 (3) |
| C7—N2—C1—Rh1 | −4.70 (8) | C8i—Rh1—C8—C11i | 60.26 (4) |
| C7—N2—C1—N1 | −178.31 (6) | C9i—Rh1—C8—C9 | −97.57 (4) |
| C1i—Rh1—C1—N1 | −83.65 (5) | C9—Rh1—C8—C11i | 124.75 (6) |
| C1i—Rh1—C1—N2 | 104.22 (5) | C9i—Rh1—C8—C11i | 27.19 (4) |
| C8—Rh1—C1—N1 | 72.88 (5) | Rh1—C8—C9—C10 | 101.36 (6) |
| C8i—Rh1—C1—N1 | 179.85 (5) | C11i—C8—C9—Rh1 | −98.12 (6) |
| C8—Rh1—C1—N2 | −99.26 (5) | C11i—C8—C9—C10 | 3.25 (9) |
| C8i—Rh1—C1—N2 | 7.72 (8) | C1—Rh1—C9—C8 | −87.40 (4) |
| C9—Rh1—C1—N1 | 109.52 (5) | C1i—Rh1—C9—C8 | 163.01 (8) |
| C9i—Rh1—C1—N1 | 25.66 (11) | C1—Rh1—C9—C10 | 149.98 (4) |
| C9—Rh1—C1—N2 | −62.61 (5) | C1i—Rh1—C9—C10 | 40.40 (11) |
| C9i—Rh1—C1—N2 | −146.48 (8) | C8i—Rh1—C9—C8 | 115.05 (4) |
| C1—N1—C2—C3 | −0.15 (7) | C8—Rh1—C9—C10 | −122.61 (6) |
| C4—N1—C2—C3 | 179.12 (5) | C8i—Rh1—C9—C10 | −7.56 (4) |
| N1—C2—C3—N2 | 0.09 (7) | C9i—Rh1—C9—C8 | 78.69 (3) |
| C1—N2—C3—C2 | −0.01 (7) | C9i—Rh1—C9—C10 | −43.92 (4) |
| C7—N2—C3—C2 | 178.27 (6) | Rh1—C9—C10—C11 | −13.94 (7) |
| C1—N1—C4—C5 | 111.55 (6) | C8—C9—C10—C11 | −93.84 (7) |
| C1—N1—C4—C6 | −124.17 (6) | C9—C10—C11—C8i | 39.69 (8) |
| C2—N1—C4—C5 | −67.63 (8) |
Symmetry codes: (i) −x+3/2, −y+1/2, z; (ii) −x+3/2, −y+3/2, z.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C2—H2···F1iii | 0.909 (11) | 2.496 (11) | 3.3975 (8) | 171.4 (10) |
| C3—H3···F2iv | 0.877 (12) | 2.478 (12) | 3.2415 (8) | 145.9 (11) |
Symmetry codes: (iii) x−1/2, −y+1, −z+1/2; (iv) x, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2478).
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 datablock(s) I, global. DOI: 10.1107/S1600536811049890/fj2478sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811049890/fj2478Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811049890/fj2478Isup3.cdx
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


