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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Nov 22;64(Pt 12):o2407. doi: 10.1107/S1600536808038300

9-Ethyl-3-(imidazo[1,2-a]pyrimidin-3-yl)-9H-carbazole

Ping-Hsin Huang a,*, Guan-Ji Chen b, Yuh-Sheng Wen b
PMCID: PMC2959935  PMID: 21581376

Abstract

The title compound, C20H16N4, is a precursor for the production of electron-transporting and -emitting materials. The bond lengths and angles in this compound are normal. In the crystal structure, there are no significant hydrogen-bonding inter­actions or π–π stacking inter­actions between mol­ecules.

Related literature

For general background to the use of small organic molecules or organic polymers as electroluminescent materials, see: Burroughes et al. (1990); Tang & VanSlyke (1987).graphic file with name e-64-o2407-scheme1.jpg

Experimental

Crystal data

  • C20H16N4

  • M r = 312.37

  • Monoclinic, Inline graphic

  • a = 13.9106 (3) Å

  • b = 9.3187 (2) Å

  • c = 12.9047 (3) Å

  • β = 112.712 (1)°

  • V = 1543.10 (6) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 100.0 (1) K

  • 0.36 × 0.32 × 0.28 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: none

  • 11748 measured reflections

  • 2717 independent reflections

  • 1991 reflections with I > 2σ(I)

  • R int = 0.033

Refinement

  • R[F 2 > 2σ(F 2)] = 0.030

  • wR(F 2) = 0.072

  • S = 0.91

  • 2717 reflections

  • 218 parameters

  • H-atom parameters constrained

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.19 e Å−3

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808038300/ww2131sup1.cif

e-64-o2407-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808038300/ww2131Isup2.hkl

e-64-o2407-Isup2.hkl (130.7KB, hkl)

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

Acknowledgments

This work was partially supported by the Institute of Chemistry, Academia Sinica, and Cardinal Tien College of Healthcare and Management.

supplementary crystallographic information

Comment

The application of organic electroluminescent (OEL) in flatpanel displays using small organic molecules or organic polymers has been intensively pursued after the reports by Kodak's team (Tang & VanSlyke, 1987) and Cambridge's group (Burroughes et al., 1990). The molecular structure of is shown in Fig. 1. The dihedral angle between the imidazole (P2) and phenyl ring of carbazole (P3) is 34.63 (8)°. Furthermore, the dihedral angles are 4.64 (8)°, 0.90 (8)° and 0.97 (8)° for P1/P2, P3/P4 and P4/P5, respectively.

Experimental

The compound was synthesized by the following procedure. Imidazo[1,2-a]pyrimidine hydrobromide (2.0 g, 0.01 mol), 3-bromo-9-ethyl-9H-carbazole (4.6 g, 1.15 eq), Pd(PPh3)4 (0.23 g, 0.02 eq), K2CO3 (2.8 g, 2 eq), and N,N-dimethylformamide (5 ml) were charged in a two-necked flask kept under nitrogen. The mixture was heated to reflux for 48 h. After cooling, it was quenched with 5 ml of water. The solvent was removed under vacuum and the residue was extracted with dichloromethane/water. The organic layer was dried over MgSO4 and filtered. Evaporation of the solvent left a brown residue that was chromatographed through silica gel using dichloromethane/hexane (19:1) mixture as eluant. The compound was obtained as yellow solid in 37% yield. FW:312.4;FAB MS: m/e 313.3 (M+ + H). 1H NMR (CDCl3, δ/ ppm): 8.68 (dd, 1H, J = 6.8 Hz, J = 1.8 Hz), 8.57 (dd, 1H, J = 3.9 Hz, J = 1.9 Hz), 8.21 (s, 1H), 8.11 (d, 1H, J = 7.8 Hz), 7.92 (s, 1H), 7.59–7.49 (m, 3H), 7.45 (d, 1H, J = 8.1 Hz), 7.26(t, 1H, J = 7.3 Hz), 6.89 (dd, 1H, J = 6.8 Hz, J = 4.0 Hz).

Refinement

H atoms were located geometrically and treated as riding atoms, with C—H = 0.93–0.96Å, and with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

A molecular structure of (I) with 30% probability displacement ellipsoids, showing the atom-numbering scheme employed.

Fig. 2.

Fig. 2.

The formation of the title compound.

Crystal data

C20H16N4 F000 = 656
Mr = 312.37 Dx = 1.345 Mg m3Dm = 1.345 Mg m3Dm measured by not measured
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 3698 reflections
a = 13.9106 (3) Å θ = 2.7–30.2º
b = 9.3187 (2) Å µ = 0.08 mm1
c = 12.9047 (3) Å T = 100.0 (1) K
β = 112.712 (1)º Prism, yellow
V = 1543.10 (6) Å3 0.36 × 0.32 × 0.28 mm
Z = 4

Data collection

Bruker SMART CCD area-detector diffractometer 1991 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.033
Monochromator: graphite θmax = 25.0º
T = 100.0(1) K θmin = 1.6º
ω and φ scans h = −16→16
Absorption correction: none k = −11→11
11748 measured reflections l = −15→15
2717 independent reflections

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.030   w = 1/[σ2(Fo2) + (0.0416P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.072 (Δ/σ)max = 0.001
S = 0.91 Δρmax = 0.19 e Å3
2717 reflections Δρmin = −0.18 e Å3
218 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0063 (8)
Secondary atom site location: difference Fourier map

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
N4 1.35147 (8) 0.58921 (11) 0.45030 (9) 0.0200 (3)
N3 0.96458 (8) 0.19984 (11) 0.66711 (9) 0.0225 (3)
N1 0.85050 (8) 0.05126 (11) 0.51971 (9) 0.0209 (3)
N2 0.98239 (8) 0.20433 (11) 0.50125 (8) 0.0166 (3)
C17 1.37034 (10) 0.48850 (14) 0.38158 (10) 0.0196 (3)
C16 1.43492 (10) 0.49764 (15) 0.32235 (11) 0.0256 (3)
H16 1.4741 0.5797 0.3258 0.031*
C14 1.43902 (10) 0.38125 (15) 0.25828 (11) 0.0279 (4)
H14 1.4817 0.3852 0.2179 0.033*
C13 1.38043 (10) 0.25737 (15) 0.25257 (11) 0.0253 (3)
H13 1.3845 0.1805 0.2085 0.030*
C12 1.31683 (10) 0.24836 (14) 0.31163 (11) 0.0210 (3)
H12 1.2784 0.1656 0.3081 0.025*
C11 1.31059 (9) 0.36437 (13) 0.37670 (10) 0.0179 (3)
C10 1.25171 (9) 0.39349 (13) 0.44510 (10) 0.0166 (3)
C9 1.17866 (9) 0.31495 (13) 0.47090 (10) 0.0171 (3)
H9 1.1602 0.2230 0.4422 0.021*
C8 1.13349 (9) 0.37494 (13) 0.53988 (10) 0.0171 (3)
C7 1.16524 (10) 0.51203 (13) 0.58548 (10) 0.0195 (3)
H7 1.1364 0.5503 0.6336 0.023*
C24 1.23750 (10) 0.59182 (14) 0.56155 (10) 0.0203 (3)
H24 1.2575 0.6824 0.5927 0.024*
C23 1.27953 (9) 0.53254 (13) 0.48938 (10) 0.0180 (3)
C18 1.39561 (10) 0.73286 (13) 0.47180 (11) 0.0248 (3)
H18A 1.4685 0.7281 0.4827 0.030*
H18B 1.3919 0.7690 0.5406 0.030*
C19 1.33998 (11) 0.83644 (15) 0.37712 (12) 0.0305 (4)
H19A 1.3718 0.9294 0.3954 0.046*
H19B 1.2680 0.8430 0.3668 0.046*
H19C 1.3449 0.8025 0.3091 0.046*
C6 1.04213 (10) 0.29149 (14) 0.66997 (11) 0.0223 (3)
H6 1.0810 0.3451 0.7331 0.027*
C4 0.92857 (10) 0.14710 (13) 0.56400 (10) 0.0181 (3)
C1 0.82339 (10) 0.02090 (13) 0.41227 (11) 0.0214 (3)
H1 0.7709 −0.0464 0.3802 0.026*
C2 0.86906 (10) 0.08412 (13) 0.34325 (11) 0.0205 (3)
H2 0.8445 0.0624 0.2671 0.025*
C3 0.94900 (10) 0.17667 (13) 0.38901 (10) 0.0184 (3)
H3 0.9804 0.2203 0.3453 0.022*
C5 1.05729 (10) 0.29722 (13) 0.57133 (10) 0.0173 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N4 0.0182 (6) 0.0194 (6) 0.0212 (6) −0.0032 (5) 0.0064 (5) 0.0020 (5)
N3 0.0221 (6) 0.0286 (7) 0.0179 (6) −0.0029 (5) 0.0090 (5) −0.0014 (5)
N1 0.0186 (6) 0.0214 (6) 0.0225 (7) −0.0001 (5) 0.0076 (5) 0.0002 (5)
N2 0.0167 (6) 0.0193 (6) 0.0148 (6) 0.0011 (5) 0.0071 (5) 0.0008 (5)
C17 0.0145 (7) 0.0257 (8) 0.0166 (7) 0.0018 (6) 0.0038 (6) 0.0037 (6)
C16 0.0167 (7) 0.0315 (8) 0.0279 (8) −0.0014 (6) 0.0077 (7) 0.0065 (7)
C14 0.0189 (8) 0.0413 (9) 0.0273 (8) 0.0068 (7) 0.0131 (7) 0.0075 (7)
C13 0.0199 (8) 0.0338 (9) 0.0225 (8) 0.0065 (7) 0.0087 (6) 0.0006 (7)
C12 0.0164 (7) 0.0244 (8) 0.0205 (7) 0.0019 (6) 0.0054 (6) 0.0029 (6)
C11 0.0138 (7) 0.0219 (7) 0.0161 (7) 0.0021 (6) 0.0038 (6) 0.0032 (6)
C10 0.0151 (7) 0.0194 (7) 0.0130 (7) 0.0022 (6) 0.0030 (6) 0.0023 (6)
C9 0.0178 (7) 0.0164 (7) 0.0145 (7) −0.0006 (6) 0.0033 (6) 0.0006 (6)
C8 0.0159 (7) 0.0206 (7) 0.0129 (7) 0.0015 (6) 0.0034 (6) 0.0021 (6)
C7 0.0207 (7) 0.0228 (7) 0.0146 (7) 0.0040 (6) 0.0065 (6) 0.0006 (6)
C24 0.0219 (7) 0.0167 (7) 0.0181 (7) 0.0001 (6) 0.0032 (6) −0.0008 (6)
C23 0.0157 (7) 0.0200 (7) 0.0158 (7) 0.0007 (6) 0.0033 (6) 0.0050 (6)
C18 0.0229 (8) 0.0214 (8) 0.0284 (8) −0.0050 (6) 0.0081 (6) 0.0026 (6)
C19 0.0288 (9) 0.0284 (8) 0.0367 (9) 0.0029 (7) 0.0152 (7) 0.0085 (7)
C6 0.0211 (7) 0.0286 (8) 0.0171 (7) −0.0035 (6) 0.0072 (6) −0.0041 (6)
C4 0.0184 (7) 0.0213 (7) 0.0166 (7) 0.0019 (6) 0.0090 (6) 0.0031 (6)
C1 0.0180 (7) 0.0207 (7) 0.0229 (8) 0.0011 (6) 0.0051 (6) −0.0020 (6)
C2 0.0192 (7) 0.0238 (8) 0.0165 (7) 0.0020 (6) 0.0048 (6) −0.0021 (6)
C3 0.0188 (7) 0.0226 (8) 0.0141 (7) 0.0045 (6) 0.0068 (6) 0.0013 (6)
C5 0.0160 (7) 0.0193 (7) 0.0157 (7) 0.0008 (6) 0.0049 (6) −0.0014 (6)

Geometric parameters (Å, °)

N4—C17 1.3841 (16) C10—C23 1.4088 (17)
N4—C23 1.3871 (15) C9—C8 1.3898 (16)
N4—C18 1.4541 (15) C9—H9 0.9300
N3—C4 1.3222 (16) C8—C7 1.4045 (17)
N3—C6 1.3652 (16) C8—C5 1.4646 (17)
N1—C1 1.3194 (15) C7—C24 1.3778 (17)
N1—C4 1.3508 (16) C7—H7 0.9300
N2—C3 1.3640 (15) C24—C23 1.3911 (17)
N2—C5 1.3874 (15) C24—H24 0.9300
N2—C4 1.4031 (15) C18—C19 1.5143 (18)
C17—C16 1.3889 (17) C18—H18A 0.9700
C17—C11 1.4115 (17) C18—H18B 0.9700
C16—C14 1.3782 (18) C19—H19A 0.9600
C16—H16 0.9300 C19—H19B 0.9600
C14—C13 1.3986 (18) C19—H19C 0.9600
C14—H14 0.9300 C6—C5 1.3693 (16)
C13—C12 1.3752 (17) C6—H6 0.9300
C13—H13 0.9300 C1—C2 1.4074 (17)
C12—C11 1.3920 (17) C1—H1 0.9300
C12—H12 0.9300 C2—C3 1.3499 (18)
C11—C10 1.4429 (16) C2—H2 0.9300
C10—C9 1.3929 (16) C3—H3 0.9300
C17—N4—C23 108.46 (10) C8—C7—H7 118.8
C17—N4—C18 125.16 (10) C7—C24—C23 117.87 (12)
C23—N4—C18 126.29 (11) C7—C24—H24 121.1
C4—N3—C6 104.37 (10) C23—C24—H24 121.1
C1—N1—C4 116.31 (11) N4—C23—C24 129.87 (12)
C3—N2—C5 132.23 (10) N4—C23—C10 109.06 (10)
C3—N2—C4 120.15 (11) C24—C23—C10 121.07 (11)
C5—N2—C4 107.14 (10) N4—C18—C19 112.72 (11)
N4—C17—C16 129.35 (12) N4—C18—H18A 109.0
N4—C17—C11 109.28 (10) C19—C18—H18A 109.0
C16—C17—C11 121.37 (12) N4—C18—H18B 109.0
C14—C16—C17 117.86 (13) C19—C18—H18B 109.0
C14—C16—H16 121.1 H18A—C18—H18B 107.8
C17—C16—H16 121.1 C18—C19—H19A 109.5
C16—C14—C13 121.53 (13) C18—C19—H19B 109.5
C16—C14—H14 119.2 H19A—C19—H19B 109.5
C13—C14—H14 119.2 C18—C19—H19C 109.5
C12—C13—C14 120.51 (13) H19A—C19—H19C 109.5
C12—C13—H13 119.7 H19B—C19—H19C 109.5
C14—C13—H13 119.7 N3—C6—C5 113.76 (11)
C13—C12—C11 119.36 (12) N3—C6—H6 123.1
C13—C12—H12 120.3 C5—C6—H6 123.1
C11—C12—H12 120.3 N3—C4—N1 127.00 (11)
C12—C11—C17 119.38 (11) N3—C4—N2 111.12 (11)
C12—C11—C10 134.22 (12) N1—C4—N2 121.88 (11)
C17—C11—C10 106.39 (11) N1—C1—C2 124.03 (12)
C9—C10—C23 119.86 (11) N1—C1—H1 118.0
C9—C10—C11 133.33 (12) C2—C1—H1 118.0
C23—C10—C11 106.80 (10) C3—C2—C1 119.18 (12)
C8—C9—C10 119.59 (12) C3—C2—H2 120.4
C8—C9—H9 120.2 C1—C2—H2 120.4
C10—C9—H9 120.2 C2—C3—N2 118.06 (12)
C9—C8—C7 119.17 (12) C2—C3—H3 121.0
C9—C8—C5 122.22 (11) N2—C3—H3 121.0
C7—C8—C5 118.54 (11) C6—C5—N2 103.61 (10)
C24—C7—C8 122.38 (12) C6—C5—C8 131.65 (12)
C24—C7—H7 118.8 N2—C5—C8 124.72 (11)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WW2131).

References

  1. Bruker (2001). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Burroughes, J. H., Bradley, D. D. C., Brown, A. R., Marks, R. N., Mackay, K., Friend, R. H., Burns, P. L. & Holmes, A. B. (1990). Nature (London), 347, 539–540.
  3. Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
  4. Farrugia, L. J. (1999). J. Appl. Cryst.32, 837–838.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Tang, C. W. & VanSlyke, S. A. (1987). Appl. Phys. Lett.51, 913–915.

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/S1600536808038300/ww2131sup1.cif

e-64-o2407-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808038300/ww2131Isup2.hkl

e-64-o2407-Isup2.hkl (130.7KB, hkl)

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


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