Literature DB >> 22059044

3-(9H-Carbazol-9-yl)-2H-chromen-2-one.

Julien Letessier1, Dieter Schollmeyer, Heiner Detert.   

Abstract

The title compound, C(21)H(13)NO(2), was prepared as an example of a new synthesis of carbazoles from a cyclic dibenzo-iodo-lium salt via a twofold Pd-catalysed aryl-ation of a primary amine. The two essentially planar π-subsystems [maximum deviations from the mean square plane of 0.038 (2) Å in the carbazole and 0.059 (2) Å in the coumarine unit] open a dihedral angle of 63.05 (4)°. Two mol-ecules form a centrosymmetrical pair connected via π-π inter-actions between the pyrrole and pyrone rings [centroid-centroid distance = 3.882 (1) Å] and one benzene of the carbazole and the pyrone unit [centroid-centroid distance 3.824 (1) Å]. The lattice is stabilized by C-H⋯O bridging to both coumarin O atoms.

Entities:  

Year:  2011        PMID: 22059044      PMCID: PMC3200909          DOI: 10.1107/S1600536811034660

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


Related literature

For alkaloids based on the carbazole core, see: Kapil (1971 ▶). For information on carbazoles used as electron-rich and rigid units in functional materials for photoconducting, sensing and luminescence purposes, see: Wakim et al. (2004 ▶); Schmitt et al. (2008 ▶). For carbazoles and δ-carbolines using the iodo­lium salt route, see Letessier (2011 ▶); Letessier et al. (2011 ▶). For the construction of carbazoles and their heteroanalogous derivatives, see: Nissen & Detert (2011 ▶); Dassonneville et al. (2011 ▶); Letessier et al. (2011 ▶). For the synthesis of annulated heterocycles, see: Nemkovich et al. (2009 ▶); Preis et al. (2011 ▶).

Experimental

Crystal data

C21H13NO2 M = 311.32 Monoclinic, a = 8.9451 (12) Å b = 11.5412 (7) Å c = 15.0477 (17) Å β = 105.871 (12)° V = 1494.3 (3) Å3 Z = 4 Cu Kα radiation μ = 0.72 mm−1 T = 193 K 0.50 × 0.20 × 0.10 mm

Data collection

Enraf–Nonius CAD-4 diffractometer Absorption correction: ψ scan (CORINC; Dräger & Gattow, 1971 ▶) T min = 0.716, T max = 0.932 2826 measured reflections 2826 independent reflections 2171 reflections with I > 2σ(I) 3 standard reflections every 60 min intensity decay: 5%

Refinement

R[F 2 > 2σ(F 2)] = 0.048 wR(F 2) = 0.142 S = 1.04 2826 reflections 217 parameters H-atom parameters constrained Δρmax = 0.21 e Å−3 Δρmin = −0.30 e Å−3 Data collection: CAD-4 Software (Enraf–Nonius, 1989 ▶); cell refinement: CAD-4 Software; data reduction: CORINC (Dräger & Gattow, 1971 ▶); program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: PLATON. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811034660/bt5627sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811034660/bt5627Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536811034660/bt5627Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C21H13NO2F(000) = 648
Mr = 311.32Dx = 1.384 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54178 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 8.9451 (12) Åθ = 45–50°
b = 11.5412 (7) ŵ = 0.72 mm1
c = 15.0477 (17) ÅT = 193 K
β = 105.871 (12)°Block, colourless
V = 1494.3 (3) Å30.50 × 0.20 × 0.10 mm
Z = 4
Enraf–Nonius CAD-4 diffractometer2171 reflections with I > 2σ(I)
Radiation source: rotating anodeRint = 0.000
graphiteθmax = 69.9°, θmin = 4.9°
ω/2θ scansh = 0→10
Absorption correction: ψ scan (CORINC; Dräger & Gattow, 1971)k = 0→14
Tmin = 0.716, Tmax = 0.932l = −18→17
2826 measured reflections3 standard reflections every 60 min
2826 independent reflections intensity decay: 5%
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.142H-atom parameters constrained
S = 1.04w = 1/[σ2(Fo2) + (0.0895P)2 + 0.1404P] where P = (Fo2 + 2Fc2)/3
2826 reflections(Δ/σ)max < 0.001
217 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = −0.30 e Å3
Experimental. 1H-NMR (400 MHz, CDCl3): δ = 8.12 (d, J=8.3Hz, 2H), 8.04 (s, 1H), 7.66 (m, 1H), 7.60 (dd, J=7.8Hz, J=1.5Hz, 1H), 7.51 (d, J=8.3Hz, 1H), 7.43 (m, 3H), 7.31 (m, 4H).
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.
xyzUiso*/Ueq
N10.35522 (19)0.44252 (14)0.28217 (10)0.0344 (4)
C20.2569 (2)0.34605 (16)0.26142 (12)0.0326 (4)
C30.2417 (2)0.26376 (18)0.19169 (13)0.0389 (5)
H30.30270.26770.14910.047*
C40.1339 (2)0.17589 (19)0.18704 (14)0.0434 (5)
H40.12180.11810.14070.052*
C50.0427 (2)0.17044 (19)0.24880 (14)0.0431 (5)
H5−0.03080.10960.24350.052*
C60.0580 (2)0.25207 (18)0.31729 (13)0.0384 (5)
H6−0.00480.24840.35890.046*
C70.1674 (2)0.34055 (16)0.32474 (12)0.0314 (4)
C80.2154 (2)0.43659 (17)0.38781 (12)0.0324 (4)
C90.1733 (2)0.47311 (19)0.46582 (13)0.0410 (5)
H90.09670.43210.48620.049*
C100.2444 (2)0.5697 (2)0.51302 (14)0.0454 (5)
H100.21550.59580.56590.054*
C110.3578 (3)0.62901 (19)0.48398 (14)0.0439 (5)
H110.40590.69470.51800.053*
C120.4028 (2)0.59507 (17)0.40682 (14)0.0394 (5)
H120.48000.63630.38720.047*
C130.3298 (2)0.49793 (16)0.35928 (12)0.0328 (4)
C140.4510 (2)0.48169 (16)0.22789 (12)0.0319 (4)
C150.5679 (2)0.41781 (16)0.21408 (13)0.0338 (4)
H150.59630.34770.24760.041*
C160.6506 (2)0.45360 (17)0.14968 (12)0.0335 (4)
C170.7664 (2)0.38761 (19)0.12769 (15)0.0421 (5)
H170.79840.31650.15880.051*
C180.8348 (2)0.4251 (2)0.06098 (16)0.0497 (6)
H180.91230.37930.04560.060*
C190.7902 (2)0.5300 (2)0.01643 (15)0.0477 (6)
H190.83760.5552−0.02950.057*
C200.6781 (2)0.5980 (2)0.03778 (14)0.0408 (5)
H200.64830.66990.00740.049*
C210.6100 (2)0.55910 (17)0.10453 (12)0.0329 (4)
O220.49743 (15)0.62816 (11)0.12387 (9)0.0355 (3)
C230.4108 (2)0.59401 (16)0.18148 (12)0.0329 (4)
O240.30993 (17)0.65883 (13)0.19049 (10)0.0444 (4)
U11U22U33U12U13U23
N10.0407 (9)0.0321 (8)0.0342 (8)−0.0038 (7)0.0168 (7)−0.0014 (6)
C20.0344 (9)0.0291 (9)0.0332 (9)0.0008 (7)0.0075 (7)0.0032 (7)
C30.0452 (11)0.0376 (11)0.0344 (10)0.0005 (9)0.0116 (8)−0.0011 (8)
C40.0493 (12)0.0377 (11)0.0387 (10)−0.0030 (9)0.0044 (9)−0.0039 (8)
C50.0384 (11)0.0419 (12)0.0434 (11)−0.0079 (9)0.0015 (9)0.0026 (9)
C60.0319 (9)0.0435 (11)0.0385 (10)−0.0030 (8)0.0077 (8)0.0074 (8)
C70.0300 (9)0.0327 (10)0.0300 (9)0.0036 (7)0.0056 (7)0.0043 (7)
C80.0300 (9)0.0353 (10)0.0311 (9)0.0040 (7)0.0071 (7)0.0048 (7)
C90.0391 (10)0.0509 (12)0.0352 (10)0.0038 (9)0.0136 (8)0.0017 (9)
C100.0487 (12)0.0541 (13)0.0355 (10)0.0092 (10)0.0153 (9)−0.0059 (9)
C110.0516 (12)0.0377 (11)0.0390 (11)0.0013 (10)0.0067 (9)−0.0070 (9)
C120.0440 (11)0.0347 (11)0.0400 (10)−0.0018 (8)0.0121 (9)−0.0008 (8)
C130.0350 (9)0.0319 (10)0.0312 (9)0.0035 (8)0.0089 (7)0.0010 (7)
C140.0360 (9)0.0301 (10)0.0311 (9)−0.0027 (8)0.0116 (7)0.0007 (7)
C150.0348 (10)0.0307 (10)0.0351 (9)−0.0001 (8)0.0081 (7)0.0023 (7)
C160.0279 (9)0.0373 (10)0.0342 (9)−0.0026 (8)0.0065 (7)−0.0036 (8)
C170.0332 (10)0.0436 (12)0.0483 (12)0.0012 (9)0.0088 (9)−0.0051 (9)
C180.0327 (10)0.0636 (15)0.0574 (13)−0.0040 (10)0.0199 (10)−0.0120 (11)
C190.0363 (10)0.0658 (15)0.0451 (11)−0.0154 (10)0.0183 (9)−0.0081 (10)
C200.0367 (10)0.0480 (12)0.0375 (10)−0.0120 (9)0.0097 (8)−0.0006 (9)
C210.0284 (9)0.0375 (10)0.0324 (9)−0.0051 (8)0.0074 (7)−0.0032 (7)
O220.0365 (7)0.0329 (7)0.0384 (7)0.0004 (6)0.0125 (6)0.0054 (5)
C230.0341 (9)0.0320 (10)0.0333 (9)−0.0012 (8)0.0106 (7)−0.0002 (7)
O240.0466 (8)0.0391 (8)0.0512 (8)0.0094 (6)0.0197 (7)0.0023 (6)
N1—C131.397 (2)C11—H110.9500
N1—C21.400 (2)C12—C131.392 (3)
N1—C141.410 (2)C12—H120.9500
C2—C31.394 (3)C14—C151.342 (3)
C2—C71.404 (3)C14—C231.470 (3)
C3—C41.388 (3)C15—C161.431 (3)
C3—H30.9500C15—H150.9500
C4—C51.395 (3)C16—C211.393 (3)
C4—H40.9500C16—C171.397 (3)
C5—C61.375 (3)C17—C181.380 (3)
C5—H50.9500C17—H170.9500
C6—C71.397 (3)C18—C191.388 (3)
C6—H60.9500C18—H180.9500
C7—C81.446 (3)C19—C201.379 (3)
C8—C91.393 (3)C19—H190.9500
C8—C131.405 (3)C20—C211.384 (3)
C9—C101.380 (3)C20—H200.9500
C9—H90.9500C21—O221.376 (2)
C10—C111.390 (3)O22—C231.369 (2)
C10—H100.9500C23—O241.208 (2)
C11—C121.385 (3)
C13—N1—C2108.33 (15)C11—C12—H12121.4
C13—N1—C14126.66 (16)C13—C12—H12121.4
C2—N1—C14124.73 (15)C12—C13—N1129.46 (18)
C3—C2—N1129.48 (18)C12—C13—C8121.80 (17)
C3—C2—C7121.57 (18)N1—C13—C8108.71 (16)
N1—C2—C7108.95 (16)C15—C14—N1122.45 (17)
C4—C3—C2117.34 (19)C15—C14—C23120.71 (16)
C4—C3—H3121.3N1—C14—C23116.74 (16)
C2—C3—H3121.3C14—C15—C16121.02 (17)
C3—C4—C5121.60 (19)C14—C15—H15119.5
C3—C4—H4119.2C16—C15—H15119.5
C5—C4—H4119.2C21—C16—C17118.19 (18)
C6—C5—C4120.78 (19)C21—C16—C15117.93 (17)
C6—C5—H5119.6C17—C16—C15123.86 (19)
C4—C5—H5119.6C18—C17—C16120.4 (2)
C5—C6—C7118.99 (19)C18—C17—H17119.8
C5—C6—H6120.5C16—C17—H17119.8
C7—C6—H6120.5C17—C18—C19119.9 (2)
C6—C7—C2119.70 (18)C17—C18—H18120.0
C6—C7—C8133.52 (18)C19—C18—H18120.0
C2—C7—C8106.77 (16)C20—C19—C18121.03 (19)
C9—C8—C13119.51 (18)C20—C19—H19119.5
C9—C8—C7133.24 (18)C18—C19—H19119.5
C13—C8—C7107.23 (16)C19—C20—C21118.5 (2)
C10—C9—C8119.06 (19)C19—C20—H20120.8
C10—C9—H9120.5C21—C20—H20120.8
C8—C9—H9120.5O22—C21—C20117.27 (18)
C9—C10—C11120.62 (18)O22—C21—C16120.75 (16)
C9—C10—H10119.7C20—C21—C16121.97 (18)
C11—C10—H10119.7C23—O22—C21122.72 (14)
C12—C11—C10121.9 (2)O24—C23—O22117.53 (17)
C12—C11—H11119.1O24—C23—C14125.86 (17)
C10—C11—H11119.1O22—C23—C14116.60 (16)
C11—C12—C13117.11 (19)
C13—N1—C2—C3−179.12 (19)C7—C8—C13—C12−178.87 (17)
C14—N1—C2—C36.6 (3)C9—C8—C13—N1177.92 (16)
C13—N1—C2—C70.6 (2)C7—C8—C13—N1−0.8 (2)
C14—N1—C2—C7−173.62 (16)C13—N1—C14—C15123.2 (2)
N1—C2—C3—C4179.88 (18)C2—N1—C14—C15−63.6 (3)
C7—C2—C3—C40.1 (3)C13—N1—C14—C23−60.6 (2)
C2—C3—C4—C50.7 (3)C2—N1—C14—C23112.6 (2)
C3—C4—C5—C6−0.6 (3)N1—C14—C15—C16172.20 (16)
C4—C5—C6—C7−0.5 (3)C23—C14—C15—C16−3.9 (3)
C5—C6—C7—C21.3 (3)C14—C15—C16—C212.5 (3)
C5—C6—C7—C8−178.49 (19)C14—C15—C16—C17−175.69 (18)
C3—C2—C7—C6−1.2 (3)C21—C16—C17—C18−1.9 (3)
N1—C2—C7—C6179.02 (16)C15—C16—C17—C18176.35 (18)
C3—C2—C7—C8178.68 (17)C16—C17—C18—C191.0 (3)
N1—C2—C7—C8−1.1 (2)C17—C18—C19—C200.1 (3)
C6—C7—C8—C92.6 (4)C18—C19—C20—C21−0.4 (3)
C2—C7—C8—C9−177.3 (2)C19—C20—C21—O22−179.40 (16)
C6—C7—C8—C13−179.0 (2)C19—C20—C21—C16−0.5 (3)
C2—C7—C8—C131.2 (2)C17—C16—C21—O22−179.53 (16)
C13—C8—C9—C100.5 (3)C15—C16—C21—O222.1 (3)
C7—C8—C9—C10178.82 (19)C17—C16—C21—C201.6 (3)
C8—C9—C10—C11−0.8 (3)C15—C16—C21—C20−176.71 (17)
C9—C10—C11—C120.7 (3)C20—C21—O22—C23173.28 (16)
C10—C11—C12—C13−0.3 (3)C16—C21—O22—C23−5.6 (3)
C11—C12—C13—N1−177.60 (19)C21—O22—C23—O24−176.57 (16)
C11—C12—C13—C80.1 (3)C21—O22—C23—C144.2 (2)
C2—N1—C13—C12178.00 (19)C15—C14—C23—O24−178.58 (19)
C14—N1—C13—C12−7.9 (3)N1—C14—C23—O245.1 (3)
C2—N1—C13—C80.1 (2)C15—C14—C23—O220.6 (3)
C14—N1—C13—C8174.22 (16)N1—C14—C23—O22−175.71 (15)
C9—C8—C13—C12−0.2 (3)
D—H···AD—HH···AD···AD—H···A
C15—H15···O24i0.952.433.366 (2)169
C11—H11···O22ii0.952.583.522 (2)170
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C15—H15⋯O24i0.952.433.366 (2)169
C11—H11⋯O22ii0.952.583.522 (2)170

Symmetry codes: (i) ; (ii) .

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