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Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

(Z)-3-(9-Anthr­yl)-1-(4-bromo­phen­yl)-2-(4-nitro-1H-imidazol-1-yl)prop-2-en-1-one

aSchool of Chemistry and Chemical Engineering, Southwest University, Chongqing 400715, People's Republic of China
*Correspondence e-mail: zhouch@swu.edu.cn

(Received 10 May 2009; accepted 14 May 2009; online 23 May 2009)

In the title mol­ecule, C26H16BrN3O3, the anthracene and benzene mean planes make dihedral angles of 63.79 (2) and 14.67 (2)°, respectively, with the plane of the imidazole ring. In the crystal structure, weak inter­molecular C—H⋯O hydrogen bonds link mol­ecules to form centrosymmetric dimers. Weak ππ stacking inter­actions, with centroid–centroid distances of 3.779 (2) and 3.826 (2) Å, supply additional stabilization. The crystal packing also exhibits short inter­molecular contacts between the nitro groups and Br atoms [Br⋯O = 3.114 (2) Å].

Related literature

For the crystal structure of the chloro analog of the title compound, see: Wang et al. (2009[Wang, G., Lu, Y., Zhou, C. & Zhang, Y. (2009). Acta Cryst. E65, o1113.]). For general background on the pharmacological activities of chalcones, see: Corréa et al. (2001[Corréa, R., Pereira, M. A. S., Buffon, D., Santos, L., Filho, V. C., Santos, A. R. S. & Nunes, R. J. (2001). Arch. Pharm. Med. Chem. 334, 332-334.]); Jasinski et al. (2009[Jasinski, J. P., Butcher, R. J., Mayekar, A. N., Yathirajan, H. S. & Narayana, B. (2009). J. Chem. Crystallogr. 39, 157-162.]); Nielsen et al. (1998[Nielsen, S. F., Christensen, S. B., Cruciani, G., Kharazmi, A. & Liljefors, T. (1998). J. Med. Chem. 41, 4819-4832.]); Vogel et al. (2008[Vogel, S., Ohmayer, S., Brunner, G. & Heilmann, J. (2008). Bioorg. Med. Chem. 16, 4286-4293.]). For the synthetic details, see: Erhardt et al. (1985[Erhardt, H., Mildenberger, H., Handte, R., Sachse, B., Hartz, P. & Bürstell, H. (1985). German Patent No. DE3406908.]); Kranz et al. (1980[Kranz, E., Krämer, W., Büchel, K. H., Brandes, W. & Forhberger, P. E. (1980). German Patent No. DE2832233.]).

[Scheme 1]

Experimental

Crystal data
  • C26H16BrN3O3

  • Mr = 498.33

  • Triclinic, [P \overline 1]

  • a = 8.1438 (11) Å

  • b = 11.0916 (14) Å

  • c = 12.7979 (17) Å

  • α = 78.146 (2)°

  • β = 86.193 (2)°

  • γ = 70.768 (2)°

  • V = 1068.2 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.96 mm−1

  • T = 292 K

  • 0.13 × 0.12 × 0.10 mm

Data collection
  • Bruker SMART APEX CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996[Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.]) Tmin = 0.775, Tmax = 0.828

  • 6422 measured reflections

  • 4315 independent reflections

  • 3095 reflections with I > 2σ(I)

  • Rint = 0.019

Refinement
  • R[F2 > 2σ(F2)] = 0.044

  • wR(F2) = 0.116

  • S = 1.02

  • 4315 reflections

  • 298 parameters

  • H-atom parameters constrained

  • Δρmax = 0.56 e Å−3

  • Δρmin = −0.67 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C23—H23⋯O3i 0.93 2.56 3.303 (4) 137
Symmetry code: (i) -x+2, -y+1, -z.

Data collection: SMART (Bruker, 2001[Bruker (2001). SAINT-Plus and SMART. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT-Plus (Bruker, 2001[Bruker (2001). SAINT-Plus and SMART. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: PLATON (Spek, 2009[Spek, A. L. (2009). Acta Cryst. D65, 148-155.]); software used to prepare material for publication: PLATON.

Supporting information


Comment top

Chalcones and their derivatives have been reported responsible for a variety of pharmacological activities, including antibacterial, antifungal, anti-leishmanial, antimalarial, analgesic, anti-inflammatory and chemopreventive ones (Corréa et al., 2001; Jasinski et al., 2009; Simon et al., 1998; Vogel et al., 2008). Due to these varied applications, we have synthesized the title compound and report its crystal structure.

In the molecular structure of the title compound (I) (Fig. 1), the dihedral angle between the anthracene unit and imidazole ring is 63.79 (2) ° and that between the imidazole ring and benzene ring is 14.67 (2) °. In the crystal structure, weak intermolecular C—H···O hydrogen bonds link molecules to form centrosymmetric dimers (Fig. 2). Weak ππ staking interactions, with centroid to centroid distances of 3.779 (2) and 3.826 (2)Å supply additional stabilization.

Related literature top

For the crystal structure of the chloro analog of the title compound, see: Wang et al. (2009). For general background on the pharmacological activities of chalcones, see: Corréa et al. (2001); Jasinski et al. (2009); Simon et al. (1998); Vogel et al. (2008). For the synthetic details, see: Erhardt et al. (1985); Kranz et al. (1980).

Experimental top

Compound (I) was synthesized according to the procedure of Erhardt et al. (1985); Kranz et al. (1980). A crystal suitable for X-ray analysis was grown from a chloroform and acetone solution of (I) by slow evaporation at room temperature.

Refinement top

H ydrogen atoms were placed in idealized positions with C—H = 0.93Å and Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: PLATON (Spek, 2009).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. Part of the crystal structure of (I). Hydrogen bonds are shown as dashed lines.
(Z)-3-(9-Anthryl)-1-(4-bromophenyl)-2-(4-nitro-1H-imidazol- 1-yl)prop-2-en-1-one top
Crystal data top
C26H16BrN3O3Z = 2
Mr = 498.33F(000) = 504
Triclinic, P1Dx = 1.549 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.1438 (11) ÅCell parameters from 2344 reflections
b = 11.0916 (14) Åθ = 2.3–26.9°
c = 12.7979 (17) ŵ = 1.96 mm1
α = 78.146 (2)°T = 292 K
β = 86.193 (2)°Block, orange
γ = 70.768 (2)°0.13 × 0.12 × 0.10 mm
V = 1068.2 (2) Å3
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
4315 independent reflections
Radiation source: fine focus sealed Siemens Mo tube3095 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.019
0.3° wide ω exposures scansθmax = 26.5°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 810
Tmin = 0.775, Tmax = 0.828k = 1313
6422 measured reflectionsl = 1615
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.044H-atom parameters constrained
wR(F2) = 0.116 w = 1/[σ2(Fo2) + (0.0524P)2 + 0.6665P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.008
4315 reflectionsΔρmax = 0.56 e Å3
298 parametersΔρmin = 0.67 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0078 (11)
Crystal data top
C26H16BrN3O3γ = 70.768 (2)°
Mr = 498.33V = 1068.2 (2) Å3
Triclinic, P1Z = 2
a = 8.1438 (11) ÅMo Kα radiation
b = 11.0916 (14) ŵ = 1.96 mm1
c = 12.7979 (17) ÅT = 292 K
α = 78.146 (2)°0.13 × 0.12 × 0.10 mm
β = 86.193 (2)°
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
4315 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
3095 reflections with I > 2σ(I)
Tmin = 0.775, Tmax = 0.828Rint = 0.019
6422 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0440 restraints
wR(F2) = 0.116H-atom parameters constrained
S = 1.02Δρmax = 0.56 e Å3
4315 reflectionsΔρmin = 0.67 e Å3
298 parameters
Special details top

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) top
xyzUiso*/Ueq
Br10.93749 (6)0.89457 (4)0.12755 (3)0.06983 (18)
C10.4551 (4)0.4031 (3)0.3854 (2)0.0356 (6)
C20.3193 (4)0.4914 (3)0.4320 (2)0.0406 (7)
C30.2357 (4)0.6217 (3)0.3799 (3)0.0496 (8)
H30.26990.65060.31110.060*
C40.1080 (5)0.7050 (4)0.4276 (4)0.0691 (11)
H40.05650.79020.39170.083*
C50.0521 (5)0.6637 (5)0.5312 (4)0.0740 (13)
H50.03420.72240.56390.089*
C60.1223 (5)0.5405 (5)0.5832 (3)0.0647 (11)
H60.08190.51440.65090.078*
C70.2583 (4)0.4483 (4)0.5363 (2)0.0510 (9)
C80.3318 (5)0.3209 (4)0.5877 (3)0.0570 (10)
H80.28930.29300.65430.068*
C90.4663 (5)0.2335 (4)0.5435 (3)0.0545 (9)
C100.5444 (7)0.1041 (4)0.5990 (3)0.0804 (14)
H100.50070.07650.66530.096*
C110.6795 (8)0.0206 (5)0.5582 (4)0.0943 (17)
H110.72730.06420.59570.113*
C120.7504 (7)0.0613 (4)0.4575 (4)0.0792 (13)
H120.84610.00340.43050.095*
C130.6790 (5)0.1839 (3)0.4007 (3)0.0538 (9)
H130.72700.20920.33530.065*
C140.5326 (4)0.2738 (3)0.4394 (2)0.0415 (7)
C150.5261 (4)0.4522 (3)0.2830 (2)0.0327 (6)
H150.56260.52350.28200.039*
C160.5458 (4)0.4098 (2)0.1916 (2)0.0308 (6)
C170.3147 (4)0.3086 (3)0.1964 (2)0.0391 (7)
H170.22150.37300.21850.047*
C180.5712 (5)0.1936 (3)0.1475 (3)0.0456 (7)
H180.68860.16980.12960.055*
C190.3157 (5)0.1937 (3)0.1754 (2)0.0448 (8)
C200.6441 (4)0.4580 (3)0.0995 (2)0.0322 (6)
C210.7038 (4)0.5703 (3)0.1060 (2)0.0332 (6)
C220.8822 (4)0.5456 (3)0.1056 (2)0.0422 (7)
H220.95690.46280.10140.051*
C230.9499 (4)0.6436 (3)0.1113 (3)0.0490 (8)
H231.06960.62670.11220.059*
C240.8383 (4)0.7651 (3)0.1157 (2)0.0438 (7)
C250.6602 (4)0.7937 (3)0.1138 (2)0.0426 (7)
H250.58610.87750.11550.051*
C260.5943 (4)0.6947 (3)0.1094 (2)0.0389 (7)
H260.47460.71210.10870.047*
N10.4811 (3)0.3085 (2)0.17774 (18)0.0342 (5)
N20.4740 (4)0.1210 (2)0.1464 (2)0.0515 (7)
N30.1680 (5)0.1482 (3)0.1818 (3)0.0663 (9)
O10.1909 (5)0.0414 (3)0.1602 (3)0.1002 (11)
O20.0289 (5)0.2194 (4)0.2088 (3)0.0920 (10)
O30.6822 (3)0.4034 (2)0.02424 (17)0.0464 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0870 (3)0.0579 (2)0.0872 (3)0.0537 (2)0.0032 (2)0.01466 (19)
C10.0423 (17)0.0457 (16)0.0284 (14)0.0269 (14)0.0004 (12)0.0071 (12)
C20.0426 (18)0.0551 (19)0.0351 (16)0.0264 (15)0.0010 (13)0.0159 (14)
C30.048 (2)0.056 (2)0.0514 (19)0.0203 (17)0.0012 (15)0.0194 (16)
C40.058 (2)0.073 (3)0.079 (3)0.012 (2)0.004 (2)0.036 (2)
C50.049 (2)0.108 (4)0.079 (3)0.021 (2)0.009 (2)0.057 (3)
C60.047 (2)0.119 (4)0.047 (2)0.040 (2)0.0134 (17)0.038 (2)
C70.0468 (19)0.089 (3)0.0349 (17)0.0403 (19)0.0018 (14)0.0203 (17)
C80.065 (2)0.090 (3)0.0297 (17)0.049 (2)0.0024 (16)0.0047 (18)
C90.074 (3)0.065 (2)0.0363 (17)0.044 (2)0.0098 (17)0.0023 (16)
C100.124 (4)0.070 (3)0.050 (2)0.049 (3)0.018 (2)0.016 (2)
C110.156 (5)0.054 (3)0.061 (3)0.030 (3)0.026 (3)0.016 (2)
C120.101 (3)0.050 (2)0.076 (3)0.008 (2)0.019 (2)0.009 (2)
C130.069 (2)0.0462 (19)0.0451 (19)0.0187 (18)0.0118 (17)0.0038 (15)
C140.0523 (19)0.0446 (17)0.0352 (16)0.0268 (15)0.0055 (14)0.0043 (13)
C150.0364 (16)0.0331 (14)0.0342 (15)0.0187 (12)0.0007 (12)0.0065 (11)
C160.0360 (15)0.0274 (13)0.0345 (15)0.0171 (12)0.0003 (11)0.0066 (11)
C170.0398 (17)0.0420 (16)0.0412 (16)0.0219 (14)0.0027 (13)0.0052 (13)
C180.054 (2)0.0340 (16)0.0535 (19)0.0187 (14)0.0031 (15)0.0123 (13)
C190.062 (2)0.0461 (17)0.0374 (16)0.0354 (17)0.0100 (15)0.0011 (13)
C200.0317 (15)0.0346 (14)0.0327 (15)0.0129 (12)0.0002 (12)0.0087 (12)
C210.0422 (17)0.0358 (15)0.0265 (14)0.0207 (13)0.0045 (11)0.0049 (11)
C220.0423 (18)0.0411 (16)0.0498 (18)0.0197 (14)0.0098 (14)0.0162 (14)
C230.0414 (18)0.058 (2)0.061 (2)0.0303 (16)0.0103 (15)0.0203 (16)
C240.061 (2)0.0409 (17)0.0423 (17)0.0348 (16)0.0083 (14)0.0084 (13)
C250.054 (2)0.0329 (15)0.0429 (17)0.0188 (14)0.0001 (14)0.0040 (13)
C260.0395 (17)0.0380 (16)0.0430 (17)0.0178 (14)0.0032 (13)0.0082 (13)
N10.0426 (14)0.0311 (12)0.0362 (12)0.0203 (11)0.0023 (10)0.0079 (10)
N20.075 (2)0.0366 (14)0.0513 (16)0.0297 (15)0.0045 (14)0.0068 (12)
N30.088 (3)0.070 (2)0.063 (2)0.061 (2)0.0171 (19)0.0032 (16)
O10.133 (3)0.089 (2)0.121 (3)0.087 (2)0.009 (2)0.0254 (19)
O20.074 (2)0.101 (2)0.121 (3)0.063 (2)0.002 (2)0.007 (2)
O30.0553 (14)0.0526 (13)0.0437 (12)0.0285 (11)0.0144 (10)0.0226 (10)
Geometric parameters (Å, º) top
Br1—C241.899 (3)C15—C161.329 (4)
C1—C21.405 (4)C15—H150.9300
C1—C141.410 (4)C16—N11.434 (3)
C1—C151.471 (4)C16—C201.487 (4)
C2—C31.419 (5)C17—C191.353 (4)
C2—C71.436 (4)C17—N11.359 (4)
C3—C41.349 (5)C17—H170.9300
C3—H30.9300C18—N21.305 (4)
C4—C51.408 (6)C18—N11.365 (4)
C4—H40.9300C18—H180.9300
C5—C61.341 (6)C19—N21.351 (4)
C5—H50.9300C19—N31.442 (4)
C6—C71.432 (5)C20—O31.211 (3)
C6—H60.9300C20—C211.497 (4)
C7—C81.379 (5)C21—C261.382 (4)
C8—C91.379 (5)C21—C221.387 (4)
C8—H80.9300C22—C231.387 (4)
C9—C101.417 (5)C22—H220.9300
C9—C141.444 (5)C23—C241.365 (5)
C10—C111.338 (7)C23—H230.9300
C10—H100.9300C24—C251.380 (5)
C11—C121.426 (7)C25—C261.384 (4)
C11—H110.9300C25—H250.9300
C12—C131.358 (5)C26—H260.9300
C12—H120.9300N3—O11.222 (4)
C13—C141.415 (5)N3—O21.224 (5)
C13—H130.9300
C2—C1—C14121.2 (3)C16—C15—H15115.2
C2—C1—C15118.2 (3)C1—C15—H15115.2
C14—C1—C15120.3 (3)C15—C16—N1121.6 (2)
C1—C2—C3123.1 (3)C15—C16—C20122.8 (2)
C1—C2—C7119.1 (3)N1—C16—C20115.5 (2)
C3—C2—C7117.7 (3)C19—C17—N1104.3 (3)
C4—C3—C2121.8 (4)C19—C17—H17127.8
C4—C3—H3119.1N1—C17—H17127.8
C2—C3—H3119.1N2—C18—N1112.3 (3)
C3—C4—C5120.4 (4)N2—C18—H18123.9
C3—C4—H4119.8N1—C18—H18123.9
C5—C4—H4119.8N2—C19—C17112.9 (3)
C6—C5—C4120.6 (4)N2—C19—N3121.2 (3)
C6—C5—H5119.7C17—C19—N3125.9 (4)
C4—C5—H5119.7O3—C20—C16120.7 (2)
C5—C6—C7121.2 (4)O3—C20—C21121.2 (2)
C5—C6—H6119.4C16—C20—C21118.0 (2)
C7—C6—H6119.4C26—C21—C22119.1 (3)
C8—C7—C2119.4 (3)C26—C21—C20124.6 (3)
C8—C7—C6122.3 (3)C22—C21—C20116.3 (3)
C2—C7—C6118.3 (3)C23—C22—C21120.5 (3)
C9—C8—C7122.1 (3)C23—C22—H22119.8
C9—C8—H8118.9C21—C22—H22119.8
C7—C8—H8118.9C24—C23—C22119.0 (3)
C8—C9—C10121.4 (4)C24—C23—H23120.5
C8—C9—C14120.0 (3)C22—C23—H23120.5
C10—C9—C14118.6 (4)C23—C24—C25122.0 (3)
C11—C10—C9121.5 (4)C23—C24—Br1117.4 (2)
C11—C10—H10119.2C25—C24—Br1120.6 (2)
C9—C10—H10119.2C26—C25—C24118.4 (3)
C10—C11—C12120.2 (4)C26—C25—H25120.8
C10—C11—H11119.9C24—C25—H25120.8
C12—C11—H11119.9C21—C26—C25121.0 (3)
C13—C12—C11120.4 (4)C21—C26—H26119.5
C13—C12—H12119.8C25—C26—H26119.5
C11—C12—H12119.8C17—N1—C18106.8 (2)
C12—C13—C14121.0 (4)C17—N1—C16125.3 (2)
C12—C13—H13119.5C18—N1—C16128.0 (2)
C14—C13—H13119.5C18—N2—C19103.7 (3)
C1—C14—C13123.7 (3)O1—N3—O2124.9 (4)
C1—C14—C9118.1 (3)O1—N3—C19117.7 (4)
C13—C14—C9118.1 (3)O2—N3—C19117.4 (3)
C16—C15—C1129.6 (2)
C14—C1—C2—C3179.0 (3)C1—C15—C16—C20170.6 (3)
C15—C1—C2—C36.7 (4)N1—C17—C19—N21.0 (3)
C14—C1—C2—C70.3 (4)N1—C17—C19—N3178.9 (3)
C15—C1—C2—C7174.6 (2)C15—C16—C20—O3168.5 (3)
C1—C2—C3—C4178.6 (3)N1—C16—C20—O38.1 (4)
C7—C2—C3—C42.6 (5)C15—C16—C20—C217.7 (4)
C2—C3—C4—C50.7 (5)N1—C16—C20—C21175.6 (2)
C3—C4—C5—C61.4 (6)O3—C20—C21—C26118.6 (3)
C4—C5—C6—C71.5 (6)C16—C20—C21—C2665.2 (4)
C1—C2—C7—C81.2 (4)O3—C20—C21—C2259.7 (4)
C3—C2—C7—C8177.6 (3)C16—C20—C21—C22116.5 (3)
C1—C2—C7—C6178.7 (3)C26—C21—C22—C231.7 (4)
C3—C2—C7—C62.5 (4)C20—C21—C22—C23180.0 (3)
C5—C6—C7—C8179.5 (3)C21—C22—C23—C241.0 (5)
C5—C6—C7—C20.5 (5)C22—C23—C24—C250.4 (5)
C2—C7—C8—C91.9 (5)C22—C23—C24—Br1178.3 (2)
C6—C7—C8—C9178.0 (3)C23—C24—C25—C261.2 (5)
C7—C8—C9—C10177.8 (3)Br1—C24—C25—C26177.4 (2)
C7—C8—C9—C141.1 (5)C22—C21—C26—C250.9 (4)
C8—C9—C10—C11177.3 (4)C20—C21—C26—C25179.1 (3)
C14—C9—C10—C111.7 (6)C24—C25—C26—C210.5 (4)
C9—C10—C11—C120.9 (7)C19—C17—N1—C180.3 (3)
C10—C11—C12—C131.6 (7)C19—C17—N1—C16178.5 (2)
C11—C12—C13—C140.4 (6)N2—C18—N1—C170.5 (3)
C2—C1—C14—C13174.5 (3)N2—C18—N1—C16177.6 (3)
C15—C1—C14—C130.3 (4)C15—C16—N1—C1753.4 (4)
C2—C1—C14—C91.1 (4)C20—C16—N1—C17129.9 (3)
C15—C1—C14—C9175.3 (3)C15—C16—N1—C18124.4 (3)
C12—C13—C14—C1178.5 (3)C20—C16—N1—C1852.4 (4)
C12—C13—C14—C93.0 (5)N1—C18—N2—C191.0 (3)
C8—C9—C14—C10.4 (4)C17—C19—N2—C181.3 (4)
C10—C9—C14—C1179.4 (3)N3—C19—N2—C18178.6 (3)
C8—C9—C14—C13175.4 (3)N2—C19—N3—O10.2 (5)
C10—C9—C14—C133.6 (5)C17—C19—N3—O1180.0 (3)
C2—C1—C15—C16126.2 (3)N2—C19—N3—O2179.8 (3)
C14—C1—C15—C1659.4 (4)C17—C19—N3—O20.3 (5)
C1—C15—C16—N15.8 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C23—H23···O3i0.932.563.303 (4)137
Symmetry code: (i) x+2, y+1, z.

Experimental details

Crystal data
Chemical formulaC26H16BrN3O3
Mr498.33
Crystal system, space groupTriclinic, P1
Temperature (K)292
a, b, c (Å)8.1438 (11), 11.0916 (14), 12.7979 (17)
α, β, γ (°)78.146 (2), 86.193 (2), 70.768 (2)
V3)1068.2 (2)
Z2
Radiation typeMo Kα
µ (mm1)1.96
Crystal size (mm)0.13 × 0.12 × 0.10
Data collection
DiffractometerBruker SMART APEX CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.775, 0.828
No. of measured, independent and
observed [I > 2σ(I)] reflections
6422, 4315, 3095
Rint0.019
(sin θ/λ)max1)0.628
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.116, 1.02
No. of reflections4315
No. of parameters298
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.56, 0.67

Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2001), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2009).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C23—H23···O3i0.932.563.303 (4)137
Symmetry code: (i) x+2, y+1, z.
 

Acknowledgements

We thank the Southwest University (grant Nos. SWUB2006018, XSGX0602 and SWUF2007023) and the Natural Science Foundation of Chongqing (grant No. 2007BB5369) for financial support.

References

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