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In the mol­ecule of the title compound, C28H23N3O2, the nitro group is almost perpendicular to the carbazole ring to which it is attached. The crystal packing is determined by C—H...O and π–π inter­actions, where the nitrated carbazole ring of one mol­ecule associates in a shifted parallel planar orientation with the centrosymmetrically related non-nitrated carbazole ring of a neighbouring mol­ecule.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806010713/bv2010sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806010713/bv2010Isup2.hkl
Contains datablock I

CCDC reference: 605002

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.038
  • wR factor = 0.106
  • Data-to-parameter ratio = 6.6

checkCIF/PLATON results

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Alert level B PLAT242_ALERT_2_B Check Low Ueq as Compared to Neighbors for N4
Alert level C PLAT089_ALERT_3_C Poor Data / Parameter Ratio (Zmax .LT. 18) ..... 6.61 PLAT340_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 7 PLAT720_ALERT_4_C Number of Unusual/Non-Standard Label(s) ........ 4
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 25.03 From the CIF: _reflns_number_total 1975 Count of symmetry unique reflns 1985 Completeness (_total/calc) 99.50% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: CAD-4 PC Software (Enraf–Nonius, 1993); cell refinement: CAD-4 PC Software; data reduction: DATRD2 in NRCVAX (Gabe et al., 1989); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97; molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2003); software used to prepare material for publication: WinGX publication routines (Farrugia, 1999).

9-Ethyl-3-(9-ethyl-9H-carbazol-3-yl)-4-nitro-9H-carbazole top
Crystal data top
C28H23N3O2F(000) = 912
Mr = 433.49Dx = 1.287 Mg m3
Monoclinic, CcMo Kα radiation, λ = 0.71073 Å
Hall symbol: C -2ycCell parameters from 25 reflections
a = 16.2810 (13) Åθ = 5.7–18.4°
b = 13.8472 (8) ŵ = 0.08 mm1
c = 9.9233 (9) ÅT = 295 K
β = 90.721 (7)°Slab, yellow
V = 2237.0 (3) Å30.51 × 0.27 × 0.17 mm
Z = 4
Data collection top
Enraf–Nonius CAD-4
diffractometer
Rint = 0.010
Radiation source: fine-focus sealed tubeθmax = 25.0°, θmin = 1.9°
Graphite monochromatorh = 1919
ω scan b/P/bk = 1616
2071 measured reflectionsl = 011
1975 independent reflections3 standard reflections every 120 min
1466 reflections with I > 2σ(I) intensity decay: 1.1%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.107H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0661P)2 + 0.1062P]
where P = (Fo2 + 2Fc2)/3
1975 reflections(Δ/σ)max = 0.017
299 parametersΔρmax = 0.14 e Å3
2 restraintsΔρmin = 0.17 e Å3
Special details top

Experimental. Spectroscopic analysis: 1H NMR (300 MHz, CDCl3, δ, p.p.m.): 8.19 (d, J = 1.83 Hz, 1H), 8.11 (d, J = 7.31 Hz, 1H), 7.98 (d, J = 8.04 Hz, 1H), 7.65–7.40 (m, 8H), 7.30–7.20 (m, 2H), 4.44 (q, J = 7.31 Hz, 2H), 4.38 (q, J = 7.31 Hz, 2H), 1.45 (t, J = 7.13 Hz, 6H).

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)

13.2893 (0.0611) x - 4.2421 (0.0826) y - 4.9618 (0.0339) z = 6.3368 (0.0537)

* 0.0000 (0.0000) N4 * 0.0000 (0.0000) O1 * 0.0000 (0.0000) O2

Rms deviation of fitted atoms = 0.0000

2.7290 (0.0139) x - 7.0608 (0.0115) y + 8.3511 (0.0043) z = 4.5188 (0.0133)

Angle to previous plane (with approximate e.s.d.) = 83.10 (1/4)

* -0.0440 (0.0039) C1 * -0.0549 (0.0037) C2 * -0.0134 (0.0036) C3 * 0.0500 (0.0037) C4 * 0.0470 (0.0038) C4a * 0.0388 (0.0040) C4b * -0.0222 (0.0040) C5 * -0.0500 (0.0041) C6 * -0.0258 (0.0044) C7 * 0.0108 (0.0039) C8 * 0.0244 (0.0044) C8a * 0.0203 (0.0039) C9a * 0.0190 (0.0036) N9

Rms deviation of fitted atoms = 0.0356

2.2053 (0.0134) x + 7.3527 (0.0107) y + 8.2831 (0.0044) z = 7.2323 (0.0053)

Angle to previous plane (with approximate e.s.d.) = 62.76 (0.05)

* 0.0053 (0.0039) C1' * 0.0357 (0.0036) C2' * 0.0117 (0.0036) C3' * -0.0238 (0.0038) C4' * -0.0378 (0.0039) C4a' * -0.0238 (0.0042) C4b' * 0.0024 (0.0041) C5' * 0.0422 (0.0039) C6' * 0.0122 (0.0044) C7' * -0.0143 (0.0041) C8' * -0.0191 (0.0041) C8a' * -0.0022 (0.0041) C9a' * 0.0115 (0.0035) N9'

Rms deviation of fitted atoms = 0.0226

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
N40.64411 (18)0.0612 (2)0.3957 (3)0.0577 (7)
O10.6469 (3)0.0107 (2)0.4645 (4)0.1079 (11)
O20.6068 (3)0.0666 (2)0.2912 (4)0.1139 (13)
N90.8983 (2)0.2210 (3)0.4367 (4)0.0572 (10)
C10.7774 (3)0.3050 (3)0.5396 (5)0.0585 (13)
H10.80690.35810.57080.07*
C20.6937 (3)0.2978 (3)0.5596 (5)0.0572 (12)
H20.66720.34710.60560.069*
C30.6472 (3)0.2188 (3)0.5130 (4)0.0514 (12)
C40.6896 (3)0.1458 (3)0.4450 (4)0.0485 (11)
C4a0.7732 (3)0.1496 (3)0.4206 (4)0.0489 (11)
C4b0.8323 (3)0.0897 (3)0.3496 (4)0.0494 (11)
C50.8275 (3)0.0051 (4)0.2724 (5)0.0621 (13)
H50.77750.02620.25970.074*
C60.8977 (3)0.0308 (4)0.2157 (5)0.0712 (14)
H60.89540.08710.16470.085*
C70.9728 (3)0.0169 (5)0.2345 (5)0.0711 (14)
H71.01960.00910.1960.085*
C80.9796 (3)0.0990 (4)0.3060 (5)0.0681 (15)
H81.03020.12940.31710.082*
C8a0.9084 (3)0.1377 (4)0.3636 (5)0.0553 (12)
C9a0.8160 (3)0.2300 (3)0.4713 (4)0.0478 (11)
C100.9628 (3)0.2899 (4)0.4738 (5)0.0714 (15)
H10A0.93950.35440.47660.086*
H10B1.00470.28930.40520.086*
C111.0019 (4)0.2674 (5)0.6083 (6)0.0922 (19)
H11A1.04410.31390.62790.138*
H11B1.02560.20390.60590.138*
H11C0.9610.26980.67710.138*
N9'0.3058 (2)0.2217 (3)0.5963 (4)0.0535 (9)
C1'0.4270 (3)0.3021 (4)0.4919 (4)0.0563 (13)
H1'0.39760.35280.45290.068*
C2'0.5104 (3)0.2958 (3)0.4790 (5)0.0571 (12)
H2'0.53750.34460.43310.069*
C3'0.5571 (3)0.2183 (3)0.5325 (4)0.0491 (11)
C4'0.5170 (3)0.1471 (3)0.6020 (4)0.0483 (11)
H4'0.54660.09560.63810.058*
C4a'0.4323 (3)0.1517 (3)0.6189 (4)0.0468 (11)
C4b'0.3736 (3)0.0925 (3)0.6887 (5)0.0511 (11)
C5'0.3793 (3)0.0082 (3)0.7651 (5)0.0592 (12)
H5'0.42970.02230.77770.071*
C6'0.3091 (3)0.0292 (4)0.8219 (5)0.0687 (14)
H6'0.3130.08420.87550.082*
C7'0.2336 (3)0.0129 (5)0.8009 (5)0.0788 (16)
H7'0.18720.01520.83790.095*
C8'0.2255 (3)0.0981 (4)0.7243 (5)0.0650 (14)
H8'0.17460.12710.71040.078*
C8a'0.2962 (3)0.1367 (3)0.6706 (4)0.0511 (11)
C9a'0.3874 (3)0.2309 (3)0.5648 (5)0.0512 (12)
C10'0.2417 (3)0.2886 (4)0.5556 (5)0.0605 (13)
H10C0.26410.35350.55380.073*
H10D0.19830.28730.62170.073*
C11'0.2052 (3)0.2646 (4)0.4167 (6)0.0807 (17)
H11D0.16250.30990.39490.121*
H11E0.18290.20040.41790.121*
H11F0.24750.26840.35030.121*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N40.0492 (16)0.0518 (18)0.072 (2)0.0027 (13)0.0035 (14)0.0034 (16)
O10.144 (3)0.0511 (15)0.128 (3)0.0102 (17)0.023 (2)0.015 (2)
O20.142 (3)0.096 (2)0.103 (2)0.031 (2)0.064 (2)0.0035 (19)
N90.051 (2)0.068 (2)0.052 (2)0.011 (2)0.0044 (18)0.000 (2)
C10.065 (3)0.053 (3)0.058 (3)0.007 (2)0.004 (2)0.000 (2)
C20.058 (3)0.059 (3)0.055 (3)0.002 (3)0.001 (2)0.009 (2)
C30.048 (3)0.057 (3)0.049 (3)0.004 (2)0.004 (2)0.004 (2)
C40.045 (3)0.045 (2)0.056 (3)0.002 (2)0.004 (2)0.004 (2)
C4a0.048 (3)0.051 (3)0.047 (3)0.000 (2)0.007 (2)0.004 (2)
C4b0.055 (3)0.054 (3)0.039 (2)0.002 (2)0.005 (2)0.010 (2)
C50.071 (3)0.058 (3)0.057 (3)0.006 (3)0.012 (2)0.000 (2)
C60.080 (4)0.067 (3)0.067 (4)0.022 (3)0.002 (3)0.005 (3)
C70.064 (3)0.084 (4)0.066 (3)0.017 (3)0.014 (3)0.008 (3)
C80.061 (3)0.087 (4)0.057 (3)0.006 (3)0.002 (3)0.013 (3)
C8a0.051 (3)0.067 (3)0.047 (3)0.003 (3)0.009 (2)0.005 (2)
C9a0.045 (3)0.055 (3)0.043 (3)0.004 (2)0.003 (2)0.002 (2)
C100.063 (3)0.082 (4)0.068 (3)0.007 (3)0.017 (3)0.007 (3)
C110.082 (4)0.124 (5)0.071 (4)0.020 (4)0.019 (3)0.010 (3)
N9'0.042 (2)0.059 (2)0.059 (3)0.0061 (19)0.0045 (17)0.0032 (19)
C1'0.062 (3)0.055 (3)0.051 (3)0.018 (2)0.005 (2)0.008 (2)
C2'0.066 (3)0.050 (3)0.055 (3)0.003 (2)0.002 (2)0.006 (2)
C3'0.056 (3)0.047 (2)0.044 (2)0.005 (2)0.002 (2)0.000 (2)
C4'0.050 (3)0.047 (2)0.048 (2)0.007 (2)0.009 (2)0.004 (2)
C4a'0.050 (3)0.049 (2)0.041 (2)0.003 (2)0.003 (2)0.001 (2)
C4b'0.049 (3)0.052 (3)0.052 (3)0.003 (2)0.008 (2)0.001 (2)
C5'0.054 (3)0.058 (3)0.066 (3)0.007 (3)0.000 (2)0.002 (3)
C6'0.079 (4)0.065 (3)0.061 (3)0.015 (3)0.004 (3)0.003 (3)
C7'0.072 (4)0.087 (4)0.077 (4)0.031 (3)0.000 (3)0.004 (3)
C8'0.043 (3)0.079 (4)0.073 (3)0.000 (2)0.004 (2)0.012 (3)
C8a'0.051 (3)0.056 (3)0.047 (3)0.001 (3)0.002 (2)0.011 (2)
C9a'0.055 (3)0.052 (3)0.047 (3)0.007 (2)0.008 (2)0.005 (2)
C10'0.048 (3)0.061 (3)0.072 (3)0.023 (2)0.001 (2)0.011 (2)
C11'0.078 (4)0.077 (3)0.086 (4)0.028 (3)0.037 (3)0.013 (3)
Geometric parameters (Å, º) top
N4—O21.197 (4)C11—H11C0.96
N4—O11.208 (4)N9'—C9a'1.374 (6)
N4—C41.466 (5)N9'—C8a'1.398 (6)
N9—C8a1.374 (6)N9'—C10'1.450 (5)
N9—C9a1.392 (6)C1'—C2'1.368 (6)
N9—C101.463 (6)C1'—C9a'1.387 (7)
C1—C21.383 (7)C1'—H1'0.93
C1—C9a1.394 (7)C2'—C3'1.415 (6)
C1—H10.93C2'—H2'0.93
C2—C31.406 (6)C3'—C4'1.373 (6)
C2—H20.93C4'—C4a'1.393 (6)
C3—C41.402 (6)C4'—H4'0.93
C3—C3'1.482 (4)C4a'—C9a'1.420 (6)
C4—C4a1.388 (6)C4a'—C4b'1.443 (6)
C4a—C9a1.403 (6)C4b'—C5'1.394 (6)
C4a—C4b1.458 (6)C4b'—C8a'1.410 (6)
C4b—C51.402 (7)C5'—C6'1.382 (6)
C4b—C8a1.410 (6)C5'—H5'0.93
C5—C61.373 (7)C6'—C7'1.374 (7)
C5—H50.93C6'—H6'0.93
C6—C71.400 (8)C7'—C8'1.408 (8)
C6—H60.93C7'—H7'0.93
C7—C81.343 (8)C8'—C8a'1.382 (6)
C7—H70.93C8'—H8'0.93
C8—C8a1.406 (7)C10'—C11'1.530 (6)
C8—H80.93C10'—H10C0.97
C10—C111.505 (7)C10'—H10D0.97
C10—H10A0.97C11'—H11D0.96
C10—H10B0.97C11'—H11E0.96
C11—H11A0.96C11'—H11F0.96
C11—H11B0.96
O2—N4—O1123.8 (3)H11B—C11—H11C109.5
O2—N4—C4119.2 (3)C9a'—N9'—C8a'108.3 (4)
O1—N4—C4117.0 (3)C9a'—N9'—C10'124.9 (4)
C8a—N9—C9a109.1 (4)C8a'—N9'—C10'126.9 (4)
C8a—N9—C10126.2 (4)C2'—C1'—C9a'118.1 (4)
C9a—N9—C10124.8 (4)C2'—C1'—H1'120.9
C2—C1—C9a117.9 (4)C9a'—C1'—H1'120.9
C2—C1—H1121.1C1'—C2'—C3'122.9 (5)
C9a—C1—H1121.1C1'—C2'—H2'118.6
C1—C2—C3122.4 (5)C3'—C2'—H2'118.6
C1—C2—H2118.8C4'—C3'—C2'118.5 (5)
C3—C2—H2118.8C4'—C3'—C3123.1 (4)
C4—C3—C2117.0 (4)C2'—C3'—C3118.4 (4)
C4—C3—C3'123.6 (4)C3'—C4'—C4a'120.4 (4)
C2—C3—C3'119.4 (5)C3'—C4'—H4'119.8
C4a—C4—C3123.1 (4)C4a'—C4'—H4'119.8
C4a—C4—N4117.7 (4)C4'—C4a'—C9a'119.7 (4)
C3—C4—N4119.2 (4)C4'—C4a'—C4b'134.1 (4)
C4—C4a—C9a116.9 (4)C9a'—C4a'—C4b'106.2 (4)
C4—C4a—C4b135.8 (4)C5'—C4b'—C8a'119.1 (5)
C9a—C4a—C4b107.3 (4)C5'—C4b'—C4a'134.1 (4)
C5—C4b—C8a119.4 (5)C8a'—C4b'—C4a'106.8 (4)
C5—C4b—C4a135.0 (4)C6'—C5'—C4b'119.0 (5)
C8a—C4b—C4a105.5 (4)C6'—C5'—H5'120.5
C6—C5—C4b119.1 (5)C4b'—C5'—H5'120.5
C6—C5—H5120.5C7'—C6'—C5'121.4 (5)
C4b—C5—H5120.5C7'—C6'—H6'119.3
C5—C6—C7120.2 (5)C5'—C6'—H6'119.3
C5—C6—H6119.9C6'—C7'—C8'121.0 (5)
C7—C6—H6119.9C6'—C7'—H7'119.5
C8—C7—C6122.5 (5)C8'—C7'—H7'119.5
C8—C7—H7118.8C8a'—C8'—C7'117.3 (5)
C6—C7—H7118.8C8a'—C8'—H8'121.3
C7—C8—C8a118.3 (5)C7'—C8'—H8'121.3
C7—C8—H8120.9C8'—C8a'—N9'128.9 (4)
C8a—C8—H8120.9C8'—C8a'—C4b'122.0 (5)
N9—C8a—C8129.8 (5)N9'—C8a'—C4b'109.0 (4)
N9—C8a—C4b109.7 (4)N9'—C9a'—C1'129.9 (4)
C8—C8a—C4b120.5 (5)N9'—C9a'—C4a'109.7 (4)
N9—C9a—C1128.9 (4)C1'—C9a'—C4a'120.4 (4)
N9—C9a—C4a108.4 (4)N9'—C10'—C11'112.5 (4)
C1—C9a—C4a122.7 (4)N9'—C10'—H10C109.1
N9—C10—C11112.5 (5)C11'—C10'—H10C109.1
N9—C10—H10A109.1N9'—C10'—H10D109.1
C11—C10—H10A109.1C11'—C10'—H10D109.1
N9—C10—H10B109.1H10C—C10'—H10D107.8
C11—C10—H10B109.1C10'—C11'—H11D109.5
H10A—C10—H10B107.8C10'—C11'—H11E109.5
C10—C11—H11A109.5H11D—C11'—H11E109.5
C10—C11—H11B109.5C10'—C11'—H11F109.5
H11A—C11—H11B109.5H11D—C11'—H11F109.5
C10—C11—H11C109.5H11E—C11'—H11F109.5
H11A—C11—H11C109.5
C9a—C1—C2—C30.5 (7)C8a—N9—C10—C1191.3 (6)
C1—C2—C3—C40.4 (6)C9a—N9—C10—C1188.4 (6)
C1—C2—C3—C3'177.1 (4)C9a'—C1'—C2'—C3'2.3 (6)
C2—C3—C4—C4a1.3 (7)C1'—C2'—C3'—C4'1.0 (6)
C3'—C3—C4—C4a176.2 (4)C1'—C2'—C3'—C3179.8 (4)
C2—C3—C4—N4179.3 (3)C4—C3—C3'—C4'61.0 (4)
C3'—C3—C4—N43.2 (6)C2—C3—C3'—C4'121.6 (6)
O2—N4—C4—C4a98.0 (5)C4—C3—C3'—C2'120.2 (6)
O1—N4—C4—C4a82.0 (5)C2—C3—C3'—C2'57.2 (3)
O2—N4—C4—C381.5 (5)C2'—C3'—C4'—C4a'0.1 (7)
O1—N4—C4—C398.6 (5)C3—C3'—C4'—C4a'178.9 (4)
C3—C4—C4a—C9a2.0 (6)C3'—C4'—C4a'—C9a'0.6 (6)
N4—C4—C4a—C9a178.5 (4)C3'—C4'—C4a'—C4b'177.3 (5)
C3—C4—C4a—C4b176.5 (5)C4'—C4a'—C4b'—C5'0.4 (9)
N4—C4—C4a—C4b3.0 (7)C9a'—C4a'—C4b'—C5'177.4 (5)
C4—C4a—C4b—C53.1 (9)C4'—C4a'—C4b'—C8a'178.6 (5)
C9a—C4a—C4b—C5175.6 (5)C9a'—C4a'—C4b'—C8a'1.6 (5)
C4—C4a—C4b—C8a179.3 (5)C8a'—C4b'—C5'—C6'0.5 (7)
C9a—C4a—C4b—C8a0.7 (5)C4a'—C4b'—C5'—C6'178.4 (5)
C8a—C4b—C5—C62.1 (7)C4b'—C5'—C6'—C7'2.2 (7)
C4a—C4b—C5—C6178.0 (5)C5'—C6'—C7'—C8'2.2 (8)
C4b—C5—C6—C70.4 (7)C6'—C7'—C8'—C8a'0.5 (8)
C5—C6—C7—C80.7 (8)C7'—C8'—C8a'—N9'177.1 (5)
C6—C7—C8—C8a0.0 (8)C7'—C8'—C8a'—C4b'1.2 (7)
C9a—N9—C8a—C8179.2 (5)C9a'—N9'—C8a'—C8'179.7 (5)
C10—N9—C8a—C81.0 (8)C10'—N9'—C8a'—C8'1.6 (7)
C9a—N9—C8a—C4b0.4 (5)C9a'—N9'—C8a'—C4b'1.2 (5)
C10—N9—C8a—C4b179.3 (4)C10'—N9'—C8a'—C4b'179.9 (4)
C7—C8—C8a—N9177.8 (5)C5'—C4b'—C8a'—C8'1.2 (7)
C7—C8—C8a—C4b1.8 (7)C4a'—C4b'—C8a'—C8'179.6 (4)
C5—C4b—C8a—N9176.8 (4)C5'—C4b'—C8a'—N9'177.4 (4)
C4a—C4b—C8a—N90.2 (5)C4a'—C4b'—C8a'—N9'1.8 (5)
C5—C4b—C8a—C82.9 (7)C8a'—N9'—C9a'—C1'179.4 (5)
C4a—C4b—C8a—C8179.9 (4)C10'—N9'—C9a'—C1'0.6 (8)
C8a—N9—C9a—C1176.8 (5)C8a'—N9'—C9a'—C4a'0.2 (5)
C10—N9—C9a—C13.5 (7)C10'—N9'—C9a'—C4a'178.9 (4)
C8a—N9—C9a—C4a0.9 (5)C2'—C1'—C9a'—N9'177.7 (5)
C10—N9—C9a—C4a178.9 (4)C2'—C1'—C9a'—C4a'2.8 (7)
C2—C1—C9a—N9178.7 (4)C4'—C4a'—C9a'—N9'178.4 (4)
C2—C1—C9a—C4a1.3 (7)C4b'—C4a'—C9a'—N9'0.9 (5)
C4—C4a—C9a—N9179.9 (4)C4'—C4a'—C9a'—C1'2.0 (6)
C4b—C4a—C9a—N91.0 (5)C4b'—C4a'—C9a'—C1'179.5 (4)
C4—C4a—C9a—C12.0 (6)C9a'—N9'—C10'—C11'87.1 (6)
C4b—C4a—C9a—C1176.9 (4)C8a'—N9'—C10'—C11'91.4 (6)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H11a···O2i0.962.523.379 (7)149
C11—H11d···O1ii0.962.593.290 (6)130
Symmetry codes: (i) x+1/2, y+1/2, z+1/2; (ii) x1/2, y+1/2, z.
 

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