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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Apr 25;65(Pt 5):o1100. doi: 10.1107/S1600536809014548

Diethyl 1,4-dioxo-1,2,2a,3,4,10b-hexahydro-5H,10H-2,3,4a,10a-tetraaza­benzo[g]cyclopenta[cd]azulene-2a,10b-dicarboxylate

Jing Qin a,*
PMCID: PMC2977778  PMID: 21583914

Abstract

In the title compound, C18H20N4O6, the dihedral angle between the two fused five-membered rings in the glycoluril unit is 64.42 (2)°. The crystal structure features inter­molecular N—H⋯O and C—H⋯O interactions. An intramolecular C—H⋯O contact is also present.

Related literature

For the preparation of the title compound, see: Wu et al. (2002a ). For crystal engineering studies of glycoluril and its derivatives, see: Chen et al. (2007); Wang et al. (2006); Johnson et al. (2002); Wu et al. (2002b ).graphic file with name e-65-o1100-scheme1.jpg

Experimental

Crystal data

  • C18H20N4O6

  • M r = 388.38

  • Triclinic, Inline graphic

  • a = 8.1394 (5) Å

  • b = 9.4425 (5) Å

  • c = 13.3576 (8) Å

  • α = 93.1550 (10)°

  • β = 96.0560 (10)°

  • γ = 112.3970 (10)°

  • V = 938.80 (9) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.11 mm−1

  • T = 294 K

  • 0.20 × 0.20 × 0.10 mm

Data collection

  • Bruker SMART 4K CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1997) T min = 0.976, T max = 0.989

  • 7700 measured reflections

  • 3624 independent reflections

  • 3028 reflections with I > 2σ(I)

  • R int = 0.020

Refinement

  • R[F 2 > 2σ(F 2)] = 0.049

  • wR(F 2) = 0.144

  • S = 1.05

  • 3624 reflections

  • 261 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.28 e Å−3

  • Δρmin = −0.20 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: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809014548/nc2142sup1.cif

e-65-o1100-sup1.cif (21.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809014548/nc2142Isup2.hkl

e-65-o1100-Isup2.hkl (177.7KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C7—H7A⋯O3 0.97 2.52 3.107 (2) 119
C17—H17B⋯O2i 0.97 2.58 3.343 (3) 136
C7—H7B⋯O3ii 0.97 2.59 3.478 (2) 153
N4—H4A⋯O2iii 0.85 (3) 2.05 (3) 2.871 (2) 165 (2)
N3—H3A⋯O5iv 0.87 (3) 2.09 (3) 2.917 (2) 159 (2)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic.

Acknowledgments

The author gratefully acknowledges support from Central China Normal University.

supplementary crystallographic information

Comment

Glycoluril and its derivatives have been widely studied in supramolecular chemistry (Johnson et al., 2002; Wu et al., 2002b). As a continuation of our recent studies in this area (Wang et al., 2006; Chen et al., 2007), we herein report the crystal structure of the title compound (Fig. 1). The dihedral angle between the two fused five-membered rings in the glycoluril unit is 64.42 (2) °. In the crystal structure the molecules are connected via weak intermolecular N—H···O hydrogen bonding (Table 1).

Experimental

The title compound was synthesized according to a literature procedure (Wu et al.; 2002a). Crystals of (I) suitable for X-ray diffraction were grown by slow evaporation of a dichloromethane-methanol (1:2) solution of the title compound at room temperature.

Refinement

All H atoms were positioned with idealized geometry with C—H = 0.93–0.97 Å (methyl H atoms allowed to rotate but not to tip) and were refined isotropic (Uiso(H) = 1.2 Ueq(C) or 1.5 Ueq(C) (methyl C)) using a riding model.

Figures

Fig. 1.

Fig. 1.

A view of (I), showing the atom-labelling scheme, with displacement ellipsoids drawn at the 30% probability level.

Crystal data

C18H20N4O6 Z = 2
Mr = 388.38 F(000) = 408
Triclinic, P1 Dx = 1.374 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.1394 (5) Å Cell parameters from 3262 reflections
b = 9.4425 (5) Å θ = 2.4–27.5°
c = 13.3576 (8) Å µ = 0.11 mm1
α = 93.155 (1)° T = 294 K
β = 96.056 (1)° Block, colorless
γ = 112.397 (1)° 0.20 × 0.20 × 0.10 mm
V = 938.80 (9) Å3

Data collection

Bruker SMART 4K CCD area-detector diffractometer 3624 independent reflections
Radiation source: fine-focus sealed tube 3028 reflections with I > 2σ(I)
graphite Rint = 0.020
φ and ω scans θmax = 26.0°, θmin = 1.5°
Absorption correction: multi-scan (SADABS; Sheldrick, 1997) h = −10→8
Tmin = 0.976, Tmax = 0.989 k = −11→11
7700 measured reflections l = −16→16

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)] = 0.049 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.144 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0741P)2 + 0.3055P] where P = (Fo2 + 2Fc2)/3
3624 reflections (Δ/σ)max = 0.005
261 parameters Δρmax = 0.28 e Å3
0 restraints Δρmin = −0.20 e Å3

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
C1 0.7535 (3) 0.3332 (2) 0.06082 (12) 0.0350 (4)
C2 0.6905 (3) 0.1940 (2) 0.00001 (15) 0.0442 (5)
H2 0.5714 0.1512 −0.0298 0.053*
C3 0.8025 (3) 0.1180 (2) −0.01692 (16) 0.0516 (5)
H3 0.7589 0.0250 −0.0579 0.062*
C4 0.9787 (3) 0.1811 (2) 0.02733 (16) 0.0515 (5)
H4 1.0552 0.1318 0.0152 0.062*
C5 1.0421 (3) 0.3177 (2) 0.08982 (15) 0.0437 (5)
H5 1.1607 0.3581 0.1207 0.052*
C6 0.9321 (2) 0.3955 (2) 0.10733 (12) 0.0352 (4)
C7 0.6302 (3) 0.4178 (2) 0.07030 (12) 0.0375 (4)
H7A 0.6781 0.5130 0.0391 0.045*
H7B 0.5141 0.3556 0.0321 0.045*
C8 1.0095 (2) 0.5470 (2) 0.17322 (13) 0.0359 (4)
H8A 1.1323 0.5666 0.2006 0.043*
H8B 1.0123 0.6287 0.1316 0.043*
C9 0.4886 (3) 0.3441 (2) 0.22434 (14) 0.0392 (4)
C10 0.9584 (3) 0.5307 (2) 0.35329 (13) 0.0395 (4)
C11 0.7426 (2) 0.5735 (2) 0.24235 (12) 0.0330 (4)
C12 0.7751 (3) 0.7358 (2) 0.20982 (13) 0.0372 (4)
C13 0.9500 (4) 1.0015 (3) 0.2570 (2) 0.0691 (7)
H13A 1.0481 1.0306 0.2168 0.083*
H13B 0.8494 1.0152 0.2195 0.083*
C14 1.0045 (7) 1.0966 (3) 0.3520 (3) 0.1181 (14)
H14A 0.9041 1.0729 0.3891 0.177*
H14B 1.0469 1.2031 0.3398 0.177*
H14C 1.0988 1.0774 0.3906 0.177*
C15 0.6771 (3) 0.5423 (2) 0.34897 (13) 0.0379 (4)
C16 0.6154 (3) 0.6578 (2) 0.40178 (14) 0.0412 (4)
C17 0.4679 (4) 0.8288 (3) 0.3831 (2) 0.0741 (8)
H17A 0.5609 0.9012 0.4335 0.089*
H17B 0.3639 0.7756 0.4160 0.089*
C18 0.4201 (6) 0.9114 (4) 0.3022 (3) 0.1120 (13)
H18A 0.5252 0.9687 0.2727 0.168*
H18B 0.3718 0.9808 0.3300 0.168*
H18C 0.3321 0.8386 0.2511 0.168*
N1 0.6035 (2) 0.45511 (17) 0.17377 (10) 0.0356 (4)
N2 0.9101 (2) 0.55255 (17) 0.25637 (10) 0.0345 (4)
N3 0.5268 (3) 0.3968 (2) 0.32473 (13) 0.0491 (4)
H3A 0.456 (3) 0.355 (3) 0.3683 (19) 0.059*
N4 0.8307 (3) 0.5358 (2) 0.40898 (13) 0.0532 (5)
H4A 0.835 (3) 0.525 (3) 0.472 (2) 0.064*
O1 0.37312 (19) 0.22369 (16) 0.18597 (12) 0.0528 (4)
O2 1.0959 (2) 0.51339 (19) 0.38374 (10) 0.0531 (4)
O3 0.7018 (2) 0.75960 (17) 0.13482 (10) 0.0552 (4)
O4 0.8984 (2) 0.84003 (15) 0.27670 (11) 0.0526 (4)
O5 0.6376 (3) 0.68292 (19) 0.49151 (11) 0.0644 (5)
O6 0.5323 (2) 0.71765 (18) 0.33836 (11) 0.0556 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0430 (10) 0.0384 (9) 0.0271 (8) 0.0191 (8) 0.0058 (7) 0.0050 (7)
C2 0.0461 (11) 0.0437 (10) 0.0410 (10) 0.0161 (9) 0.0054 (8) 0.0024 (8)
C3 0.0708 (15) 0.0391 (11) 0.0507 (12) 0.0266 (11) 0.0138 (11) 0.0024 (9)
C4 0.0657 (15) 0.0492 (12) 0.0557 (12) 0.0368 (11) 0.0181 (11) 0.0113 (10)
C5 0.0426 (11) 0.0528 (11) 0.0450 (10) 0.0261 (10) 0.0106 (9) 0.0166 (9)
C6 0.0391 (10) 0.0427 (10) 0.0286 (8) 0.0197 (8) 0.0072 (7) 0.0108 (7)
C7 0.0406 (10) 0.0476 (10) 0.0266 (8) 0.0221 (9) −0.0021 (7) −0.0009 (7)
C8 0.0340 (10) 0.0443 (10) 0.0305 (9) 0.0155 (8) 0.0059 (7) 0.0078 (7)
C9 0.0373 (10) 0.0384 (10) 0.0451 (10) 0.0186 (9) 0.0059 (8) 0.0022 (8)
C10 0.0412 (11) 0.0464 (10) 0.0293 (9) 0.0160 (9) 0.0003 (8) 0.0062 (8)
C11 0.0354 (10) 0.0382 (9) 0.0262 (8) 0.0151 (8) 0.0042 (7) 0.0044 (7)
C12 0.0419 (10) 0.0411 (10) 0.0312 (9) 0.0186 (9) 0.0061 (8) 0.0055 (7)
C13 0.0793 (18) 0.0386 (12) 0.0763 (17) 0.0093 (12) 0.0038 (14) 0.0123 (11)
C14 0.170 (4) 0.0489 (16) 0.107 (3) 0.019 (2) 0.001 (3) −0.0135 (16)
C15 0.0405 (10) 0.0436 (10) 0.0296 (9) 0.0160 (9) 0.0055 (7) 0.0056 (7)
C16 0.0412 (11) 0.0415 (10) 0.0350 (10) 0.0092 (9) 0.0087 (8) −0.0008 (8)
C17 0.0743 (18) 0.0650 (16) 0.096 (2) 0.0388 (15) 0.0268 (15) −0.0014 (14)
C18 0.123 (3) 0.088 (2) 0.143 (3) 0.070 (2) −0.014 (3) 0.001 (2)
N1 0.0346 (8) 0.0415 (8) 0.0296 (7) 0.0153 (7) 0.0002 (6) 0.0005 (6)
N2 0.0339 (8) 0.0433 (8) 0.0263 (7) 0.0155 (7) 0.0013 (6) 0.0051 (6)
N3 0.0571 (11) 0.0412 (9) 0.0423 (9) 0.0088 (8) 0.0185 (8) 0.0041 (7)
N4 0.0579 (12) 0.0867 (14) 0.0265 (8) 0.0393 (11) 0.0068 (8) 0.0152 (8)
O1 0.0427 (8) 0.0437 (8) 0.0624 (9) 0.0079 (7) 0.0054 (7) −0.0045 (7)
O2 0.0493 (9) 0.0791 (11) 0.0373 (7) 0.0323 (8) 0.0003 (6) 0.0148 (7)
O3 0.0773 (11) 0.0517 (9) 0.0407 (8) 0.0328 (8) −0.0054 (7) 0.0069 (6)
O4 0.0588 (9) 0.0372 (7) 0.0505 (8) 0.0091 (7) −0.0048 (7) 0.0069 (6)
O5 0.0891 (13) 0.0677 (10) 0.0367 (8) 0.0307 (9) 0.0136 (8) −0.0042 (7)
O6 0.0633 (10) 0.0630 (9) 0.0520 (9) 0.0378 (8) 0.0095 (7) 0.0002 (7)

Geometric parameters (Å, °)

C1—C2 1.390 (3) C11—C12 1.548 (2)
C1—C6 1.401 (3) C11—C15 1.577 (2)
C1—C7 1.513 (2) C12—O3 1.188 (2)
C2—C3 1.386 (3) C12—O4 1.317 (2)
C2—H2 0.9300 C13—C14 1.437 (4)
C3—C4 1.375 (3) C13—O4 1.466 (3)
C3—H3 0.9300 C13—H13A 0.9700
C4—C5 1.382 (3) C13—H13B 0.9700
C4—H4 0.9300 C14—H14A 0.9600
C5—C6 1.387 (3) C14—H14B 0.9600
C5—H5 0.9300 C14—H14C 0.9600
C6—C8 1.508 (3) C15—N4 1.437 (2)
C7—N1 1.466 (2) C15—N3 1.441 (3)
C7—H7A 0.9700 C15—C16 1.531 (3)
C7—H7B 0.9700 C16—O5 1.190 (2)
C8—N2 1.451 (2) C16—O6 1.311 (2)
C8—H8A 0.9700 C17—O6 1.466 (3)
C8—H8B 0.9700 C17—C18 1.471 (4)
C9—O1 1.208 (2) C17—H17A 0.9700
C9—N3 1.365 (3) C17—H17B 0.9700
C9—N1 1.376 (2) C18—H18A 0.9600
C10—O2 1.223 (2) C18—H18B 0.9600
C10—N4 1.354 (3) C18—H18C 0.9600
C10—N2 1.363 (2) N3—H3A 0.87 (3)
C11—N1 1.440 (2) N4—H4A 0.85 (3)
C11—N2 1.445 (2)
C2—C1—C6 119.23 (17) C14—C13—H13A 109.9
C2—C1—C7 119.00 (17) O4—C13—H13A 109.9
C6—C1—C7 121.69 (16) C14—C13—H13B 109.9
C3—C2—C1 121.0 (2) O4—C13—H13B 109.9
C3—C2—H2 119.5 H13A—C13—H13B 108.3
C1—C2—H2 119.5 C13—C14—H14A 109.5
C4—C3—C2 119.5 (2) C13—C14—H14B 109.5
C4—C3—H3 120.3 H14A—C14—H14B 109.5
C2—C3—H3 120.3 C13—C14—H14C 109.5
C3—C4—C5 120.1 (2) H14A—C14—H14C 109.5
C3—C4—H4 120.0 H14B—C14—H14C 109.5
C5—C4—H4 120.0 N4—C15—N3 114.94 (17)
C4—C5—C6 121.16 (19) N4—C15—C16 110.13 (16)
C4—C5—H5 119.4 N3—C15—C16 109.09 (16)
C6—C5—H5 119.4 N4—C15—C11 102.62 (15)
C5—C6—C1 118.94 (18) N3—C15—C11 101.34 (14)
C5—C6—C8 119.12 (17) C16—C15—C11 118.67 (15)
C1—C6—C8 121.91 (16) O5—C16—O6 125.5 (2)
N1—C7—C1 115.68 (14) O5—C16—C15 121.54 (18)
N1—C7—H7A 108.4 O6—C16—C15 112.92 (15)
C1—C7—H7A 108.4 O6—C17—C18 108.6 (3)
N1—C7—H7B 108.4 O6—C17—H17A 110.0
C1—C7—H7B 108.4 C18—C17—H17A 110.0
H7A—C7—H7B 107.4 O6—C17—H17B 110.0
N2—C8—C6 113.76 (15) C18—C17—H17B 110.0
N2—C8—H8A 108.8 H17A—C17—H17B 108.3
C6—C8—H8A 108.8 C17—C18—H18A 109.5
N2—C8—H8B 108.8 C17—C18—H18B 109.5
C6—C8—H8B 108.8 H18A—C18—H18B 109.5
H8A—C8—H8B 107.7 C17—C18—H18C 109.5
O1—C9—N3 126.68 (18) H18A—C18—H18C 109.5
O1—C9—N1 125.85 (18) H18B—C18—H18C 109.5
N3—C9—N1 107.45 (16) C9—N1—C11 111.93 (14)
O2—C10—N4 126.78 (16) C9—N1—C7 120.52 (15)
O2—C10—N2 125.11 (18) C11—N1—C7 121.64 (15)
N4—C10—N2 108.09 (16) C10—N2—C11 113.25 (15)
N1—C11—N2 113.91 (14) C10—N2—C8 124.21 (15)
N1—C11—C12 111.49 (13) C11—N2—C8 122.46 (13)
N2—C11—C12 109.92 (14) C9—N3—C15 114.32 (16)
N1—C11—C15 103.63 (14) C9—N3—H3A 122.6 (16)
N2—C11—C15 101.80 (13) C15—N3—H3A 122.3 (16)
C12—C11—C15 115.76 (14) C10—N4—C15 113.12 (15)
O3—C12—O4 126.43 (17) C10—N4—H4A 123.5 (17)
O3—C12—C11 124.36 (17) C15—N4—H4A 123.0 (17)
O4—C12—C11 109.19 (14) C12—O4—C13 116.92 (16)
C14—C13—O4 108.9 (2) C16—O6—C17 116.28 (18)
C6—C1—C2—C3 −1.4 (3) O1—C9—N1—C7 −17.8 (3)
C7—C1—C2—C3 175.22 (17) N3—C9—N1—C7 163.56 (16)
C1—C2—C3—C4 0.2 (3) N2—C11—N1—C9 97.72 (17)
C2—C3—C4—C5 1.3 (3) C12—C11—N1—C9 −137.17 (15)
C3—C4—C5—C6 −1.5 (3) C15—C11—N1—C9 −12.01 (18)
C4—C5—C6—C1 0.3 (3) N2—C11—N1—C7 −55.3 (2)
C4—C5—C6—C8 −177.86 (17) C12—C11—N1—C7 69.8 (2)
C2—C1—C6—C5 1.2 (2) C15—C11—N1—C7 −165.00 (14)
C7—C1—C6—C5 −175.36 (16) C1—C7—N1—C9 −78.3 (2)
C2—C1—C6—C8 179.26 (16) C1—C7—N1—C11 72.4 (2)
C7—C1—C6—C8 2.7 (2) O2—C10—N2—C11 −178.59 (18)
C2—C1—C7—N1 124.69 (18) N4—C10—N2—C11 −0.2 (2)
C6—C1—C7—N1 −58.8 (2) O2—C10—N2—C8 4.8 (3)
C5—C6—C8—N2 −126.25 (17) N4—C10—N2—C8 −176.82 (17)
C1—C6—C8—N2 55.7 (2) N1—C11—N2—C10 −116.92 (17)
N1—C11—C12—O3 −3.8 (3) C12—C11—N2—C10 117.15 (16)
N2—C11—C12—O3 123.5 (2) C15—C11—N2—C10 −6.07 (19)
C15—C11—C12—O3 −121.9 (2) N1—C11—N2—C8 59.8 (2)
N1—C11—C12—O4 177.71 (15) C12—C11—N2—C8 −66.1 (2)
N2—C11—C12—O4 −55.00 (19) C15—C11—N2—C8 170.64 (15)
C15—C11—C12—O4 59.6 (2) C6—C8—N2—C10 99.2 (2)
N1—C11—C15—N4 127.94 (15) C6—C8—N2—C11 −77.2 (2)
N2—C11—C15—N4 9.48 (18) O1—C9—N3—C15 177.73 (18)
C12—C11—C15—N4 −109.69 (17) N1—C9—N3—C15 −3.7 (2)
N1—C11—C15—N3 8.88 (17) N4—C15—N3—C9 −113.33 (19)
N2—C11—C15—N3 −109.58 (15) C16—C15—N3—C9 122.44 (18)
C12—C11—C15—N3 131.26 (16) C11—C15—N3—C9 −3.5 (2)
N1—C11—C15—C16 −110.44 (17) O2—C10—N4—C15 −174.2 (2)
N2—C11—C15—C16 131.09 (17) N2—C10—N4—C15 7.4 (2)
C12—C11—C15—C16 11.9 (2) N3—C15—N4—C10 98.4 (2)
N4—C15—C16—O5 −29.5 (3) C16—C15—N4—C10 −137.96 (18)
N3—C15—C16—O5 97.5 (2) C11—C15—N4—C10 −10.7 (2)
C11—C15—C16—O5 −147.25 (19) O3—C12—O4—C13 0.2 (3)
N4—C15—C16—O6 153.07 (17) C11—C12—O4—C13 178.62 (19)
N3—C15—C16—O6 −79.91 (19) C14—C13—O4—C12 150.2 (3)
C11—C15—C16—O6 35.3 (2) O5—C16—O6—C17 2.3 (3)
O1—C9—N1—C11 −171.16 (18) C15—C16—O6—C17 179.63 (19)
N3—C9—N1—C11 10.2 (2) C18—C17—O6—C16 166.1 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C7—H7A···O3 0.97 2.52 3.107 (2) 119
C17—H17B···O2i 0.97 2.58 3.343 (3) 136
C7—H7B···O3ii 0.97 2.59 3.478 (2) 153
N4—H4A···O2iii 0.85 (3) 2.05 (3) 2.871 (2) 165 (2)
N3—H3A···O5iv 0.87 (3) 2.09 (3) 2.917 (2) 159 (2)

Symmetry codes: (i) x−1, y, z; (ii) −x+1, −y+1, −z; (iii) −x+2, −y+1, −z+1; (iv) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NC2142).

References

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  8. Wu, A., Fettinger, J. C. & Isaacs, L. (2002b). Tetrahedron, 58, 9769–9777.

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/S1600536809014548/nc2142sup1.cif

e-65-o1100-sup1.cif (21.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809014548/nc2142Isup2.hkl

e-65-o1100-Isup2.hkl (177.7KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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