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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 Mar 29;70(Pt 4):o490. doi: 10.1107/S1600536814006266

3-(Di­phenyl­amino)­isobenzo­furan-1(3H)-one

Rodolfo Moreno-Fuquen a,*, Juan C Castillo a, Rodrigo Abonia a, Javier Ellena b, Juan C Tenorio b
PMCID: PMC3998613  PMID: 24826181

Abstract

In the title isobenzo­furan­one derivative, C20H15NO2, the planar fused-ring system (r.m.s. deviation for the 10 fitted atoms = 0.031 Å) forms dihedral angles of 63.58 (6) and 63.17 (8)° with the N-bound phenyl rings; the dihedral angle between the planes of these phenyl rings is 85.92 (7)°. In the crystal, mol­ecules are linked by weak C—H⋯O inter­actions, involving both O atoms, forming helical supra­molecular chains along [001].

Related literature  

For biological and pharmacological properties of isobenzo­furan­ones, see: Anderson et al. (2005); Malpani et al. (2013); Shode et al. (2002); Yoganathan et al. (2003). For the synthesis of diverse amino derivatives, see: Abonia et al. (2010, 2013); Moreno-Fuquen et al. (2013). For similar structures, see: Mendenhall et al. (2003); Reynolds & Scaringe (1982).graphic file with name e-70-0o490-scheme1.jpg

Experimental  

Crystal data  

  • C20H15NO2

  • M r = 301.33

  • Orthorhombic, Inline graphic

  • a = 19.1440 (13) Å

  • b = 8.9363 (6) Å

  • c = 9.1111 (3) Å

  • V = 1558.70 (16) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 295 K

  • 0.56 × 0.37 × 0.19 mm

Data collection  

  • Nonius KappaCCD diffractometer

  • 3011 measured reflections

  • 1684 independent reflections

  • 1366 reflections with I > 2σ(I)

  • R int = 0.018

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.106

  • S = 1.09

  • 1684 reflections

  • 213 parameters

  • 1 restraint

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

  • Δρmax = 0.15 e Å−3

  • Δρmin = −0.15 e Å−3

Data collection: COLLECT (Nonius, 2000); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO (Otwinowski & Minor, 1997) and SCALEPACK; 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, 2012) and Mercury (Macrae et al., 2006); software used to prepare material for publication: WinGX (Farrugia, 2012).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536814006266/tk5299sup1.cif

e-70-0o490-sup1.cif (26.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814006266/tk5299Isup2.hkl

e-70-0o490-Isup2.hkl (83KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814006266/tk5299Isup3.cml

CCDC reference: 992870

Additional supporting information: crystallographic information; 3D view; checkCIF report

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

D—H⋯A D—H H⋯A DA D—H⋯A
C3—H3⋯O2i 0.93 2.70 3.413 (3) 135
C1—H1⋯O1i 1.03 (3) 2.36 (3) 3.307 (3) 153 (2)

Symmetry code: (i) Inline graphic.

Acknowledgments

RMF and RA are grateful to the Universidad del Valle, Colombia, for partial financial support. JCC acknowledges his doctoral fellowship granted by COLCIENCIAS.

supplementary crystallographic information

1. Introduction

2. Experimental

2.1. Synthesis and crystallization

Reagents and solvents for the synthesis were obtained from the Aldrich Chemical Co., and were used without additional purification. A 5 mL pyrex test tube was charged with a mixture of di­phenyl­amine (102 mg, 0.60 mmol) and 2-formyl­benzoic acid (90 mg, 0.60 mmol) without solvent. The mixture was heated in an oil bath at 120 °C for 1 h until the starting materials were not longer detected by thin-layer chromatography. The solid formed was removed and washed with cold ethanol (1 mL). White crystals of (I) were grown by slow evaporation, under ambient conditions, from its solution in ethanol [92% yield, M.p.: 396 (1) K].

2.2. Refinement

All H-atoms, except H1, were positioned at geometrically idealized positions, C—H = 0.93 Å, and they were refined using a riding model approximation with Uiso(H) = 1.2Ueq(parent atom). Atom H1 was found from the Fourier difference map and its coordinates were freely refined. In the absence of significant anomalous scattering, Friedel pairs were merged.

3. Results and discussion

Isobenzo­furan­ones are an important class of synthetic and naturally occurring products exhibiting diverse biological and pharmacological properties. Some of them appear forming part of the structure of natural products such as fuscinarin (anti-HIV properties) (Yoganathan et al., 2003), typhaphthalide (phenolic compound isolated from Typha capensis) (Shode et al., 2002), noscapine (anti­tussive and anti-tumor properties) (Anderson et al., 2005), and synthetic compounds like some spiro­lactones (inhibitors of the influenza virus type B) (Malpani et al., 2013). Continuing with our current studies on the use of imines and imminium ions for the synthesis of diverse amino-derivatives of synthetic and biological inter­est (Abonia et al., 2010; Abonia et al., 2013; Moreno-Fuquen et al., 2013), 3-di­phenyl­amino­isobenzo­furan-1(3H)-one, (I), was obtained from the reaction of 2-formyl­benzoic acid and di­phenyl­amine through an imminium ion inter­mediate. The molecular structure of (I) is shown in Fig. 1. Taking the plane of the phthalide lactone C1—C8(=O1)—O2 (Mendenhall et al., 2003) as a point of reference, the title compound represents the first structure reported with ligands from C1. The bond lengths reported in the phthalide lactone (Reynolds & Scaringe, 1982) are very similar to those presented in (I). In the present molecule, rings A (C9—C14), B (C1—C8—O2) and C (C15—C20) are planar and show dihedral angles between them: A/B = 63.58 (6)°, C/B= 63.17 (8)° and A/C= 85.92 (7)°. In the crystal, the molecules are linked by weak C—H···O inter­actions, forming eight-membered {···HC3H···OCO} synthons, leading to a chain along [001], Table 1 and Fig. 2.

Figures

Fig. 1.

Fig. 1.

Molecular conformation and atom numbering scheme for (I) with displacement ellipsoids drawn at the 50% probability level. H atoms are shown as spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Part of the crystal structure of (I), showing the formation of helical chains running along [001]. Symmetry code: (i) -x+1/2, +y, +z-1/2.

Crystal data

C20H15NO2 Dx = 1.284 Mg m3
Mr = 301.33 Melting point: 396(1) K
Orthorhombic, Pca21 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2ac Cell parameters from 2966 reflections
a = 19.1440 (13) Å θ = 3.1–26.4°
b = 8.9363 (6) Å µ = 0.08 mm1
c = 9.1111 (3) Å T = 295 K
V = 1558.70 (16) Å3 Block, white
Z = 4 0.56 × 0.37 × 0.19 mm
F(000) = 632

Data collection

Nonius KappaCCD diffractometer 1366 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.018
Graphite monochromator θmax = 26.4°, θmin = 3.1°
CCD rotation images, thick slices scans h = −23→23
3011 measured reflections k = −11→11
1684 independent reflections l = −11→11

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.041 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.106 w = 1/[σ2(Fo2) + (0.0695P)2 + 0.0242P] where P = (Fo2 + 2Fc2)/3
S = 1.09 (Δ/σ)max < 0.001
1684 reflections Δρmax = 0.15 e Å3
213 parameters Δρmin = −0.15 e Å3
1 restraint Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.042 (9)

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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
O1 0.34995 (11) 1.2679 (2) 0.7466 (2) 0.0689 (6)
O2 0.29111 (9) 1.13804 (19) 0.5762 (2) 0.0578 (5)
N1 0.30495 (10) 0.9786 (2) 0.3646 (3) 0.0509 (5)
C1 0.28865 (13) 1.1262 (3) 0.4127 (3) 0.0517 (6)
C2 0.33858 (12) 1.2458 (3) 0.3647 (3) 0.0513 (6)
C3 0.35485 (15) 1.2966 (3) 0.2247 (3) 0.0580 (6)
H3 0.3353 1.2529 0.1417 0.070*
C4 0.40139 (16) 1.4151 (3) 0.2135 (4) 0.0672 (7)
H4 0.4129 1.4516 0.1210 0.081*
C5 0.43103 (17) 1.4803 (3) 0.3362 (4) 0.0761 (9)
H5 0.4626 1.5586 0.3248 0.091*
C6 0.41460 (15) 1.4311 (3) 0.4744 (4) 0.0705 (8)
H6 0.4343 1.4751 0.5572 0.085*
C7 0.36754 (13) 1.3130 (3) 0.4872 (3) 0.0549 (6)
C8 0.33827 (13) 1.2427 (3) 0.6184 (3) 0.0544 (6)
C9 0.37543 (12) 0.9290 (2) 0.3913 (3) 0.0487 (6)
C10 0.42604 (13) 0.9458 (3) 0.2845 (3) 0.0572 (6)
H10 0.4143 0.9877 0.1944 0.069*
C11 0.49369 (14) 0.9008 (3) 0.3103 (3) 0.0649 (7)
H11 0.5275 0.9128 0.2380 0.078*
C12 0.51118 (14) 0.8386 (3) 0.4422 (3) 0.0627 (7)
H12 0.5569 0.8083 0.4596 0.075*
C13 0.46114 (13) 0.8206 (3) 0.5498 (3) 0.0611 (6)
H13 0.4732 0.7782 0.6395 0.073*
C14 0.39338 (13) 0.8653 (3) 0.5245 (3) 0.0556 (7)
H14 0.3597 0.8526 0.5969 0.067*
C15 0.25151 (13) 0.8676 (2) 0.3667 (3) 0.0515 (6)
C16 0.26525 (14) 0.7304 (3) 0.3021 (4) 0.0699 (8)
H16 0.3089 0.7130 0.2607 0.084*
C17 0.21563 (16) 0.6196 (3) 0.2981 (5) 0.0791 (9)
H17 0.2261 0.5282 0.2547 0.095*
C18 0.15013 (16) 0.6429 (3) 0.3583 (4) 0.0710 (8)
H18 0.1167 0.5675 0.3569 0.085*
C19 0.13553 (17) 0.7796 (4) 0.4199 (4) 0.0743 (8)
H19 0.0912 0.7978 0.4576 0.089*
C20 0.18593 (15) 0.8909 (3) 0.4269 (3) 0.0663 (7)
H20 0.1757 0.9816 0.4721 0.080*
H1 0.2377 (16) 1.155 (3) 0.390 (3) 0.062 (8)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0755 (12) 0.0675 (12) 0.0638 (13) 0.0031 (9) −0.0014 (9) −0.0069 (9)
O2 0.0599 (11) 0.0522 (10) 0.0612 (11) −0.0026 (8) 0.0074 (8) −0.0047 (8)
N1 0.0455 (10) 0.0432 (10) 0.0639 (11) −0.0007 (8) −0.0019 (9) −0.0033 (9)
C1 0.0475 (15) 0.0471 (14) 0.0606 (15) 0.0006 (10) 0.0022 (10) 0.0001 (11)
C2 0.0478 (13) 0.0414 (12) 0.0647 (15) 0.0025 (9) 0.0014 (11) −0.0001 (11)
C3 0.0596 (15) 0.0501 (15) 0.0644 (16) 0.0045 (12) 0.0002 (11) 0.0004 (12)
C4 0.0746 (17) 0.0537 (15) 0.0734 (18) −0.0006 (13) 0.0104 (14) 0.0085 (14)
C5 0.083 (2) 0.0531 (15) 0.093 (2) −0.0173 (14) 0.0150 (16) −0.0035 (15)
C6 0.0754 (18) 0.0539 (15) 0.082 (2) −0.0149 (14) 0.0009 (16) −0.0087 (14)
C7 0.0539 (13) 0.0439 (13) 0.0669 (14) 0.0031 (11) 0.0010 (12) −0.0045 (12)
C8 0.0522 (13) 0.0489 (14) 0.0623 (16) 0.0059 (11) 0.0001 (11) −0.0064 (12)
C9 0.0484 (13) 0.0420 (12) 0.0556 (14) −0.0046 (10) 0.0000 (10) −0.0038 (10)
C10 0.0593 (14) 0.0572 (14) 0.0550 (13) 0.0032 (12) 0.0052 (12) 0.0058 (12)
C11 0.0542 (15) 0.0651 (16) 0.0755 (17) 0.0043 (12) 0.0137 (13) 0.0084 (14)
C12 0.0505 (14) 0.0598 (15) 0.0777 (18) 0.0022 (12) −0.0056 (12) −0.0021 (13)
C13 0.0650 (16) 0.0601 (15) 0.0581 (14) 0.0026 (13) −0.0091 (13) −0.0005 (13)
C14 0.0578 (15) 0.0550 (15) 0.0539 (16) −0.0006 (12) 0.0014 (11) −0.0014 (10)
C15 0.0529 (13) 0.0477 (12) 0.0540 (12) −0.0047 (11) −0.0036 (11) 0.0012 (10)
C16 0.0576 (16) 0.0536 (14) 0.098 (2) −0.0017 (12) −0.0010 (15) −0.0138 (16)
C17 0.074 (2) 0.0509 (15) 0.112 (3) −0.0070 (13) −0.0064 (18) −0.0137 (18)
C18 0.076 (2) 0.0639 (17) 0.0731 (17) −0.0251 (14) −0.0109 (15) 0.0048 (15)
C19 0.0645 (16) 0.087 (2) 0.0717 (17) −0.0225 (15) 0.0127 (14) −0.0074 (16)
C20 0.0624 (17) 0.0656 (16) 0.0709 (16) −0.0131 (13) 0.0122 (13) −0.0122 (14)

Geometric parameters (Å, º)

O1—C8 1.210 (4) C10—C11 1.376 (4)
O2—C8 1.355 (3) C10—H10 0.9300
O2—C1 1.494 (3) C11—C12 1.366 (4)
N1—C15 1.425 (3) C11—H11 0.9300
N1—C1 1.425 (3) C12—C13 1.380 (4)
N1—C9 1.441 (3) C12—H12 0.9300
C1—C2 1.499 (3) C13—C14 1.377 (4)
C1—H1 1.03 (3) C13—H13 0.9300
C2—C7 1.383 (4) C14—H14 0.9300
C2—C3 1.389 (4) C15—C16 1.385 (4)
C3—C4 1.388 (4) C15—C20 1.386 (4)
C3—H3 0.9300 C16—C17 1.372 (4)
C4—C5 1.383 (5) C16—H16 0.9300
C4—H4 0.9300 C17—C18 1.384 (5)
C5—C6 1.371 (5) C17—H17 0.9300
C5—H5 0.9300 C18—C19 1.373 (5)
C6—C7 1.392 (4) C18—H18 0.9300
C6—H6 0.9300 C19—C20 1.387 (4)
C7—C8 1.462 (4) C19—H19 0.9300
C9—C10 1.382 (3) C20—H20 0.9300
C9—C14 1.384 (3)
C8—O2—C1 110.6 (2) C11—C10—C9 120.5 (3)
C15—N1—C1 118.89 (19) C11—C10—H10 119.8
C15—N1—C9 117.15 (18) C9—C10—H10 119.8
C1—N1—C9 115.92 (19) C12—C11—C10 120.0 (2)
N1—C1—O2 111.4 (2) C12—C11—H11 120.0
N1—C1—C2 115.5 (2) C10—C11—H11 120.0
O2—C1—C2 102.75 (19) C11—C12—C13 120.2 (2)
N1—C1—H1 112.2 (15) C11—C12—H12 119.9
O2—C1—H1 102.2 (17) C13—C12—H12 119.9
C2—C1—H1 111.6 (15) C14—C13—C12 120.1 (3)
C7—C2—C3 120.6 (2) C14—C13—H13 120.0
C7—C2—C1 109.2 (2) C12—C13—H13 120.0
C3—C2—C1 130.1 (2) C13—C14—C9 120.0 (2)
C4—C3—C2 117.5 (3) C13—C14—H14 120.0
C4—C3—H3 121.3 C9—C14—H14 120.0
C2—C3—H3 121.3 C16—C15—C20 118.3 (2)
C5—C4—C3 121.7 (3) C16—C15—N1 118.3 (2)
C5—C4—H4 119.2 C20—C15—N1 123.4 (2)
C3—C4—H4 119.2 C17—C16—C15 121.2 (3)
C6—C5—C4 120.9 (3) C17—C16—H16 119.4
C6—C5—H5 119.5 C15—C16—H16 119.4
C4—C5—H5 119.5 C16—C17—C18 120.6 (3)
C5—C6—C7 117.9 (3) C16—C17—H17 119.7
C5—C6—H6 121.0 C18—C17—H17 119.7
C7—C6—H6 121.0 C19—C18—C17 118.7 (3)
C2—C7—C6 121.4 (3) C19—C18—H18 120.7
C2—C7—C8 108.6 (2) C17—C18—H18 120.7
C6—C7—C8 129.9 (3) C18—C19—C20 121.0 (3)
O1—C8—O2 121.7 (2) C18—C19—H19 119.5
O1—C8—C7 129.6 (2) C20—C19—H19 119.5
O2—C8—C7 108.6 (2) C19—C20—C15 120.3 (3)
C10—C9—C14 119.2 (2) C19—C20—H20 119.9
C10—C9—N1 120.3 (2) C15—C20—H20 119.9
C14—C9—N1 120.5 (2)
C15—N1—C1—O2 81.6 (3) C6—C7—C8—O2 176.1 (3)
C9—N1—C1—O2 −66.3 (3) C15—N1—C9—C10 117.8 (2)
C15—N1—C1—C2 −161.6 (2) C1—N1—C9—C10 −93.7 (3)
C9—N1—C1—C2 50.4 (3) C15—N1—C9—C14 −62.7 (3)
C8—O2—C1—N1 121.2 (2) C1—N1—C9—C14 85.9 (3)
C8—O2—C1—C2 −3.1 (3) C14—C9—C10—C11 −0.6 (4)
N1—C1—C2—C7 −119.6 (2) N1—C9—C10—C11 179.0 (2)
O2—C1—C2—C7 2.0 (3) C9—C10—C11—C12 0.2 (4)
N1—C1—C2—C3 63.7 (4) C10—C11—C12—C13 0.0 (4)
O2—C1—C2—C3 −174.8 (3) C11—C12—C13—C14 0.0 (4)
C7—C2—C3—C4 0.7 (4) C12—C13—C14—C9 −0.3 (4)
C1—C2—C3—C4 177.1 (3) C10—C9—C14—C13 0.6 (4)
C2—C3—C4—C5 0.4 (4) N1—C9—C14—C13 −178.9 (2)
C3—C4—C5—C6 −0.9 (5) C1—N1—C15—C16 171.7 (3)
C4—C5—C6—C7 0.4 (5) C9—N1—C15—C16 −40.7 (3)
C3—C2—C7—C6 −1.2 (4) C1—N1—C15—C20 −6.7 (4)
C1—C2—C7—C6 −178.3 (2) C9—N1—C15—C20 140.9 (3)
C3—C2—C7—C8 176.8 (2) C20—C15—C16—C17 −0.4 (5)
C1—C2—C7—C8 −0.3 (3) N1—C15—C16—C17 −178.8 (3)
C5—C6—C7—C2 0.7 (4) C15—C16—C17—C18 0.4 (5)
C5—C6—C7—C8 −176.9 (3) C16—C17—C18—C19 1.0 (5)
C1—O2—C8—O1 −178.2 (2) C17—C18—C19—C20 −2.3 (5)
C1—O2—C8—C7 3.0 (3) C18—C19—C20—C15 2.3 (5)
C2—C7—C8—O1 179.6 (3) C16—C15—C20—C19 −0.9 (4)
C6—C7—C8—O1 −2.6 (5) N1—C15—C20—C19 177.5 (3)
C2—C7—C8—O2 −1.7 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C3—H3···O2i 0.93 2.70 3.413 (3) 135
C1—H1···O1i 1.03 (3) 2.36 (3) 3.307 (3) 153 (2)

Symmetry code: (i) −x+1/2, y, z−1/2.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: TK5299).

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536814006266/tk5299sup1.cif

e-70-0o490-sup1.cif (26.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814006266/tk5299Isup2.hkl

e-70-0o490-Isup2.hkl (83KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814006266/tk5299Isup3.cml

CCDC reference: 992870

Additional supporting information: 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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