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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Mar 10;68(Pt 4):o1008. doi: 10.1107/S1600536812008276

4-[(3-Meth­oxy­anilino)methyl­idene]-2-phenyl-1,3-oxazol-5(4H)-one

Wan-Yun Huang a, Ye Zhang a, Kun Hu b, Qing-Mei Lin b, Xian-Xian Liu a,*
PMCID: PMC3343974  PMID: 22589883

Abstract

In the title compound, C17H14N2O3, the oxazolone ring is essentially planar [maximum deviation = 0.004 (1) Å] and is oriented with respect to the phenyl and benzene rings at 10.06 (9) and 5.63 (8)°, respectively; the dihedral angle between the phenyl ring and the benzene ring is 15.69 (8)°. In the crystal, N—H⋯O hydrogen bonds link the mol­ecules into chains running along the a axis. Neighbouring chains are inter­connected by π–π stacking, the centroid–centroid distance being 3.6201 (9) Å.

Related literature  

For background to the oxazolones, see: Fisk et al. (2007); Mosey et al. (2008); Hewlett et al. (2009). For the bioactivities of 4-(amino­methyl­ene)-2-phenyl-4H-oxazol-5-one derivatives, see: Tandon et al. (2004); John et al. (2008). For the synthesis, see: Matos et al. (2003). For related structures, see: Romeiro et al. (2010); Vasuki et al. (2002).graphic file with name e-68-o1008-scheme1.jpg

Experimental  

Crystal data  

  • C17H14N2O3

  • M r = 294.30

  • Triclinic, Inline graphic

  • a = 6.6085 (5) Å

  • b = 7.1887 (5) Å

  • c = 15.3659 (10) Å

  • α = 98.629 (5)°

  • β = 94.096 (5)°

  • γ = 108.715 (6)°

  • V = 677.96 (8) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 150 K

  • 0.25 × 0.20 × 0.15 mm

Data collection  

  • Agilent SuperNova (single source at offset) Eos diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) T min = 0.975, T max = 0.985

  • 5557 measured reflections

  • 2759 independent reflections

  • 2317 reflections with I > 2σ(I)

  • R int = 0.023

  • Standard reflections: 0

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.043

  • wR(F 2) = 0.118

  • S = 1.02

  • 2759 reflections

  • 204 parameters

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

  • Δρmax = 0.22 e Å−3

  • Δρmin = −0.29 e Å−3

Data collection: CrysAlis PRO (Agilent, 2011); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812008276/xu5464sup1.cif

e-68-o1008-sup1.cif (18.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812008276/xu5464Isup2.hkl

e-68-o1008-Isup2.hkl (135.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812008276/xu5464Isup3.cml

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
N2—H2A⋯O1i 0.92 (2) 2.26 (2) 3.0110 (18) 138.1 (17)

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank the Science Foundation of Guilin Normal College (grant No. 2008), Guilin Scientific Research and Technological Development Projects (grant No. 20110106-2) and Guangxi University Scientific Research Projects (grant No. 200103YB159).

supplementary crystallographic information

Comment

Oxazolones are heterocyclic compounds which serve as a very important role in the synthesis of amino acids, peptides and natural product (Fisk et al., 2007; Mosey et al., 2008; Hewlett et al., 2009). Among them, 4- (aminomethylene)-2-phenyl-4H-oxazol-5-one derivatives show a range of interesting and medicinally relevant bioactivities (Tandon et al., 2004; John et al., 2008). Recently, Romeiro reported the crystal structure of the 4-[(Dimethylamino)methylidene]-2- (4-nitrophenyl)-1,3-oxazol-5(4H)-one (Romeiro et al., 2010). Herein, we wish to report the synthesis and crystal structure of 4-[(3-Methoxy-phenylamino)-methylene]-2- phenyl-4H-oxazol-5-one. The molecule with the Z-configuration (Fig. 1) of the title compound is planar with the maximum deviations from the least-squares plane through all non-hydrogen atoms being 0.292 Å for atom C4 and -0.237 Å for atom C1; the r.m.s. = 0.089 Å. The sequence of C7—N1, N1—C9, C9—C10, C10—N2, and N2—C11 bond distances of 1.2917 (19), 1.407 (2), 1.372 (2), 1.337 (2), and 1.4201 (19) Å, respectively, indicate substantial delocalization of π-electron density over these atoms. The geometric parameters match closely those related structure (Romeiro et al., 2010; Vasuki et al., 2002). The crystal packing is dominated by N—H···O and π-π interactions. An intermolecular N(2)—H(2 A)···O(1) (Symmetry code: x + 1, y, z) hydrogen bond (Table 1) link the molecule into a one-dimensional chain along the a axis (Fig. 2). And the neighbouring chains are interconnected by π-π stacking interactions occurring between oxazolin-5-one and the 3-methoxy-phenyl ring with a centroid-centroid distance of 3.62 Å, which lead to form a two-dimensional network (Fig. 3).

Experimental

A mixture of 4-ethoxymethylene-2-phenyl-4H-oxazol-5-one (Matos et al., 2003) (0.01 mol) and 3-methoxy-phenylamine (0.01 mol) in THF (25 ml) was stirred at room temperature for 4 h. The solvent was then evaporated under reduced pressure and the residue was crystallized from ethyl acetate to give orange crystals suitable for X-ray analysis (yield 82%).

Refinement

Amino-H atom was located in a difference Fourier map and refined isotropically. Other H atoms were placed in calculated positions and refined as riding atoms with C—H = 0.95–0.98 Å, Uiso(H) = 1.2–1.5Ueq(C).

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound showing the atomic labeling scheme with displacement ellipsoids drawn at the 30% probability level.

Fig. 2.

Fig. 2.

A view of the one-dimensional chain along a axis sustained by N(2)—H(2 A)···O(1)(i) ((i) x + 1, y, z) hydrogen bond (shown as dashed lines).

Fig. 3.

Fig. 3.

View of the two-dimensional network constructed by hydrogen bond and π-π interactions shown as green and purple dashed lines respectively.

Crystal data

C17H14N2O3 Z = 2
Mr = 294.30 F(000) = 308
Triclinic, P1 Dx = 1.442 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 6.6085 (5) Å Cell parameters from 2524 reflections
b = 7.1887 (5) Å θ = 3.0–28.7°
c = 15.3659 (10) Å µ = 0.10 mm1
α = 98.629 (5)° T = 150 K
β = 94.096 (5)° Block, green
γ = 108.715 (6)° 0.25 × 0.20 × 0.15 mm
V = 677.96 (8) Å3

Data collection

Agilent SuperNova (single source at offset) Eos diffractometer 2759 independent reflections
Radiation source: fine-focus sealed tube 2317 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.023
ω scans θmax = 26.4°, θmin = 3.0°
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) h = −8→8
Tmin = 0.975, Tmax = 0.985 k = −8→8
5557 measured reflections l = −19→19

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)] = 0.043 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118 H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.060P)2 + 0.1704P] where P = (Fo2 + 2Fc2)/3
2759 reflections (Δ/σ)max < 0.001
204 parameters Δρmax = 0.22 e Å3
0 restraints Δρmin = −0.29 e Å3

Special details

Experimental. 1H NMR (DMSO, 500 MHz) δ: 10.70 (d, 1H, NH), 7.97–8.05 (m, 3H, Ar—H), 7.55–7.57(m, 3H, Ar—H), 7.25 (t, 1H, Ar—H), 7.10–7.14 (m, 2H, Ar—H), 6.67 (q, 1H, Ar—H), 3.78 (s, 3H, CH3). 13C NMR (DMSO, 125.77 MHz) δ: 167.11, 160.27, 154.44, 141.21, 135.31, 131.34, 130.28, 129.09, 126.55, 126.40, 125.82, 111.06, 109.81, 109.29, 102.70, 55.23.
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 0.2537 (3) 0.6133 (3) 0.85604 (11) 0.0242 (4)
H1 0.3396 0.5732 0.8151 0.029*
C2 0.3478 (3) 0.7213 (3) 0.93963 (11) 0.0311 (4)
H2 0.4981 0.7544 0.9562 0.037*
C3 0.2225 (3) 0.7811 (3) 0.99922 (11) 0.0318 (4)
H3 0.2876 0.8552 1.0565 0.038*
C4 0.0043 (3) 0.7337 (3) 0.97570 (11) 0.0297 (4)
H4 −0.0803 0.7762 1.0165 0.036*
C5 −0.0917 (3) 0.6238 (3) 0.89242 (11) 0.0243 (4)
H5 −0.2425 0.5895 0.8766 0.029*
C6 0.0327 (2) 0.5636 (2) 0.83184 (10) 0.0189 (3)
C7 −0.0642 (2) 0.4518 (2) 0.74310 (10) 0.0176 (3)
C8 −0.3384 (3) 0.2824 (2) 0.63810 (10) 0.0192 (3)
C9 −0.1337 (2) 0.3036 (2) 0.60730 (10) 0.0177 (3)
C10 −0.1006 (2) 0.2327 (2) 0.52347 (10) 0.0177 (3)
H10 −0.2216 0.1660 0.4796 0.021*
C11 0.1565 (3) 0.2043 (2) 0.41664 (9) 0.0179 (3)
C12 0.3751 (3) 0.2674 (2) 0.40875 (10) 0.0194 (3)
H12 0.4774 0.3409 0.4588 0.023*
C13 0.4433 (3) 0.2222 (2) 0.32722 (10) 0.0214 (4)
H13 0.5925 0.2669 0.3213 0.026*
C14 0.2950 (3) 0.1127 (2) 0.25468 (10) 0.0220 (4)
H14 0.3422 0.0818 0.1991 0.026*
C15 0.0758 (3) 0.0477 (2) 0.26330 (10) 0.0184 (3)
C16 0.0038 (2) 0.0943 (2) 0.34428 (10) 0.0184 (3)
H16 −0.1457 0.0522 0.3499 0.022*
C17 −0.2821 (3) −0.1308 (3) 0.19348 (11) 0.0292 (4)
H17A −0.3122 −0.2117 0.2400 0.044*
H17B −0.3592 −0.2118 0.1364 0.044*
H17C −0.3300 −0.0154 0.2077 0.044*
N1 0.0328 (2) 0.41031 (19) 0.67659 (8) 0.0183 (3)
N2 0.0970 (2) 0.2548 (2) 0.50167 (9) 0.0194 (3)
O1 −0.52599 (17) 0.20389 (18) 0.60520 (7) 0.0254 (3)
O2 −0.28635 (16) 0.38163 (16) 0.72695 (7) 0.0195 (3)
O3 −0.05667 (17) −0.06328 (17) 0.18811 (7) 0.0235 (3)
H2A 0.211 (3) 0.304 (3) 0.5461 (13) 0.036 (5)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0235 (9) 0.0242 (9) 0.0223 (8) 0.0044 (7) 0.0045 (7) 0.0031 (7)
C2 0.0262 (9) 0.0315 (10) 0.0271 (9) 0.0013 (8) −0.0029 (7) 0.0013 (8)
C3 0.0432 (11) 0.0260 (10) 0.0179 (8) 0.0048 (8) −0.0032 (8) −0.0026 (7)
C4 0.0415 (11) 0.0292 (10) 0.0195 (8) 0.0148 (8) 0.0068 (8) 0.0006 (7)
C5 0.0278 (9) 0.0256 (9) 0.0211 (8) 0.0117 (7) 0.0037 (7) 0.0033 (7)
C6 0.0229 (8) 0.0160 (8) 0.0172 (8) 0.0054 (6) 0.0026 (6) 0.0043 (6)
C7 0.0183 (8) 0.0166 (8) 0.0189 (8) 0.0063 (6) 0.0037 (6) 0.0046 (6)
C8 0.0226 (9) 0.0213 (8) 0.0153 (7) 0.0096 (7) 0.0034 (6) 0.0030 (6)
C9 0.0182 (8) 0.0186 (8) 0.0167 (7) 0.0066 (6) 0.0029 (6) 0.0034 (6)
C10 0.0190 (8) 0.0176 (8) 0.0174 (7) 0.0074 (6) 0.0016 (6) 0.0031 (6)
C11 0.0244 (8) 0.0161 (8) 0.0161 (8) 0.0098 (6) 0.0053 (6) 0.0038 (6)
C12 0.0200 (8) 0.0185 (8) 0.0188 (8) 0.0061 (6) 0.0022 (6) 0.0018 (6)
C13 0.0199 (8) 0.0222 (9) 0.0233 (8) 0.0076 (7) 0.0070 (7) 0.0047 (7)
C14 0.0247 (9) 0.0258 (9) 0.0178 (8) 0.0106 (7) 0.0086 (7) 0.0035 (7)
C15 0.0225 (8) 0.0172 (8) 0.0163 (7) 0.0075 (6) 0.0022 (6) 0.0034 (6)
C16 0.0176 (8) 0.0200 (8) 0.0201 (8) 0.0085 (6) 0.0056 (6) 0.0052 (6)
C17 0.0196 (9) 0.0384 (11) 0.0251 (9) 0.0087 (8) 0.0001 (7) −0.0043 (7)
N1 0.0184 (7) 0.0196 (7) 0.0170 (6) 0.0064 (5) 0.0037 (5) 0.0028 (5)
N2 0.0170 (7) 0.0246 (8) 0.0156 (7) 0.0073 (6) 0.0025 (5) 0.0001 (5)
O1 0.0177 (6) 0.0362 (7) 0.0209 (6) 0.0083 (5) 0.0005 (5) 0.0030 (5)
O2 0.0157 (6) 0.0264 (6) 0.0151 (5) 0.0068 (5) 0.0031 (4) −0.0003 (4)
O3 0.0217 (6) 0.0296 (7) 0.0158 (6) 0.0059 (5) 0.0027 (5) −0.0002 (5)

Geometric parameters (Å, º)

C1—C2 1.384 (2) C10—N2 1.337 (2)
C1—C6 1.395 (2) C10—H10 0.9500
C1—H1 0.9500 C11—C12 1.389 (2)
C2—C3 1.388 (3) C11—C16 1.394 (2)
C2—H2 0.9500 C11—N2 1.4201 (19)
C3—C4 1.378 (3) C12—C13 1.389 (2)
C3—H3 0.9500 C12—H12 0.9500
C4—C5 1.387 (2) C13—C14 1.381 (2)
C4—H4 0.9500 C13—H13 0.9500
C5—C6 1.396 (2) C14—C15 1.395 (2)
C5—H5 0.9500 C14—H14 0.9500
C6—C7 1.460 (2) C15—O3 1.3670 (19)
C7—N1 1.2917 (19) C15—C16 1.396 (2)
C7—O2 1.3810 (18) C16—H16 0.9500
C8—O1 1.2191 (19) C17—O3 1.4237 (19)
C8—O2 1.4051 (18) C17—H17A 0.9800
C8—C9 1.435 (2) C17—H17B 0.9800
C9—C10 1.372 (2) C17—H17C 0.9800
C9—N1 1.407 (2) N2—H2A 0.92 (2)
C2—C1—C6 120.00 (16) C12—C11—C16 121.14 (14)
C2—C1—H1 120.0 C12—C11—N2 116.95 (14)
C6—C1—H1 120.0 C16—C11—N2 121.90 (14)
C1—C2—C3 120.03 (17) C13—C12—C11 119.60 (15)
C1—C2—H2 120.0 C13—C12—H12 120.2
C3—C2—H2 120.0 C11—C12—H12 120.2
C4—C3—C2 120.38 (16) C14—C13—C12 120.30 (15)
C4—C3—H3 119.8 C14—C13—H13 119.8
C2—C3—H3 119.8 C12—C13—H13 119.8
C3—C4—C5 120.01 (16) C13—C14—C15 119.82 (14)
C3—C4—H4 120.0 C13—C14—H14 120.1
C5—C4—H4 120.0 C15—C14—H14 120.1
C4—C5—C6 120.10 (16) O3—C15—C14 115.12 (13)
C4—C5—H5 119.9 O3—C15—C16 124.11 (14)
C6—C5—H5 119.9 C14—C15—C16 120.77 (15)
C1—C6—C5 119.48 (15) C11—C16—C15 118.35 (14)
C1—C6—C7 119.49 (14) C11—C16—H16 120.8
C5—C6—C7 121.03 (15) C15—C16—H16 120.8
N1—C7—O2 115.14 (13) O3—C17—H17A 109.5
N1—C7—C6 127.89 (14) O3—C17—H17B 109.5
O2—C7—C6 116.97 (13) H17A—C17—H17B 109.5
O1—C8—O2 120.54 (14) O3—C17—H17C 109.5
O1—C8—C9 135.12 (15) H17A—C17—H17C 109.5
O2—C8—C9 104.33 (13) H17B—C17—H17C 109.5
C10—C9—N1 124.09 (14) C7—N1—C9 104.91 (13)
C10—C9—C8 126.24 (15) C10—N2—C11 128.04 (14)
N1—C9—C8 109.67 (13) C10—N2—H2A 118.3 (12)
N2—C10—C9 121.89 (15) C11—N2—H2A 113.6 (13)
N2—C10—H10 119.1 C7—O2—C8 105.95 (11)
C9—C10—H10 119.1 C15—O3—C17 117.09 (12)
C6—C1—C2—C3 −0.4 (3) C12—C13—C14—C15 0.2 (2)
C1—C2—C3—C4 0.0 (3) C13—C14—C15—O3 −178.56 (13)
C2—C3—C4—C5 0.6 (3) C13—C14—C15—C16 0.9 (2)
C3—C4—C5—C6 −0.9 (3) C12—C11—C16—C15 0.4 (2)
C2—C1—C6—C5 0.1 (2) N2—C11—C16—C15 −178.82 (13)
C2—C1—C6—C7 179.27 (15) O3—C15—C16—C11 178.24 (13)
C4—C5—C6—C1 0.5 (2) C14—C15—C16—C11 −1.2 (2)
C4—C5—C6—C7 −178.59 (14) O2—C7—N1—C9 0.53 (17)
C1—C6—C7—N1 −9.5 (2) C6—C7—N1—C9 −179.07 (14)
C5—C6—C7—N1 169.59 (15) C10—C9—N1—C7 179.11 (14)
C1—C6—C7—O2 170.88 (13) C8—C9—N1—C7 −0.69 (16)
C5—C6—C7—O2 −10.0 (2) C9—C10—N2—C11 −174.39 (14)
O1—C8—C9—C10 0.7 (3) C12—C11—N2—C10 171.24 (15)
O2—C8—C9—C10 −179.20 (14) C16—C11—N2—C10 −9.5 (2)
O1—C8—C9—N1 −179.47 (17) N1—C7—O2—C8 −0.17 (17)
O2—C8—C9—N1 0.59 (16) C6—C7—O2—C8 179.48 (12)
N1—C9—C10—N2 2.3 (2) O1—C8—O2—C7 179.78 (14)
C8—C9—C10—N2 −177.99 (14) C9—C8—O2—C7 −0.27 (15)
C16—C11—C12—C13 0.7 (2) C14—C15—O3—C17 −179.23 (14)
N2—C11—C12—C13 179.92 (14) C16—C15—O3—C17 1.3 (2)
C11—C12—C13—C14 −1.0 (2)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N2—H2A···O1i 0.92 (2) 2.26 (2) 3.0110 (18) 138.1 (17)

Symmetry code: (i) x+1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5464).

References

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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) global, I. DOI: 10.1107/S1600536812008276/xu5464sup1.cif

e-68-o1008-sup1.cif (18.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812008276/xu5464Isup2.hkl

e-68-o1008-Isup2.hkl (135.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812008276/xu5464Isup3.cml

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


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