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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Jul 25;65(Pt 8):o2002. doi: 10.1107/S1600536809028992

(2R)-2-(1,3-Dioxoisoindolin-2-yl)-4-(methyl­sulfan­yl)butanoic acid

Abdul Rauf Raza a, M Nawaz Tahir b,*, Aisha Saddiqa a, Muhammad Danish a, M Saeed Iqbal c
PMCID: PMC2977145  PMID: 21583673

Abstract

The title compound, C13H13NO4S, the 1,3-dioxoisoindolin-2-yl unit is planar (r.m.s. deviation 0.0192 Å) and is oriented at a dihedral angle of 79.14 (18)° to the carboxyl­ate group. An intra­molecular C—H⋯O hydrogen bond leads to the formation of a planar (r.m.s. deviation 0.0419 Å)R(5) ring motif. In the crystal, mol­ecules are connected through O—H⋯O and C—H⋯O hydrogen bonds with R 2 2(9) ring motifs into chains extending along the b axis.

Related literature

For the biological activity of isocoumarin and 3,4-dihydro­isocoumarin, see: Hill (1986); Canedo et al. (1997); Whyte et al. (1996). For related structures, see: Barooah et al. (2007); Feeder & Jones (1994); Rajagopal et al. (2003). For graph-set motifs, see: Bernstein et al. (1995).graphic file with name e-65-o2002-scheme1.jpg

Experimental

Crystal data

  • C13H13NO4S

  • M r = 279.30

  • Orthorhombic, Inline graphic

  • a = 6.7923 (6) Å

  • b = 9.9581 (8) Å

  • c = 20.0970 (17) Å

  • V = 1359.3 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.25 mm−1

  • T = 296 K

  • 0.20 × 0.14 × 0.10 mm

Data collection

  • Bruker Kappa APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2005) T min = 0.969, T max = 0.985

  • 7865 measured reflections

  • 1864 independent reflections

  • 1679 reflections with I > 2σ(I)

  • R int = 0.024

Refinement

  • R[F 2 > 2σ(F 2)] = 0.036

  • wR(F 2) = 0.098

  • S = 1.06

  • 1864 reflections

  • 179 parameters

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

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.33 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; 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, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: WinGX (Farrugia, 1999) and PLATON.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809028992/pb2001sup1.cif

e-65-o2002-sup1.cif (19.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028992/pb2001Isup2.hkl

e-65-o2002-Isup2.hkl (89.9KB, 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
O1—H1⋯O3i 0.77 (3) 1.96 (3) 2.673 (3) 154 (3)
C3—H3⋯O2ii 0.9300 2.4200 3.328 (4) 165.00
C9—H9⋯O4 0.96 (3) 2.48 (3) 2.905 (3) 106.4 (18)
C11—H11B⋯O1iii 0.9700 2.5400 3.443 (3) 156.00

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

Acknowledgments

The authors acknowledge the Higher Education Commission, Islamabad, Pakistan, and Bana International, Karachi, Pakistan, for funding the purchase of the diffractometer at GCU, Lahore, and for technical support, respectively.

supplementary crystallographic information

Comment

Isocoumarin and 3,4-dihydroisocoumarin have shown an impressive array of biological activities such as anti-tumor (Hill et al., 1986), anti-leucemic (Canedo et al., 1997) and anti-microbial (Whyte et al., 1996). The titled compound (I, Fig. 1) is an intermediate towards the synthesis of chiral isocoumarin. The biological activity of the title compound and synthesis of its complexes are in progress.

The crystal structures of 2-Phthalimidoethanoic acid monohydrate (Feeder & Jones, 1994), N-Phthaloylglycine (Barooah et al., 2007) and DL-Methioninium trichloroacetate (Rajagopal et al., 2003) have been published which contain the moieties of the title compound.

In the title compound the aromatic ring and heterocyclic ring along with O-atoms of carbonyl groups A (C1—C8/N1/O3/O4), the linear chain B (C9—C11/S1/C12) and the carboxylate group C (O1/C13/O2) are planar. There exists an intramolecular H-bond of type C—H···O completing a planar S(5) ring motif (Bernstein et al., 1995). The value of dihedral angle between A/B, A/C and B/C is 80.04 (7)°, 79.14 (18)° and 20.54 (30)°, respectively. Due to the intermolecular H-bonding (Table 1), the molecules are connected in one dimensional polymeric chains through ring motifs R22(9) extending along the b-axis.

Experimental

The methionine (2.0 g, 13.4 mmol) and phthalic anhydride (2.13 g, 14.38 mmol) were added to a flask with constant stirring at 423 K for 2 h. The reaction mixture was brought to room temperature and the crystalline phthallic anhydride on the walls of the flask were removed. The solid crude product was purified by crystallization from ethanol/water (7:3) that afforded colorless prisms of the title compound (I).

Yield 81%.

Refinement

All the Friedal pairs were merged.

H atoms (for hydroxy and methine) were located in a difference Fourier map and their coordinates were refined. The remaining H atoms were positioned geometrically with C-H = 0.93, 0.97 and 0.96 Å for aromatic, methylene and methyl H atoms, respectively and constrained to ride on their parent atoms, with Uiso(H) = xUeq(C,O), where x = 1.5 for methyl H and x = 1.2 for all other H atoms.

Figures

Fig. 1.

Fig. 1.

View of the title compound with the atom numbering scheme. The thermal ellipsoids are drawn at the 50% probability level. H-atoms are shown by small circles of arbitrary radii. The dotted line indicate the intramolecular H-bond.

Fig. 2.

Fig. 2.

The partial packing (PLATON; Spek, 2009) which shows that molecules form polymeric chains extending along the b-axis.

Crystal data

C13H13NO4S F(000) = 584
Mr = 279.30 Dx = 1.365 Mg m3
Orthorhombic, P212121 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2ab Cell parameters from 1864 reflections
a = 6.7923 (6) Å θ = 2.3–28.0°
b = 9.9581 (8) Å µ = 0.25 mm1
c = 20.0970 (17) Å T = 296 K
V = 1359.3 (2) Å3 Prismatic, colorless
Z = 4 0.20 × 0.14 × 0.10 mm

Data collection

Bruker Kappa APEXII CCD diffractometer 1864 independent reflections
Radiation source: fine-focus sealed tube 1679 reflections with I > 2σ(I)
graphite Rint = 0.024
Detector resolution: 7.50 pixels mm-1 θmax = 28.0°, θmin = 2.3°
ω scans h = −8→8
Absorption correction: multi-scan (SADABS; Bruker, 2005) k = −12→7
Tmin = 0.969, Tmax = 0.985 l = −23→26
7865 measured reflections

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)] = 0.036 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.098 H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.057P)2 + 0.2154P] where P = (Fo2 + 2Fc2)/3
1864 reflections (Δ/σ)max < 0.001
179 parameters Δρmax = 0.20 e Å3
0 restraints Δρmin = −0.33 e Å3

Special details

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell esds are taken into account in the estimation of distances, angles and torsion angles
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
S1 −0.16661 (11) 0.67441 (7) 0.42200 (3) 0.0592 (2)
O1 0.3364 (3) 0.2322 (2) 0.26744 (9) 0.0561 (6)
O2 0.3978 (3) 0.3163 (2) 0.36803 (8) 0.0651 (7)
O3 0.3730 (2) 0.55141 (18) 0.23747 (8) 0.0475 (5)
O4 −0.2132 (3) 0.3346 (2) 0.21563 (10) 0.0656 (7)
N1 0.0832 (3) 0.43417 (17) 0.24261 (8) 0.0355 (5)
C1 0.2192 (3) 0.5168 (2) 0.21199 (11) 0.0361 (6)
C2 0.1381 (4) 0.5487 (2) 0.14518 (10) 0.0390 (6)
C3 0.2158 (5) 0.6255 (3) 0.09427 (12) 0.0543 (8)
C4 0.1055 (5) 0.6347 (3) 0.03591 (13) 0.0638 (9)
C5 −0.0735 (6) 0.5715 (3) 0.03025 (14) 0.0668 (9)
C6 −0.1514 (5) 0.4944 (3) 0.08144 (13) 0.0594 (8)
C7 −0.0415 (4) 0.4844 (2) 0.13909 (11) 0.0430 (6)
C8 −0.0790 (3) 0.4072 (2) 0.20120 (11) 0.0422 (7)
C9 0.1029 (3) 0.3829 (2) 0.31004 (10) 0.0358 (6)
C10 0.0710 (3) 0.4911 (2) 0.36262 (11) 0.0423 (6)
C11 −0.1370 (4) 0.5462 (3) 0.36027 (11) 0.0465 (7)
C12 −0.4193 (6) 0.7176 (4) 0.40992 (18) 0.0927 (14)
C13 0.2982 (3) 0.3089 (2) 0.31883 (11) 0.0412 (6)
H1 0.435 (5) 0.196 (3) 0.2742 (16) 0.0673*
H3 0.33622 0.66910 0.09873 0.0652*
H4 0.15390 0.68438 0.00030 0.0764*
H5 −0.14459 0.58059 −0.00904 0.0801*
H6 −0.27220 0.45141 0.07712 0.0713*
H9 0.002 (4) 0.316 (3) 0.3151 (12) 0.0430*
H10A 0.09595 0.45360 0.40636 0.0507*
H10B 0.16374 0.56373 0.35543 0.0507*
H11A −0.23038 0.47436 0.36834 0.0558*
H11B −0.16321 0.58325 0.31651 0.0558*
H12A −0.43704 0.75226 0.36576 0.1385*
H12B −0.45705 0.78452 0.44181 0.1385*
H12C −0.49950 0.63905 0.41568 0.1385*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0668 (4) 0.0560 (3) 0.0549 (4) 0.0046 (3) 0.0121 (3) −0.0137 (3)
O1 0.0542 (10) 0.0646 (11) 0.0494 (10) 0.0238 (9) −0.0114 (9) −0.0182 (9)
O2 0.0685 (11) 0.0852 (14) 0.0417 (9) 0.0298 (11) −0.0157 (8) −0.0100 (9)
O3 0.0448 (8) 0.0545 (9) 0.0432 (9) −0.0130 (8) −0.0076 (7) 0.0070 (7)
O4 0.0510 (10) 0.0801 (13) 0.0656 (12) −0.0252 (10) −0.0100 (9) 0.0065 (11)
N1 0.0360 (8) 0.0381 (8) 0.0323 (8) −0.0015 (8) −0.0004 (7) 0.0012 (7)
C1 0.0399 (10) 0.0326 (9) 0.0359 (10) 0.0005 (8) 0.0000 (8) −0.0018 (8)
C2 0.0508 (12) 0.0346 (9) 0.0315 (10) 0.0027 (9) −0.0023 (9) −0.0029 (8)
C3 0.0728 (17) 0.0508 (12) 0.0394 (12) −0.0090 (12) −0.0011 (12) 0.0059 (10)
C4 0.097 (2) 0.0591 (14) 0.0353 (12) −0.0061 (16) −0.0088 (14) 0.0057 (11)
C5 0.100 (2) 0.0601 (15) 0.0404 (13) 0.0027 (17) −0.0261 (15) 0.0002 (12)
C6 0.0686 (16) 0.0573 (13) 0.0524 (14) −0.0024 (14) −0.0235 (14) −0.0051 (12)
C7 0.0502 (12) 0.0398 (10) 0.0391 (11) 0.0021 (10) −0.0066 (10) −0.0046 (9)
C8 0.0398 (11) 0.0440 (11) 0.0427 (12) −0.0016 (9) −0.0058 (9) −0.0035 (9)
C9 0.0382 (10) 0.0369 (10) 0.0324 (10) 0.0002 (9) 0.0022 (8) 0.0020 (8)
C10 0.0460 (12) 0.0467 (11) 0.0342 (10) 0.0049 (10) 0.0008 (9) −0.0039 (9)
C11 0.0494 (12) 0.0517 (12) 0.0383 (11) 0.0096 (11) 0.0036 (10) −0.0045 (10)
C12 0.089 (2) 0.111 (3) 0.078 (2) 0.053 (2) 0.0201 (19) −0.001 (2)
C13 0.0466 (11) 0.0424 (10) 0.0347 (10) 0.0074 (10) 0.0002 (9) 0.0013 (9)

Geometric parameters (Å, °)

S1—C11 1.792 (3) C7—C8 1.488 (3)
S1—C12 1.786 (4) C9—C13 1.528 (3)
O1—C13 1.311 (3) C9—C10 1.525 (3)
O2—C13 1.200 (3) C10—C11 1.516 (3)
O3—C1 1.213 (3) C3—H3 0.9300
O4—C8 1.199 (3) C4—H4 0.9300
O1—H1 0.77 (3) C5—H5 0.9300
N1—C8 1.407 (3) C6—H6 0.9300
N1—C9 1.454 (3) C9—H9 0.96 (3)
N1—C1 1.382 (3) C10—H10A 0.9700
C1—C2 1.486 (3) C10—H10B 0.9700
C2—C7 1.383 (4) C11—H11A 0.9700
C2—C3 1.382 (3) C11—H11B 0.9700
C3—C4 1.395 (4) C12—H12A 0.9600
C4—C5 1.374 (5) C12—H12B 0.9600
C5—C6 1.389 (4) C12—H12C 0.9600
C6—C7 1.382 (4)
S1···C7i 3.610 (2) C10···O3 3.301 (3)
S1···H5ii 3.1600 C11···C8 3.506 (3)
S1···H12Biii 3.1100 C13···O3 2.960 (3)
O1···N1 2.693 (3) C1···H1vi 2.96 (3)
O1···C1 3.148 (3) C1···H10B 2.9400
O1···O3iv 2.673 (3) C2···H9i 2.94 (3)
O2···C4v 3.409 (3) C3···H9i 3.02 (3)
O2···C3iv 3.328 (4) C8···H11B 2.9600
O3···C13 2.960 (3) H1···O3iv 1.96 (3)
O3···C10 3.301 (3) H1···C1iv 2.96 (3)
O3···O4i 3.165 (3) H3···O2vi 2.4200
O3···O1vi 2.673 (3) H4···O2viii 2.6800
O4···O3vii 3.165 (3) H5···S1ix 3.1600
O1···H12Avii 2.7700 H6···H12Bx 2.5100
O1···H11Bvii 2.5400 H9···O4 2.48 (3)
O2···H3iv 2.4200 H9···H11A 2.4700
O2···H10A 2.5800 H9···C2vii 2.94 (3)
O2···H4v 2.6800 H9···C3vii 3.02 (3)
O3···H10B 2.7700 H10A···O2 2.5800
O3···H1vi 1.96 (3) H10B···O3 2.7700
O4···H9 2.48 (3) H10B···C1 2.9400
N1···O1 2.693 (3) H11A···H9 2.4700
N1···H11B 2.6900 H11B···N1 2.6900
C1···O1 3.148 (3) H11B···C8 2.9600
C3···O2vi 3.328 (4) H11B···O1i 2.5400
C4···O2viii 3.409 (3) H12A···O1i 2.7700
C7···S1vii 3.610 (2) H12B···S1xi 3.1100
C8···C11 3.506 (3) H12B···H6xii 2.5100
C11—S1—C12 100.68 (15) O1—C13—O2 125.0 (2)
C13—O1—H1 108 (2) C2—C3—H3 122.00
C1—N1—C8 111.95 (17) C4—C3—H3 122.00
C1—N1—C9 124.23 (18) C3—C4—H4 119.00
C8—N1—C9 123.80 (18) C5—C4—H4 120.00
O3—C1—N1 123.8 (2) C4—C5—H5 119.00
O3—C1—C2 129.8 (2) C6—C5—H5 119.00
N1—C1—C2 106.38 (18) C5—C6—H6 121.00
C1—C2—C7 107.94 (18) C7—C6—H6 121.00
C3—C2—C7 121.8 (2) N1—C9—H9 106.0 (15)
C1—C2—C3 130.2 (2) C10—C9—H9 108.4 (16)
C2—C3—C4 117.0 (3) C13—C9—H9 105.8 (17)
C3—C4—C5 121.0 (3) C9—C10—H10A 109.00
C4—C5—C6 122.0 (3) C9—C10—H10B 109.00
C5—C6—C7 117.1 (3) C11—C10—H10A 109.00
C2—C7—C8 108.42 (19) C11—C10—H10B 109.00
C6—C7—C8 130.4 (2) H10A—C10—H10B 108.00
C2—C7—C6 121.2 (2) S1—C11—H11A 110.00
O4—C8—N1 124.6 (2) S1—C11—H11B 110.00
N1—C8—C7 105.28 (18) C10—C11—H11A 110.00
O4—C8—C7 130.1 (2) C10—C11—H11B 110.00
N1—C9—C10 112.62 (16) H11A—C11—H11B 108.00
C10—C9—C13 112.59 (17) S1—C12—H12A 109.00
N1—C9—C13 110.92 (17) S1—C12—H12B 109.00
C9—C10—C11 111.50 (18) S1—C12—H12C 109.00
S1—C11—C10 109.93 (17) H12A—C12—H12B 110.00
O1—C13—C9 111.22 (18) H12A—C12—H12C 109.00
O2—C13—C9 123.7 (2) H12B—C12—H12C 109.00
C12—S1—C11—C10 −178.69 (19) C1—C2—C7—C8 −1.1 (2)
C8—N1—C1—O3 −178.4 (2) C3—C2—C7—C6 0.0 (4)
C8—N1—C1—C2 1.0 (2) C3—C2—C7—C8 178.1 (2)
C9—N1—C1—O3 2.7 (3) C2—C3—C4—C5 1.0 (4)
C9—N1—C1—C2 −177.97 (18) C3—C4—C5—C6 −1.0 (5)
C1—N1—C8—O4 177.4 (2) C4—C5—C6—C7 0.5 (5)
C1—N1—C8—C7 −1.6 (2) C5—C6—C7—C2 0.0 (4)
C9—N1—C8—O4 −3.6 (3) C5—C6—C7—C8 −177.6 (3)
C9—N1—C8—C7 177.32 (18) C2—C7—C8—O4 −177.3 (2)
C1—N1—C9—C10 72.2 (2) C2—C7—C8—N1 1.7 (2)
C1—N1—C9—C13 −55.0 (2) C6—C7—C8—O4 0.6 (4)
C8—N1—C9—C10 −106.6 (2) C6—C7—C8—N1 179.6 (3)
C8—N1—C9—C13 126.1 (2) N1—C9—C10—C11 63.5 (2)
O3—C1—C2—C3 0.3 (4) C13—C9—C10—C11 −170.15 (18)
O3—C1—C2—C7 179.4 (2) N1—C9—C13—O1 −42.6 (2)
N1—C1—C2—C3 −179.0 (2) N1—C9—C13—O2 140.5 (2)
N1—C1—C2—C7 0.2 (2) C10—C9—C13—O1 −169.85 (18)
C1—C2—C3—C4 178.6 (2) C10—C9—C13—O2 13.3 (3)
C7—C2—C3—C4 −0.5 (4) C9—C10—C11—S1 −179.19 (15)
C1—C2—C7—C6 −179.3 (2)

Symmetry codes: (i) −x, y+1/2, −z+1/2; (ii) −x−1/2, −y+1, z+1/2; (iii) x+1/2, −y+3/2, −z+1; (iv) −x+1, y−1/2, −z+1/2; (v) −x+1/2, −y+1, z+1/2; (vi) −x+1, y+1/2, −z+1/2; (vii) −x, y−1/2, −z+1/2; (viii) −x+1/2, −y+1, z−1/2; (ix) −x−1/2, −y+1, z−1/2; (x) −x−1, y−1/2, −z+1/2; (xi) x−1/2, −y+3/2, −z+1; (xii) −x−1, y+1/2, −z+1/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H1···O3iv 0.77 (3) 1.96 (3) 2.673 (3) 154 (3)
C3—H3···O2vi 0.9300 2.4200 3.328 (4) 165.00
C9—H9···O4 0.96 (3) 2.48 (3) 2.905 (3) 106.4 (18)
C11—H11B···O1i 0.9700 2.5400 3.443 (3) 156.00

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PB2001).

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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 datablocks global, I. DOI: 10.1107/S1600536809028992/pb2001sup1.cif

e-65-o2002-sup1.cif (19.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028992/pb2001Isup2.hkl

e-65-o2002-Isup2.hkl (89.9KB, hkl)

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


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