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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Jul 4;65(Pt 8):o1742–o1743. doi: 10.1107/S1600536809024210

Methyl 3-[(1-adamantylcarbon­yloxy)amino­carbon­yl]propanoate

Joe Liu a, Jack K Clegg b, Rachel Codd a,*
PMCID: PMC2977356  PMID: 21583454

Abstract

In the title compound, C16H23NO5, the H—N—O—C torsion angle is 98.6 (1)°, which is of a similar magnitude to other N,O-diacyl­hydroxy­lamines. The N—O distance is 1.4029 (14) Å, which is similar to the N—O distance in other N,O-diacyl­hydroxy­lamines. In the crystal, intermolecular N—H⋯O hydrogen bonds generate chains of molecules.

Related literature

For the biological activity of compounds related to N,O-diacyl­hydroxy­lamines, see: Pelto & Pratt (2008). For linear N,O-diacyl­hydroxy­lamines, see: Göttlicher & Ochsenreiter (1974); Schraml et al. (2004); Baert et al. (1984); Masui et al. (1983); Grassi et al. (2002); Buscemi et al. (2006). For cyclic N,O-diacyl­hydroxy­lamines, see: Kongprakaiwoot et al. (2008). For a precursor of the title compound, see: Liu et al. (2009).graphic file with name e-65-o1742-scheme1.jpg

Experimental

Crystal data

  • C16H23NO5

  • M r = 309.35

  • Orthorhombic, Inline graphic

  • a = 15.7837 (5) Å

  • b = 21.0715 (7) Å

  • c = 9.5341 (3) Å

  • V = 3170.91 (18) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 150 K

  • 0.30 × 0.20 × 0.15 mm

Data collection

  • Bruker APEXII-FR591 diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2007) T min = 0.851, T max = 0.981

  • 22952 measured reflections

  • 4586 independent reflections

  • 2890 reflections with I > 2σ(I)

  • R int = 0.036

Refinement

  • R[F 2 > 2σ(F 2)] = 0.048

  • wR(F 2) = 0.132

  • S = 1.04

  • 4586 reflections

  • 200 parameters

  • H-atom parameters constrained

  • Δρmax = 0.25 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: APEX2 (Bruker, 2003); cell refinement: SAINT (Bruker, 2003); data reduction: SAINT and XPREP (Bruker, 2003); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997), WinGX32 (Farrugia, 1999), POV-RAY (Cason, 2002) and WebLab ViewerPro (Molecular Simulations, 2000); software used to prepare material for publication: enCIFer (Allen et al., 2004).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809024210/bg2266sup1.cif

e-65-o1742-sup1.cif (20.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809024210/bg2266Isup2.hkl

e-65-o1742-Isup2.hkl (224.8KB, 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
N1—H1⋯O3i 0.88 1.87 2.7250 (19) 165

Symmetry code: (i) Inline graphic.

Acknowledgments

Support from the NHMRC-Project Grant 570844 (RC) and from the University of Sydney (2009 Bridging Support Grant (RC), co-funded postgraduate scholarship from the Faculty of Medicine (JL)) is gratefully acknowledged.

supplementary crystallographic information

Comment

O-Adamantanecarboxoyl-N-4-methoxy-4-oxobutanoyl-hydroxylamine (I) (Fig 1.) was prepared in our laboratory as part of our program in understanding resonance and tautomerism in biologically relevant molecules such as N,O-diacylhydroxylamines and hydroxamic acids. The torsion angle defined by H—N—O—C in each of N,O-diacetylhydroxylamine (-99.0 (1) °), N-acetyl-O-benzoylhydroxylamine (-101.3 (1) °), and N-benzoyl-O-acetylhydroxylamine (-94.1 (1) °) is negative, which is distinct from the analogous angle in N,O-dibenzoylhydroxylamine determined by the same group, which is positive (99.7 (1) °) (Schraml et al., 2004). The positive torsion angle defined by H1—N1—O4—C6 in I is 98.6 (1) °, which is akin to N,O-dibenzoylhydroxylamine. The N—O distance in I (N1—O4 = 1.4029 (14) Å) is similar to the N—O distance in other N,O-diacylhydroxylamines as cited above. Intermolecular hydrogen bonds exist in I between respective amide groups, with H1···O3 = 1.87 Å (Table 1) forming an infinite one-dimensional polymer extending along the c-axis (Fig 2.).

Experimental

O-Adamantanecarboxoyl-N-4-methoxy-4-oxobutanoyl-hydroxylamine (I) was isolated from a methanol solution (14 ml) containing adamantane-1-carboxylate-2,5-pyrrolidinedione (0.25 g, 0.89 mmol) (Liu, et al., 2009) and NaOH (0.018 g, 0.45 mmol). The product was dried in vacuo; colourless crystals of I appeared after approximately 1 month from a 4.5 mg mL-1 solution of I in ethanol:water (7:3).

Refinement

C and N bound-H (atoms were included in idealized positions and refined using a riding-model approximation, with C—H bond lengths fixed at 1.00 Å, 0.99 Å, 0.98 Å for methine, methylene and methyl H atoms respectively. N—H bond lengths fixed at 0.88 Å. Uiso(H) values were fixed at 1.2Ueq of the parent atoms for all H atoms except methyl H atoms for which 1.5Ueq of the parent atoms was used.

Figures

Fig. 1.

Fig. 1.

ORTEP representation of I shown with 50% probability ellipsoids.

Fig. 2.

Fig. 2.

A schematic representation of the one dimenisonal polymer formed through hydrogen bonding interactions in I. Dashed lines indicate hydrogen bonds.

Crystal data

C16H23NO5 F(000) = 1328
Mr = 309.35 Dx = 1.296 Mg m3
Orthorhombic, Pccn Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ab 2ac Cell parameters from 3869 reflections
a = 15.7837 (5) Å θ = 2.8–30.0°
b = 21.0715 (7) Å µ = 0.10 mm1
c = 9.5341 (3) Å T = 150 K
V = 3170.91 (18) Å3 Block, colourless
Z = 8 0.30 × 0.20 × 0.15 mm

Data collection

Bruker APEXII-FR591 diffractometer 4586 independent reflections
Radiation source: rotating anode 2890 reflections with I > 2σ(I)
graphite Rint = 0.036
ω+φ scans θmax = 30.0°, θmin = 3.2°
Absorption correction: multi-scan (SADABS; Sheldrick, 2007) h = −22→22
Tmin = 0.851, Tmax = 0.981 k = −26→29
22952 measured reflections l = −13→11

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)] = 0.048 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.132 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0599P)2 + 0.4178P] where P = (Fo2 + 2Fc2)/3
4586 reflections (Δ/σ)max < 0.001
200 parameters Δρmax = 0.25 e Å3
0 restraints Δρmin = −0.25 e Å3

Special details

Experimental. The crystal was coated in Exxon Paratone N hydrocarbon oil and mounted on a thin mohair fibre attached to a copper pin. Upon mounting on the diffractometer, the crystal was quenched to 150(K) under a cold nitrogen gas stream supplied by an Oxford Cryosystems Cryostream and data were collected at this temperature.
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 −0.10511 (9) 0.03188 (7) 0.34190 (19) 0.0397 (4)
H1A −0.1286 0.0521 0.4259 0.060*
H1B −0.1195 −0.0134 0.3422 0.060*
H1C −0.1289 0.0520 0.2580 0.060*
C2 0.01542 (9) 0.09834 (6) 0.33007 (15) 0.0282 (3)
C3 0.11059 (9) 0.09992 (7) 0.32346 (18) 0.0347 (3)
H3A 0.1293 0.0852 0.2299 0.042*
H3B 0.1339 0.0704 0.3944 0.042*
C4 0.14536 (9) 0.16607 (7) 0.34972 (19) 0.0395 (4)
H4A 0.1174 0.1965 0.2855 0.047*
H4B 0.1321 0.1790 0.4471 0.047*
C5 0.24014 (10) 0.16868 (7) 0.32743 (19) 0.0381 (4)
C6 0.41331 (9) 0.12429 (6) 0.41915 (16) 0.0285 (3)
C7 0.50576 (8) 0.13370 (5) 0.38462 (14) 0.0217 (3)
C8 0.51335 (8) 0.13881 (6) 0.22281 (15) 0.0264 (3)
H8A 0.4889 0.1005 0.1782 0.032*
H8B 0.4816 0.1763 0.1890 0.032*
C9 0.60700 (8) 0.14499 (6) 0.18337 (15) 0.0272 (3)
H9 0.6124 0.1480 0.0791 0.033*
C10 0.64442 (8) 0.20472 (6) 0.25077 (15) 0.0277 (3)
H10A 0.7048 0.2090 0.2240 0.033*
H10B 0.6137 0.2427 0.2167 0.033*
C11 0.63684 (8) 0.20033 (6) 0.40991 (15) 0.0271 (3)
H11 0.6612 0.2395 0.4533 0.032*
C12 0.54299 (8) 0.19452 (6) 0.45073 (16) 0.0269 (3)
H12A 0.5114 0.2321 0.4169 0.032*
H12B 0.5375 0.1926 0.5541 0.032*
C13 0.55512 (8) 0.07550 (6) 0.43587 (16) 0.0279 (3)
H13A 0.5313 0.0366 0.3930 0.034*
H13B 0.5499 0.0718 0.5390 0.034*
C14 0.64869 (9) 0.08217 (6) 0.39547 (17) 0.0321 (3)
H14 0.6808 0.0442 0.4292 0.039*
C15 0.68529 (9) 0.14227 (7) 0.46296 (18) 0.0358 (4)
H15A 0.6804 0.1394 0.5663 0.043*
H15B 0.7460 0.1463 0.4388 0.043*
C16 0.65534 (9) 0.08664 (6) 0.23537 (17) 0.0341 (4)
H16A 0.7156 0.0898 0.2075 0.041*
H16B 0.6313 0.0479 0.1922 0.041*
N1 0.28451 (7) 0.17669 (6) 0.44376 (15) 0.0376 (3)
H1 0.2595 0.1786 0.5262 0.045*
O1 −0.01378 (6) 0.03915 (5) 0.34139 (12) 0.0391 (3)
O2 −0.02969 (6) 0.14408 (5) 0.32255 (14) 0.0420 (3)
O3 0.27389 (7) 0.16496 (7) 0.21147 (14) 0.0595 (4)
O4 0.37279 (6) 0.18202 (4) 0.43133 (12) 0.0349 (3)
O5 0.37653 (7) 0.07535 (5) 0.43361 (14) 0.0506 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0367 (8) 0.0359 (7) 0.0464 (10) −0.0018 (6) 0.0100 (8) −0.0004 (7)
C2 0.0327 (7) 0.0296 (6) 0.0223 (7) 0.0045 (5) 0.0017 (6) −0.0017 (6)
C3 0.0298 (7) 0.0359 (7) 0.0384 (9) 0.0084 (6) 0.0016 (7) −0.0012 (6)
C4 0.0256 (7) 0.0431 (8) 0.0497 (11) 0.0040 (6) −0.0011 (7) −0.0097 (7)
C5 0.0289 (7) 0.0449 (8) 0.0406 (10) 0.0021 (6) 0.0015 (8) −0.0026 (7)
C6 0.0271 (7) 0.0301 (6) 0.0281 (8) −0.0026 (5) 0.0018 (6) 0.0000 (6)
C7 0.0217 (6) 0.0227 (6) 0.0206 (7) −0.0040 (4) 0.0008 (6) 0.0009 (5)
C8 0.0281 (7) 0.0299 (6) 0.0211 (7) −0.0070 (5) −0.0028 (6) 0.0010 (5)
C9 0.0313 (7) 0.0299 (6) 0.0203 (7) −0.0075 (5) 0.0042 (6) 0.0012 (5)
C10 0.0273 (6) 0.0239 (6) 0.0318 (9) −0.0060 (5) 0.0018 (6) 0.0058 (5)
C11 0.0270 (6) 0.0253 (6) 0.0289 (8) −0.0078 (5) −0.0055 (6) −0.0005 (5)
C12 0.0305 (7) 0.0268 (6) 0.0234 (8) −0.0031 (5) −0.0018 (6) −0.0027 (5)
C13 0.0306 (7) 0.0238 (6) 0.0294 (8) −0.0035 (5) 0.0021 (7) 0.0074 (5)
C14 0.0264 (7) 0.0267 (6) 0.0433 (10) 0.0033 (5) −0.0003 (7) 0.0103 (6)
C15 0.0259 (7) 0.0435 (8) 0.0382 (9) −0.0039 (6) −0.0099 (7) 0.0099 (7)
C16 0.0304 (7) 0.0259 (6) 0.0459 (10) −0.0028 (5) 0.0123 (7) −0.0021 (6)
N1 0.0215 (6) 0.0512 (7) 0.0401 (8) 0.0015 (5) 0.0037 (6) −0.0063 (6)
O1 0.0342 (5) 0.0295 (5) 0.0538 (8) 0.0035 (4) 0.0041 (5) −0.0012 (5)
O2 0.0312 (5) 0.0327 (5) 0.0621 (8) 0.0069 (4) 0.0012 (6) 0.0032 (5)
O3 0.0365 (7) 0.1062 (11) 0.0358 (8) 0.0027 (7) 0.0009 (6) 0.0004 (7)
O4 0.0213 (5) 0.0350 (5) 0.0485 (7) 0.0011 (4) 0.0008 (5) −0.0027 (5)
O5 0.0314 (5) 0.0362 (6) 0.0841 (10) −0.0085 (4) 0.0154 (6) 0.0045 (6)

Geometric parameters (Å, °)

C1—O1 1.4498 (17) C9—C16 1.5296 (19)
C1—H1A 0.9800 C9—C10 1.5316 (18)
C1—H1B 0.9800 C9—H9 1.0000
C1—H1C 0.9800 C10—C11 1.525 (2)
C2—O2 1.2005 (16) C10—H10A 0.9900
C2—O1 1.3340 (16) C10—H10B 0.9900
C2—C3 1.5038 (19) C11—C15 1.5289 (19)
C3—C4 1.519 (2) C11—C12 1.5364 (18)
C3—H3A 0.9900 C11—H11 1.0000
C3—H3B 0.9900 C12—H12A 0.9900
C4—C5 1.512 (2) C12—H12B 0.9900
C4—H4A 0.9900 C13—C14 1.5327 (19)
C4—H4B 0.9900 C13—H13A 0.9900
C5—O3 1.230 (2) C13—H13B 0.9900
C5—N1 1.322 (2) C14—C16 1.533 (2)
C6—O5 1.1913 (16) C14—C15 1.533 (2)
C6—O4 1.3792 (16) C14—H14 1.0000
C6—C7 1.5090 (18) C15—H15A 0.9900
C7—C13 1.5329 (17) C15—H15B 0.9900
C7—C12 1.5443 (17) C16—H16A 0.9900
C7—C8 1.5510 (19) C16—H16B 0.9900
C8—C9 1.5308 (18) N1—O4 1.4029 (14)
C8—H8A 0.9900 N1—H1 0.8800
C8—H8B 0.9900
O1—C1—H1A 109.5 C11—C10—H10A 109.7
O1—C1—H1B 109.5 C9—C10—H10A 109.7
H1A—C1—H1B 109.5 C11—C10—H10B 109.7
O1—C1—H1C 109.5 C9—C10—H10B 109.7
H1A—C1—H1C 109.5 H10A—C10—H10B 108.2
H1B—C1—H1C 109.5 C10—C11—C15 109.78 (12)
O2—C2—O1 123.41 (13) C10—C11—C12 109.42 (11)
O2—C2—C3 124.90 (13) C15—C11—C12 109.55 (11)
O1—C2—C3 111.67 (11) C10—C11—H11 109.4
C2—C3—C4 111.98 (11) C15—C11—H11 109.4
C2—C3—H3A 109.2 C12—C11—H11 109.4
C4—C3—H3A 109.2 C11—C12—C7 109.24 (11)
C2—C3—H3B 109.2 C11—C12—H12A 109.8
C4—C3—H3B 109.2 C7—C12—H12A 109.8
H3A—C3—H3B 107.9 C11—C12—H12B 109.8
C5—C4—C3 111.57 (12) C7—C12—H12B 109.8
C5—C4—H4A 109.3 H12A—C12—H12B 108.3
C3—C4—H4A 109.3 C7—C13—C14 109.65 (10)
C5—C4—H4B 109.3 C7—C13—H13A 109.7
C3—C4—H4B 109.3 C14—C13—H13A 109.7
H4A—C4—H4B 108.0 C7—C13—H13B 109.7
O3—C5—N1 122.19 (14) C14—C13—H13B 109.7
O3—C5—C4 123.55 (15) H13A—C13—H13B 108.2
N1—C5—C4 114.25 (15) C13—C14—C16 108.77 (12)
O5—C6—O4 121.84 (12) C13—C14—C15 109.46 (12)
O5—C6—C7 127.62 (12) C16—C14—C15 109.96 (11)
O4—C6—C7 110.54 (10) C13—C14—H14 109.5
C6—C7—C13 108.46 (10) C16—C14—H14 109.5
C6—C7—C12 112.83 (11) C15—C14—H14 109.5
C13—C7—C12 109.90 (11) C11—C15—C14 109.49 (11)
C6—C7—C8 107.50 (11) C11—C15—H15A 109.8
C13—C7—C8 109.47 (11) C14—C15—H15A 109.8
C12—C7—C8 108.61 (10) C11—C15—H15B 109.8
C9—C8—C7 108.95 (11) C14—C15—H15B 109.8
C9—C8—H8A 109.9 H15A—C15—H15B 108.2
C7—C8—H8A 109.9 C9—C16—C14 109.75 (11)
C9—C8—H8B 109.9 C9—C16—H16A 109.7
C7—C8—H8B 109.9 C14—C16—H16A 109.7
H8A—C8—H8B 108.3 C9—C16—H16B 109.7
C16—C9—C8 109.49 (10) C14—C16—H16B 109.7
C16—C9—C10 109.40 (12) H16A—C16—H16B 108.2
C8—C9—C10 109.83 (11) C5—N1—O4 117.73 (13)
C16—C9—H9 109.4 C5—N1—H1 121.1
C8—C9—H9 109.4 O4—N1—H1 121.1
C10—C9—H9 109.4 C2—O1—C1 116.27 (11)
C11—C10—C9 109.72 (10) C6—O4—N1 113.40 (10)
O2—C2—C3—C4 17.1 (2) C13—C7—C12—C11 58.97 (15)
O1—C2—C3—C4 −164.72 (13) C8—C7—C12—C11 −60.76 (14)
C2—C3—C4—C5 −173.84 (14) C6—C7—C13—C14 177.11 (12)
C3—C4—C5—O3 70.9 (2) C12—C7—C13—C14 −59.12 (15)
C3—C4—C5—N1 −110.41 (16) C8—C7—C13—C14 60.09 (14)
O5—C6—C7—C13 −26.1 (2) C7—C13—C14—C16 −60.43 (14)
O4—C6—C7—C13 154.74 (12) C7—C13—C14—C15 59.74 (16)
O5—C6—C7—C12 −148.06 (16) C10—C11—C15—C14 −59.45 (15)
O4—C6—C7—C12 32.74 (16) C12—C11—C15—C14 60.73 (16)
O5—C6—C7—C8 92.22 (18) C13—C14—C15—C11 −60.58 (16)
O4—C6—C7—C8 −86.97 (13) C16—C14—C15—C11 58.86 (15)
C6—C7—C8—C9 −177.12 (10) C8—C9—C16—C14 −61.11 (14)
C13—C7—C8—C9 −59.50 (12) C10—C9—C16—C14 59.30 (14)
C12—C7—C8—C9 60.50 (13) C13—C14—C16—C9 60.84 (13)
C7—C8—C9—C16 59.84 (14) C15—C14—C16—C9 −59.02 (14)
C7—C8—C9—C10 −60.31 (13) O3—C5—N1—O4 1.1 (2)
C16—C9—C10—C11 −59.98 (14) C4—C5—N1—O4 −177.63 (12)
C8—C9—C10—C11 60.21 (14) O2—C2—O1—C1 1.0 (2)
C9—C10—C11—C15 60.21 (14) C3—C2—O1—C1 −177.17 (13)
C9—C10—C11—C12 −60.05 (13) O5—C6—O4—N1 −7.7 (2)
C10—C11—C12—C7 60.71 (13) C7—C6—O4—N1 171.54 (11)
C15—C11—C12—C7 −59.69 (15) C5—N1—O4—C6 −81.34 (16)
C6—C7—C12—C11 −179.84 (11)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···O3i 0.88 1.87 2.7250 (19) 165

Symmetry codes: (i) −x+1/2, y, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BG2266).

References

  1. Allen, F. H., Johnson, O., Shields, G. P., Smith, B. R. & Towler, M. (2004). J. Appl. Cryst.37, 335–338.
  2. Altomare, A., Burla, M. C., Camalli, M., Cascarano, G. L., Giacovazzo, C., Guagliardi, A., Moliterni, A. G. G., Polidori, G. & Spagna, R. (1999). J. Appl. Cryst.32, 115–119.
  3. Baert, F., Lamiot, J., Couturier, D., Roussel, D. & Ricart, G. (1984). Acta Cryst. C40, 1071–1072.
  4. Bruker (2003). APEX2, SAINT and XPREP Bruker AXS Inc., Madison, Wisconsin, USA.
  5. Buscemi, S., Pace, A., Palumbo Piccionello, A., Pibiri, I., Vivona, N., Giorgi, G., Mazzanti, A. & Spinelli, D. (2006). J. Org. Chem.71, 8106–8113. [DOI] [PubMed]
  6. Cason, C. J. (2002). POV-RAY Hallam Oaks Pty Ltd, Williamstown, Victoria, Australia.
  7. Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
  8. Farrugia, L. J. (1999). J. Appl. Cryst.32, 837–838.
  9. Göttlicher, S. & Ochsenreiter, P. (1974). Chem. Ber.107, 398–413.
  10. Grassi, G., Cordaro, M., Bruno, G. & Nicolo, F. (2002). Helv. Chim. Acta, 85, 196–205.
  11. Kongprakaiwoot, N., Noll, B. C. & Brown, S. N. (2008). Inorg. Chem.47, 11902–11909. [DOI] [PubMed]
  12. Liu, J., Clegg, J. K. & Codd, R. (2009). Acta Cryst. E65, o1740–o1741. [DOI] [PMC free article] [PubMed]
  13. Masui, M., Ueshima, T., Ozaki, S., Fujiwara, T. & Tomita, K. (1983). Chem. Pharm. Bull.31, 784–786.
  14. Molecular Simulations (2000). WebLab ViewerPro Accelrys Software Inc., San Diego, California, USA.
  15. Pelto, R. B. & Pratt, R. F. (2008). Biochemistry, 47, 12037–12046. [DOI] [PMC free article] [PubMed]
  16. Schraml, J., Sykora, J., Fiedler, P., Roithova, J., Mindl, J., Blechta, V., Cisarova, I. & Exner, O. (2004). Org. Biomol. Chem.2, 2311–2314. [DOI] [PubMed]
  17. Sheldrick, G. M. (2007). SADABS University of Göttingen, Germany.
  18. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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/S1600536809024210/bg2266sup1.cif

e-65-o1742-sup1.cif (20.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809024210/bg2266Isup2.hkl

e-65-o1742-Isup2.hkl (224.8KB, hkl)

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


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