organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Volume 64| Part 5| May 2008| Pages o824-o825

(E)-3,4-Di­hydroxy­benzaldehyde 4-ethyl­thio­semicarbazone

aSchool of Chemical Sciences and Food Technology, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, 43600 UKM Bangi, Selangor, Malaysia, and bDepartment of Chemistry, University of Otago, PO Box 56, Dunedin, New Zealand
*Correspondence e-mail: jsimpson@alkali.otago.ac.nz

(Received 3 April 2008; accepted 4 April 2008; online 10 April 2008)

The title compound, C10H13N3O2S, was prepared by condensation of 3,4-dihydroxy­benzaldehyde with 4-ethyl-3-thio­semicarbazide. The mol­ecule adopts an E configuration with respect to the C=N bond. One of the OH substituents on the dihydroxy­benzene ring is disordered over the two possible 3-positions on either side of the ordered 4-hydr­oxy group. The occupancy of the major disorder component refined to 0.633 (7). The mol­ecule is essentially planar, with an r.m.s. deviation through all non-H atoms of 0.0862 Å. An intra­molecular N—H⋯N hydrogen bond forms between the outer amine residue and the imine N atom, generating an S(5) ring motif and contributing to the planarity of the mol­ecule. In the crystal structure, an extensive network of classical O—H⋯O, O—H⋯S and N—H⋯S hydrogen bonds and weak C—H⋯O and S⋯O [3.301 (3) Å] inter­actions link mol­ecules into sheets running approximately parallel to the ab plane.

Related literature

For related structures, see: Swesi et al. (2006[Swesi, A. T., Farina, Y., Kassim, M. & Ng, S. W. (2006). Acta Cryst. E62, o5457-o5458.]); Kovala-Demertzi et al. (2004[Kovala-Demertzi, D., Yadav, P. N., Demertzis, M. A., Jasiski, J. P., Andreadaki, F. J. & Kostas, I. D. (2004). Tetrahedron Lett. 45, 2923-2926.]); Jian & Li (2006[Jian, F.-F. & Li, Y. (2006). Acta Cryst. E62, o4563-o4564.]). For reference structural data, see: Allen et al. (1987[Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1-S19.]). For ring motifs, see: Bernstein et al. (1995[Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555-1573.]).

[Scheme 1]

Experimental

Crystal data
  • C10H13N3O2S

  • Mr = 239.29

  • Monoclinic, P 21 /c

  • a = 10.6549 (12) Å

  • b = 12.9020 (16) Å

  • c = 8.6375 (11) Å

  • β = 107.910 (4)°

  • V = 1129.9 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.28 mm−1

  • T = 91 (2) K

  • 0.44 × 0.11 × 0.09 mm

Data collection
  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2006[Bruker (2006). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.818, Tmax = 0.975

  • 12327 measured reflections

  • 1998 independent reflections

  • 1507 reflections with I > 2σ(I)

  • Rint = 0.040

Refinement
  • R[F2 > 2σ(F2)] = 0.059

  • wR(F2) = 0.168

  • S = 1.05

  • 1998 reflections

  • 165 parameters

  • 2 restraints

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

  • Δρmax = 1.41 e Å−3

  • Δρmin = −0.64 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3B⋯N1 0.88 2.23 2.626 (4) 107
O5—H5A⋯S1i 0.84 2.82 3.106 (9) 102
C2—H2⋯O5ii 0.95 2.65 3.335 (8) 129
N2—H2A⋯S1iii 0.88 2.52 3.392 (4) 172
O4—H4⋯O4iv 0.84 2.16 2.988 (5) 169
C9—H9A⋯O3v 0.99 2.46 2.985 (5) 113
Symmetry codes: (i) [-x+1, y+{\script{1\over 2}}, -z+{\script{1\over 2}}]; (ii) [-x+2, y-{\script{1\over 2}}, -z+{\script{1\over 2}}]; (iii) -x+1, -y, -z+1; (iv) -x+2, -y+1, -z; (v) [x-1, -y+{\script{1\over 2}}, z+{\script{1\over 2}}].

Data collection: APEX2 (Bruker 2006[Bruker (2006). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: APEX2 and SAINT (Bruker 2006[Bruker (2006). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]) and TITAN2000 (Hunter & Simpson, 1999[Hunter, K. A. & Simpson, J. (1999). TITAN2000. University of Otago, New Zealand.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]) and TITAN2000; molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]) and Mercury (Macrae et al., 2006[Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453-457.]); software used to prepare material for publication: SHELXL97, enCIFer (Allen et al., 2004[Allen, F. H., Johnson, O., Shields, G. P., Smith, B. R. & Towler, M. (2004). J. Appl. Cryst. 37, 335-338.]) and PLATON (Spek, 2003[Spek, A. L. (2003). J. Appl. Cryst. 36, 7-13.]).

Supporting information


Comment top

For example the structure of the related molecule 2,3-dihydroxybenzaldehyde thiosemicarbazone hemihydrate has been reported by Swesi et al. (2006) as have the structures of a phenylthiocarbazole with a single hydroxy-substituent on the benzylidene ring (Jian & Li, 2006) and of a palladium(II) complex of an ethylthiosemicarbonate ligand deprotonated at the phenolate ring (Kovala-Demertzi et al., 2004).

The molecule adopts an E configuration with respect to the C=N bond and bond distances and angles are normal (Allen et al., 1987). One of the OH substituents on the dihydroxy benzene ring is disordered over the two possible 3-positions (labelled O3 and O5) on either side of the ordered O4 hydroxo group. Occupancy of the O3 and H5 atoms of the major disorder component refines to 0.633 (7). The molecule is essentially planar with an r.m.s. deviation through all non-hydrogen atoms of 0.0862 Å. An intramolecular N3—H3B···N1 hydrogen bond forms between the outer amine residue and the imine N atom generating an S(5) ring motif (Bernstein et al., 1995) which contributes to the planarity of the molecule.

In the crystal structure N2—H2A···S1 hydrogen bonds, Table 1, generate centrosymmetric R22(8) rings. Other classical O—H···O and O—H···S hydrogen bonds combine with weak C—H···O and S1···O4i interactions (d(S1···O4) = 3.301 (3) Å; i = -1 + x, 1/2 - y, 1/2 + z) to form sheets running approximately parallel to the ac diagonal, Fig 2.

Related literature top

For related structures, see: Swesi et al. (2006); Kovala-Demertzi et al. (2004); Jian & Li (2006). For reference structural data, see: Allen et al. (1987). For ring motifs, see: Bernstein et al. (1995).

Experimental top

The title compound C10H13N3O2S was prepared by heating an ethanolic (35 ml) solution of 3,4-dihydroxybenzaldehyde (1.4 g, 10 mmol) and 4-ethyl-3-thiosemicarbazide (1.2 g, 10 mmol) under reflux for 1 h. The resulting product was isolated and recrystallized from ethanol to afford red block-shaped crystals in 71% yield (m.p. 464–467 K).

Refinement top

The aromatic H atoms of the two disorder components were located in a difference Fourier map and refined with fixed isotropic displacement parameters with C—H distances restrained to 0.95 (1) Å. All other H-atoms were positioned geometrically and refined using a riding model with d(C—H) = 0.95 Å, Uiso=1.2Ueq (C) for aromatic 0.99 Å, Uiso = 1.2Ueq (C) for CH2, 0.98 Å, Uiso = 1.5Ueq (C) for CH3 0.88 Å, Uiso = 1.2Ueq (N) for NH and 0.84 Å, Uiso = 1.5Ueq (O) for the OH atoms. Close contacts involving the H atoms of the OH substituents, suggest that there may be unresolved disorder particularly with the location of the H atoms. The highest residual electron density peak is located at 2.56 Å from O5 and the deepest hole is located at 0.81 Å from S1.

Computing details top

Data collection: APEX2 (Bruker 2006); cell refinement: APEX2 (Bruker 2006) and SAINT (Bruker 2006); data reduction: SAINT (Bruker 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008) and TITAN2000 (Hunter & Simpson, 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008) and TITAN2000 (Hunter & Simpson, 1999); molecular graphics: SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008), enCIFer (Allen et al., 2004) and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The structure of (I), with atom labels and 50% probability displacement ellipsoids for non-H atoms. The intramolecular N—H···N hydrogen bond is drawn as a dashed line. For clarity only the major disorder component of the disordered OH groups is shown.
[Figure 2] Fig. 2. Crystal packing of (I) viewed down the b axis with hydrogen bonds drawn as dashed lines.
(E)-3,4-Dihydroxybenzaldehyde 4-ethylthiosemicarbazone top
Crystal data top
C10H13N3O2SF(000) = 504
Mr = 239.29Dx = 1.407 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3071 reflections
a = 10.6549 (12) Åθ = 2.6–25.0°
b = 12.9020 (16) ŵ = 0.28 mm1
c = 8.6375 (11) ÅT = 91 K
β = 107.910 (4)°Block, red
V = 1129.9 (2) Å30.44 × 0.11 × 0.09 mm
Z = 4
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1998 independent reflections
Radiation source: fine-focus sealed tube1507 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.040
ω scansθmax = 25.1°, θmin = 3.1°
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
h = 1212
Tmin = 0.818, Tmax = 0.975k = 1515
12327 measured reflectionsl = 108
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.059Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.168H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0718P)2 + 1.7231P]
where P = (Fo2 + 2Fc2)/3
1998 reflections(Δ/σ)max < 0.001
165 parametersΔρmax = 1.41 e Å3
2 restraintsΔρmin = 0.64 e Å3
Crystal data top
C10H13N3O2SV = 1129.9 (2) Å3
Mr = 239.29Z = 4
Monoclinic, P21/cMo Kα radiation
a = 10.6549 (12) ŵ = 0.28 mm1
b = 12.9020 (16) ÅT = 91 K
c = 8.6375 (11) Å0.44 × 0.11 × 0.09 mm
β = 107.910 (4)°
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1998 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
1507 reflections with I > 2σ(I)
Tmin = 0.818, Tmax = 0.975Rint = 0.040
12327 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0592 restraints
wR(F2) = 0.168H atoms treated by a mixture of independent and constrained refinement
S = 1.05Δρmax = 1.41 e Å3
1998 reflectionsΔρmin = 0.64 e Å3
165 parameters
Special details top

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) top
xyzUiso*/UeqOcc. (<1)
C10.7990 (3)0.2409 (2)0.2636 (3)0.0304 (7)
C20.9009 (3)0.1922 (2)0.2235 (3)0.0342 (7)
H20.90970.11900.23230.041*
C30.9897 (3)0.2493 (3)0.1712 (4)0.0382 (8)
H31.048 (11)0.201 (8)0.147 (17)0.046*0.367 (7)
O31.0884 (4)0.2059 (4)0.1330 (6)0.0525 (14)0.633 (7)
H3A1.13010.25160.09990.079*0.633 (7)
C50.8761 (3)0.4051 (3)0.1995 (4)0.0394 (8)
H50.862 (11)0.477 (2)0.177 (13)0.047*0.633 (7)
O50.8733 (10)0.5042 (5)0.1953 (12)0.045 (2)0.367 (7)
H5A0.88560.52480.10890.068*0.367 (7)
C40.9776 (3)0.3557 (3)0.1580 (4)0.0381 (8)
O41.0659 (2)0.4115 (2)0.1053 (3)0.0503 (7)
H41.02940.46560.05840.075*
C60.7871 (3)0.3484 (2)0.2514 (3)0.0334 (7)
H60.71780.38250.27870.040*
C70.7094 (3)0.1775 (3)0.3225 (3)0.0357 (7)
H70.72280.10470.33220.043*
N10.6134 (2)0.2175 (2)0.3612 (3)0.0390 (7)
N20.5403 (3)0.1489 (3)0.4216 (3)0.0442 (7)
H2A0.55670.08190.42440.053*
C80.4433 (3)0.1862 (3)0.4763 (4)0.0458 (9)
S10.36442 (11)0.10262 (10)0.56744 (13)0.0685 (4)
N30.4168 (3)0.2853 (3)0.4565 (3)0.0506 (8)
H3B0.46600.32330.41330.061*
C90.3112 (4)0.3371 (4)0.5010 (5)0.0678 (13)
H9A0.31180.31330.61020.081*
H9B0.22520.31770.42240.081*
C100.3260 (5)0.4506 (5)0.5024 (6)0.0804 (15)
H10A0.40420.47080.59170.121*
H10B0.24760.48310.51790.121*
H10C0.33610.47350.39870.121*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0251 (14)0.0466 (18)0.0195 (14)0.0048 (12)0.0069 (11)0.0028 (12)
C20.0353 (16)0.0376 (17)0.0304 (15)0.0009 (13)0.0112 (13)0.0039 (13)
C30.0292 (16)0.057 (2)0.0319 (16)0.0021 (14)0.0146 (13)0.0001 (15)
O30.037 (3)0.075 (3)0.059 (3)0.009 (2)0.036 (2)0.002 (2)
C50.0427 (18)0.0392 (18)0.0365 (17)0.0057 (15)0.0122 (14)0.0051 (15)
O50.048 (4)0.035 (4)0.053 (5)0.010 (4)0.015 (3)0.013 (4)
C40.0331 (16)0.056 (2)0.0265 (15)0.0149 (15)0.0113 (13)0.0037 (14)
O40.0449 (14)0.0657 (17)0.0471 (14)0.0192 (12)0.0241 (12)0.0093 (12)
C60.0304 (15)0.0422 (17)0.0295 (16)0.0020 (13)0.0119 (13)0.0009 (13)
C70.0348 (16)0.0476 (19)0.0252 (15)0.0110 (14)0.0099 (13)0.0018 (13)
N10.0281 (13)0.0639 (18)0.0267 (13)0.0131 (12)0.0110 (11)0.0059 (12)
N20.0380 (14)0.0675 (19)0.0319 (14)0.0205 (14)0.0178 (12)0.0021 (13)
C80.0331 (17)0.082 (3)0.0250 (16)0.0237 (18)0.0133 (13)0.0102 (17)
S10.0738 (7)0.0931 (9)0.0585 (7)0.0513 (6)0.0497 (6)0.0299 (6)
N30.0305 (14)0.092 (3)0.0352 (15)0.0037 (15)0.0181 (12)0.0076 (16)
C90.038 (2)0.131 (4)0.039 (2)0.008 (2)0.0176 (16)0.000 (2)
C100.076 (3)0.122 (5)0.053 (3)0.036 (3)0.034 (2)0.000 (3)
Geometric parameters (Å, º) top
C1—C21.388 (4)C7—N11.278 (4)
C1—C61.395 (5)C7—H70.9500
C1—C71.462 (4)N1—N21.384 (3)
C2—C31.380 (4)N2—C81.350 (4)
C2—H20.9500N2—H2A0.8800
C3—O31.319 (5)C8—N31.310 (5)
C3—C41.380 (5)C8—S11.702 (3)
C3—H30.950 (10)S1—O4i3.301 (2)
O3—H3A0.8400N3—C91.457 (5)
C5—O51.279 (7)N3—H3B0.8800
C5—C61.376 (4)C9—C101.473 (7)
C5—C41.394 (5)C9—H9A0.9900
C5—H50.950 (10)C9—H9B0.9900
O5—H5A0.8400C10—H10A0.9800
C4—O41.369 (3)C10—H10B0.9800
O4—H40.8400C10—H10C0.9800
C6—H60.9500
C2—C1—C6119.4 (3)N1—C7—C1121.7 (3)
C2—C1—C7118.6 (3)N1—C7—H7119.1
C6—C1—C7121.9 (3)C1—C7—H7119.1
C3—C2—C1120.6 (3)C7—N1—N2115.4 (3)
C3—C2—H2119.7C8—N2—N1119.0 (3)
C1—C2—H2119.7C8—N2—H2A120.5
O3—C3—C4117.6 (3)N1—N2—H2A120.5
O3—C3—C2122.3 (4)N3—C8—N2117.4 (3)
C4—C3—C2120.1 (3)N3—C8—S1124.2 (3)
C4—C3—H3133 (8)N2—C8—S1118.4 (3)
C2—C3—H3107 (8)C8—N3—C9124.5 (3)
C3—O3—H3A109.5C8—N3—H3B117.8
O5—C5—C6121.9 (5)C9—N3—H3B117.8
O5—C5—C4117.6 (5)N3—C9—C10111.6 (4)
C6—C5—C4120.5 (3)N3—C9—H9A109.3
C6—C5—H5120 (7)C10—C9—H9A109.3
C4—C5—H5119 (7)N3—C9—H9B109.3
C5—O5—H5A109.5C10—C9—H9B109.3
O4—C4—C3119.6 (3)H9A—C9—H9B108.0
O4—C4—C5120.8 (3)C9—C10—H10A109.5
C3—C4—C5119.6 (3)C9—C10—H10B109.5
C4—O4—H4109.5H10A—C10—H10B109.5
C5—C6—C1119.9 (3)C9—C10—H10C109.5
C5—C6—H6120.1H10A—C10—H10C109.5
C1—C6—H6120.1H10B—C10—H10C109.5
Symmetry code: (i) x1, y+1/2, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3B···N10.882.232.626 (4)107
O5—H5A···S1ii0.842.823.106 (9)102
C2—H2···O5iii0.952.653.335 (8)129
N2—H2A···S1iv0.882.523.392 (4)172
O4—H4···O4v0.842.162.988 (5)169
C9—H9A···O3i0.992.462.985 (5)113
Symmetry codes: (i) x1, y+1/2, z+1/2; (ii) x+1, y+1/2, z+1/2; (iii) x+2, y1/2, z+1/2; (iv) x+1, y, z+1; (v) x+2, y+1, z.

Experimental details

Crystal data
Chemical formulaC10H13N3O2S
Mr239.29
Crystal system, space groupMonoclinic, P21/c
Temperature (K)91
a, b, c (Å)10.6549 (12), 12.9020 (16), 8.6375 (11)
β (°) 107.910 (4)
V3)1129.9 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.28
Crystal size (mm)0.44 × 0.11 × 0.09
Data collection
DiffractometerBruker APEXII CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2006)
Tmin, Tmax0.818, 0.975
No. of measured, independent and
observed [I > 2σ(I)] reflections
12327, 1998, 1507
Rint0.040
(sin θ/λ)max1)0.596
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.059, 0.168, 1.05
No. of reflections1998
No. of parameters165
No. of restraints2
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)1.41, 0.64

Computer programs: , APEX2 (Bruker 2006) and SAINT (Bruker 2006), SAINT (Bruker 2006), SHELXS97 (Sheldrick, 2008) and TITAN2000 (Hunter & Simpson, 1999), SHELXL97 (Sheldrick, 2008) and TITAN2000 (Hunter & Simpson, 1999), SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2006), SHELXL97 (Sheldrick, 2008), enCIFer (Allen et al., 2004) and PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3B···N10.882.232.626 (4)107
O5—H5A···S1i0.842.823.106 (9)102.3
C2—H2···O5ii0.952.653.335 (8)129.1
N2—H2A···S1iii0.882.523.392 (4)172.0
O4—H4···O4iv0.842.162.988 (5)168.8
C9—H9A···O3v0.992.462.985 (5)112.6
Symmetry codes: (i) x+1, y+1/2, z+1/2; (ii) x+2, y1/2, z+1/2; (iii) x+1, y, z+1; (iv) x+2, y+1, z; (v) x1, y+1/2, z+1/2.
 

Acknowledgements

We thank the Universiti Kebangsaan Malaysia and the Ministry of Higher Education, Malaysia, for supporting this research through grant UKM-ST-01-FRGS0022–2006. We also thank the University of Otago for purchase of the diffractometer.

References

First citationAllen, F. H., Johnson, O., Shields, G. P., Smith, B. R. & Towler, M. (2004). J. Appl. Cryst. 37, 335–338.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationAllen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–S19.  CrossRef Web of Science Google Scholar
First citationBernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555–1573.  CrossRef CAS Web of Science Google Scholar
First citationBruker (2006). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationHunter, K. A. & Simpson, J. (1999). TITAN2000. University of Otago, New Zealand.  Google Scholar
First citationJian, F.-F. & Li, Y. (2006). Acta Cryst. E62, o4563–o4564.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationKovala-Demertzi, D., Yadav, P. N., Demertzis, M. A., Jasiski, J. P., Andreadaki, F. J. & Kostas, I. D. (2004). Tetrahedron Lett. 45, 2923–2926.  Web of Science CSD CrossRef CAS Google Scholar
First citationMacrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSpek, A. L. (2003). J. Appl. Cryst. 36, 7–13.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSwesi, A. T., Farina, Y., Kassim, M. & Ng, S. W. (2006). Acta Cryst. E62, o5457–o5458.  Web of Science CSD CrossRef IUCr Journals Google Scholar

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Volume 64| Part 5| May 2008| Pages o824-o825
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