Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806036828/at2091sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536806036828/at2091Isup2.hkl |
CCDC reference: 623961
Data collection: CAD-4/MACH3 (Nonius, 2000); cell refinement: CAD-4/MACH3; data reduction: HELENA (Spek, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: PLATON.
C14H8O4 | Dx = 1.284 Mg m−3 |
Mr = 240.20 | Cu Kα radiation, λ = 1.54178 Å |
Tetragonal, I4/mcm | Cell parameters from 18 reflections |
Hall symbol: -I 4 2c | θ = 19.7–33.9° |
a = 13.640 (4) Å | µ = 0.80 mm−1 |
c = 6.678 (3) Å | T = 293 K |
V = 1242.4 (8) Å3 | Thin needles, yellow |
Z = 4 | 0.50 × 0.19 × 0.15 mm |
F(000) = 496 |
Nonius diffractometer | 346 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.022 |
Graphite monochromator | θmax = 75.0°, θmin = 4.6° |
ω/2θ scans | h = 0→17 |
Absorption correction: analytical (Alcock, 1970) | k = −17→0 |
Tmin = 0.691, Tmax = 0.890 | l = −8→0 |
702 measured reflections | 3 standard reflections every 60 min |
375 independent reflections | intensity decay: 11.0% |
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)] = 0.057 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.188 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.20 | w = 1/[σ2(Fo2) + (0.1314P)2 + 0.1721P] where P = (Fo2 + 2Fc2)/3 |
375 reflections | (Δ/σ)max < 0.001 |
35 parameters | Δρmax = 0.41 e Å−3 |
41 restraints | Δρmin = −0.19 e Å−3 |
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. Structure was refined using the option Squeeze (van der Sluis, 1990) in PLATON suite. Void is present in the centre of the tetrameric assembly. This cavity potentialy hosts a cation or water molecules. Attempts to refine this electron density were niot successful. The δρmax was carefully analysed and is present on the partial double bond between C2 and C2e. This is due to the electronic resonance. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
O1 | 0.36072 (9) | −0.13928 (9) | 0.0000 | 0.0518 (7) | |
C1 | 0.42437 (12) | −0.07563 (12) | 0.0000 | 0.0368 (7) | |
C2 | 0.39765 (11) | 0.02914 (11) | 0.0000 | 0.0363 (7) | |
C3 | 0.29948 (14) | 0.05674 (13) | 0.0000 | 0.0452 (7) | |
H3 | 0.2510 | 0.0088 | 0.0000 | 0.054* | |
C4 | 0.27310 (13) | 0.15455 (14) | 0.0000 | 0.0491 (7) | |
O4 | 0.1729 (2) | 0.1675 (2) | 0.0000 | 0.0692 (10) | 0.50 |
H4 | 0.1603 | 0.2263 | 0.0000 | 0.104* | 0.50 |
H4' | 0.2068 (6) | 0.170 (2) | 0.0000 | 0.083* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0387 (9) | 0.0387 (9) | 0.0781 (14) | −0.0073 (6) | 0.000 | 0.000 |
C1 | 0.0341 (9) | 0.0341 (9) | 0.0420 (12) | −0.0023 (8) | 0.000 | 0.000 |
C2 | 0.0321 (10) | 0.0337 (10) | 0.0430 (10) | 0.0001 (7) | 0.000 | 0.000 |
C3 | 0.0333 (10) | 0.0437 (10) | 0.0585 (12) | 0.0008 (6) | 0.000 | 0.000 |
C4 | 0.0372 (10) | 0.0464 (11) | 0.0638 (13) | 0.0093 (7) | 0.000 | 0.000 |
O4 | 0.0399 (16) | 0.0483 (17) | 0.119 (2) | 0.0096 (11) | 0.000 | 0.000 |
O1—C1 | 1.228 (3) | C3—H3 | 0.9300 |
C1—C2i | 1.475 (2) | C4—O4 | 1.377 (4) |
C1—C2 | 1.475 (2) | C4—C4ii | 1.396 (4) |
C2—C3 | 1.391 (2) | C4—H4' | 0.9300 (10) |
C2—C2ii | 1.412 (3) | O4—H4 | 0.8200 |
C3—C4 | 1.382 (2) | ||
O1—C1—C2i | 120.69 (11) | C2—C3—H3 | 119.6 |
O1—C1—C2 | 120.69 (11) | O4—C4—C3 | 112.5 (2) |
C2i—C1—C2 | 118.6 (2) | O4—C4—C4ii | 127.64 (15) |
C3—C2—C2ii | 119.29 (10) | C3—C4—C4ii | 119.91 (11) |
C3—C2—C1 | 120.02 (17) | C3—C4—H4' | 118.6 (19) |
C2ii—C2—C1 | 120.69 (11) | C4ii—C4—H4' | 121.5 (19) |
C4—C3—C2 | 120.80 (17) | C4—O4—H4 | 109.5 |
C4—C3—H3 | 119.6 |
Symmetry codes: (i) y+1/2, x−1/2, −z; (ii) −y+1/2, −x+1/2, z. |