Abstract
The molecule is planar to within 0.2 A with a C(4)−C(7)−C(8)-C(9) torsion angle of − 179 (2)°. The charge-transfer axis lies along the line joining the N atom at one end of the molecule to the 0 atom at the other. The final crystal structure is the result of complicated interplay between the short-range van der Waals interactions and the long-range dipoledipole interactions, making the crystal highly polarized
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