The full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-prot purposes provided that:• a full bibliographic reference is made to the original source • a link is made to the metadata record in DRO • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders.Please consult the full DRO policy for further details. A charge-density study of the nonlinear-optical ͑NLO͒ precursor ͕4-͓bis͑diethylamino͒-methylium͔ phenyl͖dicyanomethanide ͑DED-TCNQ͒, space group P2 1 /c, aϭ11.174(2) Å; bϭ12.859(2) Å; c ϭ12.486(2) Å; ϭ112.00(1)°, is presented. The results derive from a suitable combination of complementary 20 K x-ray and neutron diffraction data, the latter being important for locating the hydrogen atoms precisely. The compound is one in a series of TCNQ derivatives that exhibit varying degrees of quinoidal and zwitterionic character, these two electronic states being very close energetically. Bond-length-alternation type calculations show that the molecule at 20 K exists in a mixture of the two states, the zwitterionic ground state being dominant ͑63:37% zwitterionic: quinoidal͒. A topological analysis of the bonding density within the benzenoid ring provides for a more direct, alternative method to calculate this ratio which utilizes ellipticity values derived from the charge-density study. Results are identical thus corroborating the validity of the ''strength-length'' relationship implicitly assumed in bond-length-alternation type calculations. The ratio determined corresponds well to the electronic configuration needed to meet the requirements of the general rule for obtaining a maximum value of  ͑a measure of the NLO response on the molecular scale͒ as a function of bond-length alternation. The promise of this class of compounds for nonlinear optics also lies partly in their high molecular dipole moments and so the pseudoatomic charges derived from this study were used to evaluate the nature of the molecular charge transfer in detail and the solid-state dipolar vector moment . Such measurements of are otherwise difficult in the solid state. A value of ͉͉ϭ91ϫ10 Ϫ30 Cm was deduced which compares with liquid and gas phase theoretical calculations of ϭ66.71ϫ10 Ϫ30 Cm and ϭ33.36 ϫ10 Ϫ30 Cm, respectively. This comparison, combined with an analysis of the sense of this vector, show that local crystal-field effects are highly influential in the solid state.