THE ORGANIC METAL (ME2-DCNQI)2CU - DRAMATIC CHANGES IN SOLID-STATE PROPERTIES AND CRYSTAL-STRUCTURE DUE TO SECONDARY DEUTERIUM EFFECTS

Although (R1,R3-DCNQI)2Cu salts (1) are isomorphic (space group I4(1)/ a), they behave differently upon cooling: The group M salts remain met allic down to the lowest temperatures, whereas the group M-I salts sho w phase transitions to semiconductors at temperatures T(M-I) = 160-230 K. With regard to the steric requirements of the methyl group, 1a (CH 3/CH3/H2) is expected to belong to group M-I, but it remains metallic even at 0.4 K (sigma = 500 000 S cm-1). Deuterated 1a, however, namely 1c (CH3/CD3/H2), 1d (CD3/CD3/H2), and 1e (CD3/CD3/D2), undergo sharp phase transitions at 58, 73, and 82 K, respectively, the lowest phase- transition temperatures observed so far for copper salts 1 at ambient pressure. Thereby, conductivities drop by 6-8 orders of magnitude with in a few kelvins, transforming 1c-e from three-dimensional into strict ly one-dimensional systems. This unprecedented strong secondary deuter ium isotope effect is also reflected in significant changes in ESR sig nals and magnetic susceptibilities. Structure determinations by X-ray analysis of 1a and 1d at various temperatures (20 K, 156 K, and room t emperature) reveal characteristic differences of the crystal structure s above and below the phase-transition temperature T(M-I) for both com pounds. The very special structural features of the crystals are relat ed to their 7-fold diamondoid superstructure, which includes infinite superhelices in the stacks of ligands and copper ions. A phase diagram of (R1,R3-DCNQI)2Cu salts (1) is derived from a comparison of tempera ture-dependent structural and conductivity data, which shows that the conductive properties of the salts depend dramatically on the N-Cu-N a ngle alpha(co). A minimal threshold value (alpha(co) almost-equal-to 1 26.4-degrees) is evaluated which determines the phase behavior of 1 up on cooling or applying pressure. In order to understand their unique p roperties as compared to those of other DCNQI metal salts, a new appro ach to DCNQI copper salts is presented in terms of a ''two conductors in one'' concept, which is a unique combination of a common one-dimens ional (anisotropic) conduction path along segregated stacks and a thre e-dimensional (isotropic) conduction path within a Robin-Day class III network of delocalized mixed-valent metal ions bridged by organic spa cers allowing electron transfer.