Abstract

A comparative study of the low-energy optical properties of the 1/4-filled two-dimensional organic conductors α-(BEDT-TTF) 2 MHg(SCN) 4 (M = K. NH4) and the 1/5-filled salt β-(BEDO-TTF) 5 [CsHg(SCN) 4 ] 2 is presented. The superconducting α-(BEDT-TTF) 2 NH 4 Hg(SCN) 4 exhibits metallic-like optical properties down to 4 K. This is in contrast to the non-superconducting salt α-(BEDT-TTF) 2 KHg(SCN) 4 where a strong feature appears at frequencies of about 200 cm -1 and temperatures below 200 K which indicates the opening of a pseudogap. In the anisotropic and poor metal β-(BEDO-TTF) 5 [CsHg(SCN) 4 ] 2 we find a similar pseudogap in the optical spectra around 300 cm -1 up to room temperature and the presence of a strong Drude-like contribution. Based on exact diagonalisation calculations of the optical conductivity on an extended Hubbard model at quarter-filling we argue that the proximity of the α-phase BEDT-TTF salts to a charge-ordering transition is responsible for the observed pseudogap. Our proposed scenario suggests that the different ground states, including superconductivity, are a consequence of the fluctuations associated with short-range charge ordering which builds up close to the quantum phase transition. In a 1/5-filled system similar features like the short-range checkerboard charge fluctuations are expected, but the Drude contribution is always present because the charge ordered state is strongly modified by the presence of mobile empty sites.

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