Ordering phenomena in quasi one-dimensional organic conductors

TL;DR

This paper reviews the ordering phenomena in quasi-one-dimensional organic conductors, focusing on how electronic correlations lead to various broken-symmetry ground states and their experimental identification.

Contribution

It provides a detailed comparison of different ordering phenomena, such as charge density waves and charge-ordered Mott insulators, highlighting their physical causes and experimental signatures.

Findings

Charge density waves involve Fermi surface nesting and gap formation.

Charge-ordered Mott insulators result from Coulomb repulsion and charge localization.

Collective phenomena emerge with symmetry breaking in these systems.

Abstract

Low-dimensional organic conductors could establish themselves as model systems for the investigation of the physics in reduced dimensions. In the metallic state of a one-dimensional solid, Fermi-liquid theory breaks down and spin and charge degrees of freedom become separated. But the metallic phase is not stable in one dimension: as the temperature is reduced, the electronic charge and spin tend to arrange themselves in an ordered fashion due to strong correlations. The competition of the different interactions is responsible for which broken-symmetry ground state is eventually realized in a specific compound and which drives the system towards an insulating state. Here we review the various ordering phenomena and how they can be identified by optic and magnetic measurements. While the final results might look very similar in the case of a charge density wave and a charge-ordered metal, for instance, the physical cause is completely different. When density waves form, a gap opens in the density of states at the Fermi energy due to nesting of the one-dimension Fermi surface sheets. When a one-dimensional metal becomes a charge-ordered Mott insulator, on the other hand, the short-range Coulomb repulsion localizes the charge on the lattice sites and even causes certain charge patterns. We try to point out the similarities and conceptional differences of these phenomena and give an example for each of them. Particular emphasis will be put on collective phenomena which are inherently present as soon as ordering breaks the symmetry of the system.