Charge-Ordered State versus Dimer-Mott Insulator at Finite Temperatures

TL;DR

This paper explores how charge order and Mott insulating states compete at finite temperatures in quasi-one-dimensional electron systems, revealing the effects of lattice dimerization and interchain interactions on phase transitions.

Contribution

It introduces a theoretical framework combining bosonization and mean-field approximation to analyze charge order and Mott phases at finite temperatures.

Findings

Lattice dimerization reduces charge-ordering transition temperature.

Interchain Coulomb interactions enlarge the dimer-Mott phase.

Derived a formula for the Knight shift in the charge-ordered phase.

Abstract

We theoretically investigate the competition between charge-ordered state and Mott insulating state at finite temperatures in quarter-filled quasi-one-dimensional electron systems, by studying dimerized extended Hubbard chains with interchain Coulomb interactions. In order to take into account one-dimensional fluctuations properly, we apply the bosonization method to an effective model obtained by the interchain mean-field approximation. The results show that lattice dimerization, especially in the critical region, and frustration in the interchain Coulomb interactions reduce the charge-ordering phase transition temperature and enlarge the dimer-Mott insulating phase. We also derive a general formula of the Knight shift in the charge-ordered phase and its implication to experiments is discussed.