Abstract

Layered triangular organic dimer Mott (DM) insulator κ -(ET)2 Cu2 (CN)3 was shown to exhibit a relaxor-like dielectric anomaly below 40 K with strong dispersion relation, reflecting its electric dipole glass (ferroelectric charge order; FCO) nature[1, 2]. The dielectric anomaly in κ -(ET)2 Cu2 (CN)3 indicates that this compound is located in the vicinity of the DM-FCO phase boundary, where ferroelectric fluctuation such as the electric dipole glass state or the polar cluster is formed in the DM phase. Optical excitation of the DM-FCO competing state by an ultrashort light pulse enables us to achieve dramatic responses, such as photoinduced ferroelectricity, photoinduced growth of the electric dipole glass or the polar clusters.

Highlights

  • In strongly correlated electron systems, the dipole field induced by the Coulomb repulsion interaction sometimes shows ferroelectricity and ferroelectric fluctuation such as the electric dipole glass state or a polar nano region (PNR)

  • The dielectric anomaly in -(ET)2Cu2(CN)3 indicates that this compound is located in the vicinity of the Dimer Mott (DM)-Ferroelectric Charge Order (FCO) phase boundary, where the electric dipole glass state or the PNR is formed in the DM phase

  • Considering that, the marked increase in the 1 THz band at

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Summary

Introduction

In strongly correlated electron systems, the dipole field induced by the Coulomb repulsion interaction sometimes shows ferroelectricity and ferroelectric fluctuation such as the electric dipole glass state or a polar nano region (PNR). An origin of the spinliquid phase has been reconsidered, i.e., this compound was shown to exhibit a DM phase (a) and FCO phase (b) are shown. The dielectric anomaly in -(ET)2Cu2(CN) indicates that this compound is located in the vicinity of the DM-FCO phase boundary (red area in Fig. 1), where the electric dipole glass state or the PNR is formed in the DM phase. In such a DM-FCO competing state, optical excitation of the DM-FCO competing state by an ultrashort light pulse enables us to achieve dramatic responses, such as photoinduced ferroelecricity, photoinduced growth of the electric dipole glass or the PNR

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