Abstract

Electrical and magnetic properties are dominated by the (de)localization and the anisotropy in the distribution of unpaired electrons in solids. In molecular materials, these properties have been indirectly controlled through crystal structures using various chemical modifications to affect molecular structures and arrangements. In the molecular crystals, since the energy band structures can be semi-quantitatively known using band calculations and solid state spectra, one can anticipate the (de)localization of unpaired electrons in particular bands/levels, as well as interactions with other electrons. Thus, direct control of anisotropy and localization of unpaired electrons by locating them in selected energy bands/levels would realize more efficient control of electrical and magnetic properties. In this work, it has been found that the unpaired electrons on Cu(II)-complex anions can be optically controlled to behave as anisotropically-delocalized electrons (under dark) or isotropically-localized electrons like free electrons (under UV), the latter of which has hardly been observed in the ground states of Cu(II)-complexes by any chemical modifications. Although the compounds examined in this work did not switch between conductors and magnets, these findings indicate that optical excitation in the [Cu(dmit)2]2− salts should be an effective method to control spin distribution and anisotropy.

Highlights

  • IntroductionDelocalized unpaired electrons can exhibit electrical conduction, while localized unpaired electrons can exhibit magnetism

  • Electrical and magnetic properties are based on unpaired electrons in solids

  • Theisotropy in the interactions among unpaired electrons matters in these properties

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Summary

Introduction

Delocalized unpaired electrons can exhibit electrical conduction, while localized unpaired electrons can exhibit magnetism This trend is true for any solid, including molecular materials. If one can switch unpaired electrons between localized and delocalized states, one may switch the solids between conductive and magnetic materials This point of view is different from that of light-induced excited spin-state trapping (LIESST), where the spin states of transition-metal complexes are switched between high- and low-spins by photoexcitations at low temperature [1,2,3,4,5,6,7,8,9]. The purpose of the present work is the control of spin distribution and anisotropy independent of thermodynamic conditions, unlike PIPTs. far, most of the studies to control the electrical and magnetic properties have utilized chemical modifications to affect molecular structures and arrangements.

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