Abstract

We report the structural and physical properties of a new organic Mott insulator (BEDT-BDT)AsF6 (BEDT-BDT: benzo[1,2-g:4,5-g′]bis(thieno[2,3-b][1,4dithiin). This AsF6 salt has the same structure as the PF6 salt. Although the anions are disordered, the donor molecules form a θ-type arrangement. The temperature dependence of the resistivity exhibits semiconducting behavior. The static magnetic susceptibility follows Curie–Weiss law over a wide temperature range; however, below 25 K, the magnetic susceptibility is in agreement with a one-dimensional chain model with the exchange coupling J = 7.4 K. No structural phase transition was observed down to 93 K. At 270 K, the Fermi surface calculated by the tight-binding approximation is a two-dimensional cylinder; however, it is significantly distorted at 93 K. This is because the dihedral angles between the BEDT-BDT molecules become larger due to lattice shrinkage at low temperatures, which results in a smaller transfer integral (t1) along the stack direction. This slight change in the dihedral angle gives rise to a significant change in the electronic structure of the AsF6 salt. Radical-cation salts using BEDT-BDT, in which the highest occupied molecular orbital does not have a dominant sign throughout the molecule, are sensitive to slight differences in the overlap between the molecules, and their electronic structures are more variable than those of conventional θ-type conductors.

Highlights

  • IntroductionMolecular conductors have a rich phase diagram, including metallic, charge-densitywave, charge-ordering, spin-Peierls, spin-density-wave, and superconducting states [1]

  • Molecular conductors have a rich phase diagram, including metallic, charge-densitywave, charge-ordering, spin-Peierls, spin-density-wave, and superconducting states [1].In these organic conductors, the transfer integrals have a significant influence on the electronic characteristics

  • We describe the ment, and discuss the characteristics of the molecular orbitals that are peculiar to BEDTcorrelation between the dihedral angle in and transfer integral in the θ-mode arrangement, BDT, which are not found and discuss the characteristics of the molecular orbitals that are peculiar to BEDT-BDT, which are not found in BEDT-TTF

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Summary

Introduction

Molecular conductors have a rich phase diagram, including metallic, charge-densitywave, charge-ordering, spin-Peierls, spin-density-wave, and superconducting states [1]. Radical-cation (RC) salts using BEDT-TTF form >200 types of molecular monotonic stacking. Radical-cation (RC) salts using BEDT-TTF form >200 types of conductors andmolecular realize aconductors wide variety of electronic states of [2]. 0 ]bis(thieno[2,3-b][1,4]dithiin), physical properties [12] Because this material remains paramagnetic even at 2 K, the BEDT-BDT is benzo[1,2-g:4,5-g and reported its structural ground state mayBecause be a quantum spin liquid. Paper, we report and the structural ethylenedithio group is introduced atsalts, the molecular terminal In of this benzodithiophene, it and physical properties of the new RC salt (BEDT-BDT)AsF6. We report the structural the correlation between the dihedral angle and transfer integral in the θ-mode arrangeand physical properties of the new RC salt (BEDT-BDT)AsF6. Discuss the characteristics of the molecular orbitals that are peculiar to BEDT-BDT, which are not found in BEDT-TTF

Experimental Methods
X-ray Diffraction and Structural Analysis
Calculation of Transfer Integrals and Fermi Surfaces
Resistivity Measurements
Magnetic-Susceptibility Measurements
Results and Discussion
Crystal
Temperature dependence of the band dispersions and surfaces of the 6 and
Dihedral-angle
Conclusions
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