Abstract

We investigate the anisotropic spin motive force in α-(BEDT-TTF)2I3, which is a multi-layered massless Dirac fermion system under pressure. Assuming the interlayer antiferromagnetic interaction and the interlayer anisotropic ferromagnetic interaction, we numerically examine the spin ordered state of the ground state using the steepest descent method. The anisotropic interaction leads to the anisotropic spin ordered state. We calculate the spin motive force produced by the anisotropic spin texture. The result quantitatively agrees with the experiment.

Highlights

  • An organic conductor α-(BEDT-TTF)2 I3 is a multi-layered massless Dirac fermion system, in which conduction layers of BEDT-TTF molecules and I3 anions stack alternatively

  • We show that anisotropic spin ordered states are realized in α-(BEDT-TTF)2 I3 because of the interlayer anisotropic interaction and anisotropic spin motive forces are produced under magnetic field

  • We investigate the spin ordered state of the ground state using the steepest descent method

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Summary

Introduction

An organic conductor α-(BEDT-TTF)2 I3 is a multi-layered massless Dirac fermion system, in which conduction layers of BEDT-TTF molecules and I3 anions stack alternatively. The spin motive force produces the voltage. We show that anisotropic spin ordered states are realized in α-(BEDT-TTF)2 I3 because of the interlayer anisotropic interaction and anisotropic spin motive forces are produced under magnetic field. For simplicity, we take a square lattice in x-z plane in this calculation and assume the magnetic field is parallel to the z-axis.

Results
Conclusion

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