On biquadratic exchange interactions in spin-1 systems

O. F. de Alcantara Bonfim, F.C. SāBarreto

Rudavsky, Vatamaniuk, S. V. Savenko

Frédéric Mila, Fu‐Chun Zhang

K. Nagata, I. Yamamoto

Mariya Iv. Trukhanova, Pavel A. Andreev

There is a version of the Landau–Lifshitz equation that takes into account the Coulomb exchange interactions between atoms, expressed by the term $${\sim}\mathbf{s}\times\triangle\mathbf{s}$$ . On the other hand, ions in magnetic materials have several valence electrons on the $$d$$ -shell, and, therefore, the Hamiltonian of many-electron atoms with spins $$S>1$$ should include a biquadratic exchange interaction. We propose a novel fundamental microscopic derivation of the spin density evolution equation with an explicit form of biquadratic exchange interaction using the method of many-particle quantum hydrodynamics. The equation for the spin density evolution is obtained from the many-particle Schrödinger–Pauli equation and contains the contributions of the usual Coulomb exchange interaction and the biquadratic exchange. Furthermore, the derived biquadratic exchange torque in the spin density evolution equation is proportional to the nematic tensor for the medium of atoms with spin $$S=1$$ . Our method may be very attractive for further studies of the magnetoelectric effect in multiferroics.

O. Vatamaniuk, Yu. K. Rudavskii

Abstract A spin‐one Ising model with biquadratic exchange interaction is investigated within a functional integration approach. The phase diagram is analyzed by means of Landau's free energy expansion. The dependence of the features of the system on the ratio of bilinear to biquadratic exchange interaction constants is discussed. In the random phase approximation, expressions for phase transition temperatures and the tricritical point for the ferromagnetic transition are obtained.