Local magnetic moments due to loop currents in metals
arXiv:2208.05587 · doi:10.1103/PhysRevB.106.214419
Abstract
We present Hartree-Fock calculations on a simple model to obtain the conditions of formation of local magnetic moments due to loop-currents and spin-loop currents and compare them to the conditions of formation of local spin-moments which were given long ago in a similar approximation by Anderson. A model with three degenerate orbitals sitting on an equilateral triangle, with on-site and nearest-neighbor repulsions and respectively, and inter-site kinetic energy, hybridizing with conduction electrons with a parameter is investigated. and are promoted by large and their magnitude is relatively unaffected by . Spin-magnetic moments promoted by large on the other hand are adversely affected by . In this model, for multiplied by the number of neighbors is approximately the same as the promoted by in Anderson's local model for . and are degenerate if exchange interactions and Hund's rule are neglected but is favored when they are included. Many of the qualitative results are visible in an expression for the Hartree-Fock ground state energy derived as a function of small and . Numerical minimization of the Hartree-Fock energy is presented for larger values. We also briefly discuss the connection and differences of the interaction generated orbital currents and spin-currents discussed here and generalized to a lattice with the topological states in metals and semi-conductors.
arXiv comment7 pages
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