Abstract
We present extensive Monte Carlo simulations for a classical antiferromagnetic Heisenberg model with both nearest (J1) and next-nearest (J2) exchange couplings on the square lattice coupled to the lattice degrees of freedom. The Ising-like phase transition, which appears for J2/J1>1/2 in the pure spin model, is strengthened by the spin-lattice coupling and is accompanied by a lattice deformation from a tetragonal symmetry to an orthorhombic one. Evidence that the universality class of the transition does not change with the inclusion of the spin-lattice coupling is reported. Implications for Li2VOSiO4, the prototype for a layered J1−J2 model in the collinear regime, are also discussed.
Original language | English |
---|---|
Article number | 024449 |
Pages (from-to) | N/A |
Number of pages | 6 |
Journal | Physical Review B |
Volume | 72 |
Issue number | 2 |
DOIs | |
Publication status | Published - 22 Jul 2005 |