We study Ising antiferromagnets that have nearest-neighbour interactions on multilayer triangular lattices with frustrated (abc and abab) stacking, and make comparisons with the unfrustrated (aaa) stacking. If interlayer couplings are much weaker than in-plane ones, the paramagnetic phase of models with frustrated stackings has a classical spin-liquid regime at low temperature, in which correlations are strong both within and between planes, but there is no long-range order. We investigate this regime using Monte Carlo simulations and by mapping the spin models to coupled height models, which are treated using renormalisation group methods and an analysis of the effects of vortex excitations. The classical spin-liquid regime is parametrical...
An Ising antiferromagnet on a stacked triangular lattice in zero field is studied by Monte Carlo sim...
A great deal of attention has been given in recent years to the search for spin systems, both theore...
We show that the honeycomb Heisenberg antiferromagnet with J(1)/2 = J(2) = J(3), where J(1), J(2), a...
International audienceWe study Ising antiferromagnets that have nearest-neighbor interactions on mul...
We study the triangular-lattice Ising model with dipolar interactions, inspired by its realisation i...
In this thesis, the physics of two systems is investigated, both of which support unconventional ph...
We analyze the formation of stripe-like and droplet-like superstructures in a plane with classical m...
In this doctoral dissertation, we investigate two magnetic systems on the triangular lattice. The ge...
5siWe investigate the spin-1/2 Heisenberg model on the triangular lattice in the presence of nearest...
The triangular lattice with Ising magnetic moments is an archetypical example of geometric frustrati...
In this article we review the effects of magnetic frustration in the stacked triangular lattice. Fru...
The triangular lattice with Ising magnetic moments is an archetypical example of geometric frustrati...
The antiferromagnetic Heisenberg model on the triangular lattice is perhaps the best known example o...
We show how spin-liquid (SL) states can be stabilized in a realistic three-dimensional model as a re...
Using a specially designed Monte Carlo algorithm with directed loops, we investigate the triangular ...
An Ising antiferromagnet on a stacked triangular lattice in zero field is studied by Monte Carlo sim...
A great deal of attention has been given in recent years to the search for spin systems, both theore...
We show that the honeycomb Heisenberg antiferromagnet with J(1)/2 = J(2) = J(3), where J(1), J(2), a...
International audienceWe study Ising antiferromagnets that have nearest-neighbor interactions on mul...
We study the triangular-lattice Ising model with dipolar interactions, inspired by its realisation i...
In this thesis, the physics of two systems is investigated, both of which support unconventional ph...
We analyze the formation of stripe-like and droplet-like superstructures in a plane with classical m...
In this doctoral dissertation, we investigate two magnetic systems on the triangular lattice. The ge...
5siWe investigate the spin-1/2 Heisenberg model on the triangular lattice in the presence of nearest...
The triangular lattice with Ising magnetic moments is an archetypical example of geometric frustrati...
In this article we review the effects of magnetic frustration in the stacked triangular lattice. Fru...
The triangular lattice with Ising magnetic moments is an archetypical example of geometric frustrati...
The antiferromagnetic Heisenberg model on the triangular lattice is perhaps the best known example o...
We show how spin-liquid (SL) states can be stabilized in a realistic three-dimensional model as a re...
Using a specially designed Monte Carlo algorithm with directed loops, we investigate the triangular ...
An Ising antiferromagnet on a stacked triangular lattice in zero field is studied by Monte Carlo sim...
A great deal of attention has been given in recent years to the search for spin systems, both theore...
We show that the honeycomb Heisenberg antiferromagnet with J(1)/2 = J(2) = J(3), where J(1), J(2), a...