Dipolar needles in the microcanonical ensemble: evidence of spontaneous magnetization and ergodicity breaking
arXiv:1305.5331 · doi:10.1209/0295-5075/104/17011
Abstract
We have studied needle shaped three-dimensional classical spin systems with purely dipolar interactions in the microcanonical ensemble, using both numerical simulations and analytical approximations. We have observed spontaneous magnetization for different finite cubic lattices. The transition from the paramagnetic to the ferromagnetic phase is shown to be first-order. For two lattice types we have observed magnetization flips in the phase transition region. In some cases, gaps in the accessible values of magnetization appear, a signature of the ergodicity breaking found for systems with long-range interactions. We analytically explain these effects by performing a nontrivial mapping of the model Hamiltonian onto a one-dimensional Ising model with competing antiferromagnetic nearest-neighbor and ferromagnetic mean-field interactions. These results hint at performing experiments on isolated dipolar needles in order to verify some of the exotic properties of systems with long-range interactions in the microcanonical ensemble.
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Cited by in corpus (8)
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- Direction of cascades in a magnetofluid model with electron skin depth and ion sound Larmor radius scales
- Dynamics and thermodynamics of a pair of interacting magnetic dipoles
- Effective negative specific heat by destabilization of metastable states in dipolar systems
- Spin waves in rings of classical magnetic dipoles