Inverse transition in the dipolar frustrated Ising ferromagnet: the role of domain walls

TL;DR

This study investigates the inverse symmetry breaking transition in ultrathin magnetic films, emphasizing the crucial role of domain wall degrees of freedom and their impact on phase behavior and stripe width divergence.

Contribution

It demonstrates that internal degrees of freedom of domain walls are essential for the inverse transition, contrasting with sharp domain wall models which lack this phenomenon.

Findings

Domain wall degrees of freedom increase entropy at high temperatures.

Inverse transition occurs as domain walls narrow and freeze at lower temperatures.

Stripe width diverges near the critical field, indicating a continuous phase transition.

Abstract

We present a theoretical study aimed to elucidate the origin of the inverse symmetry breaking transition observed in ultrathin magnetic films with perpendicular anisotropy. We study the behavior of the dipolar frustrated Ising model in a mean field approximation as well as two other models with simple domain walls. By a numerical analysis we show that the internal degrees of freedom of the domain walls are decisive for the presence of the inverse symmetry breaking transition. In particular, we show that in a sharp domain wall model the inverse transition is absent. At high temperatures the additional degrees of freedom of the extended domain walls increase the entropy of the system leading to a reduction of the free energy of the stripe phase. Upon lowering the temperature the domain walls become narrow and with the corresponding degrees of freedom effectively frozen, which eventually induces an inverse transition to the competing homogeneous phase. We also show that, for growing external field at constant temperature, the stripe width grows strongly when approaching the critical field line and diverges at the transition. These results indicate that the inverse transition is a continuous phase transition and that the domain wall profiles as well as the temperature has little effect on the critical behavior of the period of the domain as function of the applied field.