A vortex together with an antivortex form an interacting pair that is localized and has finite energy. A vortex-antivortex pair is thus, surprisingly, a more natural object from a physical and experimental point of view. We have studied theoretically the dynamics of vortex-antivortex dipoles, that is, a vortex together with an antivortex with opposite polarities. By exploiting a link between their topology and their dynamics we find that magnetic vortex-antivortex dipoles are in rotational motion, in stark contrast to vortex-antivortex pairs in fluid dynamics. [Phys. Rev. Lett. 2007].
When we include spin-transfer torque due to a spin-polarized current or the spin-Hall effect, we predict stable magnetization oscillations of the vortex-antivortex dipole due to a totally surprising cooperation of (conservative) Hamiltonian dynamics and of (non-conservative) spin torque forces [Europhys. Lett. 2012].
The equations of motion for point vortices in fluids were given by Helmholtz (1858) and by Kirchoff (1876) as a Hamiltonian system. We studied three point magnetic vortices using a method introduced by Gröbli in his seminal papers in 1877 [Vierteljahrsschrift 22/1, [Vierteljahrsschrift 22/2]. Magnetic vortices have a polarity and this is a feature not found in ordinary fluid vortices. We integrated completely the Hamiltonian system for magnetic vortices using conservation laws. [J. Math. Phys. 2010].