The relaxation phenomena of spin-torque oscillators consisting of
nanostructured ferromagnets are interesting research targets in magnetism. A
theoretical study on the relaxation time of a spin-torque oscillator from one
self-oscillation state to another is investigated. By solving the
Landau-Lifshitz-Gilbert equation both analytically and numerically, it is shown
that the oscillator relaxes to the self-oscillation state exponentially within
a few nanoseconds, except when magnetization is close to a critical point. The
relaxation rate, which is an inverse of relaxation time, is proportional to the
current. On the other hand, a critical slowing down appears near the critical
point, where relaxation is inversely proportional to time, and the relaxation
time becomes on the order of hundreds of nanoseconds. These conclusions are
primarily obtained for a spin-torque oscillator consisting of a perpendicularly
magnetized free layer and an in-plane magnetized pinned layer, and are further
developed for application to arbitrary types of spin-torque oscillators.Comment: 13 pages, 7 figure