“…This recovery rate depends not only on materials but also on the underlying nanostructure, pump-laser fluence, and other factors; thus, this process is not easily modeled. 5,[14][15][16] Here, we assume that the oscillation signals can be fitted to a damped-harmonic function added to an exponential-decaying background that is characterized by several time-independent parameters; specifically, we have a + b exp͑−t͒ + c sin͑2ft + ͒exp͑−t / ͒, where a and b are the background magnitudes and is the background recovery rate. Parameters c, f, , and are the amplitude, frequency, phase, and relaxation time of magnetization precession, respectively, as used previously.…”