Introduction
The control of the of the output power of semiconductor microwave oscillators by the bias changing on the one hand is the attractive one because of its simplicity [1], but on the other hand there is several difficulties. For example, to achieve hard-driving amplitude modulation the bias variation must be comparable to the active element bias voltage. At that the change of the stationary electrical and thermal mode of an active element [2]–[5], which can accompany with the rise of the complicated dynamic operation modes, namely: subharmonics generation, frequency and amplitude modulation, chaotic oscillations [6]–[12].