I. Introduction
High-power microwave (HPM) sources in a pulsed operation regime allows converting electron beam energy into HPM radiation with efficiency up to 70% and producing microwave output power up to 10 GW [1]. One of key problems in progress of HPM sources is the pulse shortening with increase of microwave power. Nature of that is complicated because of many causes are involved but basically all of them converge in several scenarios, namely, a reduction in the accelerating gap due to the expansion of the plasma of the explosive-emission cathode, beam instabilities, and formation of secondary plasma associated with processes inside a slow-wave structure (SWS), including field electron emission, explosive electron emission, secondary emission (multipactor effect), gas desorption and ionization [2]–[6]. Secondary plasma is the most critical cause because it manifests itself faster than gap shortening and beam instabilities [4], [5].