The Development of the Electrically Controlled High Power RF Switch and Its Application to Active RF Pulse Compression Systems

Abstract

In the past decades, there has been increasing interest in pulsed high power RF sources for building high-gradient high-energy particle accelerators. Passive RF pulse compression systems have been used in many applications to match the available RF sources to the loads requiring higher RF power but a shorter pulse. Theoretically, an active RF pulse compression system has the advantage of higher efficiency and compactness over the passive system. However, the key component for such a systeman element capable of switching hundreds of megawatts of RF power in a short time compared to the compressed pulse width -is still an open problem.In this dissertation, we present a switch module composed of an active window based on the bulk effects in semiconductor, a circular waveguide three-port network and a movable short plane, with the capability to adjust the S-parameters before and after switching. The RF properties of the switch module were analyzed. We give the scaling laws of the multiple-element switch systems, which allow the expansion of the system to a higher power level.We present a novel overmoded design for the circular waveguide three-port network and the associated circular-to-rectangular mode-converter. We also detail the design and synthesis process of this novel mode-converter.We demonstrate an electrically controlled ultra-fast high power X-band RF active window built with PIN diodes on high resistivity silicon. The window is capable of handling multi-megawatt RF power and can switch in 2-300ns with a 1000A current driver. A low power active pulse compression experiment was carried out with the switch vi module and a 375ns resonant delay line, obtaining 8 times compression gain with a compression ratio of 20.vii ACKNOWLEDGMENTS

Design and Prototyping of the Electron Ion Collider Electron Storage Ring SRF cavity

“…The main concern for this tuner is the strong standing wave between the tuner and the FPC. The analysis in this paper is based on one single matched T [7] on each FPC, as shown in Fig. 2.…”