I. Introduction
The modern superconducting linear accelerator facilities, such as the European X-ray Free Electron Laser (XFEL), use precisely controlled radio frequency (RF) field for electron beam acceleration [1]. The field parameter control is performed by a low-level radio frequency (LLRF) control system [2]–[5] that should ensure up to 0.01% of amplitude and 0.01° of phase regulation accuracy while parallel processing of about 100 RF signals from cavities. Such requirements make the design of the LLRF system a very challenging task that requires using state-of-the-art technology.