Abstract
The paper presents a new solution for sampling rate conversion and processing of harmonic signals with known but possibly varying fundamental frequency. This problem is commonly found in particle accelerators, for tracking the beam signals whose revolution frequency varies during the acceleration ramp. It is also common among many other fields such as speech and music processing, removal of mechanical noises, filtering of biomedical recordings, active crack imaging, etc. The key element in the proposed solution is a new architecture for a Farrow-based resampler, in which the resampling ratio can take any value and can be modified continuously to follow the signal fundamental frequency. The combination of two complementary resamplers creates a processing region where signal synchronous processing is performed. The resampler architecture is optimized for modern FPGA features. It decouples the processing and sampling clocks, and uses a single processing (hardware) clock whose frequency remains fixed. The functional model was migrated to Xilinx System Generator and the overall performance is evaluated with an application that filters a periodic signal whose frequency follows a known linear ramp in the presence of additive white noise.
Highlights
C IRCULAR particle accelerators transfer energy to a beam by successive small momentum kicks
The implementation of the testbench was successfully performed with a target 125 MHz processing clock for two devices, a high-grade FPGA, Xilinx Kintex-7 XCKU0401FFVA1156C and small device Xilinx Artix-7 XC7A75T2FGG484C
The DSP blocks are mainly consumed by the bank of filters of the Variable Fractional Delay (VFD)
Summary
C IRCULAR particle accelerators transfer energy to a beam by successive small momentum kicks. RF power injected into electromagnetic cavities induces electric fields which accelerate the particles at each passage. An increase in energy causes an increase in particle velocity. The effect is very small in relativistic machines, where the energy increase does not result in a significant change in velocity as it saturates at the speed of light, but is significant in smaller machines. Manuscript received May 15, 2019; revised September 3, 2019, October 19, 2019, and December 13, 2019; accepted December 14, 2019. Date of publication January 3, 2020; date of current version May 1, 2020. This article was recommended by Associate Editor G.
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More From: IEEE Transactions on Circuits and Systems I: Regular Papers
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