Abstract

The low level rf system for the superconducting Darmstadt electron linear accelerator (S-DALINAC) developed 20 years ago and operating since converts the 3 GHz signals from the cavities down to the baseband and not to an intermediate frequency. While designing the new, digital rf control system this concept was kept: the rf module does the $I/Q$ and amplitude modulation/demodulation while the low frequency board, housing an field programmable gate array analyzes and processes the signals. Recently, the flexibility of this concept was realized: By replacing the modulator/demodulators on the rf module, cavities operating at frequencies other than the one of the S-DALINAC can be controlled with only minor modifications: A 6 GHz version, needed for a harmonic bunching system at the S-DALINAC and a 324 MHz solution to be used on a room temperature cavity at GSI, are currently under design. This paper reviews the concept of the digital low level rf control loops in detail and reports on the results gained during first operation with a superconducting cavity.

Highlights

  • The superconducting Darmstadt electron linear accelerator (S-DALINAC) [1] is a recirculating linac with beam currents of up to 60 A and a maximum energy of 130 MeV

  • Even when the sc cavities are strongly coupled with a loaded quality factor of 3 Â 107, which leads to a resonance width of some 100 Hz, they are very sensitive against microphonic perturbations [2]

  • The low frequency signals, amplitude and the demodulated I=Q phasors are transmitted as analogue signals to the new field programmable gate array (FPGA) board, where they are digitized and processed

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Summary

INTRODUCTION

The superconducting Darmstadt electron linear accelerator (S-DALINAC) [1] is a recirculating linac with beam currents of up to 60 A and a maximum energy of 130 MeV It is primarily used for experiments in nuclear physics since it has been first put into operation in 1987. In order to achieve the recommended energy spread of Æ1 Â 10À4 at the experimental areas, the amplitude and phase of the cavities have to be controlled strictly to compensate the impact of microphonic perturbations.

CONTROL LOOP PRINCIPLE
PRESENT RF CONTROL SYSTEM
Layout
FPGA board
RF board
Control algorithm
Performance
CONCLUSIONS
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