Abstract

We have developed a new full 3D approach for the electromagnetic and beam dynamics design and simulation of a radio-frequency quadrupole (RFQ). A detailed full 3D model including vane modulation was simulated, which was made possible by the ever advancing computing capabilities. The electromagnetic (EM) design approach was first validated using experimental measurements on an existing prototype RFQ and more recently on the actual full size RFQ. Two design options have been studied, the original with standard sinusoidal modulation over the full length of the RFQ; in the second design, a trapezoidal modulation was used in the accelerating section of the RFQ to achieve a higher energy gain for the same power and length. A detailed comparison of both options is presented supporting our decision to select the trapezoidal design. The trapezoidal modulation increased the shunt impedance of the RFQ by 34%, the output energy by 15% with a similar increase in the peak surface electric field, but practically no change in the dynamics of the accelerated beam. The beam dynamics simulations were performed using three different field methods. The first uses the standard eight-term potential to derive the fields, the second uses 3D fields from individual cell-by-cell models, and the third uses the 3D fields for the whole RFQ as a single cavity. A detailed comparison of the results from TRACK shows a very good agreement, validating the 3D fields approach used for the beam dynamics studies. The EM simulations were mainly performed using the CST Microwave-Studio with the final results verified using other software. Detailed segment-by-segment and full RFQ frequency calculations were performed and compared to the measured data. The maximum frequency deviation is about 100 kHz. The frequencies of higher-order modes have also been calculated and finally the modulation and tuners effects on both the frequency and field flatness have been studied. We believe that with this new full 3D approach, the enhanced computing capabilities and the calculation precision the electromagnetic design software offer, we may be able to skip the prototyping phase and build the final product at once, although we recognize that prototyping is still needed to establish and validate the fabrication procedure.

Highlights

  • Since its invention by Kapchinsky and Teplyakov [1], the radio-frequency quadrupole (RFQ) has become an essential part of proton and heavy-ion accelerators

  • In the new full 3D approach developed in this work, we have modeled the full five-segment 4-m long ATLAS upgrade RFQ [6] in MWS

  • The beam dynamics design and simulation section presents a benchmark of the full 3D field approach and a detailed comparison between the sinusoidal and trapezoidal design options of the RFQ

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Summary

INTRODUCTION

Since its invention by Kapchinsky and Teplyakov [1], the radio-frequency quadrupole (RFQ) has become an essential part of proton and heavy-ion accelerators. The beam dynamics and the electromagnetic design of a RFQ are usually done separately using different tools. In the new full 3D approach developed in this work, we have modeled the full five-segment 4-m long ATLAS upgrade RFQ [6] in MWS. Verifying the beam dynamics using 3D fields from the electromagnetic design software provides a more consistent way for design evaluation. The beam dynamics design and simulation section presents a benchmark of the full 3D field approach and a detailed comparison between the sinusoidal and trapezoidal design options of the RFQ. The electromagnetic design section compares the calculated frequencies to the measured values and presents the effects of modulation and tuners on the frequency and field flatness. A comparison of the peak surface electric fields between the sinusoidal and trapezoidal designs is presented as well

DESIGN CONSIDERATIONS
Full-vane versus split-coaxial design
RFQ length and power management
External versus internal bunching
Input and output radial matchers
Trapezoidal versus sinusoidal modulation
RFQ DESIGN GOALS AND APPROACH
BEAM DYNAMICS DESIGN AND SIMULATIONS
Cell-by-cell 3D models versus the eight-term potential
Full-cavity 3D model versus cell-by-cell model
Beam dynamics: trapezoidal versus sinusoidal
Effect of nonvanishing field in the end gaps
Effect of aperture model choice
Effect of vane modulation errors
ELECTROMAGNETIC DESIGN AND SIMULATIONS
Frequency calculation
Neighboring modes
Modulation effect
Tuners effect
Peak fields: trapezoidal versus sinusoidal
Findings
CONCLUSIONS
Full Text
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