Abstract

Beam loading compensation is a key for acceleration of a high intensity proton beam in the main ring (MR) of the Japan Proton Accelerator Research Complex (J-PARC). Magnetic alloy loaded rf cavities with a Q value of 22 are used to achieve high accelerating voltages without a tuning bias loop. The cavity is driven by a single harmonic ($h=9$) rf signal while the cavity frequency response also covers the neighbor harmonics ($h=8,10$). Therefore the wake voltage induced by the high intensity beam consists of the three harmonics, $h=8,9,10$. The beam loading of neighbor harmonics is the source of periodic transient effects and a possible source of coupled bunch instabilities. In the article, we analyze the wake voltage induced by the high intensity beam. We employ the rf feedforward method to compensate the beam loading of these three harmonics ($h=8,9,10$). The full-digital multiharmonic feedforward system was developed for the MR. We describe the system architecture and the commissioning methodology of the feedforward patterns. The commissioning of the feedforward system has been performed by using high intensity beams with $1.0\ifmmode\times\else\texttimes\fi{}{10}^{14}$ proteins per pulse. The impedance seen by the beam is successfully reduced and the longitudinal oscillations due to the beam loading are reduced. By the beam loading compensation, stable high power beam operation is achieved. We also report the reduction of the momentum loss during the debunching process for the slow extraction by the feedforward.

Highlights

  • The Japan Proton Accelerator Research Complex (J-PARC) is a high intensity proton accelerator facility, which consists of the 181 MeV linac, the 3 GeV rapid cycling synchrotron (RCS), and the 30 GeV main ring (MR) [1,2]

  • The MR delivers the beams to the neutrino experiment and the hadron hall by fast extraction (FX) and slow extraction (SX) schemes, respectively

  • We employ the rf feedforward method for the multiharmonic beam loading compensation, like in the J-PARC RCS, in which the impedance seen by the beam is greatly reduced by the feedforward [11]

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Summary

INTRODUCTION

The Japan Proton Accelerator Research Complex (J-PARC) is a high intensity proton accelerator facility, which consists of the 181 MeV linac, the 3 GeV rapid cycling synchrotron (RCS), and the 30 GeV main ring (MR) [1,2]. A further beam power upgrade is to be done by increasing the beam intensity and by shortening the repetition period In both RCS and MR, the magnetic-alloy (MA) cavities are employed to realize the high accelerating voltage, which is necessary for acceleration of high intensity proton beams. We employ the rf feedforward method for the multiharmonic beam loading compensation, like in the J-PARC RCS, in which the impedance seen by the beam is greatly reduced by the feedforward [11]. The MR LLRF control system has a similar architecture of that of the RCS It consists of the main block and the feedforward block.

WAKE VOLTAGE IN MR CAVITIES
Operational principle of rf feedforward
Function of the feedforward system
COMMISSIONING OF THE FEEDFORWARD SYSTEM
Waveform data processing
Commissioning results
High power operation
Reduction of momentum loss during debunching process for slow extraction
Findings
SUMMARY AND DISCUSSIONS
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