Abstract

An x-ray free-electron laser (XFEL), SACLA, designed to open up new science, was constructed for generating coherent x rays with a peak power of more than 10 GW and a very short pulse of below 30 fs. This feature demands a very highly short-term temporal stability of less than 50 fs to the acceleration rf field of SACLA. For this reason, we developed a timing and low-level rf (LLRF) system for SACLA based on that of the SPring8 compact SASE source (SCSS) test accelerator for verifying the feasibility of an XFEL. The performance of the system using the in-phase and quadrature rf manipulation method was improved from SCSS's system. Since the facility length of SACLA is 700 m, which is 10 times longer than that of the SCSS test accelerator, a phase-stabilized optical-fiber system designed to transmit time standard rf signals with low loss was also developed and deployed. This optical-fiber system equips fiber optical-length feedback control in order to mitigate environmental effects, such as temperature and humidity changes. On the other hand, the demanded maximum rf temporal stability is less than 50 fs, which is almost 10 times smaller than that of the SCSS test accelerator. Hence, reducing electric noise and increasing the temperature stability around timing and LLRF instruments were necessary and realized with a very low-noise power supply and a hemathermal 19-inch enclosure. The short-term temporal performance of the timing LLRF system finally attained a temporal stability of less than 13.6 fs in rms measured by a beam arrival-time measurement. This stability greatly helps to achieve the stable x-ray lasing of SACLA for routine operation during user experiments.

Highlights

  • An x-ray laser, which is generated by a free-electron laser (XFEL) machine [1], using the self-amplified spontaneous emission (SASE) method, is a dream light source used to explore uncharted science

  • Optical-fiber reference signal transmission using phasestabilized optical fiber (PSOF) with optical-fiber-length control by the Michelson interferometry method was developed to be adapted to large machine size and the required temporal drift stability

  • In order to control the rf phase and amplitude of an acceleration structure, a level rf (LLRF) system based on an in-phase and quadrature (IQ) modulator and a demodulator was designed and constructed

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Summary

INTRODUCTION

An x-ray laser, which is generated by a free-electron laser (XFEL) machine [1], using the self-amplified spontaneous emission (SASE) method, is a dream light source used to explore uncharted science. Based on the bunch-compression methods, as mentioned above, the required temporal stabilities at the cavities along SACLA are tabulated in Table I [6] These values in the table were calculated under the condition where the peak current variation of the electron beam is 10% in rms. When we designed a low-level rf (LLRF) system in order to drive a klystron as a high-power rf source for electron acceleration during the construction stage of SACLA, the first priority was how to realize the demanded temporal stabilities At this point, a short-period temporal jitter of about 50 fs in rms and a temporal drift of over 300 fs in peak-to-peak (P-P) for 12 h of an electron beam were already observed by using our developed LLRF system [7] of the SPring compact SASE source (SCSS) test accelerator [8]. We describe the constructed timing and LLRF system for SACLA, the developed instruments, and its system performance, as one of the possible examples in order to realize the XFEL

System configuration
Master-terminal station
OPT TXU-A and OPT TXU-C
Optical-fiber signal transmission line
Optical-fiber-length control
System configuration of the end-terminal station
IQ modulator and demodulator
Klystron-driving amplifier
Counter for the input pulse
Water-cooled hematothermal 19-inch enclosure
Short-term temporal performances
Long-term temporal performance
Findings
SUMMARY

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