Paper |
Title |
Page |
SUPB031 |
The Nonresonant Perturbation Theory Based Field Measurement and Tuning of a Linac Accelerating Structure |
80 |
|
- W. Fang, Q. Gu, Z.T. Zhao
SINAP, Shanghai, People's Republic of China
- D.C. Tong
TUB, Beijing, People's Republic of China
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Assisted by the bead pull technique, the nonresonant perturbation theory is applied for measuring and tuning the field of the linac accelerating structure. The method is capable of making non-touch measurement, amplitude and phase diagnostics, real time mismatch feedback and field tuning. Main considerations on measurement system and of C-band traveling-wave structure are described, the bead pull measurement and the tuning of the C-band traveling-wave linac accelerating structure are presented.
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SUPB032 |
The C-band RF Pulse Compression for Soft XFEL at SINAP |
83 |
|
- C.P. Wang, Q. Gu, Z.T. Zhao
SINAP, Shanghai, People's Republic of China
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A compact soft X-ray free electron laser facility is presently being constructed at shanghai institute of applied physics (SINAP), Chinese academy of science in 2012 and will be accomplished in 2014. This facility requires a compact linac with a high-gradient accelerating structure for a limited overall length less than 230 m. The c-band technology which is already used in KEK/Spring-8 linear accelerator is a good compromise for this compact facility and a c-and traveling-wave accelerating structure was already fabricated and tested at SINAP, so a c-band pulse compression will be required. AND a SLED type RF compression scheme is proposed for the C-band RF system of the soft XFEL and this scheme uses TE0.1.15 mode energy storage cavity for high Q-energy storage. The C-band pulse compression under development at SINAP has a high power gain about 3.1 and it is designed to compress the pulse width from 2.5 μs to 0.5 μs and multiply the input RF power of 50 MW to generate 160 MW peak RF power, and the coupling coefficient will be 8.5. It has three components: 3 dB coupler, mode convertors and the resonant cavities.
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MOPB086 |
The Nonresonant Perturbation Theory Based Field Measurement and Tuning of a Linac Accelerating Structure |
375 |
|
- W. Fang, Q. Gu, Z.T. Zhao
SINAP, Shanghai, People's Republic of China
- D.C. Tong
TUB, Beijing, People's Republic of China
|
|
|
Assisted by the bead pull technique, the nonresonant perturbation theory is applied for measuring and tuning the field of the linac accelerating structure. The method is capable of making non-touch measurement, amplitude and phase diagnostics, real time mismatch feedback and field tuning. Main considerations on measurement system and of C-band traveling-wave structure are described, the bead pull measurement and the tuning of the C-band traveling-wave linac accelerating structure are presented.
|
|
|
TUPB097 |
The C-band RF Pulse Compression for Soft XFEL at SINAP |
687 |
|
- C.P. Wang, Q. Gu, Z.T. Zhao
SINAP, Shanghai, People's Republic of China
|
|
|
A compact soft X-ray free electron laser facility is presently being constructed at shanghai institute of applied physics (SINAP), Chinese academy of science in 2012 and will be accomplished in 2014. This facility requires a compact linac with a high-gradient accelerating structure for a limited overall length less than 230 m. The c-band technology which is already used in KEK/Spring-8 linear accelerator is a good compromise for this compact facility and a c-and traveling-wave accelerating structure was already fabricated and tested at SINAP, so a c-band pulse compression will be required. AND a SLED type RF compression scheme is proposed for the C-band RF system of the soft XFEL and this scheme uses TE0.1.15 mode energy storage cavity for high Q-energy storage. The C-band pulse compression under development at SINAP has a high power gain about 3.1 and it is designed to compress the pulse width from 2.5 μs to 0.5 μs and multiply the input RF power of 50 MW to generate 160 MW peak RF power, and the coupling coefficient will be 8.5. It has three components: 3 dB coupler, mode convertors and the resonant cavities.
|
|
|