Add to ORKGA broad band RF cavity loaded with magnetic alloy cores has been developed for the Japanese Hadron Facility synchrotrons. Its Q-value can be chosen at between 0.5 and 5. To reduce transient beam loading effects, a small Q-value (< 3) is preferable to shorten the transient period. However, the circulating beam current of up to 7 A will induce a spurious voltage at the accelerating gap, which deforms the gap voltage due to higher harmonics compo-nents, if the Q-value is less than 3. The resulting RF-bucket distortion may cause the beam loss. Therefore we have designed a beam loading compensation system to sup-press the higher harmonics components.
A RF acceleration system has been designed for the Joint Project for High-Intensity Proton Accelerat...
When a high-intensity beam with bunch-trains and gaps passes a cavity with a high-gain vector feedba...
We report on the commissioning of a higher harmonic radiofrequency system at the Advanced Light Sour...
A broad band RF cavity loaded with magnetic alloy cores has been developed for the Japanese Hadron F...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
Beam loading compensation is a key for acceleration of a high intensity proton beam in the main ring...
Double rf systems are used to lengthen the beam bunches in synchrotron light sources. In such a syst...
The power consumption of the rf system can be minimised by optimising the cavity detuning and the lo...
In a high intensity proton synchrotron, the wall current induced by the beam in an RF cavity can not...
A narrowband beam loading compensation system was installed for the Main Injector Accelerating Cavit...
A narrowband beam loading compensation system was installed for the Main Injector Accelerating Cavit...
Based on the measurements of the magnetic cores and R&D works, MA(Magnetic Alloy)-loaded cavity ...
Beam loading effects on the rf system of JHF proton syn-chrotrons have been investigated by both com...
Synchrotron radiation is a tool widely used in science. It is produced by electron accelerators call...
In the J-PARC Rapid Cycling Synchrotron (RCS), the heavy beam loading effects due to the high intens...
A RF acceleration system has been designed for the Joint Project for High-Intensity Proton Accelerat...
When a high-intensity beam with bunch-trains and gaps passes a cavity with a high-gain vector feedba...
We report on the commissioning of a higher harmonic radiofrequency system at the Advanced Light Sour...
A broad band RF cavity loaded with magnetic alloy cores has been developed for the Japanese Hadron F...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
Beam loading compensation is a key for acceleration of a high intensity proton beam in the main ring...
Double rf systems are used to lengthen the beam bunches in synchrotron light sources. In such a syst...
The power consumption of the rf system can be minimised by optimising the cavity detuning and the lo...
In a high intensity proton synchrotron, the wall current induced by the beam in an RF cavity can not...
A narrowband beam loading compensation system was installed for the Main Injector Accelerating Cavit...
A narrowband beam loading compensation system was installed for the Main Injector Accelerating Cavit...
Based on the measurements of the magnetic cores and R&D works, MA(Magnetic Alloy)-loaded cavity ...
Beam loading effects on the rf system of JHF proton syn-chrotrons have been investigated by both com...
Synchrotron radiation is a tool widely used in science. It is produced by electron accelerators call...
In the J-PARC Rapid Cycling Synchrotron (RCS), the heavy beam loading effects due to the high intens...
A RF acceleration system has been designed for the Joint Project for High-Intensity Proton Accelerat...
When a high-intensity beam with bunch-trains and gaps passes a cavity with a high-gain vector feedba...
We report on the commissioning of a higher harmonic radiofrequency system at the Advanced Light Sour...