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 ...
When a high-intensity beam with bunch-trains and gaps passes a cavity with a high-gain vector feedba...
In the J-PARC RCS (Rapid Cycling Synchrotron) we employ a full-digital LLRF control system to accele...
Beam loading effects on rf system is one of the most diffi-cult parts of high intensity proton synch...
In the J-PARC Rapid Cycling Synchrotron (RCS), the heavy beam loading effects due to the high intens...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
We have developed an RF acceleration system for a medical proton synchrotron. The RF cavity is a tun...
We have developed an RF acceleration system for a medical proton synchrotron. The RF cavity is a tun...
A broad band RF cavity loaded with magnetic alloy cores has been developed for the Japanese Hadron F...
A broad band RF cavity loaded with magnetic alloy cores has been developed for the Japanese Hadron F...
In a high intensity proton synchrotron, the wall current induced by the beam in an RF cavity can not...
The accelerator of the J-PARC complex consists of the 400MeV (initially 181MeV) linac, the rapid cyc...
In the framework of the LHC Injectors Upgrade project (LIU), a complete replacement of the existing ...
A major challenge in the design of rf cavities for the acceleration of medium-energy charged ions is...
Longitudinal coupled-bunch instabilities after transition crossing and at the flat-top limit the int...
In the Proton Synchrotron (PS), where the LHC protons longitudinal structure (bunch spacing) is dete...
When a high-intensity beam with bunch-trains and gaps passes a cavity with a high-gain vector feedba...
In the J-PARC RCS (Rapid Cycling Synchrotron) we employ a full-digital LLRF control system to accele...
Beam loading effects on rf system is one of the most diffi-cult parts of high intensity proton synch...
In the J-PARC Rapid Cycling Synchrotron (RCS), the heavy beam loading effects due to the high intens...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
We have developed an RF acceleration system for a medical proton synchrotron. The RF cavity is a tun...
We have developed an RF acceleration system for a medical proton synchrotron. The RF cavity is a tun...
A broad band RF cavity loaded with magnetic alloy cores has been developed for the Japanese Hadron F...
A broad band RF cavity loaded with magnetic alloy cores has been developed for the Japanese Hadron F...
In a high intensity proton synchrotron, the wall current induced by the beam in an RF cavity can not...
The accelerator of the J-PARC complex consists of the 400MeV (initially 181MeV) linac, the rapid cyc...
In the framework of the LHC Injectors Upgrade project (LIU), a complete replacement of the existing ...
A major challenge in the design of rf cavities for the acceleration of medium-energy charged ions is...
Longitudinal coupled-bunch instabilities after transition crossing and at the flat-top limit the int...
In the Proton Synchrotron (PS), where the LHC protons longitudinal structure (bunch spacing) is dete...
When a high-intensity beam with bunch-trains and gaps passes a cavity with a high-gain vector feedba...
In the J-PARC RCS (Rapid Cycling Synchrotron) we employ a full-digital LLRF control system to accele...
Beam loading effects on rf system is one of the most diffi-cult parts of high intensity proton synch...