Add to ORKGBeam loading effects on the rf system of JHF proton syn-chrotrons have been investigated by both computer simu-lation and experiment using a low energy electron beam. From the simulation results, it is found that even under the heavy beam loading the beam acceleration becomes stable if applying the beam loading compensation, and the com-pensation experiment is succeeded on proto-type Magnetic Alloy loaded cavity.
A RF acceleration system has been designed for the Joint Project for High-Intensity Proton Accelerat...
For the high-intensity electron linacs, one of the noble schemes to get a sufficient intensity is to...
The accelerator of the J-PARC complex consists of the 400MeV (initially 181MeV) linac, the rapid cyc...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
Beam loading effects on rf system is one of the most diffi-cult parts of high intensity proton synch...
In a high intensity proton synchrotron, the wall current induced by the beam in an RF cavity can not...
Beam loading compensation is a key for acceleration of a high intensity proton beam in the main ring...
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...
Beam loading of the radio-frequency (rf) accelerating cavities is an important consideration in the ...
In the J-PARC Rapid Cycling Synchrotron (RCS), the heavy beam loading effects due to the high intens...
The behavior of the CTF2 drive beam is studied through the first elements of the line for a bunch tr...
The power consumption of the rf system can be minimised by optimising the cavity detuning and the lo...
Beam-beam effects of the ring-ring scheme of FCC-he and LHeC are being studied using weak-strong sim...
Based on the measurements of the magnetic cores and R&D works, MA(Magnetic Alloy)-loaded cavity ...
A RF acceleration system has been designed for the Joint Project for High-Intensity Proton Accelerat...
For the high-intensity electron linacs, one of the noble schemes to get a sufficient intensity is to...
The accelerator of the J-PARC complex consists of the 400MeV (initially 181MeV) linac, the rapid cyc...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
Beam loading effects on rf system is one of the most diffi-cult parts of high intensity proton synch...
In a high intensity proton synchrotron, the wall current induced by the beam in an RF cavity can not...
Beam loading compensation is a key for acceleration of a high intensity proton beam in the main ring...
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...
Beam loading of the radio-frequency (rf) accelerating cavities is an important consideration in the ...
In the J-PARC Rapid Cycling Synchrotron (RCS), the heavy beam loading effects due to the high intens...
The behavior of the CTF2 drive beam is studied through the first elements of the line for a bunch tr...
The power consumption of the rf system can be minimised by optimising the cavity detuning and the lo...
Beam-beam effects of the ring-ring scheme of FCC-he and LHeC are being studied using weak-strong sim...
Based on the measurements of the magnetic cores and R&D works, MA(Magnetic Alloy)-loaded cavity ...
A RF acceleration system has been designed for the Joint Project for High-Intensity Proton Accelerat...
For the high-intensity electron linacs, one of the noble schemes to get a sufficient intensity is to...
The accelerator of the J-PARC complex consists of the 400MeV (initially 181MeV) linac, the rapid cyc...