Add to ORKGThe results of the numerical and experimental inves-tigations of the beam RF capture in the booster – fast-cycling proton synchrotron are presented in this report. The existing features of the magnetic field cycle of the accelerator are taken into account in the simulation. The time dependence of the RF voltage as well as the moment of the beam injection (during the field cycle) have been optimized to get the maximum efficiency of the capture. The experimental results giving nearly 100 % beam cap-ture in the Booster are presented
The MW proton source using a rapid cycling synchrotron (RCS) has many challenging aspects, such as (...
High average beam power proton synchrotrons in the medium energy range are under consideration at se...
A study was conducted to measure the effect of the Booster extraction equipment on the dispersion fu...
The injection and capture processes in a high intensity, rapid cycling, proton synchrotron are simul...
Fast-cycling proton synchrotron U-1.5, also known as the IHEP booster, since 1985 serves as an injec...
The difference between the rf voltage seen by the beam and the accelerating voltage required to matc...
The difference between the rf voltage seen by the beam and the accelerating voltage required to matc...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
As part of the effort to increase the number of ions per bunch in RHIC, a new scheme for RF capture ...
The transverse impedance of eight extraction pulsed kicker magnets is a strong beam instability sour...
The Fermilab Booster is a nearly 40-year-old proton synchrotron, designed to accelerate injected pro...
Simulations are presented for a proton accelerator in which a pulsed proton beam is passed through a...
The purpose of this note is to examine the likelihood and problems associated with operation of the ...
Recent efforts at the APS have focused on improving overall injector system reliability and availabi...
A synchrotron construction the magnetic field of which is without steel core is suggested. Accelerat...
The MW proton source using a rapid cycling synchrotron (RCS) has many challenging aspects, such as (...
High average beam power proton synchrotrons in the medium energy range are under consideration at se...
A study was conducted to measure the effect of the Booster extraction equipment on the dispersion fu...
The injection and capture processes in a high intensity, rapid cycling, proton synchrotron are simul...
Fast-cycling proton synchrotron U-1.5, also known as the IHEP booster, since 1985 serves as an injec...
The difference between the rf voltage seen by the beam and the accelerating voltage required to matc...
The difference between the rf voltage seen by the beam and the accelerating voltage required to matc...
Beam loading effects on the rf system of JHF proton synchrotrons have been investigated by both comp...
As part of the effort to increase the number of ions per bunch in RHIC, a new scheme for RF capture ...
The transverse impedance of eight extraction pulsed kicker magnets is a strong beam instability sour...
The Fermilab Booster is a nearly 40-year-old proton synchrotron, designed to accelerate injected pro...
Simulations are presented for a proton accelerator in which a pulsed proton beam is passed through a...
The purpose of this note is to examine the likelihood and problems associated with operation of the ...
Recent efforts at the APS have focused on improving overall injector system reliability and availabi...
A synchrotron construction the magnetic field of which is without steel core is suggested. Accelerat...
The MW proton source using a rapid cycling synchrotron (RCS) has many challenging aspects, such as (...
High average beam power proton synchrotrons in the medium energy range are under consideration at se...
A study was conducted to measure the effect of the Booster extraction equipment on the dispersion fu...