Simulations show a persisting slow emittance growth for electron cloud densities below the threshold of the fast Transverse Mode Coupling type instability, which could prove important for proton beams with negligible radiation damping, such as in the LHC. We report on a variety of studies performed to quantify the contributions to the simulated emittance growth from numerical noise in the PIC module and from an artificial resonance excitation due to the finite number of kicks per turn applied for modeling the cloud-bunch interaction
The results of an experiment aiming at colliding high brightness bunches at 6.5 TeV in the LHC and p...
After a successful scrubbing run in the beginning of 2011, the LHC can be presently operated with hi...
In positron and proton storage rings, electrons produced by photoemission, ionization, and secondary...
The electron cloud may cause transverse single-bunch instabilities of proton beams such as those in ...
The emittance growth caused by an electron cloud is simulated by the HEADTAIL code with conducting b...
Recent observations at the LHC indicate the build-up of electron clouds when 50 ns spaced beams are ...
Electron cloud effects are serious issue for LHC and future hadron colliders, FCC-hh. Electron cloud...
In proton and positron storage rings with many closely spaced bunches, a large number of electrons c...
After a successful scrubbing run in the beginning of 2011, the LHC can be presently operated with hi...
In the beam pipe of the Damping Ring (DR) of a linear collider, an electron cloud may be produced by...
Strong-strong beam-beam simulations are employed to investigate the noise sensitivity of the emittan...
The interplay between head-on beam-beam interaction and external sources of noise can be a significa...
A vertical emittance growth (beam size blow-up) due to electron cloud has been observed in the posit...
The problem of emittance growth due to random fluctuations of the magnetic field in a hadron collide...
In this paper, the effects of electron cloud are discussed for the ultra low emittance positron beam...
The results of an experiment aiming at colliding high brightness bunches at 6.5 TeV in the LHC and p...
After a successful scrubbing run in the beginning of 2011, the LHC can be presently operated with hi...
In positron and proton storage rings, electrons produced by photoemission, ionization, and secondary...
The electron cloud may cause transverse single-bunch instabilities of proton beams such as those in ...
The emittance growth caused by an electron cloud is simulated by the HEADTAIL code with conducting b...
Recent observations at the LHC indicate the build-up of electron clouds when 50 ns spaced beams are ...
Electron cloud effects are serious issue for LHC and future hadron colliders, FCC-hh. Electron cloud...
In proton and positron storage rings with many closely spaced bunches, a large number of electrons c...
After a successful scrubbing run in the beginning of 2011, the LHC can be presently operated with hi...
In the beam pipe of the Damping Ring (DR) of a linear collider, an electron cloud may be produced by...
Strong-strong beam-beam simulations are employed to investigate the noise sensitivity of the emittan...
The interplay between head-on beam-beam interaction and external sources of noise can be a significa...
A vertical emittance growth (beam size blow-up) due to electron cloud has been observed in the posit...
The problem of emittance growth due to random fluctuations of the magnetic field in a hadron collide...
In this paper, the effects of electron cloud are discussed for the ultra low emittance positron beam...
The results of an experiment aiming at colliding high brightness bunches at 6.5 TeV in the LHC and p...
After a successful scrubbing run in the beginning of 2011, the LHC can be presently operated with hi...
In positron and proton storage rings, electrons produced by photoemission, ionization, and secondary...