Emittance growth of the beam caused by power supply ripple in the Superconducting Super Collider (SSC) is studied. We find that due to nonlinear terms in the equation of the betatron oscillations, the emittance grows only during an initial transient period, after which its increase saturates at some level. An analytical formula is derived that gives the fractional increase of the emittance as a function of the amplitude of the ripple. Numerical estimates for the SSC are presented
In colliders with asymmetric rigidity such as the proposed Large Hadron electron Collider, jitter in...
Random fluctuations in the tune, beam offsets, and beam size in the presence of the beam-beam intera...
During LHC Run 1 about 30 % of the potential peak performance was lost due to transverse emittance b...
Analytical estimation of the transverse emittance growth due to a point-like perturbation is perform...
The problem of emittance growth due to random fluctuations of the magnetic field in a hadron collide...
Incoherent emittance growth caused by a strong nonlinear interaction between beam and electron cloud...
The results of collective simulation of a typical TeV Energy Superconducting Linear Accelerator (TES...
If the energies of individual particles in a bunch change as the bunch traverses a bending system, e...
Abstract i%‘e investigate the consequences of the quantum fluctuations associated with synchrotron r...
Preserving the beam size (or equivalently the emittance) is a primary aim of accelerator physics. He...
The three main components of the dipole wakefield in the collider arcs are the resistive wall wake d...
In this paper, we estimate the emittance growth in the LHeC recirculating Linac, the lattice design ...
In this paper, we estimate the emittance growth in the LHeC recirculating Linac, the lattice design ...
Multi-particle simulations are performed to study emittance growth in the Fermilab Booster. Analysis...
Turn-by-turn beam profile data measured at the Fermilab Booster are studied. Lattice models with exp...
In colliders with asymmetric rigidity such as the proposed Large Hadron electron Collider, jitter in...
Random fluctuations in the tune, beam offsets, and beam size in the presence of the beam-beam intera...
During LHC Run 1 about 30 % of the potential peak performance was lost due to transverse emittance b...
Analytical estimation of the transverse emittance growth due to a point-like perturbation is perform...
The problem of emittance growth due to random fluctuations of the magnetic field in a hadron collide...
Incoherent emittance growth caused by a strong nonlinear interaction between beam and electron cloud...
The results of collective simulation of a typical TeV Energy Superconducting Linear Accelerator (TES...
If the energies of individual particles in a bunch change as the bunch traverses a bending system, e...
Abstract i%‘e investigate the consequences of the quantum fluctuations associated with synchrotron r...
Preserving the beam size (or equivalently the emittance) is a primary aim of accelerator physics. He...
The three main components of the dipole wakefield in the collider arcs are the resistive wall wake d...
In this paper, we estimate the emittance growth in the LHeC recirculating Linac, the lattice design ...
In this paper, we estimate the emittance growth in the LHeC recirculating Linac, the lattice design ...
Multi-particle simulations are performed to study emittance growth in the Fermilab Booster. Analysis...
Turn-by-turn beam profile data measured at the Fermilab Booster are studied. Lattice models with exp...
In colliders with asymmetric rigidity such as the proposed Large Hadron electron Collider, jitter in...
Random fluctuations in the tune, beam offsets, and beam size in the presence of the beam-beam intera...
During LHC Run 1 about 30 % of the potential peak performance was lost due to transverse emittance b...
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