In this paper, we describe the single and multi-bunch sources of emittance dilution in the linacs of both 1 and 5 TeV center-of-mass energy linear colliders. The linacs operate at high rf accelerating gradients with a frequency around 30 GHz. At this high accelerating frequency, the wakefields are very strong and we discuss the BNS damping and correction procedures as well as the alignment and construction tolerances that are required to preserve the transverse emittance. Finally, because the collider must operate with long bunch trains, we consider the multi-bunch emittance dilution for a few cases where either the long-range transverse wakefield is damped or it is decreased by a combination of weak damping and detuning
The luminosity that can be achieved in a linear collider strongly depends on the vertical emittance ...
beams in a linear collider must be adequately damped in order to preserve the luminosity of the coll...
Once the tolerable emittance growth of a beam accelerated in the main linac of a linear collider, de...
The luminosity that can be achieved in a linear collider strongly depends on the vertical emittance ...
After recalling the reasons for high brighness beams in linear colliders, the question of the preser...
An electron (or positron) multi-bunch train traversing several thousand accelerator structures can b...
The main L-band linacs of the ILC accelerate 2820 bunches from a center of mass of 10 GeV to 500 GeV...
We present parameters for a linear collider with a $3$ to $5$ TeV center-of-mass energy that utilize...
The transverse emittances in the SLAC Linear Collider can be severely diluted by collective wakefiel...
The luminosity requested for linear colliders with center-of-mass energies exceeding 500 GeV, implie...
The installation of elements in the main linac of future linear colliders can only be done with a li...
We consider the emittance preservation issues in two possible linear collider main linac con-figurat...
Abstract reduced by the following factor:.4!most all 2 x 250 GeV linear collider schemes make use of...
In order to prevent electrical breakdown occurring in the JLC/NLC (Japanese Linear Collider/Next Lin...
Controlling beam emittance is important for future linear colliders as well as high-brightness light...
The luminosity that can be achieved in a linear collider strongly depends on the vertical emittance ...
beams in a linear collider must be adequately damped in order to preserve the luminosity of the coll...
Once the tolerable emittance growth of a beam accelerated in the main linac of a linear collider, de...
The luminosity that can be achieved in a linear collider strongly depends on the vertical emittance ...
After recalling the reasons for high brighness beams in linear colliders, the question of the preser...
An electron (or positron) multi-bunch train traversing several thousand accelerator structures can b...
The main L-band linacs of the ILC accelerate 2820 bunches from a center of mass of 10 GeV to 500 GeV...
We present parameters for a linear collider with a $3$ to $5$ TeV center-of-mass energy that utilize...
The transverse emittances in the SLAC Linear Collider can be severely diluted by collective wakefiel...
The luminosity requested for linear colliders with center-of-mass energies exceeding 500 GeV, implie...
The installation of elements in the main linac of future linear colliders can only be done with a li...
We consider the emittance preservation issues in two possible linear collider main linac con-figurat...
Abstract reduced by the following factor:.4!most all 2 x 250 GeV linear collider schemes make use of...
In order to prevent electrical breakdown occurring in the JLC/NLC (Japanese Linear Collider/Next Lin...
Controlling beam emittance is important for future linear colliders as well as high-brightness light...
The luminosity that can be achieved in a linear collider strongly depends on the vertical emittance ...
beams in a linear collider must be adequately damped in order to preserve the luminosity of the coll...
Once the tolerable emittance growth of a beam accelerated in the main linac of a linear collider, de...