In linear colliders in the TeV region, the synchrotron radiation occuring in the final quadrupole magnet limits the smallest vertical RMS beam size which can be reached at the interaction point. Due to the same effect, however, the distribution does not remain gaussian, which helps the luminosity: it is much larger than what is expected from the RMS beam size, but much smaller than the value without radiation in the quadrupole. The luminosity is still limited from above, but the maximum occurs at a much smaller value of the nominal beam size. A simple approximate expression for the luminosity is also proposed
At the present time, there are a number of future linear collider designs with a center-of-mass ener...
Scaling laws appropriate to future e{sup +}e{sup {minus}} linear colliders in the high upsilon regim...
At the present time, there are a number of future linear collider designs with a center-of-mass ener...
To achieve the desired high luminosity in e/sup +/e/sup -/ linear colliders with centre-of-mass ener...
To achieve the desired high luminosity in e+ e- linear colliders with centre-of-mass energies above ...
I discuss fundamental luminosity limitations at hadron col-liders, addressing head-on and long-range...
Beam-beam effects limit the luminosity of circular colliders. Once the bunch population exceeds a th...
The Oide effect considers the synchrotron radiation in the final focusing quadrupole, and it sets a ...
he number of muons per bunch, g =(E /m ), e N is the normalized emittance, and b is the collid...
The following presents a study of the accelerator physics and technology limitations to ultimate ene...
The three colliders operated to date have taught us a great deal about the behaviour of both bunched...
The counterrotating beams in collider rings consist of trains of beam bunches with N{sub B} particle...
Abstract i%‘e investigate the consequences of the quantum fluctuations associated with synchrotron r...
Beam-beam effects limit the luminosity of circular colliders. Once the bunch population exceeds a t...
The beam-beam limit at hadron colliders manifests itself in the form of degraded luminosity lifetime...
At the present time, there are a number of future linear collider designs with a center-of-mass ener...
Scaling laws appropriate to future e{sup +}e{sup {minus}} linear colliders in the high upsilon regim...
At the present time, there are a number of future linear collider designs with a center-of-mass ener...
To achieve the desired high luminosity in e/sup +/e/sup -/ linear colliders with centre-of-mass ener...
To achieve the desired high luminosity in e+ e- linear colliders with centre-of-mass energies above ...
I discuss fundamental luminosity limitations at hadron col-liders, addressing head-on and long-range...
Beam-beam effects limit the luminosity of circular colliders. Once the bunch population exceeds a th...
The Oide effect considers the synchrotron radiation in the final focusing quadrupole, and it sets a ...
he number of muons per bunch, g =(E /m ), e N is the normalized emittance, and b is the collid...
The following presents a study of the accelerator physics and technology limitations to ultimate ene...
The three colliders operated to date have taught us a great deal about the behaviour of both bunched...
The counterrotating beams in collider rings consist of trains of beam bunches with N{sub B} particle...
Abstract i%‘e investigate the consequences of the quantum fluctuations associated with synchrotron r...
Beam-beam effects limit the luminosity of circular colliders. Once the bunch population exceeds a t...
The beam-beam limit at hadron colliders manifests itself in the form of degraded luminosity lifetime...
At the present time, there are a number of future linear collider designs with a center-of-mass ener...
Scaling laws appropriate to future e{sup +}e{sup {minus}} linear colliders in the high upsilon regim...
At the present time, there are a number of future linear collider designs with a center-of-mass ener...