We review the current design of the interaction region of the TESLA superconducting linear collider. We describe in particular the recent upgrades of the collimation section and the beam extraction lines
The TESLA Technical Design Report Part III: Physics at an e+e- Linear ColliderThe TESLA Technical De...
The expected beam-beam interaction at the proposed TESLA electron-positron linear collider has a sig...
The primary goal of the interaction region (IR) is to de-magnify the transverse beam dimension to a ...
We review the current design of the interaction region of the TESLA superconducting linear collider....
TESLA is designed as an electron-positron linear collider (LC) based on super-conducting technology....
We study the main implications of increasing the last drift length l * from 3 to 5 meters, in the TE...
To appear in the proceedings of the 5th Int. Linear Colliders Workshop -Lcws2000, Fermilab, October ...
The status of the layout of the linear collider project, TESLA, which employs superconducting accele...
An overview of the proposed new BDS for the TESLA linear collider is presented. Several major change...
We review the important changes made to the optics of the Interaction Regions (IRS) in the collider ...
Vertical beam offsets at the interaction point will degrade the luminosity (3.4 · 1034 cm−2s−1) in t...
programme at the TESLA Test Facility (TTF) will be summarised. The superconducting linac technology ...
In the TESLA superconducting linear collider project, collisions occur at zero crossing angle. While...
We review the current status of the R&D results and design studies on the TESLA superconducting e$^+...
Two detector concepts are being investigated for the Next Linear Collider. This paper discusses the ...
The TESLA Technical Design Report Part III: Physics at an e+e- Linear ColliderThe TESLA Technical De...
The expected beam-beam interaction at the proposed TESLA electron-positron linear collider has a sig...
The primary goal of the interaction region (IR) is to de-magnify the transverse beam dimension to a ...
We review the current design of the interaction region of the TESLA superconducting linear collider....
TESLA is designed as an electron-positron linear collider (LC) based on super-conducting technology....
We study the main implications of increasing the last drift length l * from 3 to 5 meters, in the TE...
To appear in the proceedings of the 5th Int. Linear Colliders Workshop -Lcws2000, Fermilab, October ...
The status of the layout of the linear collider project, TESLA, which employs superconducting accele...
An overview of the proposed new BDS for the TESLA linear collider is presented. Several major change...
We review the important changes made to the optics of the Interaction Regions (IRS) in the collider ...
Vertical beam offsets at the interaction point will degrade the luminosity (3.4 · 1034 cm−2s−1) in t...
programme at the TESLA Test Facility (TTF) will be summarised. The superconducting linac technology ...
In the TESLA superconducting linear collider project, collisions occur at zero crossing angle. While...
We review the current status of the R&D results and design studies on the TESLA superconducting e$^+...
Two detector concepts are being investigated for the Next Linear Collider. This paper discusses the ...
The TESLA Technical Design Report Part III: Physics at an e+e- Linear ColliderThe TESLA Technical De...
The expected beam-beam interaction at the proposed TESLA electron-positron linear collider has a sig...
The primary goal of the interaction region (IR) is to de-magnify the transverse beam dimension to a ...