The low-frequency transverse collimator impedance constitutes a major part of the LHC impedance budget. In this paper numerical simulations for frequencies below 1 MHz using a commercial package are presented. From the 3D field solution of the two-wire simulations the transverse impedance is directly calculated. After a cross-check with theory for rotationally symmetric structures a geometry with two jaws and an LHC graphite collimator is examined. Furthermore, a simple physics picture that explains the principal characteristics of the impedance at high and low frequencies is given
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
Simulations have been performed in Omega3P to study both trapped modes and impedance contributions o...
The prediction of the resistive wall transverse beam impedance at the first unstable betatron line (...
The results of simulation of geometrical longitudinal impedance of TCDQ are presented. This impedanc...
The prediction of the transverse wall beam impedance at the first unstable betatron line (8 kHz) of ...
The prediction of the transverse wall beam impedance at the first unstable betatron line (8kHz) of t...
The LHC collimators have very complicated mechanical designs including movable jaws made of higly r...
The LHC phase 2 collimation project aims at gaining a factor ten in cleaning efficiency, robustness ...
The prediction of the transverse wall beam impedance at the first unstable betatron line (8 kHz) of ...
The results of simulation of trapped modes in LHC (phase 1) secondary collimators are presented. Bot...
The collimation system of the LHC is one of the largest impedance contributors of the machine, in pa...
The LHC collimation system is a critical element for the safe operation of the LHC machine and is su...
The transverse impedance in the LHC is expected to be dominated by the numerous collimators, most of...
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
Simulations have been performed in Omega3P to study both trapped modes and impedance contributions o...
The prediction of the resistive wall transverse beam impedance at the first unstable betatron line (...
The results of simulation of geometrical longitudinal impedance of TCDQ are presented. This impedanc...
The prediction of the transverse wall beam impedance at the first unstable betatron line (8 kHz) of ...
The prediction of the transverse wall beam impedance at the first unstable betatron line (8kHz) of t...
The LHC collimators have very complicated mechanical designs including movable jaws made of higly r...
The LHC phase 2 collimation project aims at gaining a factor ten in cleaning efficiency, robustness ...
The prediction of the transverse wall beam impedance at the first unstable betatron line (8 kHz) of ...
The results of simulation of trapped modes in LHC (phase 1) secondary collimators are presented. Bot...
The collimation system of the LHC is one of the largest impedance contributors of the machine, in pa...
The LHC collimation system is a critical element for the safe operation of the LHC machine and is su...
The transverse impedance in the LHC is expected to be dominated by the numerous collimators, most of...
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
The LHC collimation system is a critical element for the safe operation of the LHC machine. The nece...
Simulations have been performed in Omega3P to study both trapped modes and impedance contributions o...