The main aim of the MD was to study the dependency of bunch-by-bunch intensity measurements to beam position and bunch length variations. Large beam position offsets in IR4 and varying bunch length were introduced to compare the performance of the presently installed Fast Beam Current Transformers with the new Integrating Current Transformer and the new Wall Current Transformer. This note explains all the procedures of the LHC MD 398, which took place on 20/07/2015, and presents the obtained results
This document presents the LHC DC beam current transformer system, describes the main sources of unc...
The CERN Proton Synchrotron complex (CPS) has been operational for over 50 years. During this time t...
The LHC will have very tight tolerances on nearly all beam parameters. Their precise measurement is ...
During the 2010 run the LHC continuously improved its performance. In particular the bunch charge an...
The Large Hadron Collider (LHC) stores two high-energy counter-rotating particle beams consisting of...
The fast beam current transformers (FBCTs) for the Large Hadron Collider (LHC) were designed to pro...
The beam intensity (number of particles forming the beam) in the Large Hadron Collider (LHC) is meas...
CERN's Large Hadron Collider (LHC) is equipped with three distinct types of intensity measurement sy...
This document presents the LHC ring fast beam current transformer system, describes the main sources...
Stringent demands on the LHC safety and protection systems require improved methods of detecting fas...
The LHC circulating beam current measurement is provided by eight current transformers, i.e. two DC ...
The Wall Current Transformer (WCT) is a new bunch-by-bunch intensity monitor developed by the CERN B...
During the 2008 LHC injection synchronisation tests and the subsequent days with circulating beam, t...
The fast beam intensity measurements for the LHC are provided by eight Fast Beam Current Transformer...
High intensity particle beam injection into the LHC is only permitted when a low intensity pilot be...
This document presents the LHC DC beam current transformer system, describes the main sources of unc...
The CERN Proton Synchrotron complex (CPS) has been operational for over 50 years. During this time t...
The LHC will have very tight tolerances on nearly all beam parameters. Their precise measurement is ...
During the 2010 run the LHC continuously improved its performance. In particular the bunch charge an...
The Large Hadron Collider (LHC) stores two high-energy counter-rotating particle beams consisting of...
The fast beam current transformers (FBCTs) for the Large Hadron Collider (LHC) were designed to pro...
The beam intensity (number of particles forming the beam) in the Large Hadron Collider (LHC) is meas...
CERN's Large Hadron Collider (LHC) is equipped with three distinct types of intensity measurement sy...
This document presents the LHC ring fast beam current transformer system, describes the main sources...
Stringent demands on the LHC safety and protection systems require improved methods of detecting fas...
The LHC circulating beam current measurement is provided by eight current transformers, i.e. two DC ...
The Wall Current Transformer (WCT) is a new bunch-by-bunch intensity monitor developed by the CERN B...
During the 2008 LHC injection synchronisation tests and the subsequent days with circulating beam, t...
The fast beam intensity measurements for the LHC are provided by eight Fast Beam Current Transformer...
High intensity particle beam injection into the LHC is only permitted when a low intensity pilot be...
This document presents the LHC DC beam current transformer system, describes the main sources of unc...
The CERN Proton Synchrotron complex (CPS) has been operational for over 50 years. During this time t...
The LHC will have very tight tolerances on nearly all beam parameters. Their precise measurement is ...