The performance of the CERN Proton Synchrotron (PS) has been constantly increasing over the years both in terms of beam parameters (intensity and brightness) and beam manipulations (transverse and longitudinal splitting). This implies a very good knowledge of the linear and non-linear model of the ring. In this paper we report on a detailed campaign of beam measurements based on turn-by-turn orbit data aimed at measuring the optics in several conditions as well as the resonance driving terms
We review some optical measurements and correction strategies adopted for the new lattice with 90 ’ ...
The measured response matrix giving the change in orbit at beam position monitors (BPMs) with change...
The CERN Proton Synchrotron (PS) is a crucial component of the Large Hadron Collider (LHC) injector ...
For the first time, the optics of the CERN Proton Synchrotron (PS) was measured using turn-by-turn B...
Future operations for the CERN accelerator complex will require the PS Booster to deliver higher int...
The CERN Proton Synchrotron machine is built using combined function magnets. The control of the lin...
The CERN Proton Synchrotron machine is built using combined function magnets. The control of the lin...
The CERN SPS multiturn facility, based on the new beam orbit measurement system MOPOS, enables the U...
In the framework of the CERN PSMulti-Turn Extraction several campaigns of measurements probing the n...
This thesis concerns the reconstruction of a new set of extraction parameters from the Proton Synchr...
As part of the LHC Injector Upgrade Project the injection of the CERN PS Booster will be changed to ...
As part of the LHC Injector Upgrade project, the CERN PS Booster will be required to operate at near...
Following the analysis of the results obtained during the first year of beam commissioning of the CE...
Multiturn beam position measurements on one or more pickups provide very important information neede...
Refined Fourier analysis of turn-by-turn (TBT) transverse position data measurements can be used for...
We review some optical measurements and correction strategies adopted for the new lattice with 90 ’ ...
The measured response matrix giving the change in orbit at beam position monitors (BPMs) with change...
The CERN Proton Synchrotron (PS) is a crucial component of the Large Hadron Collider (LHC) injector ...
For the first time, the optics of the CERN Proton Synchrotron (PS) was measured using turn-by-turn B...
Future operations for the CERN accelerator complex will require the PS Booster to deliver higher int...
The CERN Proton Synchrotron machine is built using combined function magnets. The control of the lin...
The CERN Proton Synchrotron machine is built using combined function magnets. The control of the lin...
The CERN SPS multiturn facility, based on the new beam orbit measurement system MOPOS, enables the U...
In the framework of the CERN PSMulti-Turn Extraction several campaigns of measurements probing the n...
This thesis concerns the reconstruction of a new set of extraction parameters from the Proton Synchr...
As part of the LHC Injector Upgrade Project the injection of the CERN PS Booster will be changed to ...
As part of the LHC Injector Upgrade project, the CERN PS Booster will be required to operate at near...
Following the analysis of the results obtained during the first year of beam commissioning of the CE...
Multiturn beam position measurements on one or more pickups provide very important information neede...
Refined Fourier analysis of turn-by-turn (TBT) transverse position data measurements can be used for...
We review some optical measurements and correction strategies adopted for the new lattice with 90 ’ ...
The measured response matrix giving the change in orbit at beam position monitors (BPMs) with change...
The CERN Proton Synchrotron (PS) is a crucial component of the Large Hadron Collider (LHC) injector ...