Add to ORKGThree versions of the CLIC Transfer Structure (CTS) have been studied by means of simulations using the MAFIA set of codes. Of these the high impedance version has been built as a prototype and tested in the CTF (CLIC Test Facility). The other two versions were designed with the aim of suiting the requirements of the two Drive Beam Generation schemes presently being pursued for the CLIC scheme. Here we report the simulation results for th CTS to be used in the multi-drive beam generation scheme
The present note describes an RF power generation scheme for multibunch operation at 1 TeV CM and lu...
The CLIC Test Facility (CTF) is a prototype two-beam accelerator, in which a high-current "drive bea...
The CLIC study of a high-energy (0.5 - 5 TeV), high-luminosity (1034 - 1035 cm-2 sec-1) e+e- linear ...
INTRODUCTION In the original CTS design [1] the 2.8 mm-wide slit, joining the cylindrical beam cham...
In the so-called "Two-Beam Acceleration Scheme" the energy of a drive beam is converted to rf power ...
The CLIC study of an e+ / e- linear collider in the TeV energy range is based on Two-Beam Accelerati...
A new CLIC Test Facility (CTF3) at CERN will serve to study the drive beam generation for the Compac...
Abstract In order to demonstrate the feasibility of the CLIC multiTeV linear collider option, the dr...
It is foreseen that the transfer structures (CTS) of the drive linac will produce 40 MW, 11.4 ns, 30...
In CLIC, the rf power to accelerate the main beam is produced by decelerating a drive beam. The Test...
The 3 GHz drive beam accelerator of the CLIC Test Facility CTF3, currently under construction at CER...
The RF power necessary to accelerate the main beam of the Compact Linear Collider (CLIC) is produced...
For the CLIC two-beam scheme, a high-current, long-pulse drive beam is required for RF power generat...
The objective of the CLIC Test Facility CTF3, built at CERN by an international collaboration, is to...
The Compact Linear Collider (CLIC) PETS is required to produce about 0.5 GW RF power per metre in th...
The present note describes an RF power generation scheme for multibunch operation at 1 TeV CM and lu...
The CLIC Test Facility (CTF) is a prototype two-beam accelerator, in which a high-current "drive bea...
The CLIC study of a high-energy (0.5 - 5 TeV), high-luminosity (1034 - 1035 cm-2 sec-1) e+e- linear ...
INTRODUCTION In the original CTS design [1] the 2.8 mm-wide slit, joining the cylindrical beam cham...
In the so-called "Two-Beam Acceleration Scheme" the energy of a drive beam is converted to rf power ...
The CLIC study of an e+ / e- linear collider in the TeV energy range is based on Two-Beam Accelerati...
A new CLIC Test Facility (CTF3) at CERN will serve to study the drive beam generation for the Compac...
Abstract In order to demonstrate the feasibility of the CLIC multiTeV linear collider option, the dr...
It is foreseen that the transfer structures (CTS) of the drive linac will produce 40 MW, 11.4 ns, 30...
In CLIC, the rf power to accelerate the main beam is produced by decelerating a drive beam. The Test...
The 3 GHz drive beam accelerator of the CLIC Test Facility CTF3, currently under construction at CER...
The RF power necessary to accelerate the main beam of the Compact Linear Collider (CLIC) is produced...
For the CLIC two-beam scheme, a high-current, long-pulse drive beam is required for RF power generat...
The objective of the CLIC Test Facility CTF3, built at CERN by an international collaboration, is to...
The Compact Linear Collider (CLIC) PETS is required to produce about 0.5 GW RF power per metre in th...
The present note describes an RF power generation scheme for multibunch operation at 1 TeV CM and lu...
The CLIC Test Facility (CTF) is a prototype two-beam accelerator, in which a high-current "drive bea...
The CLIC study of a high-energy (0.5 - 5 TeV), high-luminosity (1034 - 1035 cm-2 sec-1) e+e- linear ...