The low-energy-beam transport (LEBT) system for the Low-Energy Demonstration Accelerator (LEDA) transports the beam from the ion-source plasma surface to the LEDA RFQ entrance. The code PARMELA performed these simulations of the beam transport through the LEBT. This code can simultaneously transport three particle types of different charge-to-mass ratio. Electrostatic fields, magnetic fields, and space charge influence the beam particles in this simulation. The electrostatic fields exist in the ion-source extractor. The magnetic field exists in the ion source and in the solenoid lenses. The e{sup {minus}} particles, introduced into the beam of H{sup +} and H{sub 2}{sup +}, simulate the space charge neutralization by the residual gas in the ...
This chapter gives an introduction to low-energy beam transport systems, and discusses the typically...
To fulfil the requirements of ESS on beam transmission and emittance growth a detailed knowledge of ...
Low energy particle beams pose specific challenges to simulation codes and experiments alike as a nu...
The computer codes TRACE and SCHAR model the Low-Energy Demonstration Accelerator (LEDA) Low-Energy ...
The Low-Energy Demonstration Accelerator (LEDA) injector is designed to provide 75-keV, 110-mA, prot...
Here the authors describe the High Energy Beam Transport (HEBT) for the Low Energy Demonstration Acc...
Over the past several years of ONR support for our research program we have mainly studied the vario...
A 20 MeV, 30 mA CW proton accelerator is being built in BARC which consists of 50 keV ECR ion-source...
International audienceThe dynamics of a high intensity beam with low energy is governed by its space...
The two Low Energy Beam Transport (LEBT) sections of the accelerator-driven neutron source FRANZ* co...
Linac4 is a 160 MeV H- linear accelerator which will replace the 50 MeV proton Linac2 for upgrade of...
Part of the upgrade program in the injector chains of the CERN accelerator complex is the replaceme...
The Front End Test Stand (FETS) at the Rutherford Appleton Laboratory is intended to demonstrate the...
For the transport of high-intensity hadron beams in low-energy beam lines of linear accelerators, th...
The space charge effect of low energy, unbunched ion beams can be compensated by the trapping of ion...
This chapter gives an introduction to low-energy beam transport systems, and discusses the typically...
To fulfil the requirements of ESS on beam transmission and emittance growth a detailed knowledge of ...
Low energy particle beams pose specific challenges to simulation codes and experiments alike as a nu...
The computer codes TRACE and SCHAR model the Low-Energy Demonstration Accelerator (LEDA) Low-Energy ...
The Low-Energy Demonstration Accelerator (LEDA) injector is designed to provide 75-keV, 110-mA, prot...
Here the authors describe the High Energy Beam Transport (HEBT) for the Low Energy Demonstration Acc...
Over the past several years of ONR support for our research program we have mainly studied the vario...
A 20 MeV, 30 mA CW proton accelerator is being built in BARC which consists of 50 keV ECR ion-source...
International audienceThe dynamics of a high intensity beam with low energy is governed by its space...
The two Low Energy Beam Transport (LEBT) sections of the accelerator-driven neutron source FRANZ* co...
Linac4 is a 160 MeV H- linear accelerator which will replace the 50 MeV proton Linac2 for upgrade of...
Part of the upgrade program in the injector chains of the CERN accelerator complex is the replaceme...
The Front End Test Stand (FETS) at the Rutherford Appleton Laboratory is intended to demonstrate the...
For the transport of high-intensity hadron beams in low-energy beam lines of linear accelerators, th...
The space charge effect of low energy, unbunched ion beams can be compensated by the trapping of ion...
This chapter gives an introduction to low-energy beam transport systems, and discusses the typically...
To fulfil the requirements of ESS on beam transmission and emittance growth a detailed knowledge of ...
Low energy particle beams pose specific challenges to simulation codes and experiments alike as a nu...