The ATLAS PIIECR ion source is a major component of a project which will result in the replacement of the ATLAS tandem electrostatic injector with a superconducting linac of extremely low velocity profile and an ECR ion source operating in the continuous mode. A compilation of the source parameters adopted is tabulated, and the various issues considered in the design process and decisions made regarding those issues are discussed. (LEW
The MSECRIS source has been designed with the aim to exceed the highest currents of highly charged h...
The existing superconducting linac ATLAS is in many respects an ideal secondary beam accelerator for...
Argonne Tandem Linac Accelerator System (ATLAS) is a Department of Energy (DOE) national user resear...
A new 14 GHz ECR ion source for the ATLAS facility is under construction. The new source is an evolu...
The planned positive-ion injector for ATLAS consists of an ECR ion source on a 350-kV platfrom and a...
The ATLAS Positive Ion Injector (PII) is designed to replace the tandem injector for the ATLAS heavy...
The Argonne Tandem Linear Accelerator System (ATLAS) has been operating on a twenty-four hour, seven...
The status of and the first operational experience with the he positive-ion injector for ATLAS are s...
The first beam from the Argonne PIIECR ion source was achieved on October 21, 1987. The major constr...
A major upgrade of the first ATLAS 10 GHz ECR ion source, which began operations in 1987, is in the ...
Four ECR ion sources have been operated in National Institute of Radiological Sciences (NIRS). Two E...
This paper reports the status of hardware development for the linac portion of the Argonne tandem-li...
Since the superconducting heavy ion linac ATLAS is an ideal post-accelerator for radioactive beams, ...
The Argonne Tandem Linac Accelerator System (ATLAS) is a superconducting low-energy heavy ion accele...
With the recent integration of the CARIBU-EBIS charge breeder into the ATLAS accelerator system to p...
The MSECRIS source has been designed with the aim to exceed the highest currents of highly charged h...
The existing superconducting linac ATLAS is in many respects an ideal secondary beam accelerator for...
Argonne Tandem Linac Accelerator System (ATLAS) is a Department of Energy (DOE) national user resear...
A new 14 GHz ECR ion source for the ATLAS facility is under construction. The new source is an evolu...
The planned positive-ion injector for ATLAS consists of an ECR ion source on a 350-kV platfrom and a...
The ATLAS Positive Ion Injector (PII) is designed to replace the tandem injector for the ATLAS heavy...
The Argonne Tandem Linear Accelerator System (ATLAS) has been operating on a twenty-four hour, seven...
The status of and the first operational experience with the he positive-ion injector for ATLAS are s...
The first beam from the Argonne PIIECR ion source was achieved on October 21, 1987. The major constr...
A major upgrade of the first ATLAS 10 GHz ECR ion source, which began operations in 1987, is in the ...
Four ECR ion sources have been operated in National Institute of Radiological Sciences (NIRS). Two E...
This paper reports the status of hardware development for the linac portion of the Argonne tandem-li...
Since the superconducting heavy ion linac ATLAS is an ideal post-accelerator for radioactive beams, ...
The Argonne Tandem Linac Accelerator System (ATLAS) is a superconducting low-energy heavy ion accele...
With the recent integration of the CARIBU-EBIS charge breeder into the ATLAS accelerator system to p...
The MSECRIS source has been designed with the aim to exceed the highest currents of highly charged h...
The existing superconducting linac ATLAS is in many respects an ideal secondary beam accelerator for...
Argonne Tandem Linac Accelerator System (ATLAS) is a Department of Energy (DOE) national user resear...