Results of a configuration design trade study for a 250 mA, 20 MeV proton accelerator are presented. The accelerator design is based on High Intensity Low Beta Ion Linac (HILBILAC) with superconducting solenoid beam focusing. Two variants of the accelerator are analyzed. The first includes a HILBILAC section with output energy of 3 MeV and a number of DTL sections with quadrupole focusing. The second consists completely of HILBILAC sections. The main features of a HILBILAC based system are: absence of beam funneling, use of high operating frequency for acceleration of low emittance beam, high accelerating resonator efficiency. 1
The second phase accelerator for the Dual Axis Hydrodynamic Test facility (DARHT) is designed to pro...
For the application of high intensity continuous wave (CW) proton beam acceleration, a new supercond...
The present document describes the Low- and Medium-beta section of the EURISOL DS Driver Accelerator...
At the low energy end of an induction linac HIF driver the beam current is limited by our ability to...
The Facility for Antiproton and Ion Research (FAIR) at GSI Darmstadt will provide unprecedented inte...
Proposed accelerator production of tritium (APT) project requires an accelerator providing a cw prot...
After the decomissioning of LEP-2 a considerable amount of RF hardware becomes available and can be ...
The demand for high power proton beams is at an all time high. The global community has identified m...
A 200-MeV proton linear accelerator for the JHF has been designed [1][2]. A peak current of 30 mA wi...
The baseline accelerator design for the APT (Accelerator Production of Tritium) Project [1] is a nor...
The proposed Rare Isotope Accelerator (RIA) requires the construction of a cw 1.4 GV superconducting...
For the production of Antiproton beams with sufficient intensities, a dedicated high-intensity 325 M...
A six-month design study for a future high energy hadron collider was initiated by the Fermilab dire...
The proposed Rare Isotope Accelerator (RIA) requires the construction of a cw 1.4 GV superconducting...
<span style="color: rgb(51, 51, 51); font-family: arial, helvetica, sans-serif; font-size: 13px; lin...
The second phase accelerator for the Dual Axis Hydrodynamic Test facility (DARHT) is designed to pro...
For the application of high intensity continuous wave (CW) proton beam acceleration, a new supercond...
The present document describes the Low- and Medium-beta section of the EURISOL DS Driver Accelerator...
At the low energy end of an induction linac HIF driver the beam current is limited by our ability to...
The Facility for Antiproton and Ion Research (FAIR) at GSI Darmstadt will provide unprecedented inte...
Proposed accelerator production of tritium (APT) project requires an accelerator providing a cw prot...
After the decomissioning of LEP-2 a considerable amount of RF hardware becomes available and can be ...
The demand for high power proton beams is at an all time high. The global community has identified m...
A 200-MeV proton linear accelerator for the JHF has been designed [1][2]. A peak current of 30 mA wi...
The baseline accelerator design for the APT (Accelerator Production of Tritium) Project [1] is a nor...
The proposed Rare Isotope Accelerator (RIA) requires the construction of a cw 1.4 GV superconducting...
For the production of Antiproton beams with sufficient intensities, a dedicated high-intensity 325 M...
A six-month design study for a future high energy hadron collider was initiated by the Fermilab dire...
The proposed Rare Isotope Accelerator (RIA) requires the construction of a cw 1.4 GV superconducting...
<span style="color: rgb(51, 51, 51); font-family: arial, helvetica, sans-serif; font-size: 13px; lin...
The second phase accelerator for the Dual Axis Hydrodynamic Test facility (DARHT) is designed to pro...
For the application of high intensity continuous wave (CW) proton beam acceleration, a new supercond...
The present document describes the Low- and Medium-beta section of the EURISOL DS Driver Accelerator...