The 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Protons) linac consists of eight modules of the structure SCDTL (Side Coupled Drift Tube Linac). The non axisymmetric cavities required a full 3D modelling. Electromagnetic calculations carried out by using MAFIA code gave the full mode spectrum, power losses, the coupling coefficients distribution and some indications for the tuning procedure. This paper reports a comparison between the results of this study and some RF measurements on the first module (7–13.4 MeV)
Los Alamos National Laboratory is building room-temperature rf accelerating structures for the Spall...
A new scheme has been developed for injection of the 7 MeV proton beam from an AccSys Model PL-7 lin...
A separated drift tube linac (SDTL) was adopted as an accelerating structure of Japan Proton Acceler...
The 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Pro...
The 3 GHz linac section designed for the low energy (7 – 65 MeV) part of TOP (Therapy Oncological Pr...
The 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Prot...
The Side Coupled Drift Tube Linac (SCDTL) is a 3 GHz accelerating structure for proton therapy linac...
The 3 GHz SCDTL structure has been developed at ENEA Frascati Laboratories to be used as the interme...
The medium-energy section of the proton linear accelerator for radiotherapy under realization in the...
A 230 MeV proton LINAC system for medical applications is being developed and commissioned for the L...
A 9.3 GHz 6 MeV linear accelerator (LINAC) was designed by using three-dimensional (3D) particle-in-...
Recent results in accelerator physics showed the feasibility of a coupling scheme between a cyclotro...
For high-current accelerators such as those proposed for transmutation technologies or spallation so...
ACLIP is a 3 GHz proton SCL linac designed as a booster for a 30 MeV commercial cyclotron. The fina...
The accelerator based production of tritium calls for a high-power, cw proton linac. Previous design...
Los Alamos National Laboratory is building room-temperature rf accelerating structures for the Spall...
A new scheme has been developed for injection of the 7 MeV proton beam from an AccSys Model PL-7 lin...
A separated drift tube linac (SDTL) was adopted as an accelerating structure of Japan Proton Acceler...
The 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Pro...
The 3 GHz linac section designed for the low energy (7 – 65 MeV) part of TOP (Therapy Oncological Pr...
The 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Prot...
The Side Coupled Drift Tube Linac (SCDTL) is a 3 GHz accelerating structure for proton therapy linac...
The 3 GHz SCDTL structure has been developed at ENEA Frascati Laboratories to be used as the interme...
The medium-energy section of the proton linear accelerator for radiotherapy under realization in the...
A 230 MeV proton LINAC system for medical applications is being developed and commissioned for the L...
A 9.3 GHz 6 MeV linear accelerator (LINAC) was designed by using three-dimensional (3D) particle-in-...
Recent results in accelerator physics showed the feasibility of a coupling scheme between a cyclotro...
For high-current accelerators such as those proposed for transmutation technologies or spallation so...
ACLIP is a 3 GHz proton SCL linac designed as a booster for a 30 MeV commercial cyclotron. The fina...
The accelerator based production of tritium calls for a high-power, cw proton linac. Previous design...
Los Alamos National Laboratory is building room-temperature rf accelerating structures for the Spall...
A new scheme has been developed for injection of the 7 MeV proton beam from an AccSys Model PL-7 lin...
A separated drift tube linac (SDTL) was adopted as an accelerating structure of Japan Proton Acceler...