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FrascatiPlace
The 3 GHz SCDTL structure has been developed at ENEA Frascati Laboratories to be used as the intermediate energy part of the Compact High Frequency Linac, envisaged by the TERA foundation for proto
The prototype of the Linac4 Drift Tube Linac (DTL) has undergone low power measurements in order to ...
Recent results in accelerator physics showed the feasibility of a coupling scheme between a cyclotro...
Conventional designs for proton linacs use a radiofrequency quadrupole (RFQ), followed by a drift-tu...
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 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Pro...
The Side Coupled Drift Tube Linac (SCDTL) is a 3 GHz accelerating structure for proton therapy linac...
The Coupled-Cavity Drift Tube Linac (CCDTL) is a relatively new RF accelerator structure which plays...
The medium-energy section of the proton linear accelerator for radiotherapy under realization in the...
The SPL is a high-power superconducting H- linac designed to cover the needs of future experimental ...
A short, high-power linac structure has been designed drift tubes are copper and use new neodymium-i...
The SPL is a high-power superconducting H linac de-signed to cover the needs of future experimental...
Linac4 is a new 160 MeV H − linac proposed at CERN to replace the 50 MeV Linac2 as injector to the P...
Conventional designs for proton linacs use a radio-frequency quadrupole (RFQ), followed by a drift-t...
For high-current accelerators such as those proposed for transmutation technologies or spallation so...
The prototype of the Linac4 Drift Tube Linac (DTL) has undergone low power measurements in order to ...
Recent results in accelerator physics showed the feasibility of a coupling scheme between a cyclotro...
Conventional designs for proton linacs use a radiofrequency quadrupole (RFQ), followed by a drift-tu...
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 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Pro...
The Side Coupled Drift Tube Linac (SCDTL) is a 3 GHz accelerating structure for proton therapy linac...
The Coupled-Cavity Drift Tube Linac (CCDTL) is a relatively new RF accelerator structure which plays...
The medium-energy section of the proton linear accelerator for radiotherapy under realization in the...
The SPL is a high-power superconducting H- linac designed to cover the needs of future experimental ...
A short, high-power linac structure has been designed drift tubes are copper and use new neodymium-i...
The SPL is a high-power superconducting H linac de-signed to cover the needs of future experimental...
Linac4 is a new 160 MeV H − linac proposed at CERN to replace the 50 MeV Linac2 as injector to the P...
Conventional designs for proton linacs use a radio-frequency quadrupole (RFQ), followed by a drift-t...
For high-current accelerators such as those proposed for transmutation technologies or spallation so...
The prototype of the Linac4 Drift Tube Linac (DTL) has undergone low power measurements in order to ...
Recent results in accelerator physics showed the feasibility of a coupling scheme between a cyclotro...
Conventional designs for proton linacs use a radiofrequency quadrupole (RFQ), followed by a drift-tu...
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