A separated drift tube linac (SDTL) was adopted as an accelerating structure of Japan Proton Accelerator Complex (J-PARC), which follows the DTL. The SDTL of J-PARC consists of 32 five-cell short tanks, ranging from 1.5 to 2.5 m in length. A design of frequency tuners of the SDTL was performed by taking account of 3-D field distribution calculated with MAFIA. The effects of stems on the resonant frequency and field distribution were also analyzed. An easy and effective compensation method for perturbation by stems of both end cells was proposed and applied to the SDTL tanks
J-PARC is a large scale facility of the proton accelerators for the multi-purpose of scientific rese...
65-71A 20 MeV Drift Tube Linac (DTL) was proposed to be developed for the multi-GeV proton accelera...
The design of the Drift Tube Linac (DTL) for the new linear accelerator Linac4 at CERN has been made...
In the beam commissioning of J-PARC linac, we plan to perform phase-scan with precise TOF (Time Of F...
The first tank of the DTL for Japan Proton Accelerator Research Complex (J-PARC) was installed in th...
The accelerator of the J-PARC complex consists of the 400MeV (initially 181MeV) linac, the rapid cyc...
A short, high-power linac structure has been designed drift tubes are copper and use new neodymium-i...
A conventional 20 MeV Drift Tube Linac (DTL) for the Proton Engineering Frontier Project (PEFP) has ...
A 433.3 MHz drift tube linac (DTL), whichaccelerates proton out of the 2 MeV RFQ linac to 7 MeV, is ...
Abstract At the proton linac of J-PARC (Japan Proton Accelerator Research Complex), an accelerating ...
A 200-MeV proton linear accelerator for the JHF has been designed [1][2]. A peak current of 30 mA wi...
The Drift Tube (DT) accelerating structure is very well known, developed and widely used in existent...
The first annular-ring coupled structure (ACS) cavity for the Japan Proton Accelerator Research Comp...
A rotary tuner has been developed and tested in a 425-MHz ramped gradient drift-tube linac and also ...
The 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Prot...
J-PARC is a large scale facility of the proton accelerators for the multi-purpose of scientific rese...
65-71A 20 MeV Drift Tube Linac (DTL) was proposed to be developed for the multi-GeV proton accelera...
The design of the Drift Tube Linac (DTL) for the new linear accelerator Linac4 at CERN has been made...
In the beam commissioning of J-PARC linac, we plan to perform phase-scan with precise TOF (Time Of F...
The first tank of the DTL for Japan Proton Accelerator Research Complex (J-PARC) was installed in th...
The accelerator of the J-PARC complex consists of the 400MeV (initially 181MeV) linac, the rapid cyc...
A short, high-power linac structure has been designed drift tubes are copper and use new neodymium-i...
A conventional 20 MeV Drift Tube Linac (DTL) for the Proton Engineering Frontier Project (PEFP) has ...
A 433.3 MHz drift tube linac (DTL), whichaccelerates proton out of the 2 MeV RFQ linac to 7 MeV, is ...
Abstract At the proton linac of J-PARC (Japan Proton Accelerator Research Complex), an accelerating ...
A 200-MeV proton linear accelerator for the JHF has been designed [1][2]. A peak current of 30 mA wi...
The Drift Tube (DT) accelerating structure is very well known, developed and widely used in existent...
The first annular-ring coupled structure (ACS) cavity for the Japan Proton Accelerator Research Comp...
A rotary tuner has been developed and tested in a 425-MHz ramped gradient drift-tube linac and also ...
The 3 GHz linac section designed for the low energy (7–65 MeV) part of TOP (Therapy Oncological Prot...
J-PARC is a large scale facility of the proton accelerators for the multi-purpose of scientific rese...
65-71A 20 MeV Drift Tube Linac (DTL) was proposed to be developed for the multi-GeV proton accelera...
The design of the Drift Tube Linac (DTL) for the new linear accelerator Linac4 at CERN has been made...