Synchrotron injector system and operating method for drift tube linear accelerator
When accelerating first ions, radio frequency power is fed to a drift tube linear accelerator so that the phase difference between an accelerating half cycle for accelerating the first ions in one of the plurality of drift tube gaps and the accelerating half cycle for accelerating the accelerated first ions reaching the next drift tube gap is set to a first accelerating cycle phase difference; and when accelerating second ions having a charge-to-mass ratio lower than the first ions, the radio frequency power is fed to the drift tube linear accelerator so that the phase difference between an accelerating half cycle for accelerating the second ions in the one drift tube gap and the accelerating half cycle for the accelerated second ions reaching the next drift tube gap is set to a second accelerating cycle phase difference that is larger than the first accelerating cycle phase difference.
1. A synchrotron injector system for injecting ions into a synchrotron, comprising:
a first ion source for generating first ions;
a second ion source for generating second ions having a charge-to-mass ratio (q 2 /A 2 ) lower than the charge-to-mass ratio (q 1 /A 1 ) of the first ions;
a drift tube linear accelerator including:
a cylindrical resonator; and
a plurality of drift tubes arranged linearly along the center axis of the cylindrical resonator, for accelerating ions in an accelerating half cycle that is a radio frequency half cycle containing an accelerating phase of radio frequency electric fields produced in a plurality of drift tube gaps formed between the plurality of drift tubes;
a radio frequency generator for feeding radio frequency power to the drift tube linear accelerator; and
a low-energy beam delivery line for injecting either the first ions or the second ions into the drift tube linear accelerator, wherein
when the first ions are injected from the low-energy beam delivery line, the radio frequency generator feeds the radio frequency power to the drift tube linear accelerator so that the phase difference between an accelerating half cycle for accelerating the first ions in one drift tube gap of the plurality of drift tube gaps and an accelerating half cycle for accelerating the accelerated first ions reaching the next drift tube gap is set to a first accelerating cycle phase difference and
when the second ions are injected from the low-energy beam delivery line, the radio frequency generator feeds the radio frequency power to the drift tube linear accelerator so that the phase difference between an accelerating half cycle for accelerating the second ions in the one drift tube gap and an accelerating half cycle for the accelerated second ions reaching the next drift tube gap is set to a second accelerating cycle phase difference that is larger than the first accelerating cycle phase difference.
2. The injector system for synchrotron of claim 1 , wherein the drift tube linear accelerator is an APF-IH drift-tube linear accelerator, and the first accelerating cycle phase difference is set to 0.5 cycles and the second accelerating cycle phase difference is set to (0.5+n) cycles, where n is a positive integer.
3. The injector system for synchrotron of claim 2 , wherein magnetic converging devices are provided in drift tubes.
4. The injector system for synchrotron of claim 1 , wherein the drift tube linear accelerator is an Alvarez drift-tube linear accelerator, and the first accelerating cycle phase difference is set to one cycle and the second accelerating cycle phase difference is set to (1+n) cycles, where n is a positive integer.
5. The injector system for synchrotron of claim 1 , wherein each drift tube is provided with electrodes projecting in each drift tube gap to form a quadrupole electric field in each drift tube gap.
6. The injector system for synchrotron of claim 1 , wherein the first ions are protons and the second ions are tetravalent carbon ions.
7. An operating method for a drift-tube linear accelerator that includes a cylindrical resonator and a plurality of drift tubes arranged linearly along the center axis of the cylindrical resonator, to accelerate either first ions or second ions having a charge-to-mass ratio (q 2 /A 2 ) lower than the charge-to-mass ratio (q 1 /A 1 ) of the first ions in an accelerating half cycle that is a radio frequency half cycle containing an accelerating phase of radio frequency electric fields produced in a plurality of drift tube gaps formed between the plurality of drift tubes,
the operating method for the drift-tube linear accelerator characterized in that the drift-tube linear accelerator operates so that when accelerating the first ions, radio frequency power is fed the radio frequency power to the drift tube linear accelerator so that the phase difference between an accelerating half cycle for accelerating the first ions in one drift tube gap of the plurality of drift tube gaps and an accelerating half cycle for accelerating the accelerated first ions reaching the next drift tube gap is set to a first accelerating cycle phase difference and when accelerating the second ions, the radio frequency power is fed to the drift tube linear accelerator so that the phase difference between an accelerating half cycle for accelerating the second ions in the one drift tube gap and an accelerating half cycle for the accelerated second ions reaching the next drift tube gap is set to a second accelerating cycle phase difference that is larger than the first accelerating cycle phase difference.
8. The operating method for a drift-tube linear accelerator, according to claim 7 , wherein the drift tube linear accelerator is an APF-IH linear accelerator, and the first accelerating cycle phase difference is set to 0.5 cycles and the second accelerating cycle phase difference is set to (0.5+n) cycles, where n is a positive integer.
9. The operating method for a drift-tube linear accelerator, according to claim 7 , wherein the drift tube linear accelerator is an Alvarez drift-tube linear accelerator, and the first accelerating cycle phase difference is set to one cycle and the second accelerating cycle phase difference is set to (1+n) cycles, where n is a positive integer.
10. The operating method for a drift-tube linear accelerator, according to claim 7 , wherein the first ions are protons and the second ions are tetravalent carbon ions.