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For the application of high intensity continuous wave(CW) proton beam acceleration, a new superconducting accelerating structure for extremely low β protons working in TE210 mode has been proposed at Peking University. The cavity consists of eight electrodes and eight accelerating gaps. The cavity’s longitudinal length is368.5 mm, and its transverse dimension is 416 mm. The RF frequency is 162.5 MHz, and the designed proton input energy is 200 ke V. A peak field optimization has been performed for the lower surface field. The accelerating gaps are adjusted by phase sweeping based on KONUS beam dynamics. The first four gaps are operated at negative synchronous RF phase to provide longitudinal focusing. The subsequent gaps are 0?sections which can minimize the transverse defocusing effect. Solenoids are placed outside the cavity to provide transverse focusing. Numerical calculation shows that the transverse defocusing of the KONUS phase is about three times smaller than that of the conventional negative synchronous RF phase. The beam dynamics of a 10 m A CW proton beam is simulated by the Trace Win code. The simulation results show that the beam’s transverse size is under effective control, while the increase in the longitudinal direction is slightly large. Both the Trace Win simulation and the numerical calculation show that the cavity has a relatively high effective accelerating gradient of 2.6 MV/m. On the whole, our results show that this new accelerating structure may be a possible candidate for superconducting operation at such a low energy range.
For the application of high intensity continuous wave (CW) proton beam acceleration, a new superconducting accelerating structure for extremely low beta protons working in TE210 mode has been proposed at Peking University. The cavity consists of eight electrodes and eight accelerating gaps. The cavity’s longitudinal The RF frequency is 162.5 MHz, and the designed proton input energy is 200 ke V. The accelerating gaps are adjusted by phase sweeping based on KONUS beam dynamics. The first gaps are operated at the negative synchronous RF phase to provide longitudinal focusing. The subsequent gaps are 0? sections which can minimize the transverse defocusing effect. . Numerical calculation shows that the transverse defocusing of the KONUS phase is about three times smaller than that of the conv The simulation results show the beam’s transverse size is under effective control, while the increase in the longitudinal direction is slightly large. Both the Trace Win simulation and the numerical calculation show that the cavity has a relatively high effective accelerating gradient of 2.6 MV / m. On the whole, our results show that this new accelerating structure may be a possible candidate for superconducting operation at such a low energy range.