Beam dynamics studies on the 100 MeV/100 kW electron linear accelerator for NSC KIPT neutron source  被引量:2

Beam dynamics studies on the 100 MeV/100 kW electron linear accelerator for NSC KIPT neutron source

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作  者:裴士伦 池云龙 王书鸿 裴国玺 周祖圣 侯汨 Mykola Ayzatskiy Ivan Karnaukhov Volodymyr Kushnir Viktor Mytrochenko Andrey Zelinsky 

机构地区:[1]Institute of High Energy Physics,Chinese Academy of Sciences [2]Kharkov Institute of Physics and Technology,National Science Center

出  处:《Chinese Physics C》2012年第7期653-660,共8页中国物理C(英文版)

摘  要:We designed a 100 MeV/100 kW electron linear accelerator for NSC KIPT, which will be used to drive a neutron source on the basis of subcritical assembly. Beam dynamics studies have been conducted to reach the design requirements (E=100 MeV, P=100 kW, dE/E 〈1% for 99% particles). In this paper, we will present the progress of the design and the dynamic simulation results. For high intensity and long beam pulse linear accelerators, the BBU effect is one big issue; special care has been taken in the accelerating structure design. To satisfy the energy spread requirement at the linac exit, the particles with large energy difference from the synchronous particle should be eliminated at a low energy stage to ease the design of the collimation system and radiation shielding. A dispersion free chicane with 4 bending magnets is introduced downstream of the 1st accelerating section; the unwanted particles will be collimated there.We designed a 100 MeV/100 kW electron linear accelerator for NSC KIPT, which will be used to drive a neutron source on the basis of subcritical assembly. Beam dynamics studies have been conducted to reach the design requirements (E=100 MeV, P=100 kW, dE/E 〈1% for 99% particles). In this paper, we will present the progress of the design and the dynamic simulation results. For high intensity and long beam pulse linear accelerators, the BBU effect is one big issue; special care has been taken in the accelerating structure design. To satisfy the energy spread requirement at the linac exit, the particles with large energy difference from the synchronous particle should be eliminated at a low energy stage to ease the design of the collimation system and radiation shielding. A dispersion free chicane with 4 bending magnets is introduced downstream of the 1st accelerating section; the unwanted particles will be collimated there.

关 键 词:beam dynamics linear accelerator BBU collimation system neutron source 

分 类 号:TL53[核科学技术—核技术及应用]

 

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