Magistris M, Silari M
CERN, 1211 Geneva 23, Switzerland.
Radiat Prot Dosimetry. 2005;115(1-4):491-6. doi: 10.1093/rpd/nci099.
In a beta-beam facility, a pure beam of electron neutrinos, or their antiparticles, are produced by the decay of fully stripped radioactive ions (6He and 18Ne) circulating in a storage ring. Since the beam is not extracted from the ring, all the particles will eventually be lost somewhere in the machine and thus activate the accelerator components and the surrounding concrete and rock. In particular, as nuclei change their charge in beta-decay, a large part of the particles will be lost in the arcs of the decay ring and mainly irradiate the magnets. The density of inelastic interactions of hadrons in the magnets, concrete and rock and the track-length distribution of secondary hadrons were calculated by means of the FLUKA Monte Carlo code. These values were used to estimate the induced radioactivity in the facility, the dose rates expected in the decay ring and the consequences for the environment.
在β束装置中,完全剥离的放射性离子(6He和18Ne)在储存环中循环衰变产生纯电子中微子束或其反粒子束。由于束流并非从环中引出,所有粒子最终都会在加速器的某个位置损失,从而使加速器部件以及周围的混凝土和岩石活化。特别是,由于原子核在β衰变中电荷发生变化,大部分粒子会在衰变环的弧段中损失,并主要对磁铁产生辐照。利用FLUKA蒙特卡罗代码计算了磁铁、混凝土和岩石中强子的非弹性相互作用密度以及次级强子的径迹长度分布。这些值被用于估算装置中的感生放射性、衰变环中预期的剂量率以及对环境的影响。