Abstract

The paper presents results of FLUKA simulations of the residual activity induced by heavy ions in two target configurations representing: (1) a beam pipe of an accelerator and (2) a bulky accelerator structure like a magnet yoke or a coil. The target materials were stainless steel and copper representing the most common construction materials used for basic accelerator components. For these two materials, the inventory of the induced isotopes depends mainly on the target material and much less on the projectile species. Time evolution of the induced activity can be described by means of a generic curve that is independent from the projectile mass. Dependence of the induced residual activity on selected ion beam parameters was studied. The main goal of the study was establishing a scaling law expanding the existing proton beam-loss tolerance to heavy-ion beams. This scaling law enables specifying beam-loss criteria for projectile species from proton up to uranium at energies from $200\text{ }\text{ }\mathrm{MeV}/\mathrm{u}$ up to $1\text{ }\text{ }\mathrm{GeV}/\mathrm{u}$.

Highlights

  • Activation of accelerator components due to beam losses during normal machine operation is an important issue especially for high-energy hadron accelerators [1–3]

  • The tolerable beam losses for uranium beam could be 12 W=m at 1 GeV=u, 23 W=m at 500 MeV=u, and 75 W=m at 200 MeV=u

  • The tolerable beam losses for uranium beam could be 5 W=m at 1 GeV=u, 12 W=m at 500 MeV=u, and 60 W=m at 200 MeV=u

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Summary

Introduction

Activation of accelerator components due to beam losses during normal machine operation is an important issue especially for high-energy hadron accelerators [1–3]. The radioactive nuclides are produced by primary ions (projectiles) as well as by secondary particles such as protons, neutrons, and fragments generated by interaction of the primary beam with the target material [1]. Activation by the secondary particles is a dominating mechanism for heavy-ion beams, which is experimentally manifested by its presence far beyond the range of the primary particles [7–10]. The heavy projectiles are fragmented into radioactive projectile fragments that remain implanted in the target. Their contribution to the total residual activity is negligible for high-energy heavy-ion projectiles [8–10]

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