Abstract

The European Spallation Source is being constructed in Lund, Sweden and is planned to be the world’s brightest pulsed spallation neutron source for cold and thermal neutron beams (≤ 1 eV). The facility uses a 2 GeV proton beam to produce neutrons from a tungsten target. The neutrons are then moderated in a moderator assembly consisting of both liquid hydrogen and water compartments. Surrounding the moderator are 22 beamports, which view the moderator’s outside surfaces. The beamports are connected to long neutron guides that transport the moderated neutrons to the sample position via reflections. As well as the desired moderated neutrons, fast neutrons coming directly from the target can find their way down the beamlines. These can create unwanted sources of background for the instruments. To mitigate such a kind of background, several instruments will use curved guides to lose direct line-of-sight (LoS) to the moderator and the target. In addition instruments can also use shielding collimators to reduce the amount of fast neutrons further traveling down the guide due to albedo reflections or streaming. Several different materials have been proposed for this purpose. We present the results of a study of different options for collimators and identify the optimal choices that balance cost, background and activation levels.

Highlights

  • The European Spallation Source (ESS) will be the most powerful neutron source in the world for neutron scattering studies of condensed matter

  • Neutrons will be produced by a 2 GeV proton beam impinging on a target made of tungsten

  • The tungsten target, moderator and reflector will be located inside the target monolith that will be shielded by a 3.5 m of steel which extends to a radius of 5.5 m from the moderator center

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Summary

Introduction

The European Spallation Source (ESS) will be the most powerful neutron source in the world for neutron scattering studies of condensed matter. The tungsten target, moderator and reflector will be located inside the target monolith that will be shielded by a 3.5 m of steel which extends to a radius of 5.5 m from the moderator center. Within this monolith shield wall there will be beam extraction ports for each instrument. The ESS bunker will extend from the outer surface of the monolith located at 5.5 m from the target to 15 m for the short instrument (instruments several tens of meters ) and to 28 m for long instruments (instruments up to ∼150 m in length). The choice of material for such a component is a compromise between the efficiency of reducing the neutron radiation dose, the cost, and the activation of the material

The NMX instrument
Optimisation of the collimators blocks
Activation of the collimators block
Conclusions
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