# A next-generation inverse-geometry spallation-driven ultracold neutron   source

**Authors:** K.K.H. Leung, G. Muhrer, T. H\"ugle, T.M. Ito, E.M. Lutz, M. Makela,, C.L. Morris, R.W. Pattie, Jr., A. Saunders, A.R. Young

arXiv: 1905.09459 · 2020-01-08

## TL;DR

This paper presents a novel inverse-geometry design for a high-current ultracold neutron source that significantly surpasses existing sources in UCN production, utilizing advanced cryogenic technology and optimized geometry for enhanced performance.

## Contribution

The paper introduces a next-generation UCN source design with an innovative inverse-geometry approach, achieving an order-of-magnitude higher UCN rates than previous proposals and existing sources.

## Key findings

- Achieves a UCN production rate of approximately 1.8-2.1 billion UCNs per second.
- Design allows for a useful UCN current of about 5×10^8 UCNs/sec at 5 meters from the source.
- Potential to produce high-density UCNs for advanced neutron experiments.

## Abstract

The physics model of a next-generation spallation-driven high-current ultracold neutron (UCN) source capable of delivering an extracted UCN rate of around an-order-of-magnitude higher than the strongest proposed sources, and around three-orders-of-magnitude higher than existing sources, is presented. This UCN-current-optimized source would dramatically improve cutting-edge UCN measurements that are currently statistically limited. A novel "Inverse Geometry" design is used with 40 L of superfluid $^4$He (He-II), which acts as a converter of cold neutrons (CNs) to UCNs, cooled with state-of-the-art sub-cooled cryogenic technology to $\sim$1.6 K. Our design is optimized for a 100 W maximum heat load constraint on the He-II and its vessel. In our geometry, the spallation target is wrapped symmetrically around the UCN converter to permit raster scanning the proton beam over a relatively large volume of tungsten spallation target to reduce the demand on the cooling requirements, which makes it reasonable to assume that water edge-cooling only is sufficient. Our design is refined in several steps to reach $P_{UCN}=2.1\times10^9\,/$s under our other restriction of 1 MW maximum available proton beam power. We then study effects of the He-II scattering kernel as well as reductions in $P_{UCN}$ due to pressurization to reach $P_{UCN}=1.8\times10^9\,/$s. Finally, we provide a design for the UCN extraction system that takes into account the required He-II heat transport properties and implementation of a He-II containment foil that allows UCN transmission. We estimate a total useful UCN current from our source of $R_{use}=5\times10^8\,/$s from a 18 cm diameter guide 5 m from the source. Under a conservative "no return" approximation, this rate can produce an extracted density of $>1\times10^4\,/$cm$^3$ in $<$1000~L external experimental volumes with a $^{58}$Ni (335 neV) cut-off potential.

## Full text

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## Figures

13 figures with captions in the complete paper: https://tomesphere.com/paper/1905.09459/full.md

## References

95 references — full list in the complete paper: https://tomesphere.com/paper/1905.09459/full.md

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Source: https://tomesphere.com/paper/1905.09459