Abstract

The WWR-M reactor at PNPI is planned to be equipped with a high-flux source for ultracold neutrons (UCNs). The method of UCN production is based on neutron conversion in superfluid helium, exploiting the particular qualities of that quantum liquid. As a result of optimizing the source parameters, we expect a temperature of superfluid helium of 1.2 K and a UCN density of 1.3 × 104 cm−3 in a neutron electric dipole moment (EDM) spectrometer. The expected flux densities of cold neutrons (with wavelengths in the range 2–20 Å) and very cold neutrons (50–100 Å) at the output of a neutron guide with a cross section of 30 × 200 mm2 are 9.7 × 107 cm−2s−1 and 8.3 × 105 cm−2s−1, respectively. The capability of maintaining a temperature of 1.37 K at a thermal load of 60 W was shown experimentally, while the theoretical load is expected to be 37 W. Calculations show that it is possible to decrease the helium temperature down to 1.2 K at similar heat load. The project includes the development of experimental stations at UCN beams, such as for a neutron EDM search, measurements of the neutron lifetime, and for a search for neutron-to-mirror-neutron transitions. In addition, three beams of cold and very cold neutrons are foreseen. At present, the vacuum container of the UCN source has been manufactured and the production of the low-temperature deuterium and helium parts of the source has been started.

Highlights

  • The project for creating CN and ultracold neutrons (UCNs) sources originated in the 70 s of the last century

  • UCN fluxes high for that time were obtained here by means of passing reactor neutrons through various low-temperature converters: beryllium [1], liquid hydrogen [2], liquid deuterium [3], and solid deuterium [4]

  • Yields of UCN production depend on the intensity of the reactor neutron flux and the efficiency of a cryogenic converter, with or without a cold premoderator

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Summary

The project of a UCN source at the WWR-M reactor

The project for creating CN and UCN sources originated in the 70 s of the last century. UCN fluxes high for that time were obtained here by means of passing reactor neutrons through various low-temperature converters: beryllium [1], liquid hydrogen [2], liquid deuterium [3], and solid deuterium [4]. Yields of UCN production depend on the intensity of the reactor neutron flux and the efficiency of a cryogenic converter, with or without a cold premoderator. Output optimization of UCN fluxes from the source has been carried out using a Monte-Carlo code [8], developed for neutron transport simulations with account of gravitation It resulted in determining the geometry of the source chamber (diameter 30 cm, volume 35 l) and the neutron guide from the UCN source. Foreseen is a beam of very cold neutrons (VCN) at CN3 for experiments to be defined in future

Full-scale tests of UCN source model
Brief descriptions of the source components
Vacuum module
Cryogenic module
Findings
Transport trolley

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