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Fizika Tverdogo Tela, 2010 Volume 52, Issue 5, Pages 969–973 (Mi ftt13735)

This article is cited in 12 papers

XX Anniversary Meeting on the Use of Neutron Scattering in Condensed Matter Research (RNICS-2008), Gatchina (October 13-18, 2008)
Neutron experimental techniques, instrumentation, and radiation sources

Project of the ultracold and cold neutron source at the WWR-M reactor with superfluid helium as a moderator

A. P. Serebrova, V. A. Mityukhlyaeva, A. A. Zakharova, A. N. Erikalova, M. S. Onegina, A. K. Fomina, V. A. Ilatovskiia, S. P. Orlova, K. A. Konopleva, A. G. Krivshicha, V. M. Samsonova, V. F. Ezhova, V. V. Fedorova, K. O. Keshishevb, S. T. Boldarevb, V. I. Marchenkob

a The Petersburg Nuclear Physics Institute, The National Research Center "Kurchatov Institute"
b P. L. Kapitza Institute for Physical Problems, Russian Academy of Sciences, Moscow

Abstract: The WWR-M reactor of the Petersburg Nuclear Physics Institute provides a unique opportunity for creating conditions of low radiative heat release ($\sim$4 $\times$ 10$^{-3}$ W/g) at a sufficiently high neutron flux ($\sim$3 $\times$ 10$^{12}$ neutrons/(cm$^2$ s)). This opportunity can be implemented in the reactor thermal column, which represents a 1-m-diameter channel adjacent to the reactor core. This diameter of the channel allows the arrangement of the core $\gamma$ shielding made of bismuth (15 cm thick), a graphite premoderator (300 dm$^3$) at a temperature of 20 K, and a converter with superfluid helium (35 dm$^3$) at a temperature of 1.2 K. Calculations show that the heat release in the source (20 W) can be removed by pumping helium vapor, and the density of ultracold neutrons in an experimental trap will be $\sim$10$^4$ neutrons/cm$^3$, which is higher than that of existing sources of ultracold neutrons by two to three orders of magnitude.


 English version:
Physics of the Solid State, 2010, 52:5, 1034–1039

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