Author/Authors :
Serebrov، نويسنده , , A.P. and Mityuklyaev، نويسنده , , V.A. and Zakharov، نويسنده , , A.A. and Erykalov، نويسنده , , A.N. and Onegin، نويسنده , , M.S. and Fomin، نويسنده , , A.K. and Ilatovskiy، نويسنده , , V.A. and Orlov، نويسنده , , S.P. and Konoplev، نويسنده , , K.A. and Krivshitch، نويسنده , , A.G. and Samsonov، نويسنده , , V.M. and Ezhov، نويسنده , , V.F. and Fedorov، نويسنده , , V.V. and Keshyshev، نويسنده , , K.O. and Boldarev، نويسنده , , S.T. and Marchenko، نويسنده , , V.I.، نويسنده ,
Abstract :
The WWR-M reactor of PNPI offers a unique opportunity to prepare a source for ultracold neutrons (UCN) in an environment of high neutron flux (about 3×1012 n/cm2/s) but still acceptable radiation heat release (about 4×10−3 W/g). It can be realized within the thermal column situated close to the reactor core. With its large diameter of 1 m, this channel allows to install a 15-cm-thick bismuth shielding, a graphite premoderator (300 dm3 at 20 K), and a superfluid helium converter (35 dm3). At a temperature of 1.2 K it is possible to remove the heat release power of about 20 W. Using 4π flux of cold neutrons within the reactor column can bring more than a factor 100 of cold neutron flux incident on the superfluid helium with respect to the present cold neutron beam conditions at the ILL reactor. The storage lifetime for UCN in superfluid He at 1.2 K is about 30 s, which is sufficient when feeding experiments requiring a similar filling time. The calculated density of UCN with energy between 50 and 230 neV in an experimental volume of 40 l is about 104 n/cm3. Technical solutions for realization of the project are discussed.
