333 research outputs found
Experimental investigation of the low molecular weight fluoropolymer for the ultracold neutrons storage
The experimental setup for examining the low-molecular-weight fluoropolymer
CF(CF-O-CF-O-(CFCF, which is a
promising coating material for the walls of storage chambers for ultracold
neutrons, is described. The results are detailed. The measurement data are
interpreted in the model of a multilayer complex quantum-mechanical potential
of the chamber walls.Comment: Corrected version of the paper published in Phys. of Part. and Nucl
Lett., 15 (No.5) (2018) 54
Characteristics of light charged particle emission in the ternary fission of 250Cf and 252Cf at different excitation energies
The emission probabilities and the energy distributions of tritons, α and ^6He particles emitted in the spontaneous ternary fission (zero excitation energy) of ^250Cf and ^252Cf and in the cold neutron induced fission (excitation energy ≈ 6.5 MeV) of ^249Cf and 251Cf are determined. The particle identification was done with suited ΔE-E telescope detectors, at the IRMM (Geel, Belgium) for the spontaneous fission and at the ILL (Grenoble, France) for the neutron induced fission measurements. Hence particle emission characteristics of the fissioning systems ^250Cf and ^252Cf are obtained at zero and at about 6.5 MeV excitation energies. While the triton emission probability is hardly influenced by the excitation energy, the ^4He and ^6He emission probability in spontaneous fission is higher than for neutron induced fission. This can be explained by the strong influence of the cluster preformation probability on the ternary particle emission probability
Efficient extraction of a collimated ultra-cold neutron beam using diffusive channels
We present a first experimental demonstration of a new method to extract a
well-collimated beam of ultra-cold neutrons (UCN) from a storage vessel.
Neutrons with too large divergence are not removed from the beam by an
absorbing collimation, but a diffuse or semidiffuse channel with high Fermi
potential reflects them back into the vessel. This avoids unnecessary losses
and keeps the storage time high, which may be beneficial when the vessel is
part of a UCN source with long buildup time of a high UCN density
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