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Joint Institute for Nuclear Research Relativistic ... - Index of - JINR

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STUDIES OF DEUTERON AND NEUTRON CROSS-SECTIONS IMPORTANT<br />

FOR ADS<br />

V. Wagner, M. Suchopár, O. Svoboda, J. Vrzalová<br />

<strong>for</strong> the collaboration "Energy and Transmutation <strong>of</strong> RAW"<br />

<strong>Nuclear</strong> Physics <strong>Institute</strong> <strong>of</strong> ASCR, 250 68 Řež, Czech Republic<br />

E-mail: wagner@ujf.cas.cz<br />

The collaboration Energy and Transmutation <strong>of</strong> Radioactive Waste uses different setups<br />

consisting <strong>of</strong> lead, natural uranium and graphite irradiated by relativistic protons and<br />

deuterons to study transmutation <strong>of</strong> radioactive materials by produced neutrons. The<br />

activation samples are used to determine integral <strong>of</strong> proton or deuteron beams and also<br />

produced neutron flux in different places <strong>of</strong> experimental set-ups. Un<strong>for</strong>tunately almost no<br />

experimental cross-section data <strong>for</strong> deuterons with GeV energies are available. The similar<br />

situation is also <strong>for</strong> threshold (n,xn) reactions <strong>of</strong> neutrons with higher energies. There<strong>for</strong>e we<br />

carried out series <strong>of</strong> experiments devoted to determination <strong>of</strong> deuteron reactions on copper<br />

during uranium target QUINTA irradiations by deuterons with energies from 1 GeV up to 8<br />

GeV. The cross-sections <strong>of</strong> various threshold reactions were studied by means <strong>of</strong> different<br />

quasi-monoenergetic neutron sources with possible energies from 14 MeV up to 100 MeV.<br />

As it was already mentioned, the cross-sections <strong>of</strong> deuteron reactions on copper were<br />

measured during several irradiations <strong>of</strong> big natural uranium target QUINTA. Values <strong>of</strong><br />

deuteron cross-section <strong>for</strong> energies <strong>of</strong> 1, 2, 4, 6 and 8 GeV were obtained. The beam integral<br />

was determined mainly by aluminum foil and there<strong>for</strong>e accuracy <strong>of</strong> our values are correlated<br />

to known experimental values <strong>of</strong> deuteron reaction Al(α,3p,2n) cross section on aluminum.<br />

Only this reaction was measured. This and other sources <strong>of</strong> systematic uncertainties will be<br />

discussed in detail.<br />

The cross-sections <strong>of</strong> many neutron reactions important <strong>for</strong> our activation detectors are<br />

missing. To improve situation we started a program <strong>of</strong> such cross-sections measurements by<br />

means <strong>of</strong> quasi-monoenergetic neutron sources. We use two such sources. The first facility is<br />

the neutron source based on the cyclotron at the <strong>Nuclear</strong> Physics <strong>Institute</strong> <strong>of</strong> ASCR, Řež. It<br />

provides neutron beams in the energy range from 14 MeV up to 35 MeV. The second neutron<br />

source is built around the cyclotron at TSL Uppsala. This facility provides neutron beam in<br />

the energy range from 14 MeV up to 200 MeV. We studied mainly cross-sections <strong>of</strong> neutron<br />

reactions on gold, aluminum, bismuth, cobalt and yttrium. We studied population <strong>of</strong> ground<br />

and isomeric states separately. The case <strong>of</strong> yttrium will be discussed in detail.<br />

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