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International Reactor Dosimetry File 2002 - IAEA Publications

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Fluence rate per unit energy (m –2·s –1·MeV –1 )<br />

10 20<br />

10 18<br />

10 16<br />

10 14<br />

10 12<br />

10 10<br />

10 8<br />

10<br />

10 –10 10 –9 10 –8 10 –7 10 –6 10 –5 10 –4 10 –3 10 –2 10 –1 10 0 10 1 10 2<br />

6<br />

Energy (MeV)<br />

10 14<br />

Fluence rate per unit lethargy (m –2·s –1 )<br />

10 13<br />

10 12<br />

10<br />

10 –10 10 –9 10 –8 10 –7 10 –6 10 –5 10 –4 10 –3 10 –2 10 –1 10 0 10 1 10 2<br />

11<br />

Energy (MeV)<br />

FIG. 3.1. Neutron spectrum MTR in two different representations, as used in the<br />

uncertainty calculations [3.6].<br />

IRDF-90 and the other libraries of interest, while the related uncertainty<br />

information can vary with the source of data. Reactions exhibiting this<br />

behaviour are 23 Na(n,γ) 24 Na (IRDF-90 and ENDF/B-VI), 55 Mn(n,γ) 56 Mn<br />

(IRDF-90 and JENDL/D-99), 63 Cu(n,γ) 64 Cu (IRDF-90 and ENDF/B-VI),<br />

93 Nb(n,γ) 94 Nb (IRDF-90 and ENDF/B-VI), 115 In(n,γ) 116 In m (IRDF-90 and<br />

ENDF/B-VI) and 232 Th(n,γ) 233 Th (IRDF-90 and ENDF/B-VI). IRDF-90 was<br />

taken as the source of data for IRDF-<strong>2002</strong> in these particular cases.<br />

Considering the 58 Fe(n,γ) 59 Fe reaction: the resonance integral in both<br />

cross-section files of interest (IRDF-90 and JENDL/D-99) deviates significantly<br />

from the corresponding data of Mughabghab, while the JENDL/D-99<br />

value is in good agreement with the data of Holden (as compared with the<br />

relevant uncertainties). Further clarification is required, for example, by<br />

19

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