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Fission Product Yield Data for the Transmutation of Minor Actinide ...

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42<br />

3.2. EVALUATED REFERENCE FISSION YIELD DATA FILE<br />

The Chinese reference fission yield file has<br />

been established, in which all experimental data<br />

available at <strong>the</strong> time <strong>of</strong> evaluation were considered.<br />

The data were processed using <strong>the</strong> AVERAG codes<br />

<strong>for</strong> calculating weighted averages, and ZOTT <strong>for</strong><br />

<strong>the</strong> simultaneous evaluation <strong>of</strong> experimental input<br />

data. Our evaluated data were compared with those<br />

from ENDF/B-VI, JEF-2, JENDL-3 and CENDL/<br />

FY. The data were updated and improved, and<br />

uncertainties were considerably reduced in<br />

comparison with JEF-2 and CENDL/FY.<br />

3.2.1. Introduction<br />

<strong>Fission</strong> yield data used as standards in fission<br />

yield measurements and evaluations or as monitors<br />

in <strong>the</strong> nuclear industry <strong>for</strong> decay heat calculations,<br />

burnup studies, etc., are referred to as ‘reference<br />

fission yields’. These reference fission products and<br />

<strong>the</strong>ir yields were selected and recommended by an<br />

earlier IAEA CRP [3.2.1].<br />

The uncertainties <strong>of</strong> relative yield measurements<br />

depend directly on <strong>the</strong> accuracy <strong>of</strong> <strong>the</strong><br />

standard data, and <strong>the</strong> same situation applies to<br />

yield data derived from measured ratios and<br />

R values. Applied calculations, such as decay heat<br />

and burnup, etc., also depend on <strong>the</strong> accuracy <strong>of</strong> <strong>the</strong><br />

monitor fission yield.<br />

A summary is given <strong>of</strong> <strong>the</strong> <strong>for</strong>mulation <strong>of</strong> this<br />

file, including <strong>the</strong> evaluation method and <strong>the</strong> system<br />

<strong>of</strong> supporting activities, <strong>the</strong> result <strong>of</strong> this evaluation,<br />

and <strong>the</strong> comparison with yield data from o<strong>the</strong>r<br />

evaluated libraries. Details <strong>of</strong> <strong>the</strong> evaluation can be<br />

found in Refs [3.2.2–3.2.8], which describe <strong>the</strong><br />

evaluation <strong>of</strong> 235 U and 238 U reference fission yields<br />

from 1997 to 2001.<br />

3.2.2. Evaluation method<br />

3.2.2.1. <strong>Data</strong> collection and selection<br />

Experimental data were retrieved from <strong>the</strong><br />

EXFOR master data library and evaluated by using<br />

<strong>the</strong> fission yield data evaluation system FYDES<br />

[3.2.9]. Relevant data were also collected from <strong>the</strong><br />

Liu Tingjin, Liang Qichang<br />

China Institute <strong>of</strong> Atomic Energy, China<br />

open literature. All <strong>of</strong> <strong>the</strong> data collected are listed in<br />

<strong>the</strong> tables <strong>of</strong> Refs [3.2.2–3.2.8]. The EXFOR BIB<br />

in<strong>for</strong>mation and papers were carefully studied and<br />

<strong>the</strong> method and physics background were analysed.<br />

The adoption or rejection <strong>of</strong> <strong>the</strong> data was based on<br />

<strong>the</strong> date <strong>of</strong> <strong>the</strong> original study, <strong>the</strong> measurement<br />

method and discrepancies compared with o<strong>the</strong>r<br />

data. In general, <strong>the</strong> following data were discarded:<br />

(a) The parameter(s) measured are not relevant<br />

to this evaluation.<br />

(b) There is something wrong with <strong>the</strong><br />

measurement or data analysis.<br />

(c) Compared with o<strong>the</strong>r data, <strong>the</strong> discrepancy is<br />

large and <strong>the</strong> measurement method is not<br />

reliable, or no detailed in<strong>for</strong>mation is given<br />

concerning <strong>the</strong> experiment and/or analysis.<br />

(d) The values or <strong>the</strong> reliability <strong>of</strong> <strong>the</strong> adopted<br />

standard data in measurements <strong>of</strong> relative<br />

data are not given in <strong>the</strong> paper. Such<br />

in<strong>for</strong>mation is indispensable in <strong>the</strong> evaluation<br />

<strong>of</strong> ‘reference yield data’, and data cannot be<br />

used that are based on standards <strong>of</strong> unknown<br />

value or reliability.<br />

As a result, about half <strong>of</strong> <strong>the</strong> data were discarded,<br />

and half were used (<strong>for</strong> details, see Refs [3.2.2–<br />

3.2.8]).<br />

3.2.2.2. <strong>Data</strong> correction<br />

If necessary, <strong>the</strong> measured data were<br />

corrected <strong>for</strong> <strong>the</strong> values used <strong>for</strong> <strong>the</strong> standards,<br />

g ray intensities and fission cross-sections (in<br />

absolute measurements). As mentioned above, <strong>the</strong><br />

relative data were generally not used as published.<br />

Such data were only selected when <strong>the</strong> standard<br />

yields used by <strong>the</strong> authors correspond to, or agree<br />

with, <strong>the</strong> recently evaluated values, or if <strong>the</strong>y can be<br />

corrected using our reference yields.<br />

These corrections were made by using <strong>the</strong><br />

equation:<br />

U U U<br />

= 0<br />

U<br />

8<br />

SO<br />

(3.2.1)

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