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JAEA-Data/Code 2007-004 - Welcome to Research Group for ...

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Usually, enter IRES=2 <strong>for</strong> the heavy nuclide in fuel of which cross-sections<br />

have sharp resonance structure, otherwise IRES=0. For the nuclides born during<br />

burn-up calculation, the IRES values are given in the burn-up chain library (cf.<br />

Sect.3.3).<br />

When PEACO routine is used, the IRES value given in MCROSS library is<br />

applied even if any value is entered <strong>for</strong> IRES. However, the input IRES is still<br />

effective in the evaluation of the self-shielding fac<strong>to</strong>r based on the NR<br />

approximation (applied out of the energy range of PEACO calculation).<br />

<br />

In the tabulation of P ij <strong>for</strong> PEACO calculation, the cross-sections of<br />

non-resonant nuclides are assumed as constant by using the value of the highest<br />

energy group of PEACO calculation, unless IRES=3 or IRES=4 is specified.<br />

For the systems involving coolant water with boron or control rod, the<br />

specification of IRES=3 or IRES=4 <strong>for</strong> B-10 gives more exact treatment. However,<br />

treatment by IRES=3 requires the P ij tabulation by energy group and that by<br />

IRES=4 does two-dimensional tabulation. Both treatments need much computer<br />

time.<br />

3 IXMICR Indica<strong>to</strong>r <strong>to</strong> write the effective cross-sections in<strong>to</strong> the effective microscopic crosssection<br />

file (MICREF)<br />

= 0 No edit.<br />

= 1 Write the effective microscopic cross-sections in<strong>to</strong> the MICREF file.<br />

= 2 Write the microscopic cross-sections of hyperfine group structure<br />

averaged in the cell in<strong>to</strong> UMCROSS file after PEACO calculation. The<br />

seventh and eighth characters of the member name are taken from the last<br />

half of CASENAME. During the cell burn-up calculation, the seventh<br />

character is overridden by b-tag. This option may be utilized <strong>for</strong> the<br />

output of <strong>for</strong>mer step in the treatment of double heterogeneity.<br />

= 3 both of functions of IXMICR=1 & =2.<br />

Note:<br />

If the cell burn-up routine is used (IC20=1), the same option is available in Sect.<br />

2.11 <strong>for</strong> the nuclides not appearing in this input section (e.g. MA or F.P.)<br />

127

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