Current nuclear data processing status of JAEA JAEA Research Group for Reactor Physics and Standard Nuclear Code System Kenichi Tada 1.

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Presentation transcript:

Current nuclear data processing status of JAEA JAEA Research Group for Reactor Physics and Standard Nuclear Code System Kenichi Tada 1

Contents Answer of Questionnaire Request for New Nuclear Data Processing Code Other 2

Q1 What is the end purpose of your data processing activities? JAEA develops many nuclear calculation codes Deterministic code SRAC (for thermal reactor), SLAROM-UF(for fast reactor) Continuous energy Monte Carlo (MC) code MVP (for reactor calculation), PHITS (for shielding calculation) To distribute the cross section libraries for above nuclear calculation codes, JAEA uses the nuclear data processing code Cross section libraries based on JENDL, ENDF/B and JEFF are prepared. 3

Q2 Which application code uses your processed data? JAEA uses NJOY99 and PREPRO codes To appropriately process JENDL, some modules must be modified NJOY2012 is also used for test processing NJOY2012 is not allowed to release the cross section library processed with modified code NJOY2012 has still some bugs, which are not officially fixed soon as told and we also modify NJOY2012 for JENDL For example, it took 1.5 year to update NJOY2012 from patch 8 to patch 50. For these reasons, It is difficult to make cross section libraries for publication 4

Q3 What is the processed data format? Deterministic code : Original data format SRAC : 107 groups structure SLAROM-UF : 70, 175 and 900 groups structure Continuous energy MC code MVP : Original data format PHITS : ACE format 5

Q4 What are the characteristics of the group structure for deterministic codes? (for SRAC) Current SRAC code (107 groups) Fast group : Equal lethargy width Thermal group : Finer than equal lethargy width The detail concept of the group structure is unknown Developers were already retired New SRAC code (200 groups) Similar to 172 groups XMAS energy groups structure Some energy boundaries are added Iron cross section variation is appropriately treated To improve the prediction accuracy of the shielding calculation 6

Q4 What are the characteristics of the group structure for deterministic codes? (for SLAROM-UF) 70 groups structure Equal lethargy width 175 groups structure Similar to 174 groups VITAMIN energy groups structure Add energy boundary at MeV 900 groups structure Equal lethargy width Considering the average lethargy increased by the elastic scattering of 238 U Less than 50 keV : lethargy width is Larger than 50 keV : lethargy width is

Q5 What is the status of your data processing code? Currently, JAEA uses NJOY99 and PREPRO codes 8

Q6 If enhancement of the open-source data processing capabilities is undertaken through the IAEA, are you willing to contribute your software? It is difficult to contribute the development of the open-source code Contribution to the open-source project may not be recognized as JAEA’s work JAEA may not allow to collaborate on the open-souce project We may contribute as a benchmark problem Comparing the cross section data library Comparing the k eff or reaction rate in some cases 9

Q7 Which in your opinion are the data processing modules of highest priority that are not available as open-source software? None If the open-source software permits the modification of the source code Many neutron calculation code vendors add their own functions or use their original cross section data format These functions and data format are non-disclosure information The open-source software should be allowed the modification of the source code with no restriction 10

Requests for New Nuclear Data Processing Code For function Following the designation of the evaluated nuclear data library Enhancement of data output tool For processed data format Standardization of cross section data format 11

Following the designation of the evaluated nuclear data library When JENDL-4.0 is processed by NJOY99 code, some modules process as unintended The Doppler broadening process is stopped at very low energy in some nuclei 235 U, 64 Zn, 57 Fe, etc. The thermal scattering low process ignores interpolation type written in the evaluated nuclear data library Above unintended process is difficult to find It is desirable to easily understand manual and warning message 12

Enhancement of data output tool Some drawing tools are prepared NJOY99 code has VIEWR tool for drawing the processed data Drawing tool is also used to compare the difference of the previous processed data The drawing tool only outputs the graph data The drawing tool doesn’t output the text data Text data output tool is required to compare closely the difference by other programs The text data is appropriate to compare the difference using Excel, gnuplot or other programs 13

Standardization of cross section data format NJOY99 and NJOY2012 codes make some original nuclear data formats (PENDF and GENDF) The explanation of these data formats is not found in the manual The explanation of the intermediate and the final processed data format is desirable These processed data format should be standardized The standardized processed data format is formulated by the GND project? 14

FRENDY The new nuclear data processing code of JAEA To fulfill all requirements mentioned above, JAEA has started developing a new nuclear data processing code, FRENDY, in 2013 The details of FRENDY will be presented at ND , September, 2016, Bruges Belgium 15

Conclusion Answer of Questionnaire Request for New Nuclear Data Processing Code Following the designation of the evaluated nuclear data library Enhancement of data output tool Standardization of cross section data format Developing the new processing code, FRENDY 16 Thank you for your attention!!

Calculation of the arbitrary temperature thermal scattering low (S(α,β)) data The evaluated nuclear data library only prepare a few temperature S(α,β) data Users require the arbitrary temperature S(α,β) data Though users also require the arbitrary material S(α,β) data, it will not be scope of this meeting Calculation function of the arbitrary temperature S(α,β) data is desirable 17