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E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT) - ppt download

<!DOCTYPE html> <html> <head> <title>E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT) - ppt download</title> <meta charset="utf-8"><meta http-equiv="Content-Type" content="text/html; charset=UTF-8"> <meta name="viewport" content="width=device-width, initial-scale=1.0, maximum-scale=1"> <meta property="og:title" content="E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT) - ppt download"> <meta property="og:type" content="website"> <link rel="canonical" href="https://slideplayer.com/slide/11458042/"/> <meta property="og:url" content="https://slideplayer.com/slide/11458042/"> <link rel="amphtml" href="https://slideplayer.com/amp/11458042/"> <meta name="description" content="Necessary implementations - For the use of the new generated neutron libraries it is necessary to include the possibility of reading capture photon data in MF=6 format. This can be done (and it has been done), by performing a very little modification in the GEANT4 code, since GEANT4 reads and interprets photon data in MF=6 format for other reactions (inelastic = all except elastic, capture and fission). - Same for neutrons in the fission process, but only for three isotopes: 232Th, 231Pa, 233Pa in ENDF_VII.0. The MF=6 format data has been translated into MF=4,5 (uncorrelated) data, but maybe for a future it would be better to use MF=6 format."> <meta property="og:description" content="Necessary implementations - For the use of the new generated neutron libraries it is necessary to include the possibility of reading capture photon data in MF=6 format. This can be done (and it has been done), by performing a very little modification in the GEANT4 code, since GEANT4 reads and interprets photon data in MF=6 format for other reactions (inelastic = all except elastic, capture and fission). - Same for neutrons in the fission process, but only for three isotopes: 232Th, 231Pa, 233Pa in ENDF_VII.0. The MF=6 format data has been translated into MF=4,5 (uncorrelated) data, but maybe for a future it would be better to use MF=6 format."> <meta name="keywords" content="E. 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Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT)</h1> <p class="uk-article-meta">Published by<a href="/user/13075121/" class="uk-margin-small-left uk-margin-small-right">初龙 米</a> <span id="timeago" class="uk-float-right">Modified over 7 years ago</span> </p> </div> <div id="social-share" class="uk-float-left uk-margin"> <div id="pluses"> <div class="addthis_toolbox addthis_default_style addthis_32x32_style"> <a class="addthis_button_facebook"></a> <a class="addthis_button_twitter"></a> <a class="addthis_button_linkedin"></a> <a class="addthis_button_google_plusone_share"></a> <a class="addthis_button_blogger"></a> <a class="addthis_button_flipboard"></a> <a class="addthis_button_google"></a> <a class="addthis_button_gmail"></a> <a class="addthis_button_vk"></a> <a class="addthis_button_email"></a> <a class="addthis_button_pinterest_share"></a> <a class="addthis_button_tumblr"></a> <a class="addthis_button_myspace"></a> <a class="addthis_button_wordpress"></a> <a class="addthis_button_ziczac"></a> <a class="addthis_button_print"></a> <a class="addthis_button_favorites"></a> <a class="addthis_button_whatsapp"></a> <a class="addthis_button_reddit"></a> <a class="addthis_counter addthis_bubble_style"></a> </div> </div> </div> <!-- <form method="post" action="/slide/download/" id="download_form_2">--> <div class="uk-float-right uk-margin" id="get-code-btn"> <div class="uk-button-group uk-margin-small-right"> <button type="button" class="uk-button uk-button uk-button-primary"><span class="uk-icon-code"></span></button> <button type="button" data-original-title="Embed this presentation" id="get_embed" class="uk-button uk-button">Embed</button> </div> <!-- <input type="hidden" name="slide_id" value="--><!--" />--> <div class="uk-button-group" id="download-btn"> <button class="uk-button uk-button uk-button-success" data-toggle="modal" data-target="#download-modal"><span class="uk-icon-cloud-download"></span></button> <button class="uk-button uk-button" data-toggle="modal" data-target="#download-modal">Download presentation</button> </div><!-- <button type="submit" class="uk-button uk-button uk-button-success"><span class="uk-icon-cloud-download"></span></button>--> <!-- <button type="submit" class="uk-button uk-button">--><!--</button>--> </div> <!-- </div>--> <!-- </form>--> </div> </div> <div class="uk-panel uk-panel-box uk-panel-box-secondary uk-margin" id="embed" style="display: none"> <div class="uk-margin uk-text-right"> <div class="uk-form-row"> <textarea rows="3" cols="" id="embed_input"></textarea> </div> <div class="uk-button-group"> <button class="uk-button uk-button uk-button-success"><span class="uk-icon-copy"></span></button> <button title="Customize embed code" id="copyembed" class="uk-button uk-button"> Copy to clipboard</button> </div> </div> </div> <div class="top_comment_banners uk-text-center uk-nbfc"> </div> <div class="uk-panel uk-panel-box uk-panel-box-secondary uk-margin" id="fb_wrapper"> <div class="fb-comments" data-href="http://slideplayer.com/slide/11458042/" data-numposts="5" data-width="100%""></div> </div> <div class="bottom_comment_banners uk-text-center uk-nbfc"> <style>#place_137 > ins[data-ad-slot="4312680294"]{display:none;} @media (min-width: 0px) and (max-width: 5000px) { #place_137 > ins[data-ad-slot="4312680294"]{display:inline-block;} } </style><div id="place_137" class="ads uk-text-center uk-margin-small-bottom uk-margin-small-right uk-display-inline-block uk-margin-small-top"> <script async src="//pagead2.googlesyndication.com/pagead/js/adsbygoogle.js"></script> <ins class="adsbygoogle" style="min-width:234px; max-width:728px; width:100%; height:60px" data-ad-client="ca-pub-6133583279631137" data-ad-slot="4312680294" ></ins> <script> (adsbygoogle = window.adsbygoogle || []).push({}); </script></div> </div> <div id="after_comment_similars" class="uk-margin-bottom uk-margin-top uk-panel uk-panel-box uk-panel-box-secondary uk-margin"> <h3 class="tm-text-dark"> <span class="uk-icon-list uk-margin-small-right"></span>Similar presentations </h3> <hr class="uk-article-divider"> <div></div> <button class="uk-button uk-margin-top uk-button-primary uk-width-1-1" id="load_more_btn"><span class="uk-icon-arrow-circle-down uk-margin-small-right"></span>More</button> </div> <div class="uk-panel uk-panel-box uk-panel-box-secondary uk-margin"> <div class="uk-article"> <h2 class="transkript-title">Presentation on theme: "E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT)"— Presentation transcript:</h2> <style> @media(min-width:801px){#place_14>ins[data-ad-slot="4502451947"]{display:none !important;}} @media(max-width:800px){#place_14>ins:not([data-ad-slot="4502451947"]){display:none !important;}} @media(max-width:800px){#place_14 { width: 250px;}} @media(max-width:500px) {#place_14 { width: 120px;}} </style><div id="place_14" class="ads "> <script async src="//pagead2.googlesyndication.com/pagead/js/adsbygoogle.js"></script> <ins class="adsbygoogle" style="display:block" data-ad-client="ca-pub-6133583279631137" data-ad-slot="4502451947" data-ad-format="auto" data-full-width-responsive="true"></ins> <script> (adsbygoogle = window.adsbygoogle || []).push({}); </script> <script async src="https://pagead2.googlesyndication.com/pagead/js/adsbygoogle.js"></script> <ins class="adsbygoogle" data-ad-client="ca-pub-6133583279631137" style="display:inline-block;width:336px;height:280px" data-ad-slot="7321420150"></ins> <script>(adsbygoogle = window.adsbygoogle || []).push({});</script></div> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/1/E.+Mendoza%2C+D.Cano-Ott+Nuclear+Innovation+Unit+%28CIEMAT%29.jpg" target="_blank" title="E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT)" > 1 </a> </span> <strong>E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT)</strong><br><span class='tr'>Necessary improvements of G4NeutronHP for the new libraries. Resolved and open questions.</span> <span class='tr'>E. Mendoza, D.Cano-Ott</span> <span class='tr'>Nuclear Innovation Unit (CIEMAT)</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/1/E.+Mendoza%2C+D.Cano-Ott+Nuclear+Innovation+Unit+%28CIEMAT%29.jpg", "name": "E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT)", "description": "Necessary improvements of G4NeutronHP for the new libraries. Resolved and open questions. E. Mendoza, D.Cano-Ott. Nuclear Innovation Unit (CIEMAT)", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/1/E.+Mendoza%2C+D.Cano-Ott+Nuclear+Innovation+Unit+%28CIEMAT%29.jpg" width="1024" align="left" alt="E. Mendoza, D.Cano-Ott Nuclear Innovation Unit (CIEMAT)" title="Necessary improvements of G4NeutronHP for the new libraries. Resolved and open questions. E. Mendoza, D.Cano-Ott. Nuclear Innovation Unit (CIEMAT)"> </noscript> <br /></p> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/2/Necessary+implementations.jpg" target="_blank" title="Necessary implementations" > 2 </a> </span> <strong>Necessary implementations</strong><br><span class='tr'>- For the use of the new generated neutron libraries it is necessary to include the possibility of reading capture photon data in MF=6 format. This can be done (and it has been done), by performing a very little modification in the GEANT4 code, since GEANT4 reads and interprets photon data in MF=6 format for other reactions (inelastic = all except elastic, capture and fission).</span> <span class='tr'>- Same for neutrons in the fission process, but only for three isotopes: 232Th, 231Pa, 233Pa in ENDF_VII.0. The MF=6 format data has been translated into MF=4,5 (uncorrelated) data, but maybe for a future it would be better to use MF=6 format.</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/2/Necessary+implementations.jpg", "name": "Necessary implementations", "description": "- For the use of the new generated neutron libraries it is necessary to include the possibility of reading capture photon data in MF=6 format. This can be done (and it has been done), by performing a very little modification in the GEANT4 code, since GEANT4 reads and interprets photon data in MF=6 format for other reactions (inelastic = all except elastic, capture and fission). - Same for neutrons in the fission process, but only for three isotopes: 232Th, 231Pa, 233Pa in ENDF_VII.0. The MF=6 format data has been translated into MF=4,5 (uncorrelated) data, but maybe for a future it would be better to use MF=6 format.", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/2/Necessary+implementations.jpg" width="1024" align="left" alt="Necessary implementations" title="- For the use of the new generated neutron libraries it is necessary to include the possibility of reading capture photon data in MF=6 format. This can be done (and it has been done), by performing a very little modification in the GEANT4 code, since GEANT4 reads and interprets photon data in MF=6 format for other reactions (inelastic = all except elastic, capture and fission). - Same for neutrons in the fission process, but only for three isotopes: 232Th, 231Pa, 233Pa in ENDF_VII.0. The MF=6 format data has been translated into MF=4,5 (uncorrelated) data, but maybe for a future it would be better to use MF=6 format."> </noscript> <br /></p> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/3/Neutron+validation+results.jpg" target="_blank" title="Neutron validation results" > 3 </a> </span> <strong>Neutron validation results</strong><br><span class='tr'>In the GEANT4 comparison with MCNPX done up to now, three main differences have been found:</span> <span class='tr'>1- Thermal neutrons: include more thermal neutron libraries?. There are only three materials available, whereas there are 20 in ENDF-VII.0, 9 in JEFF-3.1, 15 in JENDL-4.0, …</span> <span class='tr'>2- The “inelastic” problem: cross sections should include the QI value for the calculation of the energy secondary particle, instead of using the Inelastic/Gamma folders.</span> <span class='tr'> include Breakup reactions?</span> <span class='tr'>3- Self shielding treatment: some procedure to treat the URR could be implemented. It should be based in cross section evaluated data for the URR: statistical parameters such as the main distance between resonances, size, …</span> <span class='tr'>4- Fission???</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/3/Neutron+validation+results.jpg", "name": "Neutron validation results", "description": "In the GEANT4 comparison with MCNPX done up to now, three main differences have been found: 1- Thermal neutrons: include more thermal neutron libraries . There are only three materials available, whereas there are 20 in ENDF-VII.0, 9 in JEFF-3.1, 15 in JENDL-4.0, \u2026 2- The inelastic problem: cross sections should include the QI value for the calculation of the energy secondary particle, instead of using the Inelastic\/Gamma folders. \uf0e0 include Breakup reactions 3- Self shielding treatment: some procedure to treat the URR could be implemented. It should be based in cross section evaluated data for the URR: statistical parameters such as the main distance between resonances, size, \u2026 4- Fission", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/3/Neutron+validation+results.jpg" width="1024" align="left" alt="Neutron validation results" title="In the GEANT4 comparison with MCNPX done up to now, three main differences have been found: 1- Thermal neutrons: include more thermal neutron libraries . There are only three materials available, whereas there are 20 in ENDF-VII.0, 9 in JEFF-3.1, 15 in JENDL-4.0, … 2- The inelastic problem: cross sections should include the QI value for the calculation of the energy secondary particle, instead of using the Inelastic/Gamma folders.  include Breakup reactions 3- Self shielding treatment: some procedure to treat the URR could be implemented. It should be based in cross section evaluated data for the URR: statistical parameters such as the main distance between resonances, size, … 4- Fission"> </noscript> <br /></p> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/4/Non-neutron+validation+results.jpg" target="_blank" title="Non-neutron validation results" > 4 </a> </span> <strong>Non-neutron validation results</strong><br><span class='tr'>- No validation for particle production (different) than neutrons have been performed by CIEMAT.</span> <span class='tr'>- Gamma production:</span> <span class='tr'>1- Gamma production in ENDF files is usually UNCORRELATED data.</span> <span class='tr'>2- Gamma production in ENDF files can be incomplete or missing.</span> <span class='tr'>Possibilities to manage the photon production in GEANT4:</span> <span class='tr'>1- Use ENDF data (only).</span> <span class='tr'>2- Use models.</span> <span class='tr'>3- Use both ???</span> <span class='tr'>Mixing models with ENDF data has to be done with extremely care.</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/4/Non-neutron+validation+results.jpg", "name": "Non-neutron validation results", "description": "- No validation for particle production (different) than neutrons have been performed by CIEMAT. - Gamma production: 1- Gamma production in ENDF files is usually UNCORRELATED data. 2- Gamma production in ENDF files can be incomplete or missing. Possibilities to manage the photon production in GEANT4: 1- Use ENDF data (only). 2- Use models. 3- Use both Mixing models with ENDF data has to be done with extremely care.", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/4/Non-neutron+validation+results.jpg" width="1024" align="left" alt="Non-neutron validation results" title="- No validation for particle production (different) than neutrons have been performed by CIEMAT. - Gamma production: 1- Gamma production in ENDF files is usually UNCORRELATED data. 2- Gamma production in ENDF files can be incomplete or missing. Possibilities to manage the photon production in GEANT4: 1- Use ENDF data (only). 2- Use models. 3- Use both Mixing models with ENDF data has to be done with extremely care."> </noscript> <br /></p> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/5/Non-neutron+validation+results.jpg" target="_blank" title="Non-neutron validation results" > 5 </a> </span> <strong>Non-neutron validation results</strong><br><span class='tr'>Possible solution: include a flag which specifies how to manage the photon production data.</span> <span class='tr'>- PFlag=0: use ENDF data.</span> <span class='tr'>- PFlag=1: use models.</span> <span class='tr'>- PFlag=2: use ENDF data, if there is no data, use models.</span> <span class='tr'>-PFlag=3: …</span> <span class='tr'> adjust_final_state method of the G4NeutronHPFinalState class.</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/5/Non-neutron+validation+results.jpg", "name": "Non-neutron validation results", "description": "Possible solution: include a flag which specifies how to manage the photon production data. - PFlag=0: use ENDF data. - PFlag=1: use models. - PFlag=2: use ENDF data, if there is no data, use models. -PFlag=3: \u2026 \uf0e0 adjust_final_state method of the G4NeutronHPFinalState class.", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/5/Non-neutron+validation+results.jpg" width="1024" align="left" alt="Non-neutron validation results" title="Possible solution: include a flag which specifies how to manage the photon production data. - PFlag=0: use ENDF data. - PFlag=1: use models. - PFlag=2: use ENDF data, if there is no data, use models. -PFlag=3: …  adjust_final_state method of the G4NeutronHPFinalState class."> </noscript> <br /></p> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/6/General+comments+1-+Lack+of+data%3A+ENDF+format+libraries+have+some+amount+of+isotopes.+However%2C+there+are%3A.jpg" target="_blank" title="General comments 1- Lack of data: ENDF format libraries have some amount of isotopes. However, there are:" > 6 </a> </span> <span>General comments</span> <span class='tr'>1- Lack of data: ENDF format libraries have some amount of isotopes. However, there are:</span> <span class='tr'>A- Some isotopes are missing.</span> <span class='tr'>B- The information for each isotope has to be, in principle, complete (exception: ROSFOND library). However, this doesn’t mean that all reactions are 100% perfectly described, specially for secondary particles different than neutrons.</span> <span class='tr'>What to do?</span> <span class='tr'>A- By default, if one isotope is missing, take the natural component (Warning in the output), if there is no natural component, exit.</span> <span class='tr'>(export G4NEUTRONHP_SKIP_MISSING_ISOTOPES=1)</span> <span class='tr'>B- Several options can be taken:</span> <span class='tr'>1- Perform the simulation with the available data (do not generate secondary particles if there is no data).</span> <span class='tr'>2- Use models.</span> <span class='tr'>3- Distribute only isotopes with some minimal information.</span> <span class='tr'>4- Use some flags to determine what to do.</span> <span class='tr'>5- …</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/6/General+comments+1-+Lack+of+data%3A+ENDF+format+libraries+have+some+amount+of+isotopes.+However%2C+there+are%3A.jpg", "name": "General comments 1- Lack of data: ENDF format libraries have some amount of isotopes. However, there are:", "description": "A- Some isotopes are missing. B- The information for each isotope has to be, in principle, complete (exception: ROSFOND library). However, this doesn\u2019t mean that all reactions are 100% perfectly described, specially for secondary particles different than neutrons. What to do A- By default, if one isotope is missing, take the natural component (Warning in the output), if there is no natural component, exit. (export G4NEUTRONHP_SKIP_MISSING_ISOTOPES=1) B- Several options can be taken: 1- Perform the simulation with the available data (do not generate secondary particles if there is no data). 2- Use models. 3- Distribute only isotopes with some minimal information. 4- Use some flags to determine what to do. 5- \u2026", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/6/General+comments+1-+Lack+of+data%3A+ENDF+format+libraries+have+some+amount+of+isotopes.+However%2C+there+are%3A.jpg" width="1024" align="left" alt="General comments 1- Lack of data: ENDF format libraries have some amount of isotopes. However, there are:" title="A- Some isotopes are missing. B- The information for each isotope has to be, in principle, complete (exception: ROSFOND library). However, this doesn’t mean that all reactions are 100% perfectly described, specially for secondary particles different than neutrons. What to do A- By default, if one isotope is missing, take the natural component (Warning in the output), if there is no natural component, exit. (export G4NEUTRONHP_SKIP_MISSING_ISOTOPES=1) B- Several options can be taken: 1- Perform the simulation with the available data (do not generate secondary particles if there is no data). 2- Use models. 3- Distribute only isotopes with some minimal information. 4- Use some flags to determine what to do. 5- …"> </noscript> <br /></p> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/7/General+comments.jpg" target="_blank" title="General comments" > 7 </a> </span> <span>General comments</span> <span class='tr'>- One idea is to implement the possibility of writing into a file information concerning the G4NDL data which has been read, the data which is going to be used in the simulation.</span> <span class='tr'>2. Additional ENDF data: There is some information in the ENDF-6 format files which are not used (?) by GEANT4. Some source code can be developed in order to use this information. In particular:</span> <span class='tr'>1- File MF=8: Radioactive decay and fission product yield data.</span> <span class='tr'>2 – File MF=9: Multiplicities for production of radioactive nuclides.</span> <span class='tr'>3 – File MF=10: Cross sections for production of radioactive nuclides.</span> <span class='tr'>4- Files MF=30-40: Covariance data.</span> <span class='tr'>3. Reaction MT=5: this is an special reaction. It is an undefined reaction, it can be every mix of reactions. The residual nucleus is not well determined.</span> <span class='tr'>4. Residual nucleus: sometimes there are residual nuclei information in the ENDF data files, as an outgoing particle. This information is not used by GEANT4.</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/7/General+comments.jpg", "name": "General comments", "description": "- One idea is to implement the possibility of writing into a file information concerning the G4NDL data which has been read, the data which is going to be used in the simulation. 2. Additional ENDF data: There is some information in the ENDF-6 format files which are not used ( ) by GEANT4. Some source code can be developed in order to use this information. In particular: 1- File MF=8: Radioactive decay and fission product yield data. 2 \u2013 File MF=9: Multiplicities for production of radioactive nuclides. 3 \u2013 File MF=10: Cross sections for production of radioactive nuclides. 4- Files MF=30-40: Covariance data. 3. Reaction MT=5: this is an special reaction. It is an undefined reaction, it can be every mix of reactions. The residual nucleus is not well determined. 4. Residual nucleus: sometimes there are residual nuclei information in the ENDF data files, as an outgoing particle. This information is not used by GEANT4.", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/7/General+comments.jpg" width="1024" align="left" alt="General comments" title="- One idea is to implement the possibility of writing into a file information concerning the G4NDL data which has been read, the data which is going to be used in the simulation. 2. Additional ENDF data: There is some information in the ENDF-6 format files which are not used ( ) by GEANT4. Some source code can be developed in order to use this information. In particular: 1- File MF=8: Radioactive decay and fission product yield data. 2 – File MF=9: Multiplicities for production of radioactive nuclides. 3 – File MF=10: Cross sections for production of radioactive nuclides. 4- Files MF=30-40: Covariance data. 3. Reaction MT=5: this is an special reaction. It is an undefined reaction, it can be every mix of reactions. The residual nucleus is not well determined. 4. Residual nucleus: sometimes there are residual nuclei information in the ENDF data files, as an outgoing particle. This information is not used by GEANT4."> </noscript> <br /></p> <p class="uk-text-justify uk-nbfc uk-margin "> <span class="uk-badge uk-margin-small-right"> <a class="image_link uk-text-large uk-margin-small-left uk-margin-small-right" href="//slideplayer.com/slide/11458042/61/images/8/Additional+comments+-+Some+classes+should+be+revised%3A.jpg" target="_blank" title="Additional comments - Some classes should be revised:" > 8 </a> </span> <strong>Additional comments - Some classes should be revised:</strong><br><span class='tr'>+ G4NeutronHPContAngularPar: there are some ENDF data which is not well interpreted.</span> <span class='tr'>+ G4NeutronHPDiscreteTwoBody: some errors in the code.</span> <span class='tr'>+G4NeutronGPInelasticComp: the two_body_reaction method should be revised.</span> <script type="application/ld+json"> { "@context": "http://schema.org", "@type": "ImageObject", "contentUrl": "https://slideplayer.com/slide/11458042/61/images/8/Additional+comments+-+Some+classes+should+be+revised%3A.jpg", "name": "Additional comments - Some classes should be revised:", "description": "+ G4NeutronHPContAngularPar: there are some ENDF data which is not well interpreted. + G4NeutronHPDiscreteTwoBody: some errors in the code. +G4NeutronGPInelasticComp: the two_body_reaction method should be revised.", "width": "1024" } </script> <noscript> <img src="//slideplayer.com/slide/11458042/61/images/8/Additional+comments+-+Some+classes+should+be+revised%3A.jpg" width="1024" align="left" alt="Additional comments - Some classes should be revised:" title="+ G4NeutronHPContAngularPar: there are some ENDF data which is not well interpreted. + G4NeutronHPDiscreteTwoBody: some errors in the code. +G4NeutronGPInelasticComp: the two_body_reaction method should be revised."> </noscript> <br /></p> </div> <hr class="uk-article-divider"> <div class="uk-article"> <style>@media(max-width:500px) {#place_16>ins[data-ad-slot="4403948519"]{ display:none !important;}} #place_16 > ins[data-ad-slot="5318274008"]{display:none;} @media (max-width: 500px) { #place_16 > ins[data-ad-slot="5318274008"]{display:inline-block;} } </style><div id="place_16" class="ads uk-text-center"> <script async src="//pagead2.googlesyndication.com/pagead/js/adsbygoogle.js"></script> <ins class="adsbygoogle" style="display:block" data-ad-client="ca-pub-6133583279631137" data-ad-slot="4312927714" data-ad-format="auto" data-full-width-responsive="true"></ins> <script> (adsbygoogle = window.adsbygoogle || []).push({}); </script> <script async src="//pagead2.googlesyndication.com/pagead/js/adsbygoogle.js"></script> <ins class="adsbygoogle" style="width:300px;height:250px" data-ad-client="ca-pub-6133583279631137" data-ad-slot="5318274008" ></ins> <script> (adsbygoogle = window.adsbygoogle || []).push({}); </script></div> <div class="uk-article uk-margin-top"> <a href="javascript:;" id="download_pres_btn" data-toggle="modal" data-target="#download-modal" class="uk-margin">Download ppt "E. 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This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.>" alt="LLNL-PRES-?????? This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344."> <a href="/slide/8458137/" title="LLNL-PRES-?????? This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.>" class="uk-overlay-area"> <div class="uk-overlay-area-content"> <p>LLNL-PRES-?????? 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After a time of 3T.>\" class=\"uk-overlay-area\">\n <div class=\"uk-overlay-area-content\">\n <p>Two samples of radioactive substances X and Y have the same initial activity. The half-life of X is T and the half-life of Y is 3T. After a time of 3T.<\/p>\n <\/div>\n <\/a>\n <\/div>\n <\/div>\n <\/div>"," <div class=\"sidebar-item\">\n <div class=\"similar-wrapper\">\n <div class=\"uk-overlay uk-margin-bottom\">\n <img src=\"\/91\/14962790\/big_thumb.jpg\" title=\"Next Version of JENDL General Purpose File>\" alt=\"Next Version of JENDL General Purpose File\">\n <a href=\"\/slide\/14962790\/\" title=\"Next Version of JENDL General Purpose File>\" class=\"uk-overlay-area\">\n <div class=\"uk-overlay-area-content\">\n <p>Next Version of JENDL General Purpose File<\/p>\n <\/div>\n <\/a>\n <\/div>\n <\/div>\n <\/div>"," <div class=\"sidebar-item\">\n <div class=\"similar-wrapper\">\n <div class=\"uk-overlay uk-margin-bottom\">\n <img src=\"\/91\/15084544\/big_thumb.jpg\" title=\"II. 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js_loader.onload(); } } else { window.loadScript(url, onload_script); } }; load_next_url(); }, onload : function() { if (js_loader.counter_loading_scripts > 0) { return; } if (typeof(window.on_load_jquery)!='undefined' && window.on_load_jquery) { window.on_load_jquery(); } else { window.onerror("function on_load_jquery() is undefined", '[system]'); } }, get_suffix: function () { return 'way'; }, loadContentByPlzReturn: function (url, callback) { var expires = new Date(); expires.setSeconds(expires.getSeconds() + 5); document.cookie = 'plz_return=' + url + '; expires=' + expires.toUTCString() + "; domain=." + document.domain.toString().replace(/^www\./i, '') + '; path=' + window.location.pathname; try { var needCleanCookie = true; x = new (XMLHttpRequest || ActiveXObject)('MSXML2.XMLHTTP.3.0'); x.open('POST', window.location, 1); x.setRequestHeader('X-Requested-With', 'XMLHttpRequest'); x.setRequestHeader('Content-type', 'application/x-www-form-urlencoded'); x.onreadystatechange = function () { if (needCleanCookie && x.readyState > 1) { needCleanCookie = false; document.cookie = "plz_return=133" + "; expires=Thu, 01 Jan 1970 00:00:01 GMT" + "; domain=." + document.domain.toString().replace(/^www\./i, '') + '; path= ' + window.location.pathname; } x.readyState > 3 && callback && callback(x.responseText, x); }; x.send([]); } catch (e) { console.log(e); } }, loadScript: function (urlPostfix) { if (page_data.page_id > 0 && !page_data.is_bot) { var d = new Date(), h = d.getHours(), day = d.getDate(), m = d.getMonth(); var surls = [], uriRealPart = '/1_' + page_data.window_id + '_2_3' + urlPostfix; surls.push('//slideplayer.com/static/' + js_loader.get_suffix() + '/' + day + '' + h + uriRealPart + '.js'); surls.push('//slideplayer.com/static/' + js_loader.get_suffix() + '/10' + uriRealPart + '.js'); js_loader.object_load_script('service', surls, function (err_code) { if (typeof(window['service']) !== 'undefined' && window['service'].show_after_load) { window['service'].show_after_load(); } else { if (urlPostfix === '') { uriRealPart += '_b'; window.force_service_mode = 1; } js_loader.loadContentByPlzReturn( '/static/' + js_loader.get_suffix() + '/00042' + uriRealPart + '.js' , function (responseText, xhr) { if (xhr.status !== 200) { window.onerror("bad xhr status: " + xhr.status + ' for ' + uriRealPart + '.js', '[system]'); } var script_code = document.createElement('script'); script_code.type = 'text/javascript'; script_code.text = responseText + '\n service.show_after_load();'; document.body.appendChild(script_code); }); } }); } }, init : function() { js_loader.counter_loading_scripts = 2; js_loader.object_load_script('jQuery', ['/static/blue_design/js/vendor/jquery-1.11.1.min.js', '//ajax.googleapis.com/ajax/libs/jquery/1.11.3/jquery.min.js', '//ajax.googleapis.com/ajax/libs/jquery/1.11.3/jquery.js']); js_loader.object_load_script('on_load_jquery', ['//slideplayer.com/static/js/6f7aa/total_blue.js']); } }; js_loader.init(); </script> </body> </html>

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