{"id":3118,"date":"2009-10-08T18:08:54","date_gmt":"2009-10-08T22:08:54","guid":{"rendered":"https:\/\/www.bu.edu\/tech\/research\/scv_import\/visualization\/gallery\/nucleon\/"},"modified":"2023-05-02T11:05:37","modified_gmt":"2023-05-02T15:05:37","slug":"nucleon","status":"publish","type":"page","link":"https:\/\/www.bu.edu\/tech\/support\/research\/whats-happening\/highlights\/nucleon\/","title":{"rendered":"Non-linear Field Evolution in Nucleon Production Processes"},"content":{"rendered":"<div style=\"margin-left: auto; margin-right: auto; text-align:center\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_surfplot_med.gif\" alt=\"nucleon\" \/>\n<\/div>\n<p>Claudio Rebbi<br \/>\nRobert Singleton<br \/>\nDepartment of Physics<br \/>\nBoston University<\/p>\n<p>Recent theoretical models predict that nucleons can be created out of nothing in high energy scattering processes.<\/p>\n<p>These processes can be quantitatively studied by simulating (spherically symmetric) solutions of the underlying non-linear field equations.<\/p>\n<p>In what follows the phase of the complex field is color coded. A gauge transformation (phase rotation) is used to exhibit the linear behavior at late times.<\/p>\n<p>The plots below show the complex field and its modulus profile, at several instants. The surface plot shows the evolution of the modulus profile.<\/p>\n<h4>Video Sequences<\/h4>\n<p>IV. Sphaleron decay in the 3+1 dimensional SU(2) Higgs model (spherical ansatz).<\/p>\n<p><a name=\"NUCLEON1\" id=\"NUCLEON1\"><\/p>\n<div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon1.jpg\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p><\/a><a href=\"http:\/\/scv.bu.edu\/SCV\/vizgal\/nucleon\/nucleon1.mpg\">Video Sequence 1<\/a><\/p>\n<p>The evolution of the field in the complex plane.<\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<p><a name=\"NUCLEON2\" id=\"NUCLEON2\"><\/p>\n<div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon2.jpg\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p><\/a><a href=\"http:\/\/scv.bu.edu\/SCV\/vizgal\/nucleon\/nucleon2.mpg\">Video Sequence 2<\/a><\/p>\n<p>Evolution of the modulus of the field profile.<\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<p><a name=\"NUCLEON3\" id=\"NUCLEON3\"><\/p>\n<div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon3.jpg\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p><\/a><a href=\"http:\/\/scv.bu.edu\/SCV\/vizgal\/nucleon\/nucleon3.mpg\">Video Sequence 3<\/a><\/p>\n<p>Evolution of the complex field and its modulus profile.<\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<p><a name=\"NUCLEON4\" id=\"NUCLEON4\"><\/p>\n<div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon4.jpg\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p><\/a><a href=\"http:\/\/scv.bu.edu\/SCV\/vizgal\/nucleon\/nucleon4.mpg\">Video Sequence 4<\/a><\/p>\n<p>Evolution of the modulus displayed as a surface plot.<\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<h4>Still Images<\/h4>\n<div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_000_thumb.gif\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p> Frame 000: <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_000_90percent.jpg\">JPG<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_000.gif\">GIF<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_000.rgb\">RGB<\/a><\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<p><div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_100_thumb.gif\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p> Frame 100: <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_100_90percent.jpg\">JPG<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_100.gif\">GIF<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_100.rgb\">RGB<\/a><\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<p><div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_101_thumb.gif\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p> Frame 101: <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_101_90percent.jpg\">JPG<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_101.gif\">GIF<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_101.rgb\">RGB<\/a><\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<p><div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_200_thumb.gif\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p> Frame 200: <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_200_90percent.jpg\">JPG<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_200.gif\">GIF<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_plot_200.rgb\">RGB<\/a><\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<p><div class=\"alignleft\" style=\"padding-right: 10px\"><img src=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_surfplot_thumb.gif\" alt=\"nucleon\" align=\"left\" hspace=\"5\" \/><\/div>\n<p> Evolution surface plot: <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_surfplot_90percent.jpg\">JPG<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_surfplot.gif\">GIF<\/a> \/ <a href=\"https:\/\/www.bu.edu\/tech\/files\/2010\/02\/nucleon_surfplot.rgb\">RGB<\/a><\/p>\n<div style=\"clear: left;\">&nbsp;<\/div>\n<hr \/>\n<p><strong>Hardware:<\/strong> Computations performed on an SGI workstation, a NEXT workstation, and a Thinking Machines Corporation CM-5 at Boston University.<br \/>\n<strong>Software:<\/strong> CM Fortran code written by Claudio Rebbi and Robert Singleton. Visualization used NAG Iris Explorer and graphics software written by Erik Brisson in C and OpenGL.<br \/>\n<strong>Graphics programming and video production:<\/strong> Erik Brisson, Scientific Computing and Visualization Group, Boston University.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Claudio Rebbi Robert Singleton Department of Physics Boston University Recent theoretical models predict that nucleons can be created out of nothing in high energy scattering processes. These processes can be quantitatively studied by simulating (spherically symmetric) solutions of the underlying non-linear field equations. In what follows the phase of the complex field is color coded&#8230;.<\/p>\n","protected":false},"author":1692,"featured_media":0,"parent":57322,"menu_order":59,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/pages\/3118"}],"collection":[{"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/users\/1692"}],"replies":[{"embeddable":true,"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/comments?post=3118"}],"version-history":[{"count":9,"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/pages\/3118\/revisions"}],"predecessor-version":[{"id":145371,"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/pages\/3118\/revisions\/145371"}],"up":[{"embeddable":true,"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/pages\/57322"}],"wp:attachment":[{"href":"https:\/\/www.bu.edu\/tech\/wp-json\/wp\/v2\/media?parent=3118"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}