{"id":1654,"date":"2024-07-15T14:26:10","date_gmt":"2024-07-15T12:26:10","guid":{"rendered":"http:\/\/brera.inaf.it\/?post_type=tesi&#038;p=1654"},"modified":"2025-05-23T17:30:48","modified_gmt":"2025-05-23T15:30:48","slug":"gamma-ray-bursts-characterizing-the-non-thermal-shock-accelerated-electron-population-through-gamma-ray-burst-prompt-emission-spectra-bachelor-merate-lc","status":"publish","type":"tesi","link":"https:\/\/brera.inaf.it\/en\/tesi\/gamma-ray-bursts-characterizing-the-non-thermal-shock-accelerated-electron-population-through-gamma-ray-burst-prompt-emission-spectra-bachelor-merate-lc\/","title":{"rendered":"\u00a0Gamma Ray Bursts &#8211; Bachelor &#8211; MERATE (LC) &#8211; Characterizing the non-thermal shock accelerated electron population through Gamma Ray Burst prompt emission spectra &#8211; Ghirlanda, Nava, Salafia."},"content":{"rendered":"\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-995f960e wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"750\" height=\"522\" src=\"http:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png\" alt=\"\" class=\"wp-image-1616\"\/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h5 class=\"wp-block-heading\"><span style=\"color: #cf2e2e;\" class=\"stk-highlight\">Gamma Ray Bursts<\/span><\/h5>\n\n\n\n<h5 class=\"wp-block-heading\">Bachelor<\/h5>\n\n\n\n<h5 class=\"wp-block-heading\">Site: Merate (LC)<\/h5>\n\n\n\n<h5 class=\"wp-block-heading\">Duration<\/h5>\n\n\n\n<p class=\"wp-block-paragraph\">3 mesi<\/p>\n\n\n\n<h5 class=\"wp-block-heading\">Tutor<\/h5>\n\n\n\n<p class=\"wp-block-paragraph\">&nbsp;Ghirlanda Giancarlo,&nbsp;Nava Lara, Om Sharan Salafia<\/p>\n\n\n\n<h5 class=\"wp-block-heading\">Contact<\/h5>\n\n\n\n<p class=\"wp-block-paragraph\">giancarlo.ghirlandaAT inaf.it<br>lara.nava AT inaf.it<br>om.salafia AT inaf.it<\/p>\n\n\n\n<h5 class=\"wp-block-heading\">Description<\/h5>\n\n\n\n<div class=\"wp-block-group is-layout-constrained wp-block-group-is-layout-constrained\">\n<p class=\"wp-block-paragraph\"><strong>Background<\/strong>: Gamma Ray Bursts (GRBs) signpost the&nbsp;<strong>death<\/strong>&nbsp;of very massive isolated stars or the merger of binary compact objects (hosting at least a neutron star).<br>They are produced by the formation of a&nbsp;<strong>stellar mass black hole<\/strong>&nbsp;&#8211; accretion disk system which powers bipolar relativistic jets.<br>GRBs are the most luminous&nbsp;<strong>transient sources<\/strong>&nbsp;in the universe and are currently detected up to redshift 9.2.<br>One of the still&nbsp;<strong>open questions<\/strong>&nbsp;is what is the&nbsp;<strong>emission mechanism<\/strong>&nbsp;which makes them appear as short flashes of high energy (0.01-1 MeV) radiation.<br>The leading scenario is&nbsp;<strong>synchrotron radiation<\/strong>&nbsp;by relativistic electrons within their jets.<br>The&nbsp;<strong>observed spectrum<\/strong>&nbsp;should then bear characteristic signatures of this emission. In particular the powerlaw spectral index of the spectrum, above the SED peak, is directly related to the electron non-thermal electron energy distribution.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Scope of the thesis<\/strong>: dig into the publicly available GRB spectral catalogs and select a sample of GRBs with well measured high energy spectral index and calculate the slope of the electron energy distribution. Verify if there is any correlation of this physical parameter with other spectral\/temporal features obtainable from the public catalogs. Discuss the results in the context of current models and simulations (available in the literature) of electron acceleration at mildly relativistic highly magnetized shocks, i.e. those expected to develop within the GRB jet and responsible for the gamma ray emission we see.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Skills<\/strong>: basic theory of shock acceleration and synchrotron emission. Database query and visualization through TOPCAT. Study of the relevant literature.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">[<em>Credit image: Wikipedia<\/em>]\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Gamma Ray Bursts Bachelor Site: Merate (LC) Duration 3 mesi Tutor &nbsp;Ghirlanda Giancarlo,&nbsp;Nava Lara, Om Sharan Salafia Contact giancarlo.ghirlandaAT inaf.itlara.nava AT inaf.itom.salafia AT inaf.it Description Background: Gamma Ray Bursts (GRBs) signpost the&nbsp;death&nbsp;of very massive isolated stars or the merger of binary compact objects (hosting at least a neutron star).They are produced by the formation of [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":1617,"parent":0,"menu_order":0,"comment_status":"open","ping_status":"closed","template":"","format":"standard","meta":{"footnotes":""},"categories":[29,26],"tags":[253,129,254,130],"class_list":["post-1654","tesi","type-tesi","status-publish","format-standard","has-post-thumbnail","hentry","category-bachelor-thesis","category-thesis","tag-gamma-ray-burst-en","tag-giancarlo-ghirlanda-en","tag-nava-lara-en","tag-om-sharan-salafia-en"],"blocksy_meta":[],"featured_image_urls":{"full":["https:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png",750,522,false],"thumbnail":["https:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png",150,104,false],"medium":["https:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png",300,209,false],"medium_large":["https:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png",750,522,false],"large":["https:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png",750,522,false],"1536x1536":["https:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png",750,522,false],"2048x2048":["https:\/\/brera.inaf.it\/wp-content\/uploads\/2024\/07\/copertina-tesi-triennale-magistrale-campana1.png",750,522,false]},"post_excerpt_stackable":"<p>Gamma Ray Bursts Bachelor Site: Merate (LC) Duration 3 mesi Tutor &nbsp;Ghirlanda Giancarlo,&nbsp;Nava Lara, Om Sharan Salafia Contact giancarlo.ghirlandaAT inaf.itlara.nava AT inaf.itom.salafia AT inaf.it Description Background: Gamma Ray Bursts (GRBs) signpost the&nbsp;death&nbsp;of very massive isolated stars or the merger of binary compact objects (hosting at least a neutron star).They are produced by the formation of a&nbsp;stellar mass black hole&nbsp;&#8211; accretion disk system which powers bipolar relativistic jets.GRBs are the most luminous&nbsp;transient sources&nbsp;in the universe and are currently detected up to redshift 9.2.One of the still&nbsp;open questions&nbsp;is what is the&nbsp;emission mechanism&nbsp;which makes them appear as short flashes of high energy (0.01-1&hellip;<\/p>\n","category_list":"<a href=\"https:\/\/brera.inaf.it\/en\/category\/thesis\/bachelor-thesis\/\" rel=\"category tag\">Bachelor thesis<\/a>, <a href=\"https:\/\/brera.inaf.it\/en\/category\/thesis\/\" rel=\"category tag\">Thesis<\/a>","author_info":{"name":"Maria Rosa Panzera","url":"https:\/\/brera.inaf.it\/en\/author\/maria-rosa-panzera\/"},"comments_num":"0 comments","_links":{"self":[{"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/tesi\/1654","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/tesi"}],"about":[{"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/types\/tesi"}],"author":[{"embeddable":true,"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/comments?post=1654"}],"version-history":[{"count":9,"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/tesi\/1654\/revisions"}],"predecessor-version":[{"id":6737,"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/tesi\/1654\/revisions\/6737"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/media\/1617"}],"wp:attachment":[{"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/media?parent=1654"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/categories?post=1654"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/brera.inaf.it\/en\/wp-json\/wp\/v2\/tags?post=1654"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}