{"id":1373,"date":"2024-05-13T08:35:08","date_gmt":"2024-05-13T06:35:08","guid":{"rendered":"https:\/\/fizyka.ujk.edu.pl\/?p=1373"},"modified":"2024-05-13T08:35:08","modified_gmt":"2024-05-13T06:35:08","slug":"intermittency-in-cosmic-ray-showers-and-its-possible-consequences","status":"publish","type":"post","link":"https:\/\/fizyka.ujk.edu.pl\/index.php\/2024\/05\/13\/intermittency-in-cosmic-ray-showers-and-its-possible-consequences\/","title":{"rendered":"Intermittency in cosmic ray showers and its possible consequences"},"content":{"rendered":"<p>15 maja 2024 roku o godzinie 13:15 w sali 143 odb\u0119dzie si\u0119 seminarium Instytutu Fizyki, na kt\u00f3rym<br \/>\nProf. Tadeusz Wibig  z Wydzia\u0142u Fizyki i Informatyki Stosowanej Uniwersytetu \u0141\u00f3dzkiego<br \/>\nwyg\u0142osi referat pt.: \u201eIntermittency in cosmic ray showers and its possible consequences\u201d.<\/p>\n<p>Abstract:<br \/>\nIn the simulation calculations that form the basis for interpreting data<br \/>\nfrom EAS arrays at higher primary particle energies, we are dealing<br \/>\nwith millions of particles passing through the atmosphere.<br \/>\nIn order to speed up the calculations or to make them generally feasible,<br \/>\nthe 'thinning&#8217; method has been used for about half a century.<br \/>\nThis method consists in eliminating a fraction of the particles<br \/>\nfrom the cascade and in assigning an appropriate statistical weight<br \/>\nto the remaining particles. Such an approach is perfectly correct<br \/>\nif we are dealing with average images of showers, but it cannot describe<br \/>\nthe fluctuations in the number of particles measured by any particular<br \/>\nsingle detector. The standard approach is to assume that the particles<br \/>\nin a shower reach the ground independently. Their numbers are assumed<br \/>\nto fluctuate poissonically. This approximation does not allow a correct<br \/>\ninterpretation of the results of measurements of very small showers.<br \/>\nIt is also not entirely correct at higher energies, especially in detectors<br \/>\nfar from the shower axis where particle densities are low.<br \/>\nThe question is whether the assumption that the particles in the shower<br \/>\nare independent leads to systematic biases in the interpretation of<br \/>\nthe shower data.<br \/>\nUsing accurate simulations, we found the magnitude of the particle correlations<br \/>\nand showed that a negative binomial distribution better describes<br \/>\nthese distributions.<br \/>\nBy modifying the procedures for determining shower parameters, we have shown<br \/>\nthat changing the multiplicity statistics can change the estimated<br \/>\nshower sizes by up to a few percent.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>15 maja 2024 roku o godzinie 13:15 w sali 143 odb\u0119dzie si\u0119 seminarium Instytutu Fizyki, na kt\u00f3rym Prof. Tadeusz Wibig z Wydzia\u0142u Fizyki i Informatyki Stosowanej Uniwersytetu \u0141\u00f3dzkiego wyg\u0142osi referat pt.: \u201eIntermittency in cosmic ray showers and its possible consequences\u201d. Abstract: In the simulation calculations that form the basis for interpreting data from EAS arrays [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[14],"tags":[],"class_list":["post-1373","post","type-post","status-publish","format-standard","hentry","category-seminaria"],"_links":{"self":[{"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts\/1373","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/comments?post=1373"}],"version-history":[{"count":1,"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts\/1373\/revisions"}],"predecessor-version":[{"id":1374,"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts\/1373\/revisions\/1374"}],"wp:attachment":[{"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/media?parent=1373"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/categories?post=1373"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/fizyka.ujk.edu.pl\/index.php\/wp-json\/wp\/v2\/tags?post=1373"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}